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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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stems from the heated plasma at the flare site,<br />

<strong>and</strong> does not indicate the presence of accelerated<br />

particles. Microwave <strong>and</strong> radio emission<br />

can also continue, evidence for energetic electrons<br />

trapped in closed magnetic loops.<br />

1. Soft X-rays <strong>and</strong> Hα originate as thermal<br />

emission in a plasma with temperatures of about<br />

10 7 K. Most of the emission is continuum, lines<br />

of highly ionized O, Ca, <strong>and</strong> Fe are observed as<br />

well.<br />

2. Hard X-rays are photons with energies<br />

between a few tens of keV <strong>and</strong> a few hundred<br />

keV generated as bremsstrahlung of electrons<br />

with slightly higher energies. Only a very small<br />

amount of the total electron energy, about 1 out<br />

of 10 5 , is converted into hard X-rays.<br />

3. Microwaves are generated by the same<br />

electron population that also generates the hard<br />

X-rays as can be deduced from the similarities,<br />

in particular multiple spikes, in both intensity<br />

time profiles. Microwave emission is gyrosynchrotron<br />

emission of accelerated electrons.<br />

4. γ -rays are the best indicators for the presence<br />

of energetic particles. The spectrum can<br />

be divided into three parts: (a) bremsstrahlung<br />

of electrons <strong>and</strong>, to a lesser extent, the Doppler<br />

broadening of closely neighbored γ -ray lines<br />

leads to a γ -ray continuum. (b) Nuclear radiation<br />

of excited CNO-nuclei leads to aγ -ray line<br />

spectrum in the MeV range. The most important<br />

lines are the 2.23 MeV line due to neutron capture<br />

in the photosphere <strong>and</strong> the 4.43 MeV line<br />

from the relaxation of excited 12 C nuclei. These<br />

reactions require particle energies of some 10<br />

MeV/nucl, thus the γ -ray line emission indicates<br />

the presence of very energetic nuclei at<br />

the flare site. (c) Decaying pions lead to γ -ray<br />

continuum emission above 25 MeV.<br />

5. Radio emission results from electron<br />

streams in the corona, exciting Langmuir oscillations.<br />

Frequencies are in the meter range (see<br />

metric radio emission). According to their frequency<br />

drift, radio bursts are classified as type I<br />

to type V metric bursts. See type i radio burst, i<br />

= I ... V.<br />

flare star A star whose brightness increases<br />

detectably for a few hours at irregular intervals<br />

due to flare analogous to those in the sun (solar<br />

flares), but much brighter. They are a signature<br />

of a star that is rotating rapidly <strong>and</strong> has a strong<br />

© 2001 by CRC Press LLC<br />

flattening of the Earth<br />

magnetic field, either because it is young or because<br />

it is in a close binary system. The most<br />

conspicuous flare stars are of spectral type MV,<br />

both because the stars are intrinsically faint <strong>and</strong><br />

because the convection zones are deep, producing<br />

stronger fields <strong>and</strong> brighter flares.<br />

flaring angle On the magnetopause at a given<br />

point P on it — the angle χ (sometimes also denoted<br />

α) between the magnetopause surface <strong>and</strong><br />

the flow direction of the distant solar wind (or<br />

else, 90 ◦ − χ is the angle between flow of the<br />

distant solar wind <strong>and</strong> the normal to the magnetopause<br />

at P). By the Newtonian approximation,<br />

the perpendicular pressure of the solar wind on<br />

the magnetopause at P equals p sin χ, where p<br />

is the dynamic pressure of the solar wind.<br />

flat field, sky flat, dome flat A CCD’s pixelto-pixel<br />

variation in sensitivity is called the flat<br />

field function. To make accurate measurements<br />

of the number of counts from objects on an image,<br />

this variation (which is a multiplicative factor)<br />

must be removed. This is done by making a<br />

flat field image, <strong>and</strong> dividing this image into all<br />

the data images.<br />

There are a number of methods for obtaining<br />

a flat field image, <strong>and</strong> they are very dependent<br />

on the instrument, type of data, <strong>and</strong> filters used.<br />

Different flat field images must be obtained for<br />

each filter, as filters can modify the illumination<br />

across a CCD, <strong>and</strong> narrowb<strong>and</strong> filters can produce<br />

interference fringes. A common method is<br />

to get a number of exposures of a blank screen in<br />

the telescope dome <strong>and</strong> average them together;<br />

these are called dome flats. One may also get images<br />

of the twilight sky, or combine many data<br />

images. In these latter cases, one must be sure<br />

that no actual objects (stars, etc.) appear on the<br />

flats. If these sky flats are not of the same point<br />

in the sky, it is possible to combine them with a<br />

median filter <strong>and</strong> obtain a good flat field frame.<br />

Each data image is divided by an average flat<br />

field image of the same filter, etc.<br />

flattening of the Earth Because of its rotation<br />

the polar radius of the Earth is smaller than<br />

the equatorial radius by about 21 km. This leads<br />

to polar flattening <strong>and</strong> an equatorial bulge.<br />

175

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