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Slit and Image Slicers

The spectral resolution is basically determined by the slit or image slicer used, though the maximum resolving power is limited by the data sampling of the detector. Within this limit, the relation between the slit width and resolving power is represented as:

slit width (mm)= $1.8\times 10^{4}$/resolution (R)

(ex.) resolving power $R=90,000 \Leftrightarrow $ slit width = 0.2 mm

The image scale at the Nasmyth focus is 2.0 arcsec/mm, or 0.5 mm to 1 arcsec, thus the resolution of 90,000 corresponds to a slit that is 0.4 arcsec wide. The slit width can be set between 0.2 and 4 arcsec.

The amount of sky observed is determined by the slit length. If the slit in use is too long, overlapping of orders may occur. The maximum slit length for which orders do not overlap is given as a function of wavelength in Table [*]. It is also possible to observe in a longslit moge, where only one echelle order is recorded, and other are blocked out by apropriate filters. The maximum slit length is 60 arcsec (30 mm).


Table 2: Maximum slit length without order overlap

Wavelength
Cross disperser Maximum slit length
    (mm) (arcsec)

3100Å
Blue 2.2 4.4
3500Å Blue 2.9 5.8
4000Å Blue 3.8 7.6
4500Å Blue 4.9 9.8

4000Å
Red 2.4 4.8
4500Å Red 3.1 6.2
5000Å Red 3.8 7.6
7000Å Red 7.4 14.8
10000Å Red 15.1 30.2

Image slicers allow for observations with higher spectral resolution and S/N, especially in poor seeing conditions. Their basic characteristics are summarized in Table [*]. The entrance opening is different for each of them, but wider than the slit that gives a similar resolution, so more light is collected. Comparison of the efficiency of each IS with respect to slits of various widths, as a function of seeing, can be found here.

The image of the opening is chopped into 3- or 5-element pattern. The relation between the angular size of the pattern element and spectral resolution is similar to the one above, however the effective R is somewhate lower, e.g. the IS #1, which is 0".3×5, gives R=110,000, whereas the 0".3 slit gives 120,000.

Table 3: Basic characteristics of the image slicers
  IS #1 IS #2 IS #3
Slice pattern 0".3×5 0".45×3 0".2×3
Spectral resolution R=110,000 R=80,000 R=165,000
TypeBowen-Walraven typeBowen-Walraven type
+ Focal Length Corrector
Entrance opening φ1".5 circle 1".35×1".35 square 0".6×1".45 rectangle
Elongation along slit length 7".9
(λ > 5,000A for red settings ,
  λ > 4,000A for blue settings)
5".2
(λ > 3,800A for red settings,
  λ > 3,600A for blue settings)
5".5
(λ > 4,000A for red settings,
  λ > 3,600A for blue settings)
Material Fused quartz w/AR-coating
Efficiency > 83% (@4,000 ~ 7,000A)> 93% (@3,800 ~ 8,000A)> 73% (@4,000 ~ 8,000A)
Manufactured by OptCraft
Opened since S11BS13AS14A

All ISes are pre-slit units, thus to avoid unnecessary light blocking, the slit width is set to 4 arcsec when an IS is mounted. Guiding is done with the SV.


next up previous contents
Next: Filter Up: How to Determine HDS Previous: Cross-Dispersing Grating   Contents

aoki, helminiak, tajitsu 2014-02-11