The PCA (Jahoda 1994) consists of five Proportional Counter Units
(PCU) sensitive in the 2-60 keV range with an energy resolution less than 18% at 6 keV and a large field of view of 1
FWHM.
Each PCU has three xenon layers which provide the basic scientific
data. When running in Good Xenon configuration each photon captured in a xenon
layer is registered with a timing resolution of 1
s.
The individual
triggers do not contain any spatial information.
The PCA observed the LMC many times with PSR B0540-69 in its large field of view.
We analysed archival
data from observations performed in the Good Xenon configuration with
offset angles less than 30
and durations longer than
5 ks (see Table 1),
resulting in a total dataset containing 684 ks of exposure, after screening
for Earth occultations, South Atlantic Anomaly (SAA) passages and enhanced
background due to high-energy particles. We used this exceptionally long exposure of
PSR B0540-69 for our timing analysis. To boost the signal-to-noise ratio for this weak
source we selected the
photons registered in the first xenon layer of the PCUs.
Obs. ID | Target | Offset | Exposure |
(
![]() |
(ks) | ||
10206 | PSR B0540-69 | 0.04 | 39.1 |
10218 | SN1987A | 25.30 | 74.1 |
10250 | LMC X-1 | 24.80 | 33.4 |
20188 | LMC X-1 | 24.80 | 234.8 |
30087 | LMC X-1 | 24.77 | 73.5 |
40139 | PSR J0537-69 | 15.96 | 109.0 |
50103 | PSR J0537-69 | 15.94 | 120.0 |
The HEXTE instrument (Rothschild et al. 1998) aboard RXTE consists of two independent detector
clusters (A and B) each containing 4 Na(Tl)/CsI(Na) phoswich scintillation detectors passively
collimated to a 1
FWHM field of view and co-aligned with the PCA.
The instrument is sensitive to photons with energies in the energy range
15-250 keV with an energy resolution of about 15.4% at 60 keV. The net open
area of the 8 detectors is 1600 cm2. The events can be tagged with a
maximum time resolution of
s. In its default operation mode the field of
view of each cluster is switched on and off source to provide instantaneous background
measurements reducing the effective source-on exposure by roughly
a half. Due to high-energy particle events the overall performance of
the instrument is degraded resulting in a dead-time fraction of about 40%.
When the source of interest is observed off-axis the response is further reduced by the
collimator/detector assembly. For a source observed
off-axis the sensitive
area is reduced to about 0.5 of its on-axis value.
In the spectral analysis of HEXTE data all these effects which reduce the effective sensitive area are taken into account. Due to the co-alignment of HEXTE with the PCA the same observations have been used as for the PCA. For the spectral analysis HEXTE data from all observations listed in Table 1 have been used, not limited to those observations falling within the stable gain period used in the PCA spectral analysis.
The total dead-time and off-axis corrected Cluster-A and B on-source (=PSR B0540-69) exposures are 248.4 ks and 260.7 ks, respectively.
To extend the spectral coverage to the soft X-ray regime we also included ROSAT PSPC
data in our study. The PSPC is a gas-filled imaging proportional counter which operates
in photon counting mode (Pfeffermann & Briel 1986). It is sensitive over the 0.01-2.5 keV
energy band. The energy resolution is
.
The events are tagged
on board with a precision of
s, but the erratic spacecraft clock makes absolute
timing difficult.
We could identify in the ROSAT archive 3 PSPC observation sequences with PSR B0540-69 nearly on-axis. The observation identifiers are RP400052N00 (PSPC-B), RP150044N00 (PSPC-C) and RP400133N00 (PSPC-B), with effective exposure times of 8.5 ks, 5.1 ks and 1.7 ks, respectively.
Copyright ESO 2003