USG: CGS4 with Figaro
Figaro procedures for reducing CGS4 spectra
TRG - December 13, 1996
(note : some of the following is useful for CGS3 data reduction too)
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1. Extract positive (and negative) spectrum from rg or ro file for
subsequent analysis. You may wish to de-curve or de-slope the rg or ro
file prior to extraction (see the separate files dealing with
techniques for these).
It is possible to extract a range of rows (using EXTRACT), a single row
or portion of a row (using ISUBSET), or to optimally extract a spectrum
covering more than one row (using PROFILE and OPTEXTRACT).
1.1 Range of rows
EXTRACT
(e.g., extract rg960524_37)
the program will prompt for the range of rows and the name of the
extracted spectrum. Note that if the wavelength scale is tilted on
the array, extracting a range of rows will lower the resolution of
the spectrum. If you do not wish to do this, ectract individual
rows as in 1.2 below and shift spectra as described in 2.2 below.
1.2 Individual row
ISUBSET
(e.g. isubset rg960524_37
Prompts for (a) the row number (e.g., 27 or 36)
(b) the beginning and ending wavelengths (usually easiest to answer
MIN and MAX),
(c) a name (e.g., cygx3_37, BS5685_r36, argon_37)
1.3 Optimal extraction
A profile of signal per row as a function of row number over the rows in
which signal appears is first determined (for a high s/n spectrum) and
then the profile is used to optimally extract a low s/n spectrum. CGS4
spectra normally appear in 2-3 rows of the 256sq array.
profile rg920529_32 (high S/N spectrum)
Prompts for (a) starting row (e.g., 28)
(b) end row (e.g., 30)
(c) degree of polynomial of the fitted profile (at least 4
or 5 is needed) to get a good fit.
(d) number of points to reject (5 is OK)
(e) use errors to weight the fit (Y/N). Answer N.
(f) name of resulting profile image (e.g.,POS)
(g) name of image containing residuals (e.g., JUNK)
Do this for both the positive and negative spectrum
(i.e. rows 28-30 and 18-20) - name the negative profile NEG
optextract rg920529_40 (low S/N
spectrum)
Prompts for (a) profile image to use (e.g., POS; see above)
(b) use errors to weight the data (Y/N) - N
(c) name for optimally extracted spectrum (e.g., P)
do same for negative spectrum, using NEG, name the resulting
spectrum N
Note that if the profiles (e.g., POS, NEG) determined above are applied
to the same spectrum, the resultant spectra (e.g., P, N) are the
sums of the signals in the rows.
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2. Combine positive and negative spectra, for both standard and target.
2.1 If wavelength scale is not tilted (does not vary with row number)
this is simple; simply subtract the negative rows from the positive
rows.
e.g.
isub P N sn95b_40
or use iadd or combine if signals are same sign.
e.g., iadd BS5532_row29 BS5532_row30 BS5532rows2930
Note that IADD will add the signals of two rows, COMBINE will average
the signals, weighting them according to S/N at each point. The
commands, ICMULT and ICDIV are often useful, they multiply/divide the
spectrum by a constant.
2.2 If wavelength scale is tilted on the array, and the spectrum is
sampled once per pixel (i.e. 1x1 or 1x2 sampling), the simplest procedure
is to detilt the spectral image as described in "Coping with sloping lines
in CGS4 (/UKIRT/software/#cgs4) In short, detilt
the spectral image of an arc lamp or sky spectrum using arc, iarc, and
iscrunch and apply the same correction to the spectral image of the target
or standard. Then use the procedures described in 2.1.
Alternatively, use the procedure in 2.3 below.
2.3 If the wavelength scale is tilted on the array and the spectrum is
oversampled (i.e. 2x1, 3x2, 4x2, etc.), there may be a sawtooth on the
spectrum; if so, it will be virtually impossible to remove the sawtooth
across the entire spectrum if the procedures in 2.2 are employed (this is
because the dispersion varies across the spectrum and iscrunch rebins the
spectrum to constant dispersion per data point). To be able to remove the
sawtooth, it is necessary to measure the shift (in pixels) of each of the
extracted rows and then to shift the spectrum of each row before combining
the rows. The shifts can be measured by extracting individual rows of the
arc lamp spectrum (i.e. as in 1.2, cross-correlating them (using scross to
determine the shift, and then applying the shift to the extracted target
and standard rows using ishift, before combining them using iadd or isub,
as in 2.1.
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3. De-ripple the spectra, if necessary (not needed if S/N is very low)
first calculate the ripple function
irflat
Prompts for (a) the filename,
(b) the period of the ripple (e.g., 2 or 3 data points,
(c) the name of the resultant 2- or 3-point ripple spectrum (e.g.,
rip;
(d) the wavelength range(s) over which to calculate the ripple (avoid
the edges of spectra where the S/N is often low or the where the
edge pixels are noisy or corrupted.
the ripple function will then be printed on the screen.
Then divide out the ripple
idiv bs5685_K rip bs5685_K_drip
where the entries are the original spectrum, the ripple function, and the
name of the resultant (de-rippled) spectrum.
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4. Calibrate the wavelength scale of the arc lamp spectrum, and then copy
the wavelength scale onto the astronomical spectra. This assumes that
a 1D arc spectrum has already been extracted from a CGS4 RO or RG file.
ARC
(e.g., arc
Prompts for (a) the filename (ARGON_K_31; it is also possible to use a
sky emission spectrum or a star spectrum with telluric absorption
lines)
(b) the type of arc - answer with '' or NONE (you then specify the
wavelengths). If this doesn't work, enter ARGON. In this case, you
always can force the routine to accept a particular wavelength by
putting space E after the number when inputting it. E.g., answer
2.0992 E to the prompt. This will force the routine to use that
wavelength for the line just identified.
(c) whether to use lines from a previous fit (FALSE);
(d) order of polynomial fit (2 is sufficient, but you must have at
least three lines, with two of them near the short and long
wavelength ends); If you only have two lines, enter 1
(e) arc line half width (the default, 2 is OK).
A plot of the spectrum appears on another window. Use this plot to
select lines, entering wavelengths on the original window. There
are several techniques for doing this - the one I usually use is to
position the cursor on a line, type E (expand scale), position the
cursor accurately (to ~ 0.1 pixel) at the peak, type W (wavelength),
and type the wavelength (e.g. 2.0922 or 2.0922 e). Continue this until
you have entered at least 3 well-spaced lines (esp. at the extrema of the
spectrum). Then type Q (quit). After the parameters of the fit are
listed, type Q again. Create an output file (YES), e.g., ARGON_K_CAL.
Note that if sometimes the entire arc spectrum is not displayed. To see
an adjacent interval of spectrum, type N. Other options will be displayed
by typing a ? .
XCOPY to BS5685_K or CYGX3_K; from ARGON_K_CAL;
name of calibrated spectrum BS5685_K_CAL or CYGX3_CAL
(in practice I give the calibrated spectrum the same name as the
original, in order to reduce the number of files I have stored)
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5. Edit out spikes in the object or standard, or spectral features (e.g.,
Br gamma in a standard)
isedit BS5685_K_CAL
Prompts for (a) name of the edited spectrum (e.g., BS5685_K_CAL_E), and
(b) whether or not to plot the full spectrum (or just the portion
near the data points to be edited
There are then several ways to proceed. One of the simplest is to
interpolate across the line - position the cursor on one side, type I,
position the cursor on the opposite side, and type any letter. Another
simple technique is, for each data point, to position the cursor at the
location you want to move the data point (i.e. directly above or below the
data point) and type M. When finished type Q.
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6. Cross-correlate spectra of target and standard and shift spectra if
necessary to line up atmospheric absorption lines so that they ratio
properly. This is mainly for cases where both the continuum of the
standard and the target have been detected with good S/N.
scross std_1 target_2
specify wavelength range for calculating the shift (this should be a
range where prominent telluric absorption lines are present)
ishift target2
Specify for X shift the value calculated using SCROSS; the sign of
the shift should be correct if scross is done as above). The
shift in Y should be 0, and the X and Y subdivisions should be 1
(One could shift either the target or the standard. My preference is to
shift the target, as (i) the standard is usually brighter and better
centered on the slit and (ii) the standard may be used with more than one
target.)
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7. Divide and flux-calibrate spectra (result in mJy)
irflux
Prompts for the "star spectrum" - this is the source (CYGX3_K_CAL),
(b) the "std spectrum" (BS5685_K_CAL_E),
(c) temperature of the standard,
(d) the type of calibration (J,H,K, L, or F (flux in mJy)),
(e) the numerical value of (d) above,
(f)the name of the resultant spectrum (CYGX3_K_FNU - the result is in
mJy)
Convert to f-lambda, if desired, using IRCONV
irconv CYGX3_K_FNU CYGX3_K_FL
Correct for differences in exposure times (CGS4 only) (if this was
not done previously):
icmult CYGX3_K_FL .05 CYGX3
(or use ICDIV - icdiv CYGX3_K_FL 20 CYGX3)
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8. Smooth spectrum
ixsmooth CYGX3_K_FL
Prompts for Gaussian half width in pixels (data points) (e.g., 0.75),
Range of Gaussian (e.g., 5 pixels)
and name of resultant spectrum, (CYGX3_K_FL_SM)
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9. Plot spectrum
Soft plot:
ESPLOT (with error bars)
SPLOT (without error bars)
also queries for creation of a postscript file for hard plotting.
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10. Convert data to an ASCII file
wascii CYGX3_K_FL CYGX3_K_FL (converted spectrum is CYG_K_FL.DAT)
Last Modification Date 1996/10/07 - Last Modification Author:
frossie
Tom Geballe (tom@jach.hawaii.edu)
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