Photonic crystals in biology
Photonic crystals in biology
Photonic crystals in biology
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Poster Session, Tuesday, June 15<br />
Theme A1 - B702<br />
The fabrication THz emitt<strong>in</strong>g mesa by reactive ion beam etch<strong>in</strong>g<br />
of superconduct<strong>in</strong>g Bi2212 with Ta/PR and PR'/Ta/PR masks<br />
Hasan Köseolu 1 , Fulya Türkolu 1 , Yasem<strong>in</strong> Demirhan 1 , Lütfi Özyüzer 1 , Huab<strong>in</strong>g Wang 2<br />
1 Department of Physics, Izmir Institute Technology, 35430 Izmir, Turkey<br />
2 National Institute of Materials Science, Tsukuba, Japan<br />
Abstract— The perfect rectangular terahertz wave emitt<strong>in</strong>g superconductor Bi2212 mesas have difficulties <strong>in</strong> fabrication because of layered<br />
structure. Mesa lateral angles should be close to 90 degrees to obta<strong>in</strong> <strong>in</strong>tr<strong>in</strong>sic Josephson junctions (IJJs) with same planar dimensions for<br />
synchronization and powerful emission of IJJs. S<strong>in</strong>ce thick photoresist (PR) layer shades the lateral dimension of mesa and also is etched<br />
away dur<strong>in</strong>g ion beam etch<strong>in</strong>g, we patterned Ta/PR and PR'/Ta/PR masks on Bi2212. We used selective ion etch<strong>in</strong>g to overcome this problem.<br />
The reactive ion beam etch<strong>in</strong>gs have done with ion beam of Ar, N 2 and O 2 and we have obta<strong>in</strong>ed mesas about 1 μm thick with lateral angle of<br />
approximately 50 to 75° which is better than the mesas fabricated with s<strong>in</strong>gle layer mask.<br />
Terahertz (THz) radiation is a part of the electromagnetic<br />
spectrum, ly<strong>in</strong>g between microwaves and the far-IR. This<br />
region has frequencies rang<strong>in</strong>g from 0.1–10 THz and<br />
wavelengths from 0.03 mm to 3 mm. Electromagnetic waves<br />
with frequency below and above the THz frequency range are<br />
widely generated by semiconduct<strong>in</strong>g electronics based on<br />
high-speed transistors and the photonics based on the<br />
semiconduct<strong>in</strong>g laser, respectively. However, <strong>in</strong> this frequency<br />
range there are still lacks of THz sources and difficulties <strong>in</strong> its<br />
generation although their functional advantages <strong>in</strong> many<br />
application areas entail the evolution of the THz sources <strong>in</strong><br />
science [1]. Nowadays, the research on THz radiation sources<br />
with high power, low cost and portable has been <strong>in</strong>creas<strong>in</strong>g.<br />
S<strong>in</strong>ce they are planned to use <strong>in</strong> technological areas, they<br />
should be cont<strong>in</strong>uous, coherent and frequency tunable as well.<br />
Therefore the research has gone towards the novel THz<br />
sources which <strong>in</strong>clude technology of high temperature<br />
superconductors (HTSs) layered structure [2].<br />
High temperature superconduct<strong>in</strong>g Bi 2 Sr 2 CaCu 2 O 8+<br />
(Bi2212) s<strong>in</strong>gle <strong>crystals</strong> have natural junctions called <strong>in</strong>tr<strong>in</strong>sic<br />
Josephson Junctions (IJJs). They play an important role for<br />
generation of THz radiation when a static voltage is applied<br />
along the c-axis of Bi2212 (ac Josephson effect) [3].<br />
Generation of powerful THz radiation requires mesas with<br />
large lateral dimension but there are difficulties <strong>in</strong> fabrication<br />
of perfect rectangular mesa. It should be close to 90 degrees to<br />
obta<strong>in</strong> IJJs with same planar dimensions for synchronization<br />
of IJJs [4].<br />
Thick photoresist (PR) layer (s<strong>in</strong>gle layer mask) shades<br />
the lateral dimension of mesa dur<strong>in</strong>g ion beam etch<strong>in</strong>g.<br />
Therefore, we patterned multilayer masks on Bi2212 and used<br />
selective ion etch<strong>in</strong>g to overcome this problem [5]. Therefore,<br />
<strong>in</strong> this study, to fabricate the smooth rectangular prism shape<br />
with large area, high thickness and high lateral angle, we used<br />
three different masks that are s<strong>in</strong>gle layer mask and two<br />
different multilayer masks, which are Ta/PR and PR/Ta/PR.<br />
Dur<strong>in</strong>g the mesa fabrication, thermal evaporation was<br />
used to deposit the Au layer. Ta layer was deposited by DC<br />
magnetron sputter<strong>in</strong>g. Photolithography process was applied<br />
to cover the PR’ layer and pattern the mesa shaped PR.<br />
After the preparation of the mesa shaped PR pattern,<br />
sample is mounted <strong>in</strong>to the ion beam etch<strong>in</strong>g system that<br />
produces ion beam accelerated through the surface of sample<br />
to etch down some area unprotected by PR layer on crystal.<br />
By these masks, reactive ion beam etch<strong>in</strong>gs have done with<br />
the ion beam of Ar, N 2 and O 2 and we have obta<strong>in</strong>ed mesas<br />
with almost 1 μm thick and high lateral angle.<br />
Figure 1: AFM measurement of HC06 (Bi2212/Au/PR/Ta)<br />
Table 1: AFM analysis results of fabricated mesas<br />
Mesa height and lateral angle Edge 1 Edge 3<br />
HC09 (Bi2212/Au) 570 nm - 12° 650 nm - 13°<br />
HC06 (Bi2212/Au/PR/Ta) 860 nm - 75° 770 nm - 35°<br />
HC07 (Bi2212/Au/PR/Ta) 930 nm – 50° 820 nm - 42°<br />
SG12–1 (Bi2212/Au/Ta) 860 nm - 51° 870nm - 52°<br />
The improved lateral angle of a mesa can be seen <strong>in</strong> Fig. 1<br />
which shows AFM image of one of the edges. Table 1 shows<br />
AFM analysis results of the fabricated mesas. The results<br />
<strong>in</strong>dicate that mesas with thickness of about 1 μm can be<br />
fabricated. Us<strong>in</strong>g multilayer mask<strong>in</strong>g technique <strong>in</strong>stead of<br />
s<strong>in</strong>gle layer, the lateral angle of mesas can <strong>in</strong>crease<br />
approximately 50 to 75°. This is most important achievement<br />
of this study.<br />
THz cryostat system was used to exam<strong>in</strong>e electrical<br />
properties of mesas. R-T measurements of the Bi2212 s<strong>in</strong>gle<br />
<strong>crystals</strong> were obta<strong>in</strong>ed between 300 and 10 K and sharp phase<br />
transitions to superconduct<strong>in</strong>g state were observed. I-V<br />
measurements was obta<strong>in</strong>ed below Tc, and hysterical<br />
tunnel<strong>in</strong>g behavior of the Bi2212 mesas and many number of<br />
quasiparticle branches such a voltage jumps were observed as<br />
seen Ref. [6]. Dur<strong>in</strong>g I-V measurements, the bolometric<br />
measurements were done to detect emission from the Bi2212<br />
superconduct<strong>in</strong>g mesas.<br />
This research is supported <strong>in</strong> part by the TUBITAK<br />
(Scientic and Technical Council of Turkey) project no.<br />
108T238.<br />
*Correspond<strong>in</strong>g author: hasankoseoglu@iyte.edu.tr<br />
[1] M. Tonouchi, Nature <strong>Photonic</strong>s 1, 97-105 (2007)<br />
[2] M. Tachiki et al., Phys. Rev. B 50, 7065 (1994)<br />
[3] L. Ozyuzer et al., Science 318, 1291 (2007)<br />
[4] A. E. Koshelev et al., Phys. Rev. B 77, 014530 (2008)<br />
[5] Y. Nagai et al., IEEE Transactions on Magnetism 27, 1622 (1991)<br />
[6] L. Ozyuzer et al. Supercond. Sci. Technol. 22, 114009 (2009)<br />
6th Nanoscience and Nanotechnology Conference, zmir, 2010 312