Next: 4 Instrumental Characteristics
Up: 3 Instrument and AOT
Previous: 3.6 Focal Plane Chopper
Subsections
In this section summaries of the logic behind the ISOPHOT AOTs are given.
Only those operations that may be relevant for data processing are mentioned.
Details on the parameters to be entered by the observer are described in the
ISOPHOT Observer's Manual [10]. For details on the the filter wheel
settings see section A.1.
PHT03 includes the following operations:
- 1.
- Pointing procedure, pointing:
- on source in case of single pointing observations except when
rectangular chopped mode is requested;
- in between the source position and the chopper position in case
of rectangular chopper mode;
- on the first raster point in case of raster maps (see below).
Repeat points 2 - 5 for all detector assemblies selected:
- 2.
- In case of detectors P2 and P3, switch on heating and wait for
heating stabilization. Activate detector.
Repeat points 3 - 4 for each filter using the activated detector
- 3.
- Rotate the filter and aperture wheels to the commanded
configuration, optimised to instrument requirements.
To minimize memory effects of the detectors the measurements with the
different filter/aperture combinations are performed according to
increasing power on the detector. PGA should have warned the observer
if the ratio between the highest and the lowest flux on one detector for
the selected filter/aperture combinations is higher than 1000. Such a flux
combination within one AOT could lead to poor calibration. In order to
minimize heating and cooling stabilization times in multi-detector mode,
the detectors are used in the order:
P3 -> P1 ->P2
- 4.
- Integrate on the source for the specified or calculated exposure
time. A measurement is performed in staring mode or one of the three
following chopped modes:
(i) RECTANGULAR
(ii) SAWTOOTH
(iii) TRIANGULAR
In staring mode the observer has to provide an appropriate reference
field measurement for background subtraction, which is not part of this AOT.
- 5.
- The internal calibration is performed with the last filter/aperture
combination used with
the current detector. This means that there will be one FCS calibration
per detector used. If the observation is in staring mode a staring measurement
on FCS1 is performed. If the sky is measured in any chopper mode, both FCS's
are measured in rectangular chopped mode; FCS1 is tuned close to the
[source+background] power, FCS2 close to the background power as given by
the user.
After calibration, the FCS's are
switched off.
- 6.
- After the last integration, the electronics are set to
standby and the instrument is reconfigured to the default
state which is the C200 serendipity mode configuration.
PHT03 in raster mode:
For raster mode measurements, only one detector can be chosen per AOT.
If more than 1 filter is selected the measurements are sorted according
to increasing power on detector. While PHT is measuring, the spacecraft
independently performs a raster map giving no feedback to PHT on the pointing
progress in the raster. To synchronize the spacecraft rastering and the
instrument data collection, the AOT logic already calculated the total
time necessary to perform a complete raster including the microslews.
After the elapse of that time the integration is stopped by a
``pulse command'' (a high priority interrupt to the PHT microprocessor)
which also switches off all electronics including the detector heaters.
After the pulse command a reinitialisation of the instrument is
necessary, this is reflected in the AOT operations.
- 1.
- In case of a heated detector, switch on heating and wait for
heating stabilization. Activate detector.
Repeat points 2 - 6 for each filter:
- 2.
- Rotate the filter and aperture wheels to the commanded
configuration.
- 3.
- An internal calibration on FCS1 is performed in staring mode.
After the calibration FCS1 is switched off.
- 4.
- Set the instrument integration time such that it covers the time
needed to perform a full raster map with the specified raster point
integrations requested by the user. The spacecraft is commanded to
perform a raster according to the requested parameters. PHT is collecting
data during the raster slews. The raster point ID and the on-target flag
are recorded to reconstruct where the spacecraft was pointing.
- 5.
- After the raster has been completed the integration is halted
by a pulse command. This pulse command also stops the electronics.
The detector is activated again and in case of a heated detector, a
stabilisation heating time is included.
- 6.
- An internal calibration on FCS1 is performed in staring mode.
After the calibration FCS1 is switched off.
- 7.
- After the last integration, the electronics are set to
standby and the instrument is reconfigured to the default
state which is the serendipity mode configuration.
PHT04 includes the following operations:
- 1.
- Pointing procedure, pointing:
- on source in case of single pointing observations except when
rectangular chopped mode is requested;
- in between the source position and the chopper position in case
of rectangular chopper mode;
- 2.
- In case of a heated detector, switch on heating and wait for
heating stabilization. Activate detector.
- 3.
- Rotate filter wheel to the position of the required spectral
bandpass
Repeat points 4 - 5 for each aperture
- 4.
- Rotate the aperture wheel to the respective aperture configuration.
Measurements will be ordered with increasing power on the detector,
i.e. with increasing APERTURE size.
- 5.
- Integrate on the source for the specified (or calculated) integration
time. Measurement is performed in staring mode or one of the three
following chopped modes:
(i) RECTANGULAR
(ii) SAWTOOTH
(iii) TRIANGULAR
- 6.
- The internal calibration is performed with the last aperture used with
the current detector. This means that there will be one FCS calibration
per detector used. If the observation is in staring mode a staring measurement
on FCS1 is performed. If the sky is measured in any chopper mode, both FCS's
are measured in rectangular chopped mode; FCS1 is tuned close to the
[source+background] power, FCS2 close to the background power as given by
the user.
After calibration, the FCS's are switched off.
- 7.
- After the last integration, the electronics are set to non-prime-
state and the instrument is reconfigured to the default state.
For the absolute photometry AOT PHT05 only one filter and one aperture
can be selected. Chopped and/or raster mode is not possible.
- 1.
- Pointing on target
- 2.
- In case of heated detector, switch on heating and wait for
heating stabilization. Activate detector.
- 3.
- If a dark measurement is requested then
- rotate the filter and aperture wheels to the dark
instrument configuration for the requested subsystem
(see Table 3.5)
- perform a dark measurement of 256 s
- 4.
- Rotate the filter and aperture wheels to the commanded configuration
- 5.
- If a cold FCS measurement is requested then
- perform an internal calibration measurement of 256 s in
staring mode of FCS1 with zero electrical power applied
- 6.
- Perform the sky measurement
- 7.
- Perform the calibration measurement in staring mode on the heated FCS1
with an measurement time equal to the sky measurement. After the
calibration the FCS1 is switched off.
- 8.
- The electronics are set to standby and the instrument is
reconfigured to default mode.
Note that the dark instrument configuration is different for the different
P detectors in order to ensure that no (stray-)light can reach the detector,
see Table 3.5 for the selected filterwheel settings. The
mnemonics given in the table are explained in section A.1.
Table 3.5:
Filterwheel settings for dark measurements in AOTs
Detector |
Wheel I |
Wheel II |
Wheel III |
|
mnemonic |
mnemonic |
mnemonic |
P1 |
PHT_S |
5_SEC |
P3_100_UM |
P2 |
PHT_S |
5_SEC |
P1_3P29_UM |
P3 |
PHT_C_NO_POL |
5_SEC |
P1_11P5_UM |
C100 |
PHT_S |
C200_200_UM |
P3_100_UM |
C200 |
PHT_S |
C100_50_UM |
P3_100_UM |
SS/SL |
PHT_P_NO_POL |
180_SEC |
P1_7P3_UM |
PHT17 initiates the following operations:
- 1.
- Pointing on requested position
Repeat points 2 - 3 for each filter using the selected detector
- 2.
- Rotate the filter and aperture wheels to the commanded configuration,
optimised according to instrument requirements.
To minimize memory effects of the detectors the measurements are sorted
according to increasing power on the detector. The measurements with the
different filters are performed in the same order. The selected filters
must belong to the same detector.
- 3.
- Integrate on the source for the specified (or calculated) integration
time. Measurement is performed in staring mode.
- 4.
- The internal calibration is performed in staring mode on FCS1
with the last filter of the selected detector. After the calibration, FCS1
is switched off.
PHT18 initiates the following operations:
- 1.
- Pointing on requested position
Repeat points 2-3 for each filter using the activated detector
- 2.
- Rotate the filter (and aperture) wheel(s) to the commanded
configuration, optimised according to instrument requirements. The
measurements are sorted according to increasing power on the detector.
- 3.
- Integrate on the source for the specified (or calculated) integration
time.
PHT19 initiates the following operations:
- 1.
- Pointing on requested position
Repeat points 2-3 for each filter using the activated detector
- 2.
- Rotate the filter (and aperture) wheel(s) to the commanded
configuration, optimised according to instrument requirements.
- 3.
- Integrate on the source for the specified (or calculated) integration
time.
- 4.
- At the end of the filter sequence a calibration measurement is performed
in the last filter in staring mode on FCS1.
- 5.
- The electronics are switched to standby and the instrument is reset
to the default configuration
All measurements are performed in staring mode, thus the observer has to
provide an appropriate reference field measurement for background
subtraction, which may be one or more measurements in the sequence.
Prior to PHT18, a PHT17 must have been performed. After the last PHT18
has been done, a PHT19 is performed. Prior to a PHT19, a PHT17 must have
been performed. During the whole sequence the detector remains activated,
but the measurements are only performed on the
target positions.
PHT22 initiates the following operations:
- 1.
- Pointing procedure, pointing:
- on source in case of single pointing observations except when
rectangular chopped mode is requested;
- in between the source position and the chopper position in case
of rectangular chopper mode;
Repeat points 2 - 5 for all detector assemblies selected:
- 2.
- Switch on heating and wait for heating stabilization
in case C100 is used. Activate detector.
Repeat points 3 - 4 for each filter using the activated detector
- 3.
- Rotate the filter and aperture wheels to the commanded configuration,
optimised according to instrument requirements.
If filters of both C100 and C200 are requested, detectors will be
operated in the following order:
C200 -> C100
To minimize memory effects of the detectors the measurements per
detector are performed according to increasing power on the detector.
- 4.
- Integrate on the source for the specified (or calculated) integration
time. The measurement is performed in staring mode or chopped mode.
If only filters of the C100 filter set are selected one of the
three following chopped modes is possible:
(i) RECTANGULAR
(ii) SAWTOOTH
(iii) TRIANGULAR
If at least one filter of the C200 filter set is selected, the chopper mode
is automatically restricted to RECTANGULAR chopping with 180'' throw.
In staring mode the observer has to provide an appropriate reference field
measurement for background subtraction which is not part of this AOT.
- 5.
- The internal calibration is performed with the last filter used with
the current detector. This means that there is one FCS calibration
per detector used. If the observation is in staring mode a staring measurement
on FCS1 is performed. If the sky is measured in any chopper mode, both FCS's
are measured in rectangular chopped mode; FCS1 is tuned close to the
[source+background] power, FCS2 close to the background power as given by
the user.
After calibration, the FCS's are switched off.
- 6.
- After the last integration, the electronics are set to non-prime
state and the instrument is reconfigured to the default state.
PHT22 in raster mode (restricted to filter sets belonging to either C100
or C200):
Procedure is identical to the raster logic presented for PHT03.
See description of PHT05. The available detectors are C100 and C200 for
which C100 needs heating. The cold measurement time in the case of C200 is
128 s instead of 256 s.
PHT32 initiates the following operations:
- 1.
- Pointing on the first raster point
- 2.
- Activate either PHT C100 or C200 depending on selection of filters
and wait for stabilization of the detector in case C100 has
been selected.
Repeat steps 3-7 for all filters:
- 3.
- Rotate the filter wheel to the commanded filter position.
- 4.
- An FCS1 calibration measurement is performed in staring mode.
- 5.
- Set the instrument integration time such that it covers the time
needed to perform a full raster map with the specified raster point
integrations requested by the user. The spacecraft is commanded to
perform a raster according to the requested parameters. On each
raster position a number of chopper sweeps are performed.
PHT is collecting data during the raster slews.
- 6.
- After the raster has been completed the integration is halted by a pulse
command (see PHT03 raster description). This pulse command also stops the
electronics. The detector is activated again and in case of a heated
detector, a stabilisation heating time is included.
- 7.
- The map is concluded by a repetition of an FCS1 calibration measurement
in the last commanded filter at the last raster position.
- 8.
- After the last filter, the electronics are set to standby
and the instrument is reconfigured to the default state.
The PHT37 AOT is the first AOT in the cocatenated sequence PHT37, [PHT38], PHT39
which form the sparse map. It initiates the following operations:
- 1.
- Pointing on requested position
- 2.
- For C100 switch on heating and wait for heating stabilization.
Activate detector.
Repeat points 3 - 4 for each filter using the activated detector.
To minimize memory effects of the detectors the measurements are
sorted to increasing power on the detector.
- 3.
- Rotate the filter wheel to the commanded configuration, optimised
according to instrument requirements.
- 4.
- Integrate on source for the specified (or calculated) integration
time.
- 5.
- Perform calibration in staring mode on FCS1.
PHT38 will initiate the following operations:
- 1.
- Pointing on requested position
Repeat points 2-3 for each filter using the activated detector
To minimize memory effects of the detectors the measurements are
sorted to increasing power on the detector.
- 2.
- Rotate the filter wheel to the commanded configuration, optimised
according to instrument requirements.
- 3.
- Integrate on the source for the specified (or calculated) integration
time.
PHT39 is the last AOT in the concatenated sequence PHT37, [PHT38], PHT39
which form the sparse map. It will initiate the following operations:
- 1.
- Pointing on requested position
Repeat points 2-3 for each filter using the activated detector
To minimize memory effects of the detectors the measurements are
sorted to increasing power on the detector.
- 2.
- Rotate the filter wheel to the commanded configuration, optimised
according to instrument requirements.
- 3.
- Integrate on source for the specified (or calculated) integration
time. Measurement is performed in the staring mode, thus the observer
has to provide an appropriate reference field measurement for background
subtraction, which may be one or more positions in the sequence.
- 4.
- Perform calibration measurement in staring mode on FCS1.
- 5.
- Switch electronics to standby and reset instrument to default
configuration.
The minimum number of sparse maps is two: one PHT37 followed by one PHT39.
PHT40 will initiate the following operations:
- 1.
- Pointing procedure, pointing:
- on source in case of single pointing observations except when
rectangular chopped mode is requested;
- in between the source position and the chopper position in case
of rectangular chopper mode;
- on the first raster point in case of raster mapping.
- 2.
- Activate detectors
- 3.
- Rotate wheels to configure DARK configuration for PHT-S
(see Table 3.5).
- 4.
- Integrate in dark position for the specified dark current measurement
time of 32 s. Measurement is performed in staring mode.
- 5.
- Rotate wheels to configure beam path to PHT-S.
- 6.
- Integrate on the source for the specified (or calculated) integration
time. Measurement is performed in staring mode or one of the three
following chopped modes:
(i) RECTANGULAR
(ii) SAWTOOTH
(iii) TRIANGULAR
- 7.
- After the integration the electronics are set to standby
and the instrument is reconfigured to the default state.
PHT40 in raster mode:
Start with points 2- 6 at first raster position. Set the integration time
such that it is longer than the time to perform the requested raster map.
Perform point 6 in staring mode. After the raster has been completed the
integration is halted by a pulse command (see PHT03 raster description).
The instrument is measuring during micro-slews.
Proceed with point 7.
For PHT50 only the 25 m filter can be used with the 79'' aperture.
The logic rounds the requested integration time per polariser to the
nearest higher multiple of 128 s with a minimum of 256 s.
A description of CHW1 (change wheel I) is given in
section A.1.4.
PHT50 initiates the following operations:
- 1.
- Pointing on target
- 2.
- Switch on heating, wait for heating stabilisation, and activate P2
- 3.
- Rotate the filter to P_25 and aperture wheel to 79''
repeat steps 4-6 to accumulate the requested integration time per polariser
- 4.
- Rotate CHW1 to PHT-P polariser 1 () and perform measurement of 128 s
- 5.
- Rotate CHW1 to PHT-P polariser 2 () and perform measurement of 128 s
- 6.
- Rotate CHW1 to PHT-P polariser 3 () and perform measurement of 128 s
- 7.
- Rotate CHW1 to PHT-P polariser 1 () and perform measurement of 128 s
- 8.
- Rotate CHW1 to PHT-P `no polariser' position
and perform a sky measurement of 128 s
- 9.
- Perform the calibration measurement in staring mode on the heated FCS1
with an measurement time of 128 s. After the
calibration the FCS1 is switched off.
- 10.
- The electronics are set to standby and the instrument is
reconfigured to default mode.
The additional measurement in the polariser at the end of the
polariser cycle is introduced to correct for long term drifts of the P2
detector.
For PHT51 only the C200 detector array with the 170 m filter can be used.
The logic rounds the requested integration time per polariser to the
nearest higher multiple of 128 s with a minimum of 256 s.
A description of the first filterwheel (CHWI) is given in
section A.1.4. PHT51 initiates the following operations:
- 1.
- Pointing on target
- 2.
- Activate the C200 detector
- 3.
- Rotate the filterwheel 2 to C_160
repeat steps 4-6 to accumulate the requested integration time per polariser
- 4.
- Rotate CHW1 to PHT-C polariser 1 () and perform measurement of 128 s
- 5.
- Rotate CHW1 to PHT-C polariser 2 () and perform measurement of 128 s
- 6.
- Rotate CHW1 to PHT-C polariser 3 () and perform measurement of 128 s
- 7.
- Rotate CHW1 to PHT-C `no polariser' position.
and perform a sky measurement of 128 s
- 8.
- Perform the calibration measurement in staring mode on the heated FCS1
with an measurement time of 128 s. After the
calibration the FCS1 is switched off.
- 9.
- The electronics are set to standby and the instrument is
reconfigured to default mode.
In many cases the full sequence is repeated in a raster map
with 1 pixel displacement and the source centred on each pixel. This
yields a 4-fold redundancy for the central position of the resulting
raster map. This method gives the highest source to background
contrast and provides a consistency check from the results of the 4
individual pixels.
Next: 4 Instrumental Characteristics
Up: 3 Instrument and AOT
Previous: 3.6 Focal Plane Chopper
ISOPHOT Data Users Manual, Version 4.1, SAI/95-220/Dc