HRS (decommissioned) Configurations
N.B., this information applies to the original HRS, which has been decommissioned and will be replaced by HRS-2 at a time to be determined.
HRS
See the HRS Configurations Check
to see if a configuration is valid or not |
HRS_ResPower_echelle_CrossDisp_fiber_skyfibers_slicer_gascell_binning |
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ResPower = 15k, 30k, 60k, or 120k
These values set the slit width for resolving powers of 15,000, 30,000, 60,000, and 120,000, respectively
If you wish to use higher resolution modes below 4000 Å then consider using
the special K configuration. This configuration has its best focus at the
Ca K line. If you are interested in the higher resolution modes above 4400 Å then we suggest you don't use the special K version of the cross disperser. |
echelle = blue, central, red
These values set the echelle rotation angle for changing the position of
the orders on the CCD, primarily
to move spectral features of interest off CCD defects.
- Central: Default value. It is intended to center the orders on the CCD, and yield the
(theoretical) wavelengths given below in the CrossDisp table. In practice, the blaze peaks are
slightly to the red side of the CCD.
- Blue: Causes the wavelength approximately at the blue end
of the orders to be moved to the center
of the CCD. The blaze peak of the order (peak efficiency) moves
near the red edge of the CCD.
- Red: Causes the wavelength approximately at the red end of the orders to be moved to the center
of the CCD. The blaze peak of the order (peak efficiency) moves
near the blue edge of the CCD.
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CrossDisp |
| Wavelength (Å) | | | | | | | |
| Wavelength (Å) |
CrossDisp | Begin | Central | End | Orders | | | | |
CrossDisp | Begin | Central | End | Orders | 316g4931K see NOTE below## | *3057 | 4931 | 6793 | 200 | 124 | 90 | | | | |
600g4739K | *3751 | 4739 | 5732 | 163 | 129 | 106 |
316g4931 see NOTE below## | *3057 | 4931 | 6793 | 200 | 124 | 90 | | | | |
600g4739 | *3751 | 4739 | 5732 | 163 | 129 | 106 |
316g5936 | 4076 | 5936 | 7838 | 150 | 103 | 78 | | | | |
600g5271 | 4275 | 5271 | 6263 | 143 | 116 | 97 |
316g6948 | 5095 | 6948 | 8860 | 120 | 88 | 69 | | | | |
600g5822 | 4814 | 5822 | 6793 | 127 | 105 | 90 |
316g7940 | 6114 | 7940 | 9861 | 100 | 77 | 61 | | | | |
600g6302 | 5316 | 6302 | 7278 | 115 | 97 | 84 |
316g8991 | 7109 | 8991 | **10917 | 86 | 68 | 56 | | | | |
600g6869 | 5879 | 6869 | 7838 | 104 | 89 | 78 |
316g10022 | 8152 | 10022 | **11757 | 76 | 61 | 52 | | | | |
600g7366 see NOTE ### | 6369 | 7366 | 8375 | 96 | 83 | 73 |
| | | | | | | | | | |
600g7940 see NOTE ### | 6948 | 7940 | 8861 | 88 | 77 | 69 |
| | | | | | | | | | |
600g8375 see NOTE ### | 7456 | 8375 | 9406 | 82 | 73 | 65 |
| | | | | | | | | | |
600g8990 see NOTE ### | 7940 | 8990 | 9861 | 77 | 68 | 62 |
| | | | | | | | | | |
600g9405 see NOTE ### | 8491 | 9405 | 10362 | 72 | 65 | 59 |
*HRS+HET flux below 4000 Å drops sharply but the focus also degrades. If you wish to use higher resolution modes below 4000 Å then consider using
the special K configuration. This configuration has its best focus at the
Ca K line. If you are interested in the higher resolution modes above 4400 Å then we suggest you don't use the special K version.
**HRS+HET delivers very little flux above 10400 Å
## For the bluest settings of the 316g the orders get very close together and the
PI is strongly urged to use the 600g which has wider order spacing and
higher blue throughput!!
### The g600 grating does not have as good throughput in the red as the g316 grating. It is not advised to use this grating far out in the red.
These values set the rotation of the cross disperser to:
- select which orders fall on the CCD
- set how much inter-order space there is for sky fibers
The three wavelengths given above for each value of CrossDisp are the blaze (central) wavelengths of the blue-most order,
the central order that falls between the two CCDs, and the red-most order.
The wavelengths given are for the echelle=central setting.
The longest wavelength observable is approximately 1050nm due to the drop in the
CCD quantum efficiency.
The central wavelength of any order can be calculated from any other order of known central wavelength and order
number (eg. those in the table) by using the relationship:
- lambda * order = constant
eg. for 316g4931, where lambda=4931 and order=124, the central wavelength of order 150 is (4931*124)/150=4076.
The spectral coverage of a given order (its FSR or Free Spectral Range) is lambda/order number. eg. 316g4931: for order 124,
lambda=4931 so FSR=39.8 Å
A filter is always used for rejecting the 2nd order of the cross disperser, and
it is selected automatically.
|
fiber = 2as or 3as (as=arcsecond)
Angular diameter on the sky of the fiber to be used for feeding light from the telescope to the spectrometer.
An important consideration for observing faint objects is that the 3as fiber collects 225% more "sky" than the 2as fibers. |
skyfibers = 0sky, 1sky, 2sky
The maximum number of sky fibers that can be used without order overlap
depends upon the values of "CrossDisp" and "fiber". The limiting wavelengths are:
- 316g and 2as: 4000+ for 0sky, 5880+ for 2sky
- 316g and 3as: 4000+ for 0sky, 5880+ for 1sky, 7100+ for 2sky
- 600g and 2as: 4000+ for 0sky, 4200+ for 2sky
- 600g and 3as: 4000+ for 0sky, 4200+ for 1sky, 5100+ for 2sky
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slicer = IS0 or IS1
- 0 = no slicer
- 1 = image slicer #1
Available when fiber=3as, skyfibers=0sky, and ResPower is one of30k, 60k, or 120k. The increase in throughput verses the 3as fiber is 41%. Or
ders overlap depending upon "CrossDisp" as follows:
- all 316g settings: orders overlap below 5880 Å
- all 600g settings: orders overlap below 4200 Å
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gascell = GC0 or GC1
- 0 = iodine gas cell out of beam
- 1 = iodine gas cell in beam
|
binning = 2x1, 2x2, 2x3, 2x4, 2x5, 2x6 (or 1xN)
The format is (column binning)x(row binning), where
- column binning is in the cross dispersion dimension
- row binning is in the echelle dispersion dimension
Typical binnings for each "ResPower" are:
ResPower | Binnings | Recommended Binning(s)(pixels per resolution element) |
120k | 2x1 (or 1x1) | 2x1 | (2.0) |
60k | 2x1 2x2 (or 1xN) | 2x1 or 2x2 | (4.0 or 2.0) |
30k | 2x2 2x3 2x4 (or 1xN) | 2x3 | (2.7) |
15k | 2x4 2x5 2x6 (or 1xN) | 2x5 | (3.2) |
The width of the orders as a function of "fiber" is
- for fiber = 2as: 13 pixels for column binning = 1
- for fiber = 3as: 20 pixels for column binning = 1
NOTE: YOU PROBABLY SHOULD NOT USE COLUMN BINNING OF 1 BECAUSE YOUR READ NOISE WILL GROW TO BE SIGNIFICANT
The number of pixels per resolution element can be calculated as
(240,000)/(Resolving power)/(row binning)
Note that this value varies along the orders.
NOTE: YOU SHOULD PROBABLY USE OUR SUGGESTED BINNING; IF YOU OVER-RESOLVE THE LINE YOU WILL NOT GAIN ANY INFORMATION DUE TO FIBER SCRAMBLING; YOU WILL JUST HAVE A SQUARE PSF WITH MORE READNOISE
Example: with 2x3 binning and ResPower=30k (30,000), there are approximately 2.7 pixels per resolution element.
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Example HRS configurations:
- HRS_15k_central_316g7940_3as_2sky_IS0_GC0_2x5
- HRS_30k_central_600g5271_2as_2sky_IS0_GC0_2x3
- HRS_60k_central_316g5936_3as_0sky_IS0_GC0_2x1
- HRS_120k_central_316g6948_3as_0sky_IS0_GC0_2x1
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Clarifications or bug reports:
Contact Phillip MacQueen at
pjm@astro.as.utexas.edu or (512) 471-1470. |
N.B., this information applies to the original HRS, which has been decommissioned and will be replaced by HRS-2 at a time to be determined.
Last updated: Fri, 29 Dec 2023 11:52:03 +0000 stevenj
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