Lecture 10: Echelle Spectrograph & Etendue Flashcards
(28 cards)
spectrum of a particular order is contaminated by light from adjacent orders - solution
use a second, vertical grating to separate the overlapping orders
basis of echelle technique
echelle spectrograph
collimating mirror
echelle grating - high order diffraction
cross disperser grating
detector
cross disperser grating
grooves perpendicular to echelle grating so that the spectral orders are mapped out in 2D
solid angle
area of segment on a unit sphere
units of sr
full space solid angle
4 pi sr
radiance
flux emitted per unit projected area per unit solid angle
“brightness”
lambertian
radiance independent of angle
etendue
G=A omega
from small angle approx and simplifying integral
etendue is a geometric quantity and can be thought of as
a measure of the flux gathering capability of an optical system
the greater the area
the greater the flux collected
etendue - the solid angle takes into account
all the directions from which light can arrive at the aperture and so contribute to the flux
the stop
the limiting aperture in an optical system
Once set by the stop, the etendue of an optical system remains
unchanged as the light is transformed by the lenses, mirrors and other optical components
etendue is conserved
can also derive the entendue in terms of
half angle measured from the optical axis
small angle approx gives G=piA theta^2
The instrumental width gives
the angular separation at
which individual spectral lines
are just resolved
this assumes the slit has zero width
with a finite width
the entrance slit also
introduces an angular spread due to diffraction
- In designing a spectrometer, the slit width is chosen so that
the spread in wavelengths due to diffraction from the slit matches the spread in wavelengths due to diffraction from the grating
if the slit is too large
it will degrade resolution
if the slit is too narrow
it won’t pass enough light
A good compromise is if the resolution
is degraded equally by diffraction from the slit and diffraction from the grating
resolution delta lambda=
d lambda/dx deltax0
inverse of linear disp x width of exit slit
the exit slit width is chosen so that
the resolution of the device is set by the diffraction limit of the beam at the focusing lens
smaller than this - lose signal
larger - degrade resolution
minimum wavelength
resolution that can be achieved taking into account diffraction
from both the grating and from the entrance slit
delta xi = dx/dlambda delta lambda_bp
etendue at the entrance slit is proportional to
height of slit
bandpass
order number
illuminated area