| Space Telescope Imaging Spectrograph Instrument Handbook for Cycle 14 | |||||
|
| ||||||
Echelle Grating E140H
Description
The
E140Hgrating is used with theFUV-MAMAand provides echelle spectra at a resolving power of ~110,000 from 1140 to 1700 ÅSpecial Considerations
A single
E140Hechellogram covers 210 Å over ~50 orders. The order separation is ~16 pixels (0.47 arcseconds) at 1150 Å and ~36 pixels (1.05 arcseconds) at 1700 Å. The grating must be scanned, with exposures taken at three distinct settings to cover the full spectral range of the grating.The secondary central wavelength at 1271 Å has had direct sensitivity and wavelength calibrations performed during Cycle 7 to support the large number of observations using these positions.
Figure 13.58: Wavelength Ranges for the E140H Grating Settings
E140H Sensitivity
Table 13.16: E140H Throughputs & Sensitivities for a Point Source
Figure 13.59: E140H Point Source (left axis), and Diffuse Source (right axis) Sensitivities. Throughput curve traces the peaks of the blaze function for each order.
Note
Point source sensitivity assumes full transmission (zero slit losses). Diffuse source sensitivity assumes a 0.1" wide slit. To convert point source sensitivities to diffuse source sensitivities multiply the point source values by the grating spatial (cross dispersion) plate scale in units of arcseconds per pixel and by the width of the desired slit in units of arcseconds.
E140H Signal-to-Noise
Note:
The top axis displays constant F
Figure 13.60: Diffuse Source Signal-to-Noise as a Function of STMAG for E140Hvalues corresponding to the STMAG units (V+STMAG
) on the bottom axis. Recall that STMAG=0 is equivalent to F
= 3.63E-9 erg cm-2 s-1 Å-1. The curves are labeled with exposure times in seconds.
Figure 13.61: Point Source Signal-to-Noise as a Function of STMAG for E140H
|
|
|||||
|
Space Telescope Science Institute http://www.stsci.edu Voice: (410) 338-1082 help@stsci.edu |