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Overview
SPIFFI is a near-infrared integral field
spectrograph
for the VLT. It allows observers to obtain simultaneously spectra of
2048
pixels in a 32x64 pixel field-of-view. In conjunction with the adaptive
optics system MACAO it is possible to perform spectroscopy with
variable
slit widths sampling the diffraction limit of an 8m-class telescope.
SPIFFI
covers the near-infrared wavelength range from 1.1µm to
2.45µm with a moderate spectral resolving power ranging from
R=1500 to R=6000.
Characteristics
- 2048x2048 HAWAI 2RG array increases both spatial and
spectral coverage by a factor of 8 over the preceding instrument 3D
- The field of view is sliced into 32 slices
- With a scale changer in the pre-optics the slit width
is selectable between 0.25", 0.1" and 0.025"
- Corresponding field-of-view sizes are 8"×8",
3.2"×3.2" and 0.8"×0.8"
- Each one of the 32 slitlets is imaged onto 64
detector
pixels.
- Four gratings on a wheel provide spectral resolving
powers of R=2000, 3000, 4000, 1500 in J, H, K, and H+K band,
respectively, in the largest pixel scale.
- The high spectral resolving power allows one to
"suppress" the OH sky-lines to achieve deeper integrations.
- A sky spider facilitates the simultaneous observation
of blank sky in one corner of the field of view, allowing long
integrations without nodding the telescope
Image Slicer
The heart of SPIFFI is its image slicer, which converts the
two-dimensional field of view into a one-dimensional slit. This slit is
fed into a long-slit spectrograph to disperse the light of each pixel
in the two-dimensional
field of view at the same time. During the data reduction the
two-dimensional
spatial information together with the spectral information is used to
create a data cube. The basic concept of image slicing is shown here:
The SPIFFI image slicer consists of two sets of plane mirrors. The
first
set of mirrors, the "Small Slicer" labeled B in the cartoon below,
consists
of a stack of 32 mirrors which slice the image into 32 slitlets. The
second
set of mirrors, the "Big Slicer" or A in the cartoon, rearranges the
fan
of 32 slitlets to form a pseudo long-slit.
Spectrograph
After the SPIFFI field of view is sliced into a one-dimensional slit,
a long-slit spectrograph disperses the light onto a HAWAII detector.
In theory:
Shown here is an overview perspective of SPIFFI.
| H : Sky spider |
F : Filter wheel |
V : Pre-optics |
| B : Image slicer |
K1-3 : Collimator |
G : Grating wheel |
| C : Camera |
D : Detector |
L : Enclosure |
| S : Enforcing structure |
In Reality:
Detector
The detector used in SPIFFI is a Rockwell HAWAII Focal Plane Array with
20482 detector elements.
Control Electronics
The control electronics of SPIFFI is based on the ESO control scheme
developed for VLT instruments. An HP workstation runs the graphical
user
interface for controlling the instrument and the detector and for
displaying
the data. A VME-bus-based real-time computer actually controls
motorized
functions and reads sensor and status signals. A SUN workstation in
conjunction
with an ESO IRACE controller collects the data from the detector.
Sensitivities
Assumptions for the computation of the limiting magnitudes:
- S/N of 10 per spectral channel in 1 hour integration
time on source (6×600sec on source, 6x600sec on sky)
- Encircled energy
- 250 mas scale: 50 % in 0.65'' diameter.
- 100 mas scale: 50 % in 0.20'' diameter.
- 25 mas scale: 25 % in 0.10'' diameter.
Not using OH avoidance
|
250 mas scale
|
100 mas scale
|
25 mas scale
|
J
|
17.6
|
18.1
|
16.7
|
H
|
17.2
|
18.2
|
17.0
|
K
|
16.6
|
17.7
|
16.8
|
H+K
|
17.4
|
18.6
|
17.9
|
Using OH
avoidance
|
250 mas scale
|
100 mas scale
|
25 mas scale
|
J
|
17.8
|
18.2
|
16.7
|
H
|
18.0
|
18.5
|
17.0
|
K
|
17.3
|
18.2
|
16.9
|
H+K
|
18.4
|
19.2
|
18.0
|
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