Abstracts (PDF) - Sodankylä Geophysical Observatory
Abstracts (PDF) - Sodankylä Geophysical Observatory
Abstracts (PDF) - Sodankylä Geophysical Observatory
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports<br />
No. 60<br />
38th Annual European Meeting on Atmospheric Studies by Optical<br />
Methods<br />
Siuntio, Finland, 22–26 August 2011<br />
Abstract book<br />
Carl-Fredrik Enell, editor<br />
17th August 2011
38th Annual European Meeting on Atmospheric Studies by Optical Methods
4<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
38th Annual European Meeting on Atmospheric Studies by Optical Methods<br />
Siuntio, Finland, 22–26 August 2011<br />
Abstract book
6<br />
Carl-Fredrik Enell (ed.)<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
c○ University of Oulu, <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> 2011<br />
ISSN: 0359-3657<br />
ISBN: 978-951-42-9494-5 (<strong>PDF</strong>)<br />
University of Oulu, <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong><br />
Tähteläntie 62, FIN-99600 <strong>Sodankylä</strong>, Finland<br />
Typeset by the editor in L A TEX<br />
Cover photo c○ Carl-Fredrik Enell 2008<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
7<br />
38th Annual European Meeting on<br />
Atmospheric Studies by Optical Methods<br />
Optical methods have been used for studies of the atmosphere for centuries. A wealth of information about the<br />
whole atmosphere, from the troposphere to the thermosphere, can be obtained by active or passive optical measurements.<br />
Recent technological developments have also opened up a panorama of new possibilities for high-resolution<br />
measurements and measurements coordinated with other types of instruments. The Annual European Meetings on<br />
Atmospheric Studies by Optical Methods bring together scientists from Europe as well as from other parts of the<br />
world to exchange experience, share scientific results, and plan and coordinate future experiments.<br />
We have the honour and pleasure to organise the 38th meeting in the series at Siuntio Spa, Finland, during<br />
August 22–26 2011.<br />
Scientific Programme Committee<br />
Kirsti Kauristie (chair), Finnish Meteorological Institute, Helsinki, Finland<br />
Anita Aikio, University of Oulu, Finland<br />
Kari Kaila, University of Oulu, Finland<br />
Erkki Kyrölä, Finnish Meteorological Institute, Helsinki, Finland<br />
Robert Lowe, University of Western Ontario, London, Ontario, Canada<br />
Tom McElroy, Environment Canada, Canada<br />
Vladimir Safargaleev, Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
Georg Witt, Stockholm University, Sweden<br />
Local Organisation Committee<br />
Noora Partamies (chair), Finnish Meteorological Institute, Helsinki, Finland<br />
Carl-Fredrik Enell (co-chair, webmaster), <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong>, University of Oulu, <strong>Sodankylä</strong>,<br />
Finland<br />
Kirsi Kari (secr.), Finnish Meteorological Institute, Helsinki, Finland<br />
Kari Kaila, University of Oulu, Finland<br />
Laureline Sangalli, Royal Military College, Kingston, Ontario, Canada<br />
Thomas Ulich, <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong>, University of Oulu, <strong>Sodankylä</strong>, Finland<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
8<br />
In memoriam: Ingrid Sandahl, 1949–2011<br />
The meeting is dedicated to the memory of Professor Ingrid Sandahl, who was an active member of the optical<br />
auroral research community, and sadly passed away during the preparations for the meeting.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
9<br />
Contents<br />
38th Annual European Meeting on Atmospheric Studies by Optical Methods 7<br />
Contents 9<br />
Sponsors 13<br />
List of optical meetings 14<br />
Programme 15<br />
Posters 16<br />
Social programme 17<br />
<strong>Abstracts</strong> 19<br />
Aerosols in the atmosphere . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21<br />
Aaltonen, Veijo; Rodriguez, Edith; Mielonen, Tero; Sogacheva, Larisa; Lihavainen, Heikki;<br />
Aalto, Pasi; Arola, Antti; de Leeuw, Gerrit: Effects of the Russian forest fires over<br />
Finland in summer 2010. Poster presentation . . . . . . . . . . . . . . . . . . . . . . 23<br />
Cachorro, Victoria; Toledano, Carlos; Gausa, Michael; Stebel, Kerstin; Aaltonen, Veijo;<br />
Berjón, Alberto; Ortiz de Galisteo, J. Pablo; Bennouna, Yasmine; Blindheim, Sandra;<br />
de Frutos, Angel M.; Myhre, Cathrine Lund; Zibordi, Giuseppe; Wehrli, Christoph;<br />
Kratzer, Sussane; Håkansson, Bertil; Carlund, Thomas; de Leeuw, Gerrit; Herber,<br />
Andreas; Torres, Benjamin: Characterization of columnar atmospheric aerosols:<br />
Special focus in Scandinavian area. Oral presentation . . . . . . . . . . . . . . . . . 24<br />
Kannel, Martin; Ohvril, Hanno; Okulov, Oleg: A shortcut from broadband to spectral<br />
aerosol optical depth. Poster presentation . . . . . . . . . . . . . . . . . . . . . . . . 25<br />
Hannukainen, Meri; Rodriguez, Edith; Sofiev, Michael; Kolmonen, Pekka; Sundström, Anu-<br />
Maija; Sogacheva, Larisa; de Leeuw, Gerrit: Megacities inventory base on optical<br />
properties, using satellite and SILAM model results. Poster presentation . . . . . . 26<br />
Ionosphere, mesosphere and lower thermosphere . . . . . . . . . . . . . . . . . . . . . . . . . . . 27<br />
Nikolaishvili, Sergey; Belyaev, Alexey: An enhancement of the airglow brightness by the<br />
gravity waves. Poster presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29<br />
Chernouss, Sergey; Platov, Yuly; Alpatov, Victor; Uspensky, Mikhail: Optical signatures<br />
of rocket exhaust phenomena in Arctic atmosphere. Oral presentation . . . . . . . . 30<br />
Dyrland, Margit Elisabet; Sigernes, Fred: Using Airglow observations in high-latitude<br />
climate studies. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31<br />
Enell, Carl-Fredrik; Gustavsson, Björn; Sergienko, Tima; Verronen, Pekka. T; Hedin, Jonas;<br />
Witt, Georg; Brändström, Urban; Rydesäter, Peter: Subsidence of thermospheric<br />
air observed by the Hotel Payload 2 measurements on January 31, 2008. Oral presentation<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 32<br />
Hoppe, Ulf-Peter: What can we learn about upper mesosphere dynamics by four-dimensional<br />
lidar measurements?. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . 33<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
10<br />
Lorentzen, D.A.; Johnsen, M.G.: The dayside open closed field line boundary - a statistical<br />
study using ground-based optics. Oral presentation . . . . . . . . . . . . . . . . . . 34<br />
McCarthy, Dean; Mulligan, Frank; Mooney, Priscilla: Implementing a chemical scheme for<br />
OH* in the University College London CMAT2 3D Global Model. Oral presentation 35<br />
Medvedeva, Irina; Chernigovskaya, Marina; Perminov, Vladimir; Semenov, Anatoly: Study<br />
on the impact of sudden stratospheric warmings in mid-latitude MLT region according<br />
to ground-based and satellite temperature measurements. Oral presentation . . 36<br />
Mulligan, Frank J.; Lowe, Robert P.: Gravity wave characteristics measured in Ireland by<br />
UWOSCR during the 2010-2011 NDMC campaign. Oral presentation . . . . . . . . 37<br />
Semenov, Anatoly: Longitudinal variations of the atmospheric temperature at altitudes of<br />
lower thermosphere on the characteristics of the 557.7 nm atomic oxygen emission.<br />
Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38<br />
Taylor, Michael; Zhao, Yucheng; Pautet, Pierre-Dominique; Pendleton Jr., William: How<br />
to Use Airglow Measurements in Atmospheric Wave Activity Studies. Oral presentation<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39<br />
Aurora . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41<br />
Aikio, Anita: Nighttime auroras for remote sensing of magnetospheric processes. Oral<br />
presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43<br />
Andalsvik, Yngvild Linnea; Sandholt, Per Even; Farrugia, Charles J. : Ground - satellite<br />
observations of dynamics of the magnetosphere - ionosphere system during the<br />
Superstorm on Nov. 20, 2003. Poster presentation . . . . . . . . . . . . . . . . . . . 44<br />
Axelsson, Katarina; Sergienko, Tima; Brändström, Urban: Statistical study of temporal<br />
and spatial variations in diffuse aurora. Oral presentation . . . . . . . . . . . . . . . 45<br />
Belakhovsky, Vladimir; Kozlovsky, Alexander; Pilipenko, Slava: The morning auroral arcs<br />
associated with Pc5 geomagnetic pulsations. Poster presentation . . . . . . . . . . . 46<br />
Chernouss, Sergey: Ideas of Lomonosov in field of auroral research. Oral presentation . . . 47<br />
Dahlgren, Hanna: On small-scale aurora. Oral presentation . . . . . . . . . . . . . . . . . 48<br />
Donovan, Eric: The Magnetospheric Drivers of Aurora. Oral presentation . . . . . . . . . 49<br />
Gustavsson, Björn; Tuttle, Sam; Dahlgren, Hanna; Lanchester, Betty; Ivchenko, Nickolay:<br />
Optical Measurements of F-region Ion-Convection. Oral presentation . . . . . . . . 50<br />
Gustavsson, Björn; Dahlgren, Hanna; Lanchester, Betty; Ivchenko, Nickolay: On Filamentation<br />
and Anti-Filamentation of Auroral Arcs . Oral presentation . . . . . . . . . . 51<br />
Vorobjev, V. G.; Yagodkina, O. I. ; Katkalov, Yu. V.; Kirillov, A. S.: Planetary distribution<br />
of auroral luminosity inferred from APM. Oral presentation . . . . . . . . . . . . . 52<br />
Kauristie, Kirsti; Kleimenova, Nataly ; Kozyreva, Olga; Uspensky, Mikhail; Vlasov, Alexey:<br />
A case study about the connection of optical auroral activity and geomagnetic Pc5<br />
pulsations. Poster presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 53<br />
Kozelov, Boris; Golovchanskaya, Irina; Mingalev, Oleg: Inverse cascade in the auroral<br />
structure and numerical model of current filaments. Oral presentation . . . . . . . . 54<br />
Kozelov, Boris: Multi-scale auroral observations in Apatity: equipment and preliminary<br />
results. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 55<br />
Partamies, Noora; Kauristie, Kirsti; Ketola, Anneli; Mattanen, Jyrki; Mäkinen, Sanna:<br />
Long-term changes in the auroral occurrence in Finland and Svalbard. Poster presentation<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 56<br />
Partamies, Noora; Sangalli, Laureline; Gustavsson, Björn; Syrjäsuo, Mikko; Donovan, Eric;<br />
Connors, Martin; Charrois, Dan; Kryzanowsky, Zane: On tomography-like reconstruction<br />
from colour auroral images. Oral presentation . . . . . . . . . . . . . . . . 57<br />
Frissell, Nathaniel A.; Reistad, Jone Peter; Partamies, Noora; Lorentzen, Dag: Characteristic<br />
energy in an auroral Spiral. Oral presentation . . . . . . . . . . . . . . . . . . 58<br />
Roldugin, Valentin; Roldugin, Alexey; Pilgaev, Sergey: Pc2 auroral pulsations. Poster<br />
presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59<br />
Sangalli, Laureline; Gustavsson, Björn; Partamies, Noora; Kauristie, Kirsti: Event Study<br />
of the Peak Auroral Emission Altitude from All-sky Images. Oral presentation . . . 60<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
11<br />
Sergienko, Tima; Axelsson, Katarina; Gustavsson, Björn; Sandahl, Ingrid; Brändström, Urban:<br />
Multi-station optical study of substorm breakup auroral arcs. Oral presentation<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61<br />
Sigernes, Fred; Dyrland, Margit; Brekke, Pål; Chernouss, Sergey; Lorentzen, Dag Arne;<br />
Oksavik, Kjellmar; Deehr, Charles: Two methods to forecast auroral displays. Oral<br />
presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 62<br />
Simon Wedlund, Cyril; Lamy, Hervé; Barthélemy, Mathieu; Lilensten, Jean; Gronoff, Guillaume;<br />
López Ariste, Arturo; Bommier, Véronique: Polarisation of emission lines in<br />
upper atmospheres of planets. Oral presentation . . . . . . . . . . . . . . . . . . . . 63<br />
Simon Wedlund, Cyril; Lamy, Hervé; Gustavsson, Björn; Sergienko, Tima; Brändström, Urban:<br />
3D reconstruction of N + 2 and OI auroral emissions using the Auroral Large<br />
Imaging System (ALIS). Poster presentation . . . . . . . . . . . . . . . . . . . . . . 64<br />
Whiter, Daniel; Partamies, Noora; Sangalli, Laureline: Statistical study of the peak auroral<br />
emission height using the MIRACLE all-sky camera network. Oral presentation . . 65<br />
Troposphere and stratosphere . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 67<br />
Sofieva, Viktoria: Studying gravity waves and turbulence in the stratosphere using satellite<br />
observations of stellar scintillation. Oral presentation . . . . . . . . . . . . . . . . . 69<br />
Radiation and atmospheric components . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71<br />
Bennouna, Yasmine; Ortiz de Galisteo, Jose Pablo; Cachorro, Victoria; Toledano, Carlos;<br />
Berjón, Alberto; Fuertes, David; Gonzalez, Ramiro; Torres, Benjamin; Marcos,<br />
Jose Luis; Martín, Leticia; de Frutos, Angel Maximo: The annual cycle of precipitable<br />
water vapor over the Iberian Peninsula inferred from MODIS observations<br />
and its comparison with GPS data. Poster presentation . . . . . . . . . . . . . . . . 73<br />
Yankovsky, Valentine; Fedotova, Ekaterina: Theoretical validation of the method of retrieval<br />
of atomic oxygen altitude profile from intensity of the electronic-vibrationally<br />
excited molecule O 2 (b 1 Σ + g , v=2) emission in the MLT. Poster presentation . . . . . 74<br />
Gavrilov, N. M.; Semyonov, V. K.; Sinyakov, V. P.; Tans, P.; Guenther, D.; Kashin, F. V.:<br />
Longterm CO 2 changes in the tropo-stratosphere from in situ and optical measurements.<br />
Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75<br />
Kyrölä, Erkki: GOMOS/ENVISAT overview. Oral presentation . . . . . . . . . . . . . . . 76<br />
Lakkala, Kaisa: Long-term Arctic and Antarctic UV measurements. Oral presentation . . 77<br />
Yankovsky, Valentine; Martishenko, Xenia; Manuilova, Rada: Retrieval of ozone altitude<br />
profile from O 2 (b 1 Σ g , v=0,1) emission intensity in the middle atmosphere. Poster<br />
presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 78<br />
Yagovkina, Irina; Polyakov, Alexander; Timofeyev, Yuri; Walker, Kaley: Comparison of<br />
satellite and ground-based spectroscopic measurements of HF total column amount.<br />
Poster presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 79<br />
Yankovsky, Valentine; Manuilova, Rada; Semenov, Aleksey: Possibility of ozone and atomic<br />
oxygen retrievals from measured intensities of the molecule O 2 (b1Σ+g,v≤ 2) emissions<br />
in the mesosphere and lower thermosphere.. Oral presentation . . . . . . . . . 80<br />
Instrumentation and techniques . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 81<br />
Alpatov, Victor; Belyaev, Alexey: A gravity wave spectrometry from space and ground.<br />
Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 83<br />
Belyaev, Alexey: The central slice theorem for a gravity wave spectrometry. Poster presentation<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 84<br />
Brändström, Urban; Wang, Zilu; Sergienko, Tima; Gustavsson, Björn; Axelsson, Katarina;<br />
Enell, Carl-Fredrik; Mäkinen, Sanna; Sigernes, Fred: Calibrating auroral cameras.<br />
Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 85<br />
Fastig, Shlomo; Ehrlich, Yossi; Pearl, Shaul; Naor, Eran; Kraus, Yaniv; Inbar, Tuvia ;<br />
Katz, David: Multi-spectral LIDAR system — Design, build and test. Poster presentation<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 86<br />
Hildebrand, Jens; Baumgarten, Gerd; Fiedler, Jens; Lübken, Franz-Josef; von Cossart, Götz:<br />
Wind measurements by Doppler lidar. Oral presentation . . . . . . . . . . . . . . . 87<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
12<br />
Polyakov, Alexander; Timofeyev, Yuri; Uspensky, Alexander; Kostsov, Vladimir: Numerical<br />
modeling of sounding of the atmosphere based on combined IR and microwave<br />
measurements on board ”Meteor-3M” satellite. Oral presentation . . . . . . . . . . . 88<br />
Roldugin, Alexey; Chernouss, Sergey; Pilgaev, Sergey; Kuznetsova, Marina; Milichenko, Alexander;<br />
Fedorenko, Yuri: Mobile unit for optical instruments installation at Barentsburg<br />
observatory. . Poster presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 89<br />
Saari, Heikki: Novel MEMS and Piezoactuated Fabry-Perot spectral imagers for atmospheric<br />
studies. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 90<br />
Sigernes, Fred; Ivanov, Yuriy; Chernouss, Sergey; Trondsen, Trond; Roldugin, Alexey;<br />
Fedorenko, Yury; Kozelov, Boris; Kirillov, Andrey; Safargaleev, Vladimir; Dyrland,<br />
Margit; Lorentzen, Dag; Oksavik, Kjellmar: A new auroral hyperspectral<br />
all-sky camera. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 91<br />
Rao, Jayasimha Ramachandra; Syrjäsuo, Mikko: Transferring historical auroral films into<br />
digital format. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 92<br />
Syrjäsuo, Mikko; Hollmén, Jaakko: A review of automated analysis of auroral images —<br />
current status and new prospects. Oral presentation . . . . . . . . . . . . . . . . . . 93<br />
Facilities and experiments . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 95<br />
Aikio, Anita; Ulich, Thomas; Lehtinen, Markku; Turunen, Esa: EISCAT_3D, New generation<br />
Incoherent Scatter Radar to Northern Fennoscandia. Oral presentation . . . . 97<br />
Baddeley, Lisa: SPEAR (Space Plasma Exploration by Active Radar): An ionospheric<br />
heater in the high arctic. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . 98<br />
Dahle, Kolbjørn Blix; Abrahamsen, Trond: Andøya Rocket Range - ”Wind of Change”.<br />
Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 99<br />
NLC and PMC . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 101<br />
Pérot, Kristell; Hauchecorne, Alain; Montmessin, Franck: NLC climatology from GOMOS<br />
observations. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 103<br />
Witt, Georg: Probing the atmosphere with optical methods: Lessons learned and challenges<br />
for the future. Oral presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 104<br />
Author index 105<br />
Registered participants 107<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
13<br />
Sponsors<br />
The 38AM LOC gratefully acknowledges support from<br />
Emil Aaltonen Foundation<br />
http://www.emilaaltonen.fi/brieflyeng.html<br />
Academy of Finland<br />
http://www.aka.fi/en-GB/A<br />
Federation of Finnish Learned Societies<br />
http://www.tsv.fi/engl/<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
14<br />
List of optical meetings<br />
AM No Date Place Country Participants<br />
1 12–13 Nov 1973 Stockholm Sweden 20<br />
2 12–13 Aug 1974 Liège Belgium 10<br />
3 16–18 Oct 1975 Halvorsbøle (Oslo) Norway 41<br />
4 16–18 Aug 1976 Garmisch-Partenkirchen Germany 21<br />
5 26–29 Sep 1977 Granada Spain<br />
6 18–21 Sep 1978 Aberdeen Scotland 42<br />
7 25–28 Jun 1979 Tromsø Norway 38<br />
8 8–11 Sep 1980 Dublin Ireland 26<br />
9 27–30 Oct 1981 Albano Laziale (Rome) Italy few<br />
10 6–11 Sep 1982 Grasse France 26 or more<br />
11 29 Aug–2 Sep 1983 Lindau am Harz Germany 21 or more<br />
12 3–7 Sep 1984 Stockholm Sweden 35<br />
13 19–23 Aug 1985 Oslo Norway<br />
14 17–22 Aug 1986 Cambridge England 48<br />
15 6–11 Sep 1987 Granada Spain 50<br />
16 1988 Oulu Finland few<br />
17 24–29 Sep 1990 Abastumani Georgia 9 or more<br />
18 17–21 Jun 1991 Tromsø Norway 83<br />
19 10–14 Aug 1992 Kiruna Sweden 124<br />
20 13–17 Sep 1993 Apatity Russia<br />
21 12–16 Sep 1994 London England 61 or more<br />
22 28 Aug–1 Sep 1995 Nurmijärvi Finland 69<br />
23 2–6 Sep 1996 Kiev Ukraine 78<br />
24 18–22 Aug 1997 Andenes Norway 54<br />
25 21–25 Sep 1998 Granada Spain 72<br />
26 30 Aug–3 Sep 1999 Lindau am Harz Germany 42<br />
27 21–25 Aug 2000 Stockholm Sweden 51<br />
28 19–24 Aug 2001 Oulu Finland 57<br />
29 3–6 Sep 2002 Kühlungsborn Germany 37<br />
30 13–17 Aug 2003 Longyearbyen Norway 50<br />
31 22–28 Aug 2004 Ambleside (Lake District) England 41<br />
32 29 Aug–1 Sep 2005 London, Ontario Canada 47<br />
33 28 Aug–1 Sep 2006 Kiruna Sweden 67<br />
34 27–31 Aug 2007 Andenes Norway 52<br />
35 24–29 Aug 2008 Maynooth Ireland 63<br />
36 17–22 Aug 2009 Kyiv Ukraine 49<br />
37 23–27 Aug 2010 Valladolid Spain 70<br />
38 22–26 Aug 2011 Siuntio Finland 56 registered<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Programme<br />
Time Monday Tuesday Wednesday Thursday Friday<br />
Chair: Axelsson Chair: Sangalli Chair: Manuilova Chair: Gausa<br />
09:00 Semenov Dahlgren Aikio Donovan<br />
09:10<br />
09:20 Mulligan Baddeley<br />
09:30<br />
09:40 Medvedeva Kozelov<br />
09:50<br />
10:00 Coffee Coffee Coffee Coffee<br />
Chair: Baddeley<br />
10:30 Pérot Simon Wedlund Lakkala Rao<br />
10:40<br />
10:50 Syrjäsuo<br />
11:00 Registration Sofieva Partamies Whiter<br />
11:10 Blix Dahle<br />
11:20 Frissell Sangalli<br />
11:30 Witt<br />
11:40 Vorobjev Kyrölä<br />
11:50<br />
12:00 Lunch Lunch Lunch Lunch Lunch 12:30<br />
Chair: Dyrland<br />
Chair: Whiter<br />
13:00 Welcome McCarthy Excursion Gavrilov<br />
13:10 Chair: Pérot<br />
13:20 Chernouss Lorentzen Yankovsky<br />
13:30 Wrap-up<br />
13:40 Enell Axelsson Hildebrand discussions<br />
13:50<br />
14:00 Cachorro Chernouss Polyakov<br />
14:10<br />
14:20 Gustavsson Alpatov<br />
14:30 Dyrland<br />
14:40 Kozelov Sigernes<br />
14:50<br />
15:00 Coffee Coffee Coffee<br />
Chair: McCarthy<br />
15:30 Hoppe Sigernes Saari<br />
15:40<br />
15:50 Taylor Aikio<br />
16:00 Brändström<br />
16:10<br />
16:20 Posters<br />
16:30<br />
16:40<br />
16:50 Gustavsson<br />
17:00 Excursion ends<br />
17:10 Sergienko<br />
18:00 Icebreaker<br />
19:00 38AM dinner<br />
Contributed (20 min) Invited (30 min) Tutorial (1 h)
16<br />
Posters<br />
Posters can be on display Monday–Thursday and a dedicated poster session will take place on Monday afternoon.<br />
The maximum poster size is A0 (portrait format).<br />
Poster First author<br />
Title<br />
number<br />
1 Aaltonen Effects of the Russian forest fires over Finland in summer<br />
2010<br />
2 Hannukainen Megacities inventory base on optical properties, using<br />
satellite and SILAM model results<br />
3 Kannel A shortcut from broadband to spectral aerosol optical<br />
depth<br />
4 Nikolaishvili An enhancement of the airglow brightness by the gravity<br />
waves<br />
5 Andalsvik Ground - satellite observations of dynamics of the magnetosphere<br />
- ionosphere system during the Superstorm on<br />
Nov. 20, 2003.<br />
6 Belakhovsky The morning auroral arcs associated with Pc5 geomagnetic<br />
pulsations<br />
7 Kauristie A case study about the connection of optical auroral activity<br />
and geomagnetic Pc5 pulsations<br />
8 Partamies Long-term changes in the auroral occurrence in Finland<br />
and Svalbard<br />
9 Roldugin Pc2 auroral pulsations<br />
10 Simon Wedlund 3D reconstruction of N + 2 and OI auroral emissions using<br />
the Auroral Large Imaging System (ALIS)<br />
11 Belyaev The central slice theorem for a gravity wave spectrometry<br />
12 Fastig Multi-spectral LIDAR system — Design, build and test<br />
13 Roldugin Mobile unit for optical instruments installation at Barentsburg<br />
observatory.<br />
14 Bennouna The annual cycle of precipitable water vapor over the<br />
Iberian Peninsula inferred from MODIS observations and<br />
its comparison with GPS data<br />
15 Yagovkina Comparison of satellite and ground-based spectroscopic<br />
measurements of HF total column amount<br />
16 Yankovsky Theoretical validation of the method of retrieval of atomic<br />
oxygen altitude profile from intensity of the electronicvibrationally<br />
excited molecule O 2 (b 1 Σ + g , v=2) emission in<br />
the MLT.<br />
17 Yankovsky Retrieval of ozone altitude profile from O 2 (b 1 Σ g , v=0,1)<br />
emission intensity in the middle atmosphere<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
17<br />
Social programme<br />
Monday Icebreaker party 18:00. Outdoor barbecue if weather allows, otherwise in the poster area. Price for<br />
accompanying persons: 30 EUR.<br />
Wednesday Excursion to Porkkala. Bus(es) leave from the spa at 13:00 and we will return at 17:00. Price for<br />
accompanying persons: 35 EUR.<br />
Thursday Conference dinner at Lepopirtti 19:00. Price for accompanying persons: 60 EUR.<br />
The swimming pool and sauna are open Mon-Fri 7:00–20:30 and Sat-Sun 8:00–20:00.<br />
Excursion on Wednesday:<br />
The Porkkala Parenthesis part of Cold War<br />
history<br />
Pictures: Wikimedia Commons,www. degerby.fi, www.seaction.com<br />
The Porkkala region, which includes parts of Siuntio, hosted a<br />
Soviet navy base from 1944 to 1955. The population was<br />
evacuated. Trains from Helsinki to Turku had to cover their<br />
windows before passing “the longest railway tunnel in the<br />
world”. How did this happen? And who was Igor?<br />
Join our excursion to find out! Included is:<br />
● Guided bus tour<br />
● Coffee<br />
● Entrance to museums<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
18<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
19<br />
<strong>Abstracts</strong><br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
20<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
21<br />
Aerosols in the atmosphere<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
22<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Effects of the Russian forest fires over Finland in summer 2010<br />
Aaltonen, Veijo 1 , Rodriguez, Edith 1 , Mielonen, Tero 2 , Sogacheva, Larisa 1 , Lihavainen, Heikki 1 , Aalto, Pasi 3 ,<br />
Arola, Antti 2 and de Leeuw, Gerrit 1<br />
1 Finnish Meteorological Institute, Helsinki, Finland<br />
2 Finnish Meteorological Institute, Kuopio, Finland<br />
3 University of Helsinki, Helsinki, Finland<br />
23<br />
Abstract<br />
Summer 2010 was characterized by intensive forest fires in Russia causing plumes drifted to Finland. On the<br />
ground level, high turbidity was observed by the decrease of visibility and breathing difficulties. Aerosol optical<br />
depth (AOD), which gives the columnar measure of light extinction due to aerosol particles, was recorded to be<br />
significantly higher during that time than the long-time average in Finland.<br />
Ground based AOD measurements were carried out with Cimel and PFR sun photometers in Helsinki, Hyytiälä,<br />
Jokioinen, Kuopio and <strong>Sodankylä</strong>. Manually checked Level 2.0 AERONET data and cloud-screened GAW-PFR<br />
data were exploited in the analysis. In this study, we report the Finnish AOD observations which are expected to<br />
be related to the Russian forest fires and are remarkably higher than the long time average AOD of around 0.1<br />
at 500 nm. The considered time fulfilling this expectation is mid-May and throughout the period between July<br />
and mid-August, 2010. The results were checked using backward trajectories, fire maps and MODIS and AATSR<br />
satellite figures as well as ground based aerosol particle measurements and wind data.<br />
In mid-May, hourly extremes of AOD measured at Kuopio and Jokioinen were 0.3 and 0.6, respectively, thought<br />
the latter might be due to some residual cloud contamination. Late summer was characterized by two clear time<br />
periods with high AODs especially in Kuopio and Hyytiälä. First occurred between 4th and 16th of July and was<br />
recorded in Hyytiälä and Kuopio, where the peak values were 0.3 and 0.6, respectively. AOD at Jokioinen also<br />
showed somewhat high values, with a peak observation of 0.3. The second one, more impressive, happened between<br />
July 22nd and August 14th. Extreme values during that period were observed on 8th August, with maximum AOD<br />
being 1.1 both in Helsinki and Hyytiälä, and 1.5 in Kuopio. In <strong>Sodankylä</strong>, northern Finland, an extreme AOD of<br />
0.9 was observed in July 30th. Interestingly, in Jokioinen we did not find values higher than 0.3 during that time.<br />
After mid-August, there were only a few occasions with hourly averages higher than typically.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
24<br />
Characterization of columnar atmospheric aerosols: Special focus in Scandinavian area<br />
Cachorro, Victoria 1 , Toledano, Carlos 1 , Gausa, Michael 2 , Stebel, Kerstin 3 , Aaltonen, Veijo 4 , Berjón, Alberto 5 ,<br />
Ortiz de Galisteo, J. Pablo 6 , Bennouna, Yasmine 1 , Blindheim, Sandra 7 , de Frutos, Angel M. 1 , Myhre, Cathrine<br />
Lund 3 , Zibordi, Giuseppe 8 , Wehrli, Christoph 9 , Kratzer, Sussane 10 , Håkansson, Bertil 11 , Carlund, Thomas 11 , de<br />
Leeuw, Gerrit 4 , Herber, Andreas 12 and Torres, Benjamin 1<br />
1 University of Valladolid, Valladolid, Spain<br />
2 Andøya Rocket Range, Andenes, Norway<br />
3 Norwegian Institute for Air Research, Kjeller, Norway<br />
4 Finnish Meteorological Institute, Helsinki, Finland<br />
5 Spanish Meteorological Agency, Tenerife, Spain<br />
6 Spanish Meteorological Agency, Valladolid, Spain<br />
7 Andøya Rocket Range, Andenes, Norway<br />
8 Joint Research Centre, Ispra, Italy<br />
9 World Radiation Center, Davos, Switzerland<br />
10 Stockholm University, Stockholm, Sweden<br />
11 Swedish Meteorological & Hydrological Institute, Sweden<br />
12 Alfred-Wegener-Institut for Polar- and Marine Research, Bremerhaven, German<br />
Abstract<br />
The columnar aerosol properties measured in Northern Europe have been investigated. The investigation includes<br />
both data gathered in the Arctic as well as measurements collected in nearby areas (e.g. subarctic), which are of<br />
maximum interest to get a correct analysis of Arctic aerosols and transport patterns. We have evaluated the data<br />
from a set of operational sun photometer sites belonging either to national or international measurement networks<br />
(AERONET, GAW-PFR), located in Scandinavia and Svalbard. An evaluation and analysis of aerosol properties<br />
was carried out as well as a review of previous results. Aerosol optical depth (AOD) and Ångström exponent (AE)<br />
are the parameters with sufficient long-term records for a first evaluation. At the AERONET sites, microphysical<br />
properties derived from inversion of sun-sky radiance data are also available. AOD (500nm) ranged from 0.08 to 0.10<br />
in Arctic and sub-Arctic sites (Ny-Ålesund: 0.09; Andenes: 0.10; <strong>Sodankylä</strong>: 0.08). The aerosol load is higher in<br />
more populated areas in Southern Scandinavia (AOD about 0.10-0.12 at 500 nm). On the Norwegian coast, aerosols<br />
show larger mean size (AE=1.2 at Andenes) than in Finland, with continental climate (AE=1.5 at <strong>Sodankylä</strong>).<br />
Columnar particle size distributions and related parameters are used to evaluate aerosol volume efficiencies. Special<br />
emphasis must be given to the joint and collaborative effort of the various groups from different countries maintaining<br />
the observation sites.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
25<br />
A shortcut from broadband to spectral aerosol optical depth<br />
Kannel, Martin 1 , Ohvril, Hanno 1 and Okulov, Oleg 2<br />
1 Laboratory of Atmospheric Physics, Institute of Physics, University of Tartu<br />
2 Estonian Meteorological and Hydrological Institute<br />
Abstract<br />
The concept behind the shortcut idea is a close correlation between column broadband aerosol optical depth (BAOD)<br />
and aerosol optical depth at 500 nm (AOD500). The method uses only two input parameters: (a) the Bouguer<br />
broadband coefficient of column transparency for optical mass m = 2 (solar elevation about 30 deg); and (b)<br />
integrated column precipitable water vapor which can be roughly estimated using surface water vapor pressure.<br />
Creating the method, a large database, including almost 20 000 complex, spectral and broadband direct solar<br />
beam observations at Tõravere, Estonia during all seasons of a 8-year period, 2002–2009, was used. The AOD500<br />
observations were performed by AERONET and the broadband direct beam ones by the Estonian Meteorological<br />
and Hydrological Institute. Analyze of this database revealed a high correlation between BAOD and AOD500 which<br />
enabled transition from broadband to spectral AOD. Almost 82% of the observations in the database belonged to<br />
lower turbities when AOD500 < 0.2. The RMS error for AOD500 prediction in this range was 0.022. For AOD500<br />
= 0.2–0.4, the RMSE was 0.035, for 0.4–0.6, the RMSE was 0.042. Relative RMSE for these ranges was about 22%,<br />
12% and 9%, respectively. For AOD500 > 0.6, relative RMSE remained 9%. For comparison, the same database<br />
was used to test Gueymard’s broadband parameterization based on his SMARTS2 classic model. The last one,<br />
apparently due to problems with circumsolar radiation, systematically underestimated the AOD500. However, there<br />
was also a close correlation between our shortcut-results and Gueymard’s broadband parameterization.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
26<br />
Megacities inventory base on optical properties, using satellite and SILAM model<br />
results<br />
Hannukainen, Meri 1 , Rodriguez, Edith 2 , Sofiev, Michael 3 , Kolmonen, Pekka 2 , Sundström, Anu-Maija 1 , Sogacheva,<br />
Larisa 2 and de Leeuw, Gerrit 4<br />
1 University of Helsinki, Dept. of Physics, Helsinki, Finland<br />
2 FMI, Climate Change Unit, Erik Palmen Aukio 1, 00101, Helsinki, Finland<br />
3 FMI, Air Quality Unit, Erik Palmen Aukio 1, 00101, Helsinki, Finland<br />
4 FMI, Climate Change Unit, Erik Palmen Aukio 1, 00101, Helsinki, Finland; University of Helsinki, Dept. of Physics,<br />
Helsinki, Finland; TNO, Utrecht, The Netherlands<br />
Abstract<br />
The increasing of population in Megacities causes an increase in the level of contamination with impact at urban,<br />
regional and global levels. Nowadays air pollution is one of the most important problems in megacities. Photochemical<br />
smog primarily from traffic, but also from industrial activities, power generation, and solvents are becoming<br />
more and more important sources of concern for air quality. The impact of the aerosol particles emitted in the area<br />
of megacities and the their effect in the local and regional scale are studies using two methods: the determination<br />
of emissions from Megacities using satellite observations and model results obtained with System for Integrated<br />
modeLling of Atmospheric coMposition (SILAM). SILAM has been created to provide an environment capable of<br />
supporting various types of dispersion models and suitable for approaching a wide range of tasks. The satellite data<br />
used for this study were provided with two instruments. Advanced Along Track Scanning Radiometer (AATSR) on<br />
board ENVISAT, and the Moderate Resolution Imaging Spectroradiometer (MODIS), on board Terra (EOS AM-1).<br />
Retrievals of aerosol optical properties were done for both satellite measurements. Satellite and model results were<br />
validated by ground base measurements with results provides from AErosol RObotic NETwork (AERONET) sun<br />
photometer. AERONET results are used also for classification of aerosol type. Our interest is to do a current<br />
emission inventory for selected megacities around the world. The parameter used for the study is Aerosol Optical<br />
Depth (AOD) as the optical parameter that gives information of the aerosol particles concentration. Selected time<br />
period for study is year 2008. Preliminary results show good agreement between satellites retrieved AOD as well as<br />
with the sun photometer.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
27<br />
Ionosphere, mesosphere and lower thermosphere<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
28<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
29<br />
An enhancement of the airglow brightness by the gravity waves<br />
Nikolaishvili, Sergey 1 and Belyaev, Alexey 1<br />
1 Institute of Applied Geophysics, Moscow, Russia<br />
Abstract<br />
The global observations of the O 2 atmospheric band nightglow performed by the high resolution Doppler imager<br />
(HRDI) on the Upper Atmosphere Research Satellite (UARS) have shown bright regions of the nightglow. It was<br />
supposed that these regions are caused either by meridional circulation, or by descending motion associated with<br />
tides and gravity wave (GW) forcing. In this study we describe and speculate an additional mechanism of the<br />
brightness enhancement. It is nonlinear enhancement of the entire emission layer caused by GWs passing through<br />
one. Its magnitude is proportional to the square of the GW amplitude. We speculate this effect as an emission layer<br />
response to the GW disturbance. To estimate the magnitude of this effect we use the global two-dimensional model<br />
of the zonally averaged circulation.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
30<br />
Optical signatures of rocket exhaust phenomena in Arctic atmosphere<br />
Chernouss, Sergey 1 , Platov, Yuly 2 , Alpatov, Victor 3 and Uspensky, Mikhail 4<br />
1 Polar <strong>Geophysical</strong> Institute of KSC RAS<br />
2 IZMIRAN, Troitsk, Moscow region, Russia<br />
3 Institute of Applied Geophysics, Moscow, Russia<br />
4 Finnish Meteorological Institute, Helsinki, Finland<br />
Abstract<br />
The results of research of the optical phenomena connected with rocket exhaust in the upper atmosphere are<br />
submitted. The most intensive, large-scale and dynamical phenomena are caused by special modes of operation of<br />
rocket engines, in particular, separation of rocket stages and shut off solid propellant of rocket engines and physical<br />
conditions in the field of a rocket flight. The optical signatures in the upper atmosphere accompanying rocket<br />
launches made from the Archangelsk region ranges have been registered for many years by ground-based network<br />
of all-sky cameras in the northern regions of Russia and Finland as a part of routine auroral recordings. Rocket<br />
plumes and large-scale diffuse formations have been captured both on photographic film cameras C-180, spectral<br />
cameras C-.180-S, low light level TV cameras and amateur films. Purpose of the report is a classification of gas-dust<br />
formations from rocket exhaust in the upper atmosphere by scale and dynamics. At registration of these optical<br />
phenomena two mechanisms of luminosity are observed as a rule. It is Rayleigh and Mie scattering of the solar<br />
radiation.and resonant scattering of the solar radiation on AlO and Li molecules.After the ending of a dynamic<br />
phase of development of the phenomenon, the rather weak diffuse luminosity was observed during long time (till<br />
several hours after the start of the pattern development of the phenomenon up to sunrise) at the place of cut off the<br />
launcher stage i.e. connected with injected of gas components of rocket exhaust. The dynamic and morphological<br />
features of the artificial clouds are a function of the relative quantities of gaseous and dispersed solid components<br />
from the rocket exhaust. Acoustic- gravity waves (AGW) in the upper atmosphere after launches demonstrated too.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
31<br />
Using Airglow observations in high-latitude climate studies<br />
Dyrland, Margit Elisabet 1 and Sigernes, Fred 1<br />
1 The University Centre in Svalbard, Longyearbyen, Norway<br />
Abstract<br />
The polar mesopause region (80-100 km) is highly dynamic with large gradients in temperature and large variability<br />
in vertical, zonal and meridional circulation resulting from atmospheric waves passing and breaking. There is<br />
increasing evidence that the dynamics of the mesosphere can be coupled to the dynamics of the troposphere and<br />
ground, and the importance of studying the weather and climate of the mesosphere is therefore emphasized. The<br />
existence of the hydroxyl (OH) airglow layer at ≈87 km allows for a way to monitor the state of this region remotely.<br />
Rotational temperatures can be derived from passive optical measurements of airglow intensity during the polar<br />
night, and gravity wave parameters from all-sky images. At the Kjell Henriksen <strong>Observatory</strong> (KHO) at Svalbard<br />
(78 degrees north) an Ebert-Fastie spectrometer is employed which has monitored the OH rotational temperatures<br />
since the early 1980’s. For the winter season 2010-2011 an all-sky airglow imager was installed which monitors the<br />
gravity wave activity. Co-located with KHO are several radars which complement the optical measurements, and<br />
allows for extraction of additional information. This talk gives an overview of how these instruments can be used<br />
for high-latitude climate studies, and presents the latest results.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
32<br />
Subsidence of thermospheric air observed by the Hotel Payload 2 measurements on<br />
January 31, 2008<br />
Enell, Carl-Fredrik 1 , Gustavsson, Björn 2 , Sergienko, Tima 3 , Verronen, Pekka. T 4 , Hedin, Jonas 5 , Witt, Georg 5 ,<br />
Brändström, Urban 3 and Rydesäter, Peter 6<br />
1 <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong>, University of Oulu, <strong>Sodankylä</strong>, Finland<br />
2 University of Southampton, UK<br />
3 Swedish Institute of Space Physics, Kiruna, Sweden<br />
4 Finnish Meteorological Institute, Helsinki, Finland<br />
5 Stockholm University, Sweden<br />
6 SenseAir AB, Delsbo, Sweden<br />
Abstract<br />
In the Hotel Payload 2 rocket campaign on January 31, 2008 (Enell et al, JASTP, in press) profiles of atomic oxygen<br />
and electron density measured in the lower thermosphere indicated subsidence of air.<br />
For the evening before the launch, tomography-like estimates of the volume emission rates from Auroral Large<br />
Imaging System (ALIS) data have been shown (Enell et al, 37AM, Valladolid, Spain; in preparation for submission).<br />
The common volume of ALIS, however, was above the Scandinavian mainland and did not cover the rocket trajectory<br />
from Andøya. The altitude profiles of spectroscopic ratios interpolated from the volume emission estimates do not<br />
unambiguously indicate anything unusual. This is consistent with EOS Aura/MLS CO measurements indicating<br />
highly structured subsidence in vortex filaments and with the structure of the NO profiles measured by SciSat/ACE.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
What can we learn about upper mesosphere dynamics by four-dimensional lidar measurements?<br />
Hoppe, Ulf-Peter 1<br />
1 University of Oslo, Norway<br />
33<br />
Abstract<br />
Lidar instruments have been used in atmosphere research for many years. Most lidar instruments measure profiles<br />
of one or few atmospheric parameters in a certain height range, giving range-resolved profiles of that parameter and<br />
their time evolution. For instance a simple Rayleigh lidar measures total number density profiles from the middle<br />
stratosphere to the upper mesosphere. An advanced Na lidar measures profiles of Na number density, neutral<br />
temperature and line-of-sight wind velocity in the height region where there are free Na atoms: 80 to 110 km.<br />
Several of these instruments are capable of measuring in full daylight, but all require a cloudless sky in order to<br />
measure above the troposphere.<br />
Most lidars capable of measuring line-of-sight wind velocities are used in several positions in the sky, sequentially<br />
or quasi-simultaneously. Measurements in zenith give profiles of vertical velocity. Vertical velocities in the upper<br />
mesosphere are usually within approximately ±7 m/s. This value is somewhat greater than the typical velocity<br />
resolution of such an instrument. Many lidars use slant beams 20 ◦ or 30 ◦ off-zenith, e.g., to the north and to the<br />
east. Under the assumption (a) that the vertical velocity is much smaller than the horizontal velocity, and (b) that the<br />
horizontal wind is the same at the two positions several tens of km distant from each other, a horizontal wind vector<br />
can be estimated. Another mode uses two beams 20 ◦ or 30 ◦ off-zenith towards east and west to estimate the flux of<br />
gravity wave pseudo-momentum in the zonal direction. Profiles of such gravity momentum flux measurements let us<br />
estimate the divergence or convergence of the momentum flux, which is the cause of background wind acceleration.<br />
Momentum flux measurements depend on statistics and must therefore continue for a large number of typical gravity<br />
wave periods without interruption.<br />
This presentation proposes a lidar similar to the Weber Na Lidar at ALOMAR, but employing three beams in a<br />
triangular configuration centered on zenith or at an off-zenith direction. The smallest feasible distance between the<br />
beams is ≈ 1 ◦ field of view, a few tens or hundreds of meters at 90 km. Larger interbeam distances will increase the<br />
instrument’s sensitivity to gravity waves with horizontal wavelengths approximately twice the interbeam distance.<br />
The presentation will discuss if such an instrument can give us new insight into gravity wave propagation, spectra,<br />
dissipation, or turbulence. Possible designs for the lidar transmitter and receiver with available components will be<br />
evaluated.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
34<br />
The dayside open closed field line boundary - a statistical study using ground-based<br />
optics<br />
Lorentzen, D.A. 1 and Johnsen, M.G. 2<br />
1 UNIS, Longyearbyen, Norway<br />
2 The Univ. of Tromsø, Tromsø, Norway<br />
Abstract<br />
This presentation is based on a paper by Johnsen and Lorentzen, [2011]. Several studies have been made to determine<br />
the statistical location of the cusp - the vast majority using satellite data. In this work, ground-based optical data<br />
have been used in order to study the location of the open-closed magnetic field line boundary (OCB) in the cusp<br />
region. The data set used covers 15 auroral seasons - corresponding to two solar minimums and one solar maximum.<br />
Using a meridian scanning photometer, the dayside OCB can be determined using the equatorward edge of the 6300<br />
Å [OI] emission as a proxy. The statistical location of the OCB is compared to both solar- and solar wind activity<br />
indices and coupling functions. It was found that the average optical OCB is located at 75.4 degrees magnetic<br />
latitude, and that there is a statistical significant relationship between the seasonal median of the OCB latitude and<br />
the solar cycle. It was also found that the statistical location of the OCB found by ground-based optics compares<br />
very well with satellite based statistical studies of the cusp location. The statistical OCB location was also found<br />
to have a remarkable fit to the PCN (polar cap magnetic activity) index, thus indicating how well the latitudinal<br />
location of the OCB reflects the degree of interconnection between the solar wind and the magnetosphere/ionosphere<br />
system.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Implementing a chemical scheme for OH* in the University College London CMAT2<br />
3D Global Model<br />
McCarthy, Dean 1 , Mulligan, Frank 1 and Mooney, Priscilla 1<br />
1 National University of Ireland Maynooth, Maynooth, Ireland<br />
35<br />
Abstract<br />
The Coupled Middle Atmosphere and Thermosphere (CMAT2) Model is a general circulation model under continuous<br />
development at University College London. Work is underway to improve the already existing chemical scheme<br />
focusing on the modelling of vibrationally excited hydroxyl (OH*) at mesopause altitudes.<br />
The existing chemical scheme considers ground state OH and vibrationally excited states as a single species. In<br />
the new implementation, the ground state and each of the nine lowest vibrational states have been incorporated as<br />
distinct chemical constituents.<br />
The chemical production of OH* through the reaction H + O 3 -> OH*(v=6-9) + O 2 has been altered to include<br />
branching ratios into vibrational levels 6 – 9. The loss of OH* is governed through a series of chemical reactions,<br />
both single and multi-quantum collision deactivation, as well as radiative loss.<br />
The model output with be presented and compared to the model output of Picket et al. (2006) as well as<br />
observational data from NASA’s SABER instrument onboard the TIMED satellite.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
36<br />
Study on the impact of sudden stratospheric warmings in mid-latitude MLT region<br />
according to ground-based and satellite temperature measurements<br />
Medvedeva, Irina 1 , Chernigovskaya, Marina 1 , Perminov, Vladimir 2 and Semenov, Anatoly 2<br />
1 Institute of Solar-Terrestrial Physics (ISTP), Siberian Branch, Russian Academy of Sciences, Irkutsk, Russia<br />
2 Obukhov Institute of Atmospheric Physics (IAP), Russian Academy of Sciences, Moscow, Russia<br />
Abstract<br />
Sudden stratospheric warmings (SSW) are an important manifestation of vertical dynamical coupling in the atmosphere.<br />
This work presents the results of studies of variations in atmospheric temperature at the mesopause<br />
and lower thermosphere (MLT) heights in different longitudinal sectors during the sudden stratospheric warming<br />
events in 2008-2011. The research is made on the data of ground-based and satellite temperature measurements.<br />
We analyzed variations of upper mesosphere temperature at ≈87 km inferred from OH (6,2) airglow observations<br />
at two mid-latitude observation points: the ISTP <strong>Geophysical</strong> observatory (East Siberian region, 52N, 103E) and<br />
Zvenigorod station (56N, 37E). Satellite data on atmospheric temperature vertical profiles obtained by the EOS<br />
Aura Microwave Limb Sounder (MLS) were involved. It was shown that SSWs affect on the temperature regime of<br />
the atmosphere at the MLT heights. However, the character of the manifestations at different longitudinal stations<br />
was not always identical. In the European longitudinal zone the upper mesosphere temperature decreased during all<br />
analyzed SSWs. In the East Siberian – reaction of the upper mesosphere temperature on SSW did not show such a<br />
stable tendency. We carried out correlation analysis of temperature variations in the stratosphere and upper mesosphere<br />
and obtained regression equations. The behaviour and magnitude of the mesopause temperature decrease<br />
depends on the intensity of stratospheric warming. Practically during all analyzed SSW events, when the stratospheric<br />
temperature increased by ≈30 K, the mesopause temperature decreased by ≈20 K. The work is supported<br />
by Grants from RFBR-10-05-00062 and RFBR-09-05-00757.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Gravity wave characteristics measured in Ireland by UWOSCR during the 2010-2011<br />
NDMC campaign<br />
Mulligan, Frank J. 1 and Lowe, Robert P. 2<br />
1 National University of Ireland Maynooth, Maynooth, Ireland<br />
2 The University of Western Ontario, London, Ontario, Canada<br />
37<br />
Abstract<br />
A scanning radiometer developed at the University of Western Ontario was installed at Maynooth, Ireland (53.4 ◦<br />
N, 6.6 ◦ W) in August 2010 for the purpose of recording gravity wave characteristics during an NDMC (Network<br />
for Detection of Mesopause Change) campaign. Wave directions, speeds, periods and wavelengths were determined<br />
from 50 clear nights. Propagation directions were found to be northward in summer and early autumn, but changed<br />
to southward in mid-winter. This pattern agrees well with observations made at other mid-latitude sites. Horizontal<br />
wavelengths ranged from 5-70 km, with the most frequently occurring wavelength in the vicinity of 10 km. Periods<br />
ranged from 2-15 minutes with a maximum occurrence frequency in the 3 minute region. Apparent speeds were<br />
found to be between 30 m/s and 150 m/s with the most frequently occurring speed near 65 m/s. A brief description<br />
of the instrument, the method of analysis and results will be presented.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
38<br />
Longitudinal variations of the atmospheric temperature at altitudes of lower thermosphere<br />
on the characteristics of the 557.7 nm atomic oxygen emission<br />
Semenov, Anatoly 1<br />
1 Institute of Atmospheric Physics of Russian Academy of Sciences, Moscow, Russia<br />
Abstract<br />
On the basis of statistical regularities of longitudinal variations of intensity and temperature of atomic oxygen<br />
emission 557.7 nm have been obtained approximation ratio, allowing to make estimations of longitudinal values of<br />
temperature at heights of 95-100 km in the latitudinal zone 30-55N for conditions of a minimum of solar activity.<br />
The harmonious analysis of the revealed variations has shown, that amplitudes of the corresponding harmonic for<br />
intensity and temperatures have proportional values. It has allowed us to construct average longitudinal variations<br />
of temperature of a emitting layer of emission of 557.7 nm. Comparisons to data of direct measurements of temperature<br />
by interferometric, lidar and satellite methods have shown that they correspond to the empirical regularities.<br />
Dependences of amplitudes of seasonal variations of temperature on latitudes are obtained. The work is supported<br />
by Grants from RFBR-10-05-00062 Keywords: longitudinal variations, intensity, temperature, emission of atomic<br />
oxygen<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
39<br />
How to Use Airglow Measurements in Atmospheric Wave Activity Studies<br />
Taylor, Michael 1 , Zhao, Yucheng 1 , Pautet, Pierre-Dominique 1 and Pendleton Jr., William 1<br />
1 Utah State University<br />
Abstract<br />
The naturally occurring airglow emission layers provide an important capability for studying the dynamics of the<br />
Earth’s upper atmosphere. Several emissive layers occur in relatively close proximity to each other in the mesosphere<br />
and lower thermosphere (≈80–100 km) region. These comprise the relatively bright near infrared OH Meinel bands<br />
(peak altitude ≈87 km), the O 2 (0,1) Atmospheric band (altitude ≈94 km), and the weaker, visible wavelength OI<br />
(557.5 nm) line emission (altitude ≈96 km) and Na (589.2 nm) doublet emissions (peak altitude ≈90 km). The<br />
nocturnal half-width of each of these layers is ≈8–10 km, providing a unique method for studying the dynamics of<br />
a wide variety of wave phenomena including gravity waves, tides and planetary waves at MLT heights, and their<br />
latitudinal and seasonal variability. At higher altitudes (≈250 km) the OI (630 nm) emission layer continues to<br />
be used extensively to study ionospheric processes associated with strong plasma upwellings at equatorial latitudes<br />
as well as the propagation of large- and medium-scale Traveling Ionospheric Disturbances (TIDs). A number of<br />
instrumental techniques have been developed to investigate these atmospheric phenomena utilizing these airglow<br />
emissions. These include photometers, spectrometers, interferometers and imagers. In particular, imagers have<br />
evolved considerably over the past 20 years and are now an essential component of a well-founded observatory. This<br />
talk focuses on how to use digital (CCD) airglow imagers for atmospheric wave studies. As well as providing wide<br />
field data on wave propagation through the MLT layers, new systems can now map the wave-induced temperature<br />
and intensity perturbations, key for investigating their momentum fluxes and hence impact on the MLT dynamics.<br />
Recent observations using new InGaAs IR sensors will also be presented to illustrate current capabilities for high<br />
time (few sec) and precision (≈1–2 K) intensity and temperature measurements.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
40<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
41<br />
Aurora<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
42<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
43<br />
Nighttime auroras for remote sensing of magnetospheric processes<br />
Aikio, Anita 1<br />
1 University of Oulu, Finland<br />
Abstract<br />
Auroral structures are located within the auroral ovals, which comprise both the day and nightside and the northern<br />
and southern hemispheres. Auroras appear during quiet and disturbed conditions. The overall picture of solar wind<br />
driving the magnetosphere-ionosphere interaction producing auroras is understood to some extent, but much of the<br />
details are still unknown. This tutorial talk will focus on some aspects of nighttime auroras and their origin.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
44<br />
Ground - satellite observations of dynamics of the magnetosphere - ionosphere system<br />
during the Superstorm on Nov. 20, 2003<br />
Andalsvik, Yngvild Linnea 1 , Sandholt, Per Even 1 and Farrugia, Charles J. 2<br />
1 Department of Physics, University of Oslo, Oslo, Norway<br />
2 Space Science Center, University of New Hampshire, Durham, NH, USA<br />
Abstract<br />
We report observations from a ground - satellite conjunction in the Scandinavian sector at the time of a substorm<br />
breakup in the early main phase of the superstorm on Nov. 20, 2003. Observations of plasma convection, particle<br />
precipitation, field-aligned currents (FACs), aurora, and ground magnetic deflections are discussed in the context of<br />
multi-stage evolution of the Dungey convection and flux circulation cycle during strong forcing of the magnetosphere<br />
at the time of interplanetary CME passage at Earth. We take advantage of the good latitudinal coverage (polar<br />
cap to subauroral latitudes) of the IMAGE chain of magnetometers and meridional profiles of ion drift - particle<br />
precipitation - FACs obtained from spacecraft DMSP F13 and F15 in the 1800 - 2000 MLT sector.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
45<br />
Statistical study of temporal and spatial variations in diffuse aurora<br />
Axelsson, Katarina 1 , Sergienko, Tima 1 and Brändström, Urban 1<br />
1 IRF, Kiruna, Sweden<br />
Abstract<br />
Optical, radar and satellite measurements have demonstrated that diffuse aurora contains fine structures. Data<br />
analysis shows that these fine structures are a result of modulation of high energy precipitating electrons. Pitch<br />
angle diffusion in the loss cone due to interaction of whistler mode wave with plasma sheet electrons is the most<br />
feasible mechanism leading to high-energy electron precipitation. This suggests that the fine structure is an indication<br />
of modulations of the efficiency of the wave-particle interaction. One type of such fine structures is regular, parallel<br />
auroral stripes. Spatial and temporal structures of diffuse aurora stripes can give us information about modulation<br />
mechanisms. In this study we use ALIS data for statistical study of such characteristics.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
46<br />
The morning auroral arcs associated with Pc5 geomagnetic pulsations<br />
Belakhovsky, Vladimir 1 , Kozlovsky, Alexander 2 and Pilipenko, Slava 3<br />
1 Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
2 Sodankyla <strong>Geophysical</strong> <strong>Observatory</strong> of the University of Oulu, Oulu, Finland<br />
3 Institute of the Earth Physics, Moscow, Russia<br />
Abstract<br />
We study the event of Pc5 geomagnetic pulsations observed in the morning sector on 18 December 2001 at the<br />
stations of IMAGE magnetometer network. The pulsations were observed in the wide range of latitudes from 58 ◦ to<br />
76 ◦ MLAT. Geomagnetic Pc5 pulsations exhibit signatures of the filed-line resonance (FLR), namely, the decrease<br />
of the frequency with increase of the latitude, change of the ellipse during the propagation thought the resonance<br />
region, and phase propagation from low to high latitudes. Corresponding variations of the ionosphere plasma velocity<br />
were seen by the VHF EISCAT radar, which beam was pointed to north at low elevation (30 ◦ ) to the horizon. The<br />
frequency of pulsations in the ionosphere plasma velocity decreases with latitude. Signatures of the Pc5 pulsations<br />
were also seen in the data of ionosphere plasma velocity, density, and ion temperature obtained from the EISCAT<br />
Svalbard radar. The cosmic noise absorption did not demonstrate significant signatures of Pc5 pulsations in the<br />
data of riometers in KIL (IRIS) and HOR (Spitsbergen). At the same time, during the event of Pc5 geomagnetic<br />
pulsations, auroral arcs were observed by the all-sky TV camera in Barentsburg (Spitsbergen). The period of<br />
appearance of the auroral arcs was approximately coinciding with the period of Pc5 geomagnetic pulsations. We<br />
suppose that Pc5 geomagnetic pulsations generated by FLR modulate the intensity of morning auroral arcs.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
47<br />
Ideas of Lomonosov in field of auroral research<br />
Chernouss, Sergey 1<br />
1 Polar <strong>Geophysical</strong> Institute of KSC RAS<br />
Abstract<br />
This year we celebrate the 300 anniversary of the birth of Russian Academician Lomonosov. He was encyclopedic<br />
scientists, left more than 15 volumes of publications in physics, chemistry, geophysics, geography, philology, and<br />
other sciences and arts. Mikhail Vasilyevich Lomonosov (1711-1765) was born and raised in the Arkhangelsk region<br />
in pomors family, where his childhood was lucky to repeatedly watch the aurora. Later, when he became interested<br />
in their physical nature, it does not rely on other people’s descriptions are often far removed from reality, but on<br />
his own observations. Academicians Kraft, Meyer and Geynzenus in the Russian Imperial Academy of Sciences<br />
tried to study the aurora thoroughly and seriously. Academician Craft prints extensive historical information about<br />
the aurora to bringing the hypotheses of the optical and cosmic character that existed in Western Europe in 1730.<br />
Views of Meyer were connected with the growth of autumn ”cold” from the ground up warm air and on the contact<br />
line of hot and cold air ignition of vapors. Academician Geynzenus was a supporter of the newly published work<br />
of the Frenchman de Meran that lights should come from matter ejected Sun (which, generally speaking, is a<br />
conjecture about the existence of the solar wind), and in 1740 published an article in which he tried to explain to<br />
a single cause zodiacal light and the aurora. However, the first who proposed the electrical nature of the aurora<br />
was Lomonosov. The main his work on the aurora nature was the ”Oration on aerial phenomena, proceeding from<br />
the force of electricity proposed by Mikhail Lomonosov” , which was reported at the meeting of the Academy of<br />
Sciences November 26, 1753. According to Lomonosov, the electric force may be cause for auroras glow which in<br />
appearance resembles the glow of the gas discharge. In particular, he writes ”So, it is likely that the northern lights<br />
are born from occurring of the electric force in the air. It is confirmed by likeness of the phenomenon appearance<br />
and disappearance, movement, color and form, which are shown in the northern lights and the electric light of the<br />
third kind. ”. Fundamental task for a long time was to determine the height of the aurora. Lomonosov wrote, ”The<br />
position of the northern lights above the limits of the atmosphere shows a comparison of dawn with them” Once he<br />
carried out a direct measurement of the height of the upper edge of the aurora, which according to his calculations<br />
was equal to 420 miles (448 km). This agrees well with modern measurements of the upper edge of the radiant arcs.<br />
Thus, estimates of Lomonosov received three centuries before are closed to modern results. In those times and later<br />
the scientists were challenged to define what constitutes the aurora - intrinsic luminescence of the atmosphere, or<br />
reflected, scattered, or diffracted rays from external light sources. Lomonosov noticed that the stars can be seen<br />
through the lights, and on this basis concluded that ”All of the northern lights shown that light species may not<br />
be vapor or clouds, shining under some lighting. They are almost always have a regular figure, and stars clearly<br />
seen through the northern light luminousity”. Thus it was shown that aurora is self luminosity phenomena of the<br />
atmosphere but not reflected or scattered light of remote source. This speculation of the scientist were subsequently<br />
confirmed by direct instrumental measurements just one hundred years later by famous Swedish physicist Angstrom<br />
in 1866-67 years. The thought of Lomonosov on relationship of auroral colors with the particular substance was<br />
also promising: ”By the way if some main colors composed the white color born in the air then no doubt be that<br />
the main components separately may seen too”. Great interest are pictures and drawings of the aurora taken by<br />
Lomonosov. Forty-seven drawings were engraved on 11 copper engraving and stored in the Museum of Lomonosov<br />
in St.- Petersburg. We can see the typical forms of auroras on them. One can only wonder at the foresight of genius,<br />
who anticipated that knowledge of the nature of the aurora, which have become accessible to us only in the 20<br />
century.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
48<br />
On small-scale aurora<br />
Dahlgren, Hanna 1<br />
1 Boston University, Boston, USA<br />
Abstract<br />
Both active auroral displays and diffuse aurora have been found to contain internal structuring when measured with<br />
sufficiently high temporal and spatial resolution. Small-scale aurora is the general term given to auroral features with<br />
scale sizes transverse to the background magnetic field of less than 1 km and with time scales of less than a second.<br />
The fine-scale morphology is related to structuring of auroral currents and electric fields, but the details behind<br />
these structures are still not fully resolved – dispersive Alfven waves have been proposed as a possible source of<br />
the particle acceleration, but observations and simulations are inconclusive. Detailed spatial, spectral and temporal<br />
observations of the aurora are crucial in understanding the electrodynamic processes taking place in the ionosphere<br />
and in its coupling to the magnetosphere. In this tutorial, an overview will be given of the latest techniques and<br />
instruments used to measure the rapid phenomenon. Examples of different forms of small-scale aurora will be shown<br />
as observed by ground-based imagers. In light of the observations, the current understanding of the formation of<br />
auroral fine-scale structures is discussed and a review given of important studies which lead the way to a better<br />
understanding of the topic.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
49<br />
The Magnetospheric Drivers of Aurora<br />
Donovan, Eric 1<br />
1 University of Calgary, Canada<br />
Abstract<br />
The aurora results from the precipitation of electrons and protons into the upper atmosphere. The aurora is<br />
called diffuse and discrete if that precipitation is caused by pitch angle scattering or field-aligned acceleration,<br />
respectively. The energy that powers the discrete aurora and the pitch angle scattering that causes the diffuse<br />
aurora are consequences of magnetospheric processes. Much of the motion and structure of the aurora arises as a<br />
consequence of magnetospheric plasma physical processes. In this tutorial, I will present a review of our present<br />
understanding of the magnetospheric drivers of auroral power, structure, and dynamics.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
50<br />
Optical Measurements of F-region Ion-Convection<br />
Gustavsson, Björn 1 , Tuttle, Sam 2 , Dahlgren, Hanna 3 , Lanchester, Betty 2 and Ivchenko, Nickolay 4<br />
1 School of Physics and Astronomy University of Southampton, Southampton, UK<br />
2 School of Physics and Astronomy University of Southampton Southampton, UK<br />
3 Boston University, Boston, MA, USA<br />
4 School of Electrical Engineering Royal institute of Technology, Stockholm, Sweden<br />
Abstract<br />
The long life-time of the oxygen ion state that emits the 7320 Å lines makes the emitting ions move between the<br />
instance of excitation and emission. It is therefore possible to estimate the ion-convection from spectral imaging<br />
at magnetic zenith. Here we present a novel algorithm to estimate the ion-convection around auroral arcs based<br />
on spectral imaging with ASK and incoherent scatter observations with the EISCAT UHF radar. The performance<br />
characteristics of the algorithm are evaluated and a direct comparison with EISCAT observations of ion drift is<br />
made.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
51<br />
On Filamentation and Anti-Filamentation of Auroral Arcs<br />
Gustavsson, Björn 1 , Dahlgren, Hanna 2 , Lanchester, Betty 3 and Ivchenko, Nickolay 4<br />
1 School of Physics and Astronomy University of Southampton, Southampton, UK<br />
2 Boston University, Boston, MA, USA<br />
3 School of Physics and Astronomy University of Southampton Southampton, UK<br />
4 School of Electrical Engineering Royal institute of Technology, Stockholm, Sweden<br />
Abstract<br />
Small-scale structures are often observed in aurora but their appearance and cause are not well understood. One<br />
suggestion is that arc splitting is caused by inertial Alfven waves. In this presentation we use multi-monochromatic<br />
observations of filamenting and anti-filamenting auroral arcs made with the ASK instrument from several events, to<br />
test the predictions of spatio-temporal variations of electron energies and fluxes that can be derived from this model.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
52<br />
Planetary distribution of auroral luminosity inferred from APM<br />
Vorobjev, V. G. 1 , Yagodkina, O. I. 1 , Katkalov, Yu. V. 1 and Kirillov, A. S. 1<br />
1 Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
Abstract<br />
Statistical treatment of DMSP F6 and F7 spacecraft observations during more than 35000 passes through the auroral<br />
zones of both hemispheres was used to create the interactive Auroral Precipitation Model (APM) which is placed<br />
now on http://webapps.pgia.ru/apm/. The model at a level of magnetic activity (AL and Dst indexes) set by<br />
the user allows to receive: (1) global distribution of different types of auroral precipitation, (2) planetary picture of<br />
average electron energy in different precipitating zones, (3) the that of energy fluxes. Observatories or any points<br />
interested by the user can be mark off on the picture by the geographical coordinate dimensioning or a click by<br />
”the mouse” on Google maps. The model allows us to calculate the precipitation power in different zones and the<br />
global distribution of auroral luminosity in visible and UVI spectral ranges. Integral intensities of the N 2 LBH(L)<br />
band near 170.0nm, 1NG N + 2 at 391.4 nm, (OI) 557.7 nm (the transition 1 S → 1 D in atomic oxygen), and the 1PG<br />
N 2 band near 669.0 nm have been calculated. To calculate (OI) 557.7 nm intensity the production of O( 1 S) in the<br />
electron energy transfer process N 2 (A 3 Σ + u ) + O( 3 P), the dissociative recombination, auroral electron impact and<br />
the production of electronically excited N 2 by auroral electron impact were taken into account. A good agreement<br />
was revealed by comparison of the LBH(L) global distribution observed by the IMAGE spacecraft and calculated<br />
from APM.<br />
This study is supported by the RFBR grant 09-05-00818 and Program 4 of the RAS Presidium.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
A case study about the connection of optical auroral activity and geomagnetic Pc5<br />
pulsations<br />
Kauristie, Kirsti 1 , Kleimenova, Nataly 2 , Kozyreva, Olga 2 , Uspensky, Mikhail 1 and Vlasov, Alexey 1<br />
1 Finnish Meteorological Institute, Helsinki, Finland<br />
2 Russian Academy of Sciences, Moscow, Russia<br />
53<br />
Abstract<br />
We study geomagnetic Pc5 pulsations which were observed on Jan 18 2008 during 0400-0600 UT in the dawn sector<br />
of the high-latitude ionosphere. Like typical for Pc5 activity also in our case the main driver of the pulsations was<br />
an enhancement in the solar wind velocity. In addition, changes in the IMF direction played an important role in<br />
setting up suitable conditions for the pulsations. The enhancement in solar wind velocity took place in two steps<br />
and during the analysed event the IMF Bz had two different types of behavior: a 0.5 hour period with variations<br />
around zero which was surrounded by periods with clearly positive values. The amplitude and period of Pc5 showed<br />
significant variations during the two hour sequence. With the help of solar wind, magnetospheric and ionospheric<br />
observations we discuss the different processes which caused the changes in the Pc5 appearance. In particular, we<br />
study the relationship between the magnetic pulsations and auroral activity observed both in the dawn sector by<br />
MIRACLE ASCs and in the midnight sector by THEMIS ASCs. THEMIS instrumentation recorded during our<br />
event two small substorms. Around the times of the substorm onsets MIRACLE magnetometers recorded sudden<br />
impulses (with 10 min duration and 100-300 nT amplitude) in the magnetic field. The first impulse was accompanied<br />
by an enhancement in high-latitude dawn sector auroras and it was followed by a drop in the Pc5 intensity. The<br />
second impulse was prominent in a wider latitude range than the first one, but its impact in the Pc5 activity was<br />
not as dramatic as in the first case. In the presentation we investigate whether the simultaneous appearance of<br />
the two substorm onsets and the impulses in the dawn sector magnetic activity was just a pure coincidence or<br />
whether these phenomena are signs of a larger scale re-organization in the magnetosphere. In addition, we compare<br />
our observations of Pc5 activity with previous studies discussing the linkage between dawn sector pulsations and<br />
substorm activity.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
54<br />
Inverse cascade in the auroral structure and numerical model of current filaments<br />
Kozelov, Boris 1 , Golovchanskaya, Irina 1 and Mingalev, Oleg 1<br />
1 Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
Abstract<br />
By now, different types of scale-free behavior exhibited by auroral variations have been presented from analyzing<br />
ground-based and satellite imaging observations. Signatures of spatial and temporal scaling in the magnetosphereionosphere<br />
system have also been reported for fluctuations of electric and magnetic fields on the auroral field lines.<br />
Within the second order statistics, scaling properties of fluctuations can be characterized by scaling index. Using<br />
UVI images from the Polar satellite, we show that for auroral structures observed at the beginning of substorm<br />
expansion, the scaling index varies from values less than unity to 1.5, increasing with breakup progress. Similar<br />
scaling features are deduced at smaller scales from the ground-based observations. The observed auroral features are<br />
compared with the structures in the field-aligned current simulated by numerical model of non-linear interaction of<br />
current filaments according to the Chang et al. [2004] scenario. We discuss how the observed scaling in the aurora<br />
can be explained by its relation to scaling in the turbulent/scale-free electric fields and Alfvénic coherent structures.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
55<br />
Multi-scale auroral observations in Apatity: equipment and preliminary results<br />
Kozelov, Boris 1<br />
1 Polar <strong>Geophysical</strong> Institute, Russia<br />
Abstract<br />
New equipments contained of 5 cameras were installed at Kola Peninsula for observations of auroral structures at<br />
different scales: (i) all-sky TV camera LCL-902 (1/2” CCD) with Fujinon lens YV2.2×1.4A-SA2; (ii) two monochromatic<br />
cameras Guppy F-044B NIR (1/2”CCD) with Fujinon lens HF25HA-1B for 15 ◦ field of view and glass filter<br />
558 nm; (iii) two color cameras Guppy F-044C NIR (1/2”CCD) with Fujinon lens DF6HA-1B for 60 ◦ field of<br />
view. The cameras installed at the main building of Apatity division of PGI (67 ◦ 34’13"N, 33 ◦ 23’54"E) and at<br />
Apatity range (67 ◦ 34’42"N, 33 ◦ 18’35"E). The distance between these points is 3850 m, so the identical cameras<br />
are used as a stereoscopic system. For winter season 2010-2011 the equipment were upgraded by special blocks of<br />
GPS-synchronized time triggering, temperature control and motorized pan-tilt rotation mounts. All cameras are<br />
accessible and operated remotely via Internet. The observational complex is aimed to following scientific problems:<br />
(i) Scaling in small-scale structures of aurora; (ii) Spatial structure of pulsating aurora; (iii) Vertical distribution in<br />
rayed structures; (iv) Relations between proton and electron precipitations (as a support of spectral observations at<br />
Apatity range). The report presents preliminary analysis of the auroral events observed.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
56<br />
Long-term changes in the auroral occurrence in Finland and Svalbard<br />
Partamies, Noora 1 , Kauristie, Kirsti 1 , Ketola, Anneli 1 , Mattanen, Jyrki 2 and Mäkinen, Sanna 1<br />
1 FMI, Helsinki, Finland<br />
2 FMI, <strong>Sodankylä</strong>, Finland<br />
Abstract<br />
Digital all-sky camera (ASC) imaging of the aurora started in the MIRACLE network in late 90ś. While the first<br />
couple of seasons, there were only a few stations in routine operation, by the year 2000 already 7 ASCs were<br />
continuously monitoring the night sky above Finland and Svalbard. We used the quicklook data (keograms) from 5<br />
ASC stations to describe the solar cycle driven variation in the auroral occurrence in 2000-2010. The locations of<br />
our sample stations range over the auroral oval latitudes in the MIRACLE sector. The results reveal that during<br />
the past solar minimum the auroral occurrence decreased fastest and most significantly in the southern latitudes,<br />
remarkably in the average oval latitudes and least in the poleward part of the auroral oval. The available long time<br />
series of systematic auroral occurrence from several latitudinally spread stations is a unique data set but very tedious<br />
to investigate manually. Automated image analysis is required for more detailed studies of solar cycle variation in<br />
aurora.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
On tomography-like reconstruction from colour auroral images<br />
Partamies, Noora 1 , Sangalli, Laureline 2 , Gustavsson, Björn 3 , Syrjäsuo, Mikko 1 , Donovan, Eric 4 , Connors, Martin 5 ,<br />
Charrois, Dan 6 and Kryzanowsky, Zane 4<br />
1 FMI, Helsinki, Finland<br />
2 RMC, Kingston, ON, Canada<br />
3 University of Southampton, Southampton, UK<br />
4 University of Calgary, Calgary, AB, Canada<br />
5 University of Alberta, Athabasca, AB, Canada<br />
6 Syzygy Research & Technology, Legal, AB, Canada<br />
57<br />
Abstract<br />
We briefly describe a Canadian colour camera imaging system (Dense Array Imaging SYstem, DAISY) for aurora.<br />
The main goals of DAISY were to measure previously less observed scale sizes of the aurora, and to study the<br />
possibility of using colour images in tomography-like applications to determine the altitude distribution of the<br />
auroral emissions. Our first attempts to do auroral tomography on colour images show that the most dominant<br />
green (557.7 nm) emission line can be well-reconstructed with meaningful peak emission altitudes and horizontal<br />
scales. Fainter emissions at red (630.0 nm) and blue (427.8 nm and other N 2 emission) wavelengths could not be<br />
separated from the green spectral line due to the lack of spectral resolution of the colour CCD.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
58<br />
Characteristic energy in an auroral Spiral<br />
Frissell, Nathaniel A. 1 , Reistad, Jone Peter 2 , Partamies, Noora 3 and Lorentzen, Dag 4<br />
1 Virginia Tech, Blacksburg, USA<br />
2 University of Bergen, Bergen, Norway<br />
3 Finnish Meteorological Institute, Helsinki, Finland<br />
4 University Centre in Svalbard, Longyearbyen, Norway<br />
Abstract<br />
We are presenting a multi-instrument study of an auroral spiral observed during substorm conditions on February 17,<br />
2010 from the Kjell Henriksen <strong>Observatory</strong>, Svalbard. Probing the vicinity of the spiral using a meridian-scanning<br />
photometer reveals that the characteristic energy of the precipitating particles are increasing and decreasing as the<br />
spiral winds and unwinds as seen in the all-sky images. Also, the rate of energization is an order of magnitude larger<br />
than the de-energization rate. In terms of size, lifetime and winding direction this spiral is behaving according to<br />
existing theories. Evidence of an enhancement in the upward field-aligned current 30-45 seconds before the apparent<br />
maximum optical spiral winding is found in the magnetometer data. Optical intensities and hence the modelled<br />
energies also shows an intensification prior to the optical winding with the prior mentioned time. With a proxy<br />
in this time lag we are discussing where this spiral structure is likely to be formed. A rough trace back from the<br />
ionosphere with the Alfvén velocity for 45 seconds indicate that the observed disturbance formed about 17R E from<br />
the earth.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
59<br />
Pc2 auroral pulsations<br />
Roldugin, Valentin 1 , Roldugin, Alexey 1 and Pilgaev, Sergey 1<br />
1 Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
Abstract<br />
There are regular optical observations of aurora in Lovozero (ϕ = 68.0 ◦ N, λ = 35.0 ◦ E, φ = 64.4 ◦ , Λ = 114.3 ◦ ) by<br />
all sky camera ”Spica”. This camera consists of ”fish-eye” lens of model FE-0.8-MAO(4.2) manufactured by Main<br />
Astronomical <strong>Observatory</strong> UAS, and CCD F-046 Stingray. The frame rate is one per second, the resolution is 360<br />
x 360 pixels with two bytes per pixel.<br />
The event of 2 February 2011 morning is considered. During recovery phase of negative bay about of 40 nT<br />
between 0200 and 0400 UT some trains of geomagnetic pulsations Pc2 with 7.5 sec period and about of 0.04 nT<br />
intensity appeared. Near the northern horizon a homogeneous arc was observed, and to the South from it weak<br />
auroras with indistinct form were situated. We discriminate 11 circles in field of view: 3 near zenith and 8 along<br />
azimuth every 45 ◦ , and determine averaged light intensity in each circle. Thus obtained variations of luminosity<br />
with 1 sec resolution in different circles are compared with magnetic pulsations with 0.1 sec resolution.<br />
It is found that in the circles with aurora the luminosity variations correlate well with the geomagnetic Pc2<br />
pulsations. The ”pearl” structure is observed both in magnetic and auroral oscillations. The luminosity bursts are<br />
accompanied by positive half-periods in Z-component, by negative ones in D-component, and the positive peaks in<br />
H lag with the luminous peaks about of π/2.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
60<br />
Event Study of the Peak Auroral Emission Altitude from All-sky Images<br />
Sangalli, Laureline 1 , Gustavsson, Björn 2 , Partamies, Noora 3 and Kauristie, Kirsti 3<br />
1 Royal Military College, Kingston, Ontario, Canada<br />
2 University of Southampton, UK<br />
3 Finnish Meteorological Institute, Helsinki, Finland<br />
Abstract<br />
The MIRACLE network monitors auroral activity in the Fennoscandian sector of Europe. Network stations cover<br />
the range of 55 ◦ to 57 ◦ magnetic latitude North and span two hours in magnetic local time. Some of the MIRACLE<br />
network stations include digital all-sky cameras (ASC). Some of the ASCs currently in use are: systems with an<br />
image intensifier in front of a CCD (iCCD), systems with electron multiplying CCD (emCCD). Both iCCD and<br />
emCCD cameras in the MIRACLE network operate at three different wavelengths: 427.8 nm, 557.7 nm and 630.0<br />
nm. Each wavelength is selected using narrow band filters on a filter wheel placed in front of the CCD. Our goal is<br />
to evaluate the peak auroral emission altitude using ASC images at different stations pairs for a set of auroral event<br />
in order to evaluate the altitude of peak auroral emissions for different auroral structures. We adapted the AIDA<br />
software package developed by Björn Gustavsson in Kiruna for ASC images. Position calibrated images at two (or<br />
more) ASC stations are for optical triangulation of a set of auroral structures.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
61<br />
Multi-station optical study of substorm breakup auroral arcs<br />
Sergienko, Tima 1 , Axelsson, Katarina 1 , Gustavsson, Björn 2 , Sandahl, Ingrid 1 and Brändström, Urban 1<br />
1 Swedish institute of space physics, Kiruna, Sweden<br />
2 University of Southampton, Southampton, U. K<br />
Abstract<br />
This report presents a detailed case study of the temporal evolution of growth-phase and substorm breakup auroral<br />
arcs. On December 18, 2006 a substorm breakup was observed above Kiruna, Sweden with the high-resolution<br />
multi-station and multi-wavelength Auroral Large Imaging System (ALIS). Multi-station auroral observations allow<br />
us running tomography-like reconstruction of the volume distribution of auroral emissions. The 3D distribution of<br />
the volume emission rates was converted to characteristics of the precipitating auroral electrons and, thereby, the<br />
temporal and spatial dynamics of the auroral particles were studied. The event we have examined indicates: 1) the<br />
system of growth-phase arcs consisted of four auroral arcs with approximately same width (≈7–10 km) and same<br />
intensity in the green (557.7 nm) line; 2) the two most equatorward arcs were formed by more energetic electrons<br />
(>3 keV) while less energetic electrons (
62<br />
Two methods to forecast auroral displays<br />
Sigernes, Fred 1 , Dyrland, Margit 1 , Brekke, Pål 2 , Chernouss, Sergey 3 , Lorentzen, Dag Arne 1 , Oksavik, Kjellmar 1<br />
and Deehr, Charles 4<br />
1 UNIS, Longyearbyen, Norway<br />
2 Norwegian Space Centre, Oslo, Norway<br />
3 Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
4 <strong>Geophysical</strong> Institute, Fairbanks, USA<br />
Abstract<br />
This work compares the methods by Starkov (1994a) and Zhang & Paxton (2008), that calculate the size and location<br />
of the auroral ovals as a function of planetary Kp index. The ovals are mapped in position and time onto a solar<br />
illuminated surface model of the Earth. It displays both the night- and dayside together with the location of the<br />
twilight zone as Earth rotates under the ovals. The graphical display serves as a tool to forecast auroral activity<br />
based on the predicted value of the Kp index. The Zhang & Paxton (2008) ovals are wider in latitude than the<br />
Starkov (1994a) ovals. The nightside model ovals coincide fairly well in shape for low to normal auroral conditions.<br />
The equatorward border of the diffuse aurora is well defined by both methods on the nightside for Kp
Polarisation of emission lines in upper atmospheres of planets<br />
Simon Wedlund, Cyril 1 , Lamy, Hervé 1 , Barthélemy, Mathieu 2 , Lilensten, Jean 2 , Gronoff, Guillaume 3 , López<br />
Ariste, Arturo 4 and Bommier, Véronique 5<br />
1 Belgian Institute for Space Aeronomy BIRA-IASB, Brussels, Belgium<br />
2 Institut de Planétologie et Astrophysique IPAG-LPG, Grenoble, France<br />
3 NASA Langley Research Center, Hampton, VA, USA<br />
4 THEMIS, La Laguna, Tenerife, Spain<br />
5 LESIA, Observatoire de Paris, Paris, France<br />
63<br />
Abstract<br />
The polarisation of electromagnetic radiations is a key observable that enables the retrieval of essential information<br />
encoded in the emissions of planetary upper atmospheres. Polarisation may arise from spherical symmetry departures<br />
in the line or continuum formation, which in the case of space plasmas, may be due to magnetic or electric fields,<br />
scattering of directive radiation, scattering by aligned dust particles or direct impact from electrons or particles.<br />
In this paper, new spectropolarimetric observations of planetary upper atmospheres including those of Earth,<br />
Jupiter and Mercury are presented with special focus on the theoretics behind them.<br />
Recently, observations by Lilensten et al. (2008) and Barthélemy et al. (2011) reported that Earth’s auroral<br />
red line (λ = 6300 Å O I) is around 1–2% radially polarised, a much lower value than theoretically predicted by<br />
Bommier et al. (2011). Depolarisation processes involving collisions can explain these differences. Theory predicts<br />
that this measurement is not sensitive to the energy of precipitating electrons but can provide an estimate of their<br />
densities through depolarisation processes. A new dedicated spectropolarimeter currently built between BIRA and<br />
IPAG will provide better polarisation measurements of the auroral red line as well as that of other emissions (e.g.,<br />
λ = 8446 Å O I, λ = 4278 Å N + 2 1NG, other N 2 bands, etc.).<br />
At Jupiter, polarisation of the λ = 3.95µm H + 3 emission was observed in the auroral zone with the UKIRT<br />
telescope (Barthélemy et al., 2011): although no explanation exists at present, it may be due to local anisotropies<br />
such as electric and magnetic fields. At Mercury, the polarisation of the exospheric λ=5891 Å Na D 2 line was<br />
discovered using the solar telescope THEMIS (López Ariste et al., 2011): arising from solar light scattering in a<br />
collision-free exosphere, this polarisation is sensitive to the direction of the magnetic field (but not its intensity)<br />
through the Hanle effect and may also give upper limits for exospheric densities.<br />
Perspectives for future studies and how spectropolarimetry may help characterise planetary upper atmospheres,<br />
from airglow and aurorae to aerosols, will be discussed.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
64<br />
3D reconstruction of N + 2<br />
System (ALIS)<br />
and OI auroral emissions using the Auroral Large Imaging<br />
Cyril Simon Wedlund 1 , Hervé Lamy 1 , Björn Gustavsson 2 , Tima Sergienko 3 and Urban Brändström 3<br />
1 Belgian Institute for Space Aeronomy, BIRA-IASB, Brussels, Belgium<br />
2 Space Environment Physics Group, University of Southampton, UK<br />
3 Swedish Institute of Space Physics, IRF, Kiruna, Sweden<br />
Abstract<br />
In 2008 and 2009, coordinated campaigns were organised between the European Incoherent Scatter Radar (EISCAT)<br />
and the Auroral Large Imaging System (ALIS) situated in Northern Scandinavia in order to study stable discrete<br />
auroral arcs. With ALIS the N + 2 (4278 Å) 1NG band, the oxygen lines OI (5577 Å) and OI (6300 Å) can be observed<br />
and their profiles can be reconstructed in 3D by means of tomography-like reconstruction techniques.<br />
Inversions of the 3D reconstructed volume emission rate of N + 2 and of the electron densities measured by EISCAT<br />
yield energy spectra of the precipitating auroral electrons that can be used as input into transport kinetic/fluid models<br />
such as TRANS4.<br />
Both inversions give matching results with a typical average precipitation energy of a few keV. The spatial and<br />
temporal extent of the auroral arcs is assessed using average arc width in different wavelengths and the distribution<br />
of the characteristic electron energy as parameters.<br />
In the memory of Prof. Ingrid Sandahl, who has been the constant inspiration behind this work.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Statistical study of the peak auroral emission height using the MIRACLE all-sky<br />
camera network<br />
Whiter, Daniel 1 , Partamies, Noora 1 and Sangalli, Laureline 2<br />
1 Finnish Meteorological Institute, Helsinki, Finland<br />
2 Royal Military College of Canada, Kingston, Ontario<br />
65<br />
Abstract<br />
The aurora is often assumed to have a peak emission height of about 110 km. An assumed auroral height has been<br />
used in simple geometrical calculations to determine auroral horizontal spatial scales and optical flow velocities,<br />
among other properties. However, the height of the aurora is not constant, and the accuracy and validity of assumed<br />
heights are not clear. A statistical study of the auroral height using many years of observations will lead to more<br />
accurate assumed heights with quantitative error estimates, and therefore more accurate estimates of parameters<br />
derived using these assumed auroral heights. An automated correlation process for quickly determining the average<br />
peak auroral emission height of a structure observed by a pair of all-sky cameras will be presented, along with<br />
preliminary results of a statistical study using MIRACLE all-sky camera images.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
66<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
67<br />
Troposphere and stratosphere<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
68<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Studying gravity waves and turbulence in the stratosphere using satellite observations<br />
of stellar scintillation<br />
Sofieva, Viktoria 1<br />
1 Finnish Meteorological Institute, Helsinki, Finland<br />
69<br />
Abstract<br />
Stellar scintillation observed through the Earth atmosphere is the result of interaction of light wave and turbulent<br />
atmosphere. This presentation is dedicated to using satellite stellar scintillation measurements for studies of gravity<br />
waves and turbulence in the Earth atmosphere. A methodology for retrieving the information about the small-scale<br />
air density irregularities from scintillation measurements is discussed. The overview of the main geophysical results<br />
that are obtained from EFO-2/MIR and GOMOS/Envisat fast photometer measurements is presented. The benefits<br />
of the scintillation method in studies of the structure of air density irregularities and its limitations will be also<br />
discussed.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
70<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
71<br />
Radiation and atmospheric components<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
72<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
The annual cycle of precipitable water vapor over the Iberian Peninsula inferred from<br />
MODIS observations and its comparison with GPS data<br />
Bennouna, Yasmine 1 , Ortiz de Galisteo, Jose Pablo 2 , Cachorro, Victoria 1 , Toledano, Carlos 1 , Berjón, Alberto 3 ,<br />
Fuertes, David 1 , Gonzalez, Ramiro 1 , Torres, Benjamin 1 , Marcos, Jose Luis 4 , Martín, Leticia 1 and de Frutos, Angel<br />
Maximo 1<br />
1 Atmospheric Optics Group (GOA), University of Valladolid, Valladolid, Spain<br />
2 Meteorological State Agency of Spain (AEMET), Territorial Delegation of Castilla y León, Valladolid, Spain<br />
3 Izaña Atmospheric Research Center, Meteorological State Agency of Spain (AEMET), Santa Cruz de Tenerife,<br />
Spain<br />
4 Department of Agriculture and Forestry Engineering, University of Valladolid, Palencia, Spain<br />
73<br />
Abstract<br />
Water vapor is well known to be the most dominant greenhouse gas in the Earth’s atmosphere, and yet its high<br />
variability in both space and time constrains our understanding of the global energy and water balance. To study<br />
the spatial and temporal distribution of water vapor amount, one of the most common term is precipitable water<br />
vapor (PWV), referring to column integrated water vapor.<br />
The locations of ground monitoring stations are sparse, and the periods covered by the datasets are generally<br />
limited to a few years. In order to monitor drought conditions and characterize regional climatic variability, a<br />
detailed description of seasonal and annual changes in PWV on regional scales is essential. There is thus a crucial<br />
need for accurate remote sensing techniques that can provide water vapor information on a daily basis with a spatial<br />
resolution of the order of 1 to 5 km and over a long period of time. With the deployment of a new generation<br />
of earth observation satellites in the past decade, considerable improvement of coverage and quality of remotely<br />
sensed moisture parameters has been achieved. The MODIS (Moderate Resolution Imaging Spectrometer) sensor<br />
flown on the Terra and Aqua satellites is well suited for the monitoring of atmospheric properties from space. The<br />
standard MODIS level 2 products MOD05(Terra) and MYD05(Aqua) provide two different PWV datasets based on<br />
the retrievals of independent algorithms: the MODIS near-infrared algorithm (for daytime only), and the MODIS<br />
infrared algorithm (for both night and day). Near-infrared PWV data are given at a resolution of 1x1 km, and<br />
infrared PWV data at a resolution of 5x5 km.<br />
This study comes to complement a previous study on the annual cycle of precipitable water vapor (PWV) over<br />
the Iberian Peninsula derived from 7 years of GPS, Radio Sounding and sun photometer data. Here, the annual<br />
cycle of PWV is derived from satellite data of both MODIS Terra and Aqua for the same period (2002-2008), at<br />
18 sites of the Iberian Peninsula. At all sites the annual cycle presents the typical shape with low values in the<br />
winter and high values in the summer, and the north-south gradient is clearly depicted. The differences between the<br />
two techniques used to derive the PWV from MODIS observations (i.e. infrared and near infrared) are estimated.<br />
Besides, these annual cycles are evaluated by means of comparison with those obtained with the GPS network.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
74<br />
Theoretical validation of the method of retrieval of atomic oxygen altitude profile<br />
from intensity of the electronic-vibrationally excited molecule O 2 (b 1 Σ + g , v=2) emission<br />
in the MLT<br />
Yankovsky, Valentine 1 and Fedotova, Ekaterina 1<br />
1 Atmospheric Physics Department of St. Petersburg State University, St. Petersburg, Russia<br />
Abstract<br />
There is a problem of determining the vertical profile of concentration of atomic oxygen O( 3 P), in the lower thermosphere<br />
and the mesosphere above the mesopause. The study shows that the volume emission rate generated by<br />
emissions from excited levels of molecules O 2 (b 1 Σ + g , v=0-2) depend strongly on the vertical profiles of [O( 3 P)], [O 3 ]<br />
and other atmospheric components.<br />
For a comparative analysis of the influence of these factors on the profiles of [O 2 (b 1 Σ + g , v=0-2)] the modern<br />
model of kinetics of electronic-vibrationally excited products of photodissociation of ozone and molecular oxygen in<br />
the Earth’s middle atmosphere, YM2010, are used [1]. Model YM2010 takes into account 27 processes of production<br />
and deactivation of excited levels of oxygen molecules in the states O 2 (b 1 Σ + g , v=0-2) including the processes of O 2<br />
photodissociation in the Schumann-Runge continuum, J(SRC), and in Lyman-Alpha line , J(Ly α ), O 3 photodissociation<br />
in the Hartley band, J(Hartley), and resonant absorption of solar radiation by O 2 molecules in the bands<br />
762, 689 and 629 nm, J(b0), J(b1), J(b2), respectively. In order to clarify the role of atomic oxygen in the formation<br />
of vertical profiles of O 2 (b 1 Σ + g , v=0-2), we carried out the sensitivity analysis of the model to variations of the<br />
following parameters: J(SRC), J(Ly α ), J(Hartley), J(b0), J(b1), J(b2), [O 3 ], [N 2 ], [O 2 ], Tg, quantum yields and rate<br />
constants of aeronomical reactions.<br />
It is shown, that the profile of [O 2 (b 1 Σ + g , v=2)] significantly more sensitive to variations of atomic oxygen<br />
concentration than the profiles of [O 2 (b 1 Σ + g , v=0-1)] [2]. It is important to note, that the height profile of [O 2 (b 1 Σ + g ,<br />
v=2)] does not depend on ozone concentration. The results of sensitivity analysis allowed us to formulate and solve<br />
the inverse problem of retrieval of [O( 3 P)] vertical profile from the height profile of [O 2 (b 1 Σ + g , v=2)] in the altitude<br />
range 85-120 km. Approbation of the proposed method of [O( 3 P)] retrieval was based on numerical simulation using<br />
the data on atmospheric models for the satellite TIMED-SABER experiment.<br />
1. Yankovsky V.A., Manuilova R.O. Model of daytime emissions of electronically-vibrationally excited products<br />
of O 3 and O 2 photolysis: Application to ozone retrieval. Annales Geophysicae, 2006, 24, 11, 2823.<br />
2. Yankovsky V.A., Fedotova E.A. New method for retrieving the atomic oxygen vertical profile from measured<br />
intensity of the emission of electronically-vibrationally excited O 2 band in the mesosphere and lower thermosphere,<br />
5 international conference ’Atmospheric physics, climate, and environment’, 2010, 64.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Longterm CO 2 changes in the tropo-stratosphere from in situ and optical measurements<br />
Gavrilov, N. M. 1 , Semyonov, V. K. 2 , Sinyakov, V. P. 2 , Tans, P. 3 , Guenther, D. 4 and Kashin, F. V. 5<br />
1 Saint-Petersburg State University, Atmospheric Physics Dept., Petrodvorets,198504, Russia<br />
2 Kyrgyz National University, Institute of Fundamental Research, Bishkek, Kyrgyzstan<br />
3 Climate Monitoring and Diagnostics Laboratory, NOAA, Boulder, USA<br />
4 Cooperative Institute for Research in Environmental Sciences, University of Colorado, Boulder, USA<br />
5 Institute of Experimental Meteorology, SPA ”Typhoon”, Obninsk, Russia<br />
75<br />
Abstract<br />
Spectroscopic measurements of CO 2 mixing ratio are important for validating existed and future satellite observations.<br />
Therefore, validating and improvement of main assumptions used in spectroscopic CO 2 studies are of interest.<br />
Spectroscopic measurements of CO 2 contant in the atmospheric column have been made since year 1980 at the<br />
Issyk-Kul station (42 o N, 77 o E). One of the main assumptions of the method is constant CO 2 mixing ratio at all<br />
altitudes in the atmosphere. In this study we analyze vertical changes of CO 2 mixing ratio and its seasonal variations<br />
in the troposphere from the data of flask aircraft measurements at Carr (41 o N, 105 o W) during many years. These<br />
measurements are made over Rocky Mountains at approximately same latitude as Issyk-Kul station. The results are<br />
compared with optical CO 2 measurements and surface data for sites close to Carr and Issyk-Kul station. Statistical<br />
analysis of airplane, surface and optical CO 2 measurements over USA and Middle Asia during many years shows<br />
that general trends and seasonal CO 2 variations are almost the same at all altitudes 3 – 8 km in well mixed region<br />
over Rocky Mountains. Surface and low-altitude CO 2 variations show larger dependence on local conditions. Optical<br />
measurements give information about CO 2 variations mainly in free troposphere, which are more homogeneous over<br />
the globe.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
76<br />
GOMOS/ENVISAT overview<br />
Kyrölä, Erkki 1<br />
1 Finnish Meteorological Institute, Helsinki, Finland<br />
Abstract<br />
GOMOS (Global Ozone Monitoring by Occultation of Stars) on ESA’s Envisat-satellite measures transmission of<br />
light through the Earth’s atmosphere in the limb direction using the stellar occultation method. From transmissions<br />
it is possible to retrieve vertical density profiles of ozone, NO 2 , NO 3 , H 2 O, O 2 , and aerosols in the stratosphere and<br />
ozone also in the MLT region. High-resolution temperature profiles in the 15–35 km altitude range can be retrieved<br />
using data from the two fast photometers. In this presentation we will show main scientific results from GOMOS<br />
during the nine years in operation. We will show climatological and time series analysis of ozone, NO 2 , NO 3 from<br />
2002–2011. Results about OClO, mesopause sodium layer, polar mesospheric clouds, gravity waves and turbulence<br />
and impact of energetic particles on polar NO y and ozone will be highlighted. We also review the development of<br />
the GOMOS data quality during 2002–2011.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
77<br />
Long-term Arctic and Antarctic UV measurements<br />
Lakkala, Kaisa 1<br />
1 Finnish Meteorological Institution, Finland<br />
Abstract<br />
The Earth’s ecosystems are protected from the dangerous part of the solar ultraviolet (UV) radiation by stratospheric<br />
ozone, which absorbs most of the harmful UV wavelengths. Severe depletion of stratospheric ozone has been observed<br />
in the Antarctic region, and to a lesser extent in the Arctic and mid-latitudes. Concern about the effects of increasing<br />
UV radiation on human beings and the natural environment has led to ground based monitoring of UV radiation.<br />
The Finnish Meteorological Institute (FMI) was among the first institutes to monitor UV radiation at high northern<br />
latitudes, in areas where spring-time polar stratospheric ozone loss was observed. Spectral UV measurements were<br />
started in 1990 at the FMI Arctic Research Centre at <strong>Sodankylä</strong> (67N). There, due to stratospheric dynamics, the<br />
natural variability in UV radiation is high, especially in springtime. The variability is enhanced by the influence<br />
of the ground snow cover, whose amount and duration vary from year to year. This combination, together with<br />
the possible chemical ozone loss, makes measurements at the site important from an ecological point of view.<br />
The Antarctic NILU-UV network was founded in 1999 and 2000 as a Spanish-Argentinian-Finnish co-operation<br />
project. Three NILU-UV multichannel filter radiometer have been setup at Antarctic stations in order to monitor<br />
ground-based ozone, UV and photosynthetically active (PAR) radiation. The location of the stations with respect<br />
to the stratospheric polar vortex is interesting, as the vortex plays an important role in the mechanism of ozone<br />
depletion. Belgrano, (77S), is mostly located inside the vortex; Marambio (64S) is at various time inside, on the<br />
edge of, or outside the vortex, while Ushuaia (54S) is mostly outside the vortex. Ushuaia is one of the few inhabited<br />
towns situated in an area of severe Antarctic ozone loss. These stations make possible real-time studies of the<br />
impact of daily changes in the polar vortex on total ozone and UV radiation reaching the ground. Atmospheric<br />
conditions both in Finland and in the Antarctic region are challenging for UV measurements: e.g., most of the<br />
measurements are performed at high solar zenith angle (SZA), most of the time the sky has changing cloud cover,<br />
and the temperatures below freezing occur during wintertime. The key question and the most challenging part of<br />
the UV radiation measurements is the quality control (QC) and quality assurance (QA) of the data. This QC/QA<br />
includes daily maintenance, laboratory characterizations, corrections for all known measurement errors, and control<br />
of the homogeneity of the data time series. Only homogeneous time series allow the drawing of conclusions regarding<br />
long-term changes in the UV radiation amount.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
78<br />
Retrieval of ozone altitude profile from O 2 (b 1 Σ g , v=0,1) emission intensity in the middle<br />
atmosphere<br />
Yankovsky, Valentine 1 , Martishenko, Xenia 1 and Manuilova, Rada 1<br />
1 St.Petersburg State University, St. Petersburg, Russia<br />
Abstract<br />
The study considers the possibility of retrieval of ozone vertical profile from observations of emissions of molecules<br />
O 2 (b 1 Σ g , v=0,1). For the analysis we used a model of electronic-vibrationally excited products of photodissociation<br />
of ozone and molecular oxygen in the mesosphere and lower thermosphere, YM2010 [1]. Using YM2010 model in the<br />
direct problem we calculated the vertical profiles of O 2 (b 1 Σ g , v=0), O 2 (b 1 Σ g , v=1) and O( 1 D) concentrations. In<br />
the calculations we used the atmospheric models from the series of events TIMED-SABER satellite experiment (for<br />
middle latitudes), as well as the rates and quantum yields of 27 aeronomical reactions and the rates of O 3 photolysis<br />
in the Hartley band and O 2 photolysis in the Schumann-Runge continuum and Lyman-α line. In the inverse problem<br />
the calculated concentration of O 2 (b 1 Σ g , v=0) and O 2 (b 1 Σ g , v=1) were considered as known and used to retrieve<br />
the height profile of ozone. For this purpose we analyzed the sensitivity of the model of electronic- vibrational<br />
kinetics of the photolysis of O 2 and O 3 depending on the variations of all model parameters (the concentrations of<br />
atmospheric components, gas temperature, photodissociation rates, reaction rate constants and quantum yields of<br />
the products of these reactions) [2]. As a result, the components and reactions which have the greatest influence<br />
on the calculations have been revealed.O 2 (b 1 Σ g , v=1) concentration has a higher sensitivity to variations of ozone<br />
in the altitude range 50-92 km in comparison with O 2 (b 1 Σ g , v=0) concentration. O 2 (b 1 Σ g , v=0) has a relatively<br />
high sensitivity to variations of ozone at altitudes interval 90–103 km. Along with a complete solution of the inverse<br />
problem the parameterization of solution, in which the reactions with the lowest sensitivity is ignored, is considered.<br />
Work is supported by RFBR grant 09-05-00694.<br />
1. Yankovsky V.A., Manuilova R.O. Model of daytime emissions of electronically-vibrationally excited products<br />
of O 3 and O 2 photolysis: Application to ozone retrieval. Annales Geophysicae, 2006, 24, 11, 2823. 2. Yankovsky<br />
V. A., Kuleshova V. A. Model of daytime emissions of electronically-vibrationally excited products of O 3 and O 2<br />
photolysis: sensitivity analysis of direct and inverse problems 37th Annual European Meeting on Atmospheric Studies<br />
by Optical Methods, 23-27 August 2010, Valladolid, Spain; http://goa.uva.es/37AM/media/presentaciones/7.<br />
5-VA_Yankovsky.pdf, 2010.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Comparison of satellite and ground-based spectroscopic measurements of HF total<br />
column amount<br />
Yagovkina, Irina 1 , Polyakov, Alexander 1 , Timofeyev, Yuri 1 and Walker, Kaley 2<br />
1 Saint-Petersburg State University, Saint-Petersburg, Russia<br />
2 University of Toronto, Toronto, Ontario , USA<br />
79<br />
Abstract<br />
During 2009–2010 near St.Petersburg (Russia) the values of HF total column amount were derived from groundbased<br />
measurements of direct solar radiation by Fourier-spectrometer Bruker FS-125. Different estimates of errors<br />
of ground-based measurements have shown that random and systematic errors are 1–5% and 5–6%, respectively.<br />
Comparison of ground-based HF measurements with data of ACE FTS instrument demonstrated good agreement<br />
with consideration for measurement errors of both instruments and spatial-temporal mismatch. This work has been<br />
partly supported by Min. Education and Science grants in the frame of Federal Purposive Program ”Scientific and<br />
Educational Pool of Innovational Russia” P969 from 27.05.2010.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
80<br />
Possibility of ozone and atomic oxygen retrievals from measured intensities of the<br />
molecule O 2 (b1Σ+g,v≤ 2) emissions in the mesosphere and lower thermosphere.<br />
Yankovsky, Valentine 1 , Manuilova, Rada 1 and Semenov, Aleksey 1<br />
1 Atmospheric Physics Department of St. Petersburg State University, St. Petersburg, Russia<br />
Abstract<br />
The extended model (YM2006) of photodissociation of O 2 and O 3 in the mesosphere and lower thermosphere<br />
(Yankovsky V.A., Manuilova R.O., Annales Geophysicae, 2006, V 24, N 11, P 2823) is used for detailed analysis<br />
of electronic-vibrationally excited levels O 2 (b 1 Σ + g ,v≤ 2) populations. In the framework of this problem system<br />
of kinetic balance equations were considered for 4 levels: 3 electronic-vibrationally excited levels O 2 (b 1 Σ + g ,v≤ 2)<br />
and first excited level of atomic oxygen O( 1 D). Besides of photolysis of O 3 in Hartley bands, photolysis of O 2 in<br />
the Schuman-Runge continuum and Lyman-α line and excitation of all three considered vibrational levels of the<br />
electronic state O 2 (b 1 Σ + g ) due to direct absorption of solar radiation in 762, 689, 629 nm bands are considered. All<br />
processes of quenching of excited states O 2 (b 1 Σ + g ,v≤ 2) and O( 1 D) in collision with O( 3 P), O 2 , N 2 , O 3 and CO 2<br />
are taken into account. In whole, 27 processes of excitation and deactivation of O 2 (b 1 Σ + g ,v≤ 2) and O( 1 D) levels<br />
were included. Using the sensitivity study we have shown that the altitude profiles of O 2 (b1Σ+g, v≤ 2) populations<br />
substantially depend on O( 3 P) and O 3 concentrations. In the altitude interval 85–120 km excited level O 2 (b1Σ+g,<br />
v=2) is deactivated mainly in collisional processes with O( 3 P). The altitude profile of O 2 (b 1 Σ + g , v=1) population is<br />
mainly connected with [O 3 ] altitude dependence. The altitude profile of O 2 (b1Σ+g, v=0) population depends both<br />
on [O 3 ] and [O( 3 P)] altitude profiles. The study shows the possibilities of ozone and atomic oxygen retrievals from<br />
measured intensities of different emissions from excited levels O 2 (b 1 Σ + g , v=0, 1, 2) in the mesosphere and lower<br />
thermosphere. The work was partly supported by RFBR grant 09-05-00694.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
81<br />
Instrumentation and techniques<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
82<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
83<br />
A gravity wave spectrometry from space and ground<br />
Alpatov, Victor 1 and Belyaev, Alexey 1<br />
1 Institute of Applied Geophysics, Moscow, Russia<br />
Abstract<br />
There are no methods that are currently in use that can obtain the three-dimensional wave number (3D) spectrum<br />
of the atmospheric gravity waves (GW). The aim of this work is to develop the methodology which can be used<br />
to infer the 3D GW spectra from the images obtained by ground-based and space-borned airglow imagers. The<br />
method is developed to estimate 3D spectrum parameters directly from a set of the images obtained under different<br />
foreshortenings. It is shown how the data obtained by a space-borned airglow imager may be treated to infer<br />
the 3D wave number spectrum of the temperature fluctuations caused by the GW-ensemble. We describe also a<br />
configuration of several airglow imagers which are to be placed on the ground to achieve multiple perspectives of the<br />
emission layer as it is perturbed by gravity waves. This approach is demonstrated by the results of a simulation.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
84<br />
The central slice theorem for a gravity wave spectrometry<br />
Belyaev, Alexey 1<br />
1 Institute of Applied Geophysics, Moscow, Russia<br />
Abstract<br />
It is derived the Fredholm equation of the first kind, which describes the relations between the GW spectrum and<br />
the horizontal structure of the airglow wave perturbations registered by the airglow imager. This equation can be<br />
seen as an analogue of the projection-slice theorem (or central-slice theorem) in the computer tomography. It is<br />
shown that its solution is a central slice through 3D GW spectrum. The plane of this slice is perpendicular to the<br />
optical axis of the airglow imager. Thus, in order to retrieve the 3D GW spectrum from the airglow observations it<br />
is needed to obtain a set of the images of the local area of the emission layer under various foreshortenings.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Calibrating auroral cameras<br />
Brändström, Urban 1 , Wang, Zilu 1 , Sergienko, Tima 1 , Gustavsson, Björn 2 , Axelsson, Katarina 1 , Enell, Carl-<br />
Fredrik 3 , Mäkinen, Sanna 4 and Sigernes, Fred 5<br />
1 Swedish Institute of Space Physics, Kiruna, Sweden<br />
2 University of Southampton, Southampton, U. K<br />
3 <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong>, <strong>Sodankylä</strong>, Finland<br />
4 Finnish Meteorological Institute, Helsinki, Finland<br />
5 The Kjell Henriksen <strong>Observatory</strong>, UNIS, Longerbyen, Norway<br />
85<br />
Abstract<br />
This paper is presented in memoriam: Professor Ingrid Sandahl 1949-2011.<br />
Absolute calibration of auroral photometers has a long history in the optical communities. The main means<br />
of calibration has been low-light sources inter-calibrated at regular calibration workshops held during the optical<br />
meetings. This technique was to some extent inherited when the need for accurate absolute calibration of auroral<br />
imagers arose in the late 1980’s. However, calibrating an auroral imager is a significantly more difficult task. Before<br />
absolute calibration, the instrument signature must be removed. For wide field-of-view imaging the major obstacle<br />
here is obtaining an acceptable flat-field correction image, but there are also other problems related to this.<br />
Three methods are currently in use for absolute calibration of auroral imagers: (1) The traditional method<br />
involving inter-calibrated low-intensity light-standards; (2) High-intensity light-standards combined with Lambertian<br />
screens (or integrating spheres) and Neutral-Density (ND) filters; and (3) Techniques involving imaging of catalogue<br />
stars with well-known spectras. While each of these methods can provide acceptable results, the last one also takes the<br />
atmosphere and domes into account; most notably, it can be applied directly on the measurement site. Unfortunately<br />
these three methods are not compared on a regular basis and actions should be taken by the community to remedy<br />
this.<br />
The task of mapping the field-of-view of each pixel to the observed object is called geometrical calibration. A<br />
common, well-developed method is to obtain a set of star-images for each of the viewing directions under consideration.<br />
Then the positions of the stars are calculated from a star catalogue and mapped down to the image coordinates.<br />
Then preferably more than 100 stars, evenly distributed across the image, are identified. Finally a transfer function<br />
is adjusted so that the calculated and actual positions of the stars overlap. This transfer function is then used to<br />
calculate the field-of-view of each pixel of the CCD.<br />
This paper will discuss the various calibration techniques for auroral imagers and present preliminary results<br />
of a recent comparison of traditional absolute calibration of ALIS with a calibration using well-known spectras of<br />
catalogue stars.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
86<br />
Multi-spectral LIDAR system — Design, build and test<br />
Fastig, Shlomo 1 , Ehrlich, Yossi 1 , Pearl, Shaul 1 , Naor, Eran 1 , Kraus, Yaniv 1 , Inbar, Tuvia 1 and Katz, David 1<br />
1 Soreq NRC, Yavne, Israel<br />
Abstract<br />
Long range, UV-IR combined LIDAR system was built and tested. The systemś modes of operation are: multiwavelength<br />
DIAL in the IR (8–11 µm), dual excitation wavelengths LIF LIDAR in the UV, and aerosol optical<br />
scattering for mapping and tracking at 1.5 µm. The IR transmitter is a continuous tunable solid-state Tandem<br />
Optical Parametric Oscillator (OPO) that was developed and built at Soreq. The first OPO stage generates a 1.5<br />
µm beam and which is used to a second OPO stage to generates the continuously tunable IR band. In the UV<br />
the transmitter generates and transmits either the 266 nm or the 355 nm wavelengths sequentially to generate LIF<br />
measurements simultaneously at 8 bands spanning ≈200 nm, starting from 280 nm and above. All the outgoing<br />
laser beams are aligned to ensure geometric overlap over the measured paths. Energy references are measured for<br />
each beam on every pulse. The receiver is based on a single reflective telescope with coatings optimized for both<br />
the UV and the IR. The optical signal received is routed between the different detection packages of the receiver<br />
by means of a fast computerized optical scanner mirror. The receiver-transmitter layout is based on the periscope<br />
geometry and is equipped with a large θ-φ scanner. Computer control enables fast switching between the different<br />
types of measurement and wavelengths, the data acquisition and the spatial scan as well. The system was built<br />
inside a mobile trailer and was field tested to discriminate different aerosol types in a complex environment.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
87<br />
Wind measurements by Doppler lidar<br />
Hildebrand, Jens 1 , Baumgarten, Gerd 1 , Fiedler, Jens 1 , Lübken, Franz-Josef 1 and von Cossart, Götz 1<br />
1 Leibniz-Institute of Atmospheric Physics, Kühlungsborn, Germany<br />
Abstract<br />
Wind measurements are essential for a comprehensive understanding of dynamical and thermal processes in the<br />
atmosphere. Winds determine the filtering of waves and reflect the balance between sources and sinks of energy<br />
and momentum. Unfortunately wind measurements are difficult in a large part of the middle atmosphere between<br />
about 30 and 70 km. This region is too high for balloons and the absence of free electrons prevents radar soundings.<br />
Rockets and satellites may cover part of this region but the first allow only sporadic snapshots while the latter have<br />
limited horizontal and temporal resolution. The Rayleigh/Mie/Raman (RMR) lidar at the ALOMAR observatory<br />
in Northern Norway (69 ◦ N, 16 ◦ E) covers the whole altitude range between about 15 and 90 km. Since 1997<br />
it measures temperatures and aerosols on routine basis and is fully daylight capable. During the last years it<br />
was successfully upgraded to additionally determine winds in the middle atmosphere. The technique is based on<br />
measuring the Doppler shift of light backscattered from moving molecules using the steep edge of an iodine absorption<br />
line. This requires a sophisticated laser and detection control since the relative Doppler shift is on the order of only<br />
∆ν/ν ∼ 10 −8 –10 −7 . The frequency of the transmitter is controlled by injection-seeding with an extremely stable<br />
seed laser and monitored to take offsets into account. Additionally the performance of the detection system is<br />
investigated continuously during measurement. The ALOMAR RMR lidar is designed as a twin system: it uses<br />
two transmitting lasers (each 150 MW peak power) and two independently tiltable telescopes (each 1.8 m diameter<br />
primary mirrors) which allows measuring vertical profiles of two wind components simultaneously. The retrieval<br />
currently provides winds in aerosol free parts of the middle atmosphere without external calibration. First results<br />
show good agreement with winds derived by radar, sodium resonance lidar and ECMWF re-analyses. We present<br />
our technical setup for wind measurements in the middle atmosphere and first results obtained during the last three<br />
years.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
88<br />
Numerical modeling of sounding of the atmosphere based on combined IR and microwave<br />
measurements on board ”Meteor-3M” satellite<br />
Polyakov, Alexander 1 , Timofeyev, Yuri 1 , Uspensky, Alexander 2 and Kostsov, Vladimir 1<br />
1 Saint-Petersburg state university, Saint-Petersburg, Russia<br />
2 SRC ”Planeta”, Moscow, Russia<br />
Abstract<br />
The technique for temperature-humidity sounding of the atmosphere based on combined IR and microwave measurements<br />
by IKFS-2 and MTVZA-GYa instruments onboard «Meteor-3M» satellite has been developed. The<br />
method provides the possibility for both separate and joint interpretation of IR and microwave measurements for<br />
cloudy conditions (cloud parameters - the height of upper boundary and the cloud amount are derived independently).<br />
The technique is based on the linear regression method and a non-linear implementation of the optimal<br />
estimation method. The proposed method was tested and analyzed by means of closed-loop numerical experiments.<br />
Ensemble of atmospheric parameters used in the numerical experiments included profiles of temperature, humidity,<br />
ozone, methane, nitrogen dioxide and also cloud amount, cloud liquid water content, surface temperature and emissivity.<br />
Errors of the retrieval of temperature and humidity profiles, cloud and surface characteristics and mixing<br />
ratio values for greenhouse gases have been estimated under different conditions of satellite measurements. This<br />
work has been partly supported by grant of Russian Foundation for Basic Research 09-05-00797-a.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Mobile unit for optical instruments installation at Barentsburg observatory.<br />
Roldugin, Alexey 1 , Chernouss, Sergey 1 , Pilgaev, Sergey 1 , Kuznetsova, Marina 1 , Milichenko, Alexander 2 and Fedorenko,<br />
Yuri 1<br />
1 Polar geophysical institute, Apatity, Russia<br />
2 Polar geophysical institute, Murmansk, Russia<br />
89<br />
Abstract<br />
Mobile unit for optical instruments installation at Barentsburg observatory.<br />
Roldugin A.V., Pilgaev S.V., Kuznetsova M.V., Chernouss S.A., Milichenko A.N., Fedorenko Yu.V. Polar <strong>Geophysical</strong><br />
Institute of KSC RAS, Apatity-Murmansk.<br />
The mobile research unit is created in the Polar <strong>Geophysical</strong> Institute in 2010. This unit is designed to accommodate<br />
the scientific equipment used for carrying out of regular observations and special experiments. It is<br />
a standard 20-foot container, equipped with a powerful thermal insulation, temperature control system and nodes<br />
for the installation and holding of optical equipment. The unit is easily transported by a lorry, train and ship and<br />
can be installed at any minimally prepared site. It protects indoor equipment against any weather. To bring the<br />
equipment located in the unit to operating condition, it is sufficient to connect the Internet network cable and a<br />
power cable with 220 V voltage. The unit is divided into two rooms, one is designed for assemblage and adjustment<br />
of instrumentation, as well as the placement of data acquisition system and personnel accommodation, and<br />
second one is designed for optical equipment installation. The unit is currently equipped with a black-white all-sky<br />
CCD camera, visible range meridianal CCD spectrometer, and will be equipped by hiperspectral emission imager<br />
in frame of NORUSKA-2 programme for simultaneous observations by identical cameras at Barentsburg and KHO<br />
observatories in 2011–2012 years.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
90<br />
Novel MEMS and Piezoactuated Fabry-Perot spectral imagers for atmospheric studies<br />
Saari, Heikki 1<br />
1 VTT Technical Research Centre of Finland, Espoo, Finland<br />
Abstract<br />
Push broom imaging spectrometers has been used in instruments like GOMOS, SCIAMACHY, OMI and GOME.<br />
In these instruments the light is dispersed by means of a prism or by a diffraction grating. These push broom<br />
instruments form a 2D image on detector in which one axis is spectral and the other spatial dimension making it<br />
impossible to get an image of the atmospheric limb instantaneously. In ALTIUS (Fussen et.al.) the concept is to<br />
use the entire detector as an imager of the atmospheric limb to solve the tangent altitude registration problem (ref.<br />
http://altius.oma.be). In ALTIUS the acousto-optical tunable filters (AOTF) are used. A similar type of mission<br />
titled ”Spectral Imaging of Middle Atmosphere for Climate Change (SIMACC)”was proposed by Erkki Kyrölä, et.al.<br />
in response to ESA Call. In SIMACC instrument the Fabry-Perot Interferometer (FPI) tunable filters are used. The<br />
advantages of FPI technology over AOTF technology are higher optical throughput and flexibility in the wavelength<br />
range.<br />
This paper describes the technology and properties of the MEMS and Piezo-actuated FPI modules and spectral<br />
imagers based on them. The instrument concepts to utilize this technology in atmospheric studies will also be<br />
discussed. VTT has developed MEMS and Piezo-actuated Fabry-Perot Interferometer (FPI) modules for miniaturized<br />
spectrometers covering spectral regions from UV to thermal IR since 1990. This technology enables to build<br />
extremely compact imaging spectrometers. VTT has built a spectral imager for UAV that can be used in forest<br />
and agriculture applications. It is based on a Piezo-actuated FPI accompanied with a 5 Mpixel RGB CMOS image<br />
sensor. The mass of the spectral imager is less than 400 grams, and dimensions are 120 mm x 60 mm x 60 mm. The<br />
MEMS FPI is a monolithic device, i.e. it is made entirely on one substrate in a batch process, without assembling<br />
separate pieces together like in Piezo-actuated device. The gap is adjusted by moving the upper mirror with electrostatic<br />
force, so there are no actual moving parts. Benefit of the MEMS FPI is a low mass. The spectral imager<br />
based on MEMS FPI has been selected as the main Earth observation payload for the Finnish Student satellite,<br />
Aalto-1 by Aalto University.<br />
References<br />
1. Praks, J., et al. ”Aalto-1: Multi-Payload, Remote Sensing Nanosatellite Mission”, 1st IAA Conference on<br />
University Satellite missions and CubeSat Workshop, Rome, January 24-29, 2011.<br />
2. Saari, H., et.al., ”Novel hyperspectral imager for lightweight UAVs”, Proc. SPIE 7668 (2010).<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
A new auroral hyperspectral all-sky camera<br />
Sigernes, Fred 1 , Ivanov, Yuriy 2 , Chernouss, Sergey 3 , Trondsen, Trond 4 , Roldugin, Alexey 3 , Fedorenko, Yury 3 ,<br />
Kozelov, Boris 3 , Kirillov, Andrey 3 , Safargaleev, Vladimir 3 , Dyrland, Margit 1 , Lorentzen, Dag 1 and Oksavik, Kjellmar 1<br />
1 UNIS, Longyearbyen, Norway<br />
2 Main Astronomical <strong>Observatory</strong>, Kiev, Ukraine<br />
3 Polar <strong>Geophysical</strong> Institute, Apatity, Russia<br />
4 Keo Scientific Ltd., Calgary, Canada<br />
91<br />
Abstract<br />
A prototype auroral hyperspectral all-sky camera has been constructed that uses electro-optical tunable filters to<br />
image the night sky as a function wavelength in the visible with no moving mechanical parts. The core optical<br />
system includes a new high power all-sky lens with F-number equal to f/1.1. The camera is capable of detecting a<br />
few kR aurora at an exposure time of only 100 ms.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
92<br />
Transferring historical auroral films into digital format<br />
Rao, Jayasimha Ramachandra 1 and Syrjäsuo, Mikko 2<br />
1 Finnish Meteorological Institute, Arctic Research<br />
2 Finnish Meteorological Institute, Earth Observation<br />
Abstract<br />
In 1973–98, the Finnish Meteorological Institute regularly operated up to 14 auroral all-sky cameras in the Finnish<br />
Lapland. Their operation was carried out in a routine fashion with the aim to record the sky every. A downward<br />
looking film camera captured the whole sky by using a spherical mirror. A custom-built electronic control system<br />
initiated the operation at dusk and the imaging was carried out until the dawn. Nominal temporal resolution was<br />
one minute, even though 20-second cadence was occasionally used during campaigns. In addition to the reflection<br />
of whole sky in the mirror, each film frame also captured a station identification plaque and the current date and<br />
time. Three colour standards were also visible to guide the film development process.<br />
For daily research use, the auroral films were later transferred to videotapes. Each video frame then corresponded<br />
to one individual image and one could rewind the tape back and forth to study the auroral display. The time instant<br />
was visually verified from the images.<br />
We have now digitised the videotapes into a computer compatible format. In order to integrate the data to modern<br />
data systems, however, there are a number of practical details that need to be dealt with. The key information to<br />
automatically identify includes the station and the capture date and time. As the actual content within the frame<br />
may vary, the first task is to determine the sky image and the locations of the colour standards as well as the area<br />
containing the date and time display. The actual sky image is copied into a predetermined location in a template<br />
image frame. Relevant meta-data are included in the final digital image stored on disk. This allows treating the data<br />
as if they originated from a modern digital all-sky camera. Generation of summary plots (keograms) and distributing<br />
data, for example, within a virtual observatory framework becomes feasible.<br />
Making the historical all-sky image data easily accessible for the science community at large significantly extends<br />
the current data archives to cover several solar cycles. We present the very first results of our ongoing work and<br />
discuss the techniques we have evaluated and used to automate the data processing.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
A review of automated analysis of auroral images — current status and new prospects<br />
Syrjäsuo, Mikko 1 and Hollmén, Jaakko 2<br />
1 Finnish Meteorological Institute, Helsinki, Finland<br />
2 Aalto University, Espoo, Finland<br />
93<br />
Abstract<br />
Observing and measuring the auroral displays has been a central part in space research since the beginning. Even<br />
before space-born experiments were possible, cameras and other optical instruments were used to record the light<br />
show in the polar sky for later visual analysis. The arrival of satellite instruments revealed the magnitude of<br />
the plasma phenomena in the upper atmosphere and beyond it. In the present day, arrays of ground-based stations<br />
complement the data from a fleet of satellites, whose orbits have been selected to maximise the scientific output. The<br />
existing tools for further analysis, however, cannot efficiently and meaningfully handle the continuously increasing<br />
flow of incoming data. Full exploitation is, in our opinion, not possible without new methodology. Exploiting results<br />
from computer science and applying proven techniques to auroral image data creates fresh possibilities.<br />
There are several major applications that would greatly benefit from computer-aided analysis — with human in<br />
the loop — or fully automated analysis tools. A persistent question concerns the existence of aurora in a given image.<br />
This is a surprisingly difficult task to perform automatically especially with data from panchromatic (”white light”)<br />
imager such as those used in THEMIS. After the existence of aurora is confirmed, we can continue with identifying<br />
image regions with auroral activity. Objective analysis of auroral morphology allowing quantitative comparisons<br />
to models and simulations becomes possible. Tracking individual auroral patches further leads to spatio-temporal<br />
analysis.<br />
We review the existing literature of automated auroral image analysis. The differences in analysis of satellite<br />
and ground-based images are contrasted. The emergence of dedicated virtual observatories allows truly large-scale<br />
and global analysis of the aurora. We extend the literature review to selected areas within the field of computer<br />
science to introduce state-of-the-art methodology for handling multidimensional and complex data. For example,<br />
parsimonious modelling aims at achieving maximally simple and compact models as a result of data analysis. This<br />
often results in more understandable models from which the properties of the underlying phenomena are easier to<br />
infer.<br />
Our emphasis is on proven learning algorithms as well as those that would require little effort in implementation<br />
but could result in significant impact on auroral research methodology. Key directions for future research and<br />
collaboration with computer scientists are identified.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
94<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
95<br />
Facilities and experiments<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
96<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
EISCAT_3D, New generation Incoherent Scatter Radar to Northern Fennoscandia<br />
Aikio, Anita 1 , Ulich, Thomas 2 , Lehtinen, Markku 2 and Turunen, Esa 3<br />
1 Department of Physics, University of Oulu, Finland<br />
2 <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong>, Finland<br />
3 EISCAT Scientific Association, Kiruna, Sweden<br />
97<br />
Abstract<br />
In this presentation, we describe the present status of the EISCAT_3D incoherent scatter radar, which is planned to<br />
replace the existing EISCAT radars in Tromsø (Norway), Kiruna (Sweden) and <strong>Sodankylä</strong> (Finland). EISCAT_3D<br />
will be a key facility for many research areas including atmospheric science, auroral and space physics as well as space<br />
weather applications. EISCAT_3D has been accepted on the ESFRI Roadmap for Large-Scale European Research<br />
Infrastructures for the next 20–30 years. The design work of the new phased array radar is going on under the<br />
EU-funded FP7 Preparatory Phase project. In addition, national funding is used to build a phased array receiver<br />
called KAIRA at Kilpisjärvi. The installation work will start in summer 2011.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
98<br />
SPEAR (Space Plasma Exploration by Active Radar): An ionospheric heater in the<br />
high arctic<br />
Baddeley, Lisa 1<br />
1 UNIS, Longyearbyen, Norway<br />
Abstract<br />
The SPEAR high power heating facility is located on Svalbard at 75 ◦ CGM latitude and as such is 10 ◦ closer to a<br />
geomagnetic pole than any current ionospheric heating facility. It thus has the unique ability to perform heating<br />
experiments inside the polar cap at all local times. It is co-located with several facilities, including the EISCAT<br />
Svalbard Radar, the SOUZY radar and the Kjell Henriksen <strong>Observatory</strong> as well as lying in the fields-of-view of two<br />
SuperDARN HF radars. The facility was put into operation in 2004, and has a detailed and successful research<br />
history, with experiments undertaken by scientists from 11 different research institutes in 6 different countries. Recent<br />
upgrades to the facility have increased the experimental capabilities of the system, allowing sub-second modulation<br />
pulse schemes. A summary of the facility, in addition to information regarding access to the system and possibilities<br />
for future experimental collaborations will be presented.<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
99<br />
Andøya Rocket Range - ”Wind of Change”<br />
Dahle, Kolbjørn Blix 1 and Abrahamsen, Trond 2<br />
1 Andøya Rocket Range, Andenes, Norway<br />
Abstract<br />
”A wind of change is blowing” over Andøya Rocket Range, and we are heading for some very interesting times. New<br />
businesses like unmanned aircraft systems (UAS), expanded activities within ARR subsidiaries with major synergies<br />
to the telemetry side of our sounding rocket activity and huge infrastructural upgrades is going to change both the<br />
diversity and the quality of our services.<br />
In 2010, a completely new building for our Payload department and UAS activity marked the beginning of a<br />
two year long rework of the ARR facilities, including a new main building providing over 30 new offices. Everything<br />
will be ready by August 12th 2012 when ARR celebrates its 50 years anniversary. In addition to a wide range<br />
of upcoming, regular scientific sounding rockets, Andøya Rocket Range, the National Centre for Space-Related<br />
Education (NAROM) and the universities of Oslo and Tromsø have for some time worked to compile a joint Canadian-<br />
Norwegian student sounding rocket program.<br />
Named CaNoRock, the 10-year program, including both smaller troposphere sounding rockets and regular scientific<br />
missions is scientifically controlled and focuses heavily on bilateral cooperation and the exchange of physics- and<br />
technology students between the two countries. The CaNoRock group has also planned to establish an ”International<br />
Space Science Degree” to be awarded to outstanding students in the CaNoRock program which was officially started<br />
by the Canadian Ambassador to Norway in January this year.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
100<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
101<br />
NLC and PMC<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
102<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
103<br />
NLC climatology from GOMOS observations<br />
Pérot, Kristell 1 , Hauchecorne, Alain 1 and Montmessin, Franck 1<br />
1 LATMOS, Guyancourt, France<br />
Abstract<br />
Noctilucent clouds (NLC), also called polar mesospheric clouds when observed from space, are the visible manifestation<br />
of water ice particles persistently present in the polar summer mesopause region, which is the coldest place on<br />
Earth. Because of their extraordinary height of about 83 km, they can become visible to the naked eye when the sun<br />
sinks below the horizon, providing a dazzling display of bluish light. Since these clouds are extremely sensitive to<br />
changes in their environment, their observation conveys unique information concerning the various processes taking<br />
place in the mesosphere.<br />
GOMOS is a stellar occultation instrument combining 4 spectrometers in the spectral range 250 to 950 nm<br />
(UV-visible-near IR) and 2 fast photometers (470–520 nm and 650–700 nm). On the day side, in addition to star<br />
light, GOMOS measures also the solar light scattered by the atmospheric molecules. In the summer polar days,<br />
NLC are clearly detected using the photometers signals. The sun-synchronous orbit of ENVISAT allows observing<br />
them in both hemispheres. The main properties of these clouds (occurrence frequency, radiance, altitude) have been<br />
retrieved from GOMOS data. A very high accuracy is possible thanks to the stellar occultation technique. Moreover,<br />
the observation of these clouds with the spectrometers provides the spectral dependence of the light scattered by<br />
the NLC particles, from which it is possible to derive their radii.<br />
These clouds at the edge of space have been studied using GOMOS data from 2002 to 2010. After a brief overview<br />
of retrieval methods, the climatology obtained for the main NLC characteristics will be presented, focusing on the<br />
seasonal and latitudinal coverage.<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
104<br />
Probing the atmosphere with optical methods: Lessons learned and challenges for the<br />
future<br />
Witt, Georg 1<br />
1 Dept. of Meteorology, Stockholm University, Sweden<br />
Abstract<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
105<br />
Author index<br />
Aalto, Pasi, 23<br />
Aaltonen, Veijo, 23, 24<br />
Abrahamsen, Trond, 99<br />
Aikio, Anita, 43, 97<br />
Alpatov, Victor, 30, 83<br />
Andalsvik, Yngvild Linnea, 44<br />
Arola, Antti, 23<br />
Axelsson, Katarina, 45, 61, 85<br />
Baddeley, Lisa, 98<br />
Barthélemy, Mathieu, 63<br />
Baumgarten, Gerd, 87<br />
Belakhovsky, Vladimir, 46<br />
Belyaev, Alexey, 29, 83, 84<br />
Bennouna, Yasmine, 24, 73<br />
Berjón, Alberto, 24, 73<br />
Blindheim, Sandra, 24<br />
Bommier, Véronique, 63<br />
Brändström, Urban, 32, 45, 61, 64, 85<br />
Brekke, Pål, 62<br />
Cachorro, Victoria, 24, 73<br />
Carlund, Thomas, 24<br />
Charrois, Dan, 57<br />
Chernigovskaya, Marina, 36<br />
Chernouss, Sergey, 30, 47, 62, 89, 91<br />
Connors, Martin, 57<br />
Dahle, Kolbjørn Blix, 99<br />
Dahlgren, Hanna, 48, 50, 51<br />
Deehr, Charles, 62<br />
de Frutos, Angel M., 24<br />
de Frutos, Angel Maximo, 73<br />
de Leeuw, Gerrit, 23, 24, 26<br />
Donovan, Eric, 49, 57<br />
Dyrland, Margit, 62, 91<br />
Dyrland, Margit Elisabet, 31<br />
Ehrlich, Yossi, 86<br />
Enell, Carl-Fredrik, 32, 85<br />
Farrugia, Charles J. , 44<br />
Fastig, Shlomo, 86<br />
Fedorenko, Yuri, 89<br />
Fedorenko, Yury, 91<br />
Fedotova, Ekaterina, 74<br />
Fiedler, Jens, 87<br />
Frissell, Nathaniel A., 58<br />
Fuertes, David, 73<br />
Gausa, Michael, 24<br />
Gavrilov, N. M., 75<br />
Golovchanskaya, Irina, 54<br />
Gonzalez, Ramiro, 73<br />
Gronoff, Guillaume, 63<br />
Guenther, D., 75<br />
Gustavsson, Björn, 32, 50, 51, 57, 60, 61, 64, 85<br />
Håkansson, Bertil, 24<br />
Hannukainen, Meri, 26<br />
Hauchecorne, Alain, 103<br />
Hedin, Jonas, 32<br />
Herber, Andreas, 24<br />
Hildebrand, Jens, 87<br />
Hollmén, Jaakko, 93<br />
Hoppe, Ulf-Peter, 33<br />
Inbar, Tuvia , 86<br />
Ivanov, Yuriy, 91<br />
Ivchenko, Nickolay, 50, 51<br />
Johnsen, M.G., 34<br />
Kannel, Martin, 25<br />
Kashin, F. V., 75<br />
Katkalov, Yu. V., 52<br />
Katz, David, 86<br />
Kauristie, Kirsti, 53, 56, 60<br />
Ketola, Anneli, 56<br />
Kirillov, A. S., 52<br />
Kirillov, Andrey, 91<br />
Kleimenova, Nataly , 53<br />
Kolmonen, Pekka, 26<br />
Kostsov, Vladimir, 88<br />
Kozelov, Boris, 54, 55, 91<br />
Kozlovsky, Alexander, 46<br />
Kozyreva, Olga, 53<br />
Kratzer, Sussane, 24<br />
Kraus, Yaniv, 86<br />
Kryzanowsky, Zane, 57<br />
Kuznetsova, Marina, 89<br />
Kyrölä, Erkki, 76<br />
Lübken, Franz-Josef, 87<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
106<br />
López Ariste, Arturo, 63<br />
Lakkala, Kaisa, 77<br />
Lamy, Hervé, 63, 64<br />
Lanchester, Betty, 50, 51<br />
Lehtinen, Markku, 97<br />
Lihavainen, Heikki, 23<br />
Lilensten, Jean, 63<br />
Lorentzen, D.A., 34<br />
Lorentzen, Dag, 58, 91<br />
Lorentzen, Dag Arne, 62<br />
Lowe, Robert P., 37<br />
Mäkinen, Sanna, 56, 85<br />
Manuilova, Rada, 78, 80<br />
Marcos, Jose Luis, 73<br />
Martín, Leticia, 73<br />
Martishenko, Xenia, 78<br />
Mattanen, Jyrki, 56<br />
McCarthy, Dean, 35<br />
Medvedeva, Irina, 36<br />
Mielonen, Tero, 23<br />
Milichenko, Alexander, 89<br />
Mingalev, Oleg, 54<br />
Montmessin, Franck, 103<br />
Mooney, Priscilla, 35<br />
Mulligan, Frank, 35<br />
Mulligan, Frank J., 37<br />
Myhre, Cathrine Lund, 24<br />
Naor, Eran, 86<br />
Nikolaishvili, Sergey, 29<br />
Ohvril, Hanno, 25<br />
Oksavik, Kjellmar, 62, 91<br />
Okulov, Oleg, 25<br />
Ortiz de Galisteo, J. Pablo, 24<br />
Ortiz de Galisteo, Jose Pablo, 73<br />
Pérot, Kristell, 103<br />
Partamies, Noora, 56–58, 60, 65<br />
Pautet, Pierre-Dominique, 39<br />
Pearl, Shaul, 86<br />
Pendleton Jr., William, 39<br />
Perminov, Vladimir, 36<br />
Pilgaev, Sergey, 59, 89<br />
Pilipenko, Slava, 46<br />
Platov, Yuly, 30<br />
Polyakov, Alexander, 79, 88<br />
Saari, Heikki, 90<br />
Safargaleev, Vladimir, 91<br />
Sandahl, Ingrid, 61<br />
Sandholt, Per Even, 44<br />
Sangalli, Laureline, 57, 60, 65<br />
Semenov, Aleksey, 80<br />
Semenov, Anatoly, 36, 38<br />
Semyonov, V. K., 75<br />
Sergienko, Tima, 32, 45, 61, 64, 85<br />
Sigernes, Fred, 31, 62, 85, 91<br />
Simon Wedlund, Cyril, 63, 64<br />
Sinyakov, V. P., 75<br />
Sofiev, Michael, 26<br />
Sofieva, Viktoria, 69<br />
Sogacheva, Larisa, 23, 26<br />
Stebel, Kerstin, 24<br />
Sundström, Anu-Maija, 26<br />
Syrjäsuo, Mikko, 57, 92, 93<br />
Tans, P., 75<br />
Taylor, Michael, 39<br />
Timofeyev, Yuri, 79, 88<br />
Toledano, Carlos, 24, 73<br />
Torres, Benjamin, 24, 73<br />
Trondsen, Trond, 91<br />
Turunen, Esa, 97<br />
Tuttle, Sam, 50<br />
Ulich, Thomas, 97<br />
Uspensky, Alexander, 88<br />
Uspensky, Mikhail, 30, 53<br />
Verronen, Pekka. T, 32<br />
Vlasov, Alexey, 53<br />
von Cossart, Götz, 87<br />
Vorobjev, V. G., 52<br />
Walker, Kaley, 79<br />
Wang, Zilu, 85<br />
Wehrli, Christoph, 24<br />
Whiter, Daniel, 65<br />
Witt, Georg, 32, 104<br />
Yagodkina, O. I. , 52<br />
Yagovkina, Irina, 79<br />
Yankovsky, Valentine, 74, 78, 80<br />
Zhao, Yucheng, 39<br />
Zibordi, Giuseppe, 24<br />
Rao, Jayasimha Ramachandra, 92<br />
Reistad, Jone Peter, 58<br />
Rodriguez, Edith, 23, 26<br />
Roldugin, Alexey, 59, 89, 91<br />
Roldugin, Valentin, 59<br />
Rydesäter, Peter, 32<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
107<br />
Registered participants<br />
Last name First name Institution Department Address Email<br />
Aaltonen Veijo Finnish Meteorological<br />
Climate Change Helsinki, Finland veijo.aaltonen@fmi.fi<br />
Institute<br />
Aikio Anita University of Oulu Department of Oulu, Finland aaikio@sun3.oulu.fi<br />
Physics<br />
Andalsvik Yngvild University of Oslo Department of Oslo, Norway y.l.andalsvik@fys.uio.no<br />
Physics<br />
Axelsson Katarina Swedish Institute Kiruna Kiruna, Sweden katarina@irf.se<br />
of Space Physics<br />
Baddeley Lisa University Centre<br />
Longyearbyen,<br />
in Svalbard<br />
Svalbard, Norway<br />
Belyaev Alexey Institute of Applied<br />
Department of At-<br />
Moscow, Russia anb52@mail.ru<br />
Geophysics mospheric Dynam-<br />
ics and Optics<br />
Brändström Urban Swedish Institute Kiruna Kiruna, Sweden urban.brandstrom@irf.se<br />
of Space Physics<br />
Cachorro Victoria University of Valladolid<br />
Grupo de Óptica Valladolid , Spain , chiqui@goa.uva.es<br />
Atmosférica Spain<br />
Chernouss Sergey Polar <strong>Geophysical</strong> Optical methods Apatity, Murmansk<br />
chernouss@pgia.ru<br />
Institute<br />
region,<br />
Russia<br />
Dahlgren Hanna Boston University Center for Space Boston, Massachusetts,<br />
hannad@bu.edu<br />
Physics<br />
USA<br />
Donovan Eric University of Calgary<br />
Dept. of Physics Calgary, Alberta,<br />
and Astronomy Canada<br />
Dyrland Margit The University Dept. of Arctic Longyearbyen, margit.dyrland@unis.no<br />
Centre in Svalbard<br />
(UNIS)<br />
Geophysics Svalbard, Norway<br />
Enell Carl-Fredrik <strong>Sodankylä</strong> <strong>Geophysical</strong><br />
University of Oulu <strong>Sodankylä</strong>, Fin-<br />
carl-fredrik.enell@sgo.fi<br />
Observaland<br />
tory<br />
Fastig Shlomo Soreq NRC Yavne, Israel fshlomo@soreq.gov.il<br />
Fedotova Ekaterina St. Petersburg Atmospheric St. Petersburg, godograf87@mail.ru<br />
State University Physics Departmensian<br />
Petrodvorets, Rus-<br />
Federation<br />
de Frutos Ángel University of Valladolid<br />
Grupo de Óptica Valladolid, Spain angel@goa.uva.es<br />
Atmosférica<br />
Gavrilov Nikolai M. Saint-Petersburg Atmospheric Petrodvorets, gavrilov@pobox.spbu.ru<br />
State University Physics Department<br />
Saint-Petersburg,<br />
Russia<br />
Gausa Michael Andøya Rocket ALOMAR Andenes, Norway michael.gausa@rocketrange.no<br />
Range<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
108<br />
Gustavsson Björn University of<br />
Southampton<br />
Hildebrand Jens Leibniz-Institut<br />
of Atmospheric<br />
Physics<br />
Physics Southampton, UK bjorn@irf.se<br />
Kühlungsborn,<br />
Mecklenburg-<br />
Vorpommern,<br />
Germany<br />
hildebrand@iapkborn.de<br />
Hoppe Ulf-Peter University of Oslo Physics Oslo, Norway u.p.hoppe@fys.uio.no<br />
Kannel Martin University of Institute of Tartu, Estonia martin.kannel@ut.ee<br />
Tartu<br />
Physics<br />
Kari Kirsi Finnish Meteorological<br />
Helsinki, Finland kirsi.kari@fmi.fi<br />
Institute<br />
Katkalov Yury Polar <strong>Geophysical</strong> Apatity Departmenmansk<br />
Apatity, Mur-<br />
yury.katkalov@me.com<br />
Institute<br />
region,<br />
Russia<br />
Kauristie Kirsti Finnish Meteorological<br />
Arctic Research Helsinki, Finland kirsti.kauristie@fmi.fi<br />
Institute<br />
Kozelov Boris Polar <strong>Geophysical</strong> Apatity Departmenmansk<br />
Apatity, Mur-<br />
Boris.Kozelov@gmail.com<br />
Institute<br />
region,<br />
Russia<br />
Kyrölä Erkki Finnish Meteorological<br />
Earth observation Helsinki, Finland Erkki.Kyrola@fmi.fi<br />
Institute<br />
Lakkala Kaisa FMI Arctic Research Rovaniemi, Finland<br />
kaisa.lakkala@fmi.fi<br />
Lorentzen Dag UNIS Geophysics Longyearbyen, dagl@unis.no<br />
Svalbard, Norway<br />
Manuilova Rada Valentine<br />
St. Petersburg 198504 St. Petersburg,<br />
nansey@yandex.ru<br />
Yankovsky State University<br />
Petrod-<br />
vorets, Russia<br />
Marx Gregory Air Force Research<br />
United States Gregory.Marx@wpafb.af.mil<br />
Laboratory<br />
McCarthy Dean National University<br />
Maynooth Maynooth, Kil-<br />
dean.mccarthy@nuim.ie<br />
of Ireland<br />
dare, Ireland<br />
Medvedeva Irina Institute of Solar-<br />
Terrestrial Physics<br />
(ISTP)<br />
Siberian Branch Russia ivmed@mail.ru<br />
Mulligan Frank National University<br />
of Ireland<br />
Maynooth<br />
Nikolayshvili Sergey Fedorov Institute<br />
for Applied Geophysics<br />
Experimental<br />
Physics<br />
Department of atmospheric<br />
dynamics<br />
and optics<br />
Kil-<br />
Maynooth,<br />
dare, Ireland<br />
Moscow, Russia<br />
frank.mulligan@nuim.ie<br />
ser58ge@gmail.com<br />
Oner Ceren Finnish Meteorological<br />
Helsinki, Finland cerenka@gmail.com<br />
Institute<br />
Partamies Noora FMI ARK Helsinki, Finland noora.partamies@fmi.fi<br />
Pérot Kristell LATMOS Atmospheric Science<br />
Guyancourt, kristell.perot@latmos.ipsl.fr<br />
France<br />
Polyakov Alexander Saint-Petersburg<br />
State university<br />
Atmospheric<br />
physics<br />
Saint-Petersburg,<br />
Petrodvorets,<br />
polyakov@troll.phys.spbu.ru<br />
Rao<br />
Jayasimha<br />
Ramachandra<br />
Finnish Meteorological<br />
Institute<br />
Russia<br />
Arctic research Helsinki, Finland Jayasimha.Ramachandra.Rao@fmi.fi<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Reistad Jone Peter University of Department of Bergen, Norway jreistad@gmail.com<br />
Bergen<br />
Physics and Technology<br />
Rodriguez Edith Finnish Meteorological<br />
Helsinki, Finland edith.rodriguez@fmi.fi<br />
Institute<br />
Saari Heikki VTT Technical Photonic Devices Espoo, Finland heikki.saari@vtt.fi<br />
Research Centre and Measurement<br />
of Finland<br />
Solutions<br />
Sangalli Laureline Royal Military<br />
Kingston, Ontario, laureline.sangalli@rmc.ca<br />
College<br />
Canada<br />
Semenov Anatoly Institute of Atmospheric<br />
Laboratory of Up-<br />
Moscow, RF anasemenov@yanex.ru<br />
Physics of per Atmospheric<br />
Russian Academy Physics<br />
of Sciences<br />
Sergienko Tima Swedish institute STP Kiruna, Sweden tima@irf.se<br />
of space physics<br />
Sigernes Fred UNIS Geophysics Longyearbyen, freds@unis.no<br />
Svalbard, Norway<br />
Simon Wedluntute<br />
Cyril Belgian Insti-<br />
Space Physics Brussels, Belgium cyril.simon@aeronomie.be<br />
for Space Group<br />
Aeronomy<br />
Sofieva Viktoria FMI Earth Observation Helsinki, Finland viktoria.sofieva@fmi.fi<br />
Syrjäsuo Mikko Finnish Meteorological<br />
Earth observation Helsinki, Finland mikko.syrjasuo@fmi.fi<br />
Institute<br />
Taylor Michael Utah State Universitspheric<br />
Center for Atmo-<br />
Logan, Utah, USA mike.taylor@usu.edu<br />
and Space<br />
Sciences<br />
Uspensky Mikhail Finnish Meteorological<br />
Helsinki, Finland Mikhail.Uspensky@fmi.fi<br />
Institute<br />
Whiter Daniel FMI Arctic Research Helsinki, Finland daniel.whiter@fmi.fi<br />
Witt Georg Stockholm Univer-<br />
Dept. of Meteorol-<br />
Stockholm, Swe-<br />
gwitt@misu.su.se<br />
sity<br />
Yankovsky Valentine St. Petersburg<br />
State University<br />
Yagodkina Oksana Polar <strong>Geophysical</strong><br />
Institute<br />
ogy<br />
den<br />
Atmospheric St. Petersburg,<br />
Physics Departmensian<br />
Petrodvorets, Rus-<br />
Federation<br />
Apatity Apatity, Murmansk<br />
region,<br />
Russia<br />
VYankovsky@gmail.com<br />
oksana41@mail.ru<br />
109<br />
http://www.sgo.fi/38AM/abstracts/38am-abstracts.pdf 17th August 2011
110<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
38 AM Abstract book
Photo c○ Carl-Fredrik Enell 2008<br />
Carl-Fredrik Enell (ed.)<br />
<strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> Reports No. 60<br />
c○ University of Oulu, <strong>Sodankylä</strong> <strong>Geophysical</strong> <strong>Observatory</strong> 2011<br />
ISSN: 0359-3657<br />
ISBN: 978-951-42-9494-5 (<strong>PDF</strong>)