| RXTE GOF |
2002 RXTE IAU Circulars | RXTE FAQ |
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With the kind permission of Dr Brian Marsden of the International Astronomical Union's Central Bureau for Astronomical Telegrams, the full text of IAU circulars concerning RXTE is reprinted here - a week after their original promulgation by the IAU.
Please note that the text below includes only the parts of the IAUC relevant to RXTE, and that some IAUC contain more than one bulletin about RXTE.
<7993,
7932,
7926,
7924,
7920,
7912,
7906,
7900,
7897,
7893,
7888,
7886,
7880,
7870,
7867,
7856,
7843,
7831,
7792,
SAX J1808.4-3658
C. B. Markwardt, University of Maryland and Goddard Space
Flight Center; J. M. Miller, Harvard-Smithsonian Center for
Astrophysics; and R. Wijnands, University of St. Andrews, report a
new outburst of the millisecond accreting pulsar SAX J1808.4-3658
(cf. IAUC} 7369). In RXTE PCA scans of the Galactic center on Oct.
13.279 UT, an x-ray source whose position is consistent with SAX
J1808.4-3658 was detected with a flux of 65 mCrab (2-10 keV). On
Oct. 9.5, the PCA flux was < 0.5 mCrab. Two minutes of pointed
data detected x-ray pulsations at the frequency 400.953 +/- 0.008
Hz (barycentered). This frequency is consistent with the known
pulsar spin frequency and orbital Doppler modulation. The RXTE ASM
instrument detected the source on Oct. 14.30 and 14.37 at fluxes of
105 and 76 mCrab, respectively. In its 1998 outburst, the source
also exhibited fast radio and optical transients, so
multiwavelength observing is encouraged.
TRANSIENT X-RAY PULSARS
R. Corbet, Goddard Space Flight Center (GSFC) and Universities
Space Research Association; C. B. Markwardt, GSFC and University of
Maryland; F. E. Marshall, GSFC; and S. Laycock and M. Coe,
University of Southampton, report their detection of two transient
x-ray pulsars in the direction of the Small Magellanic Cloud from
RXTE Proportional Counter Array observations having 2-degree FWZI
fields-of-view centered at R.A. = 0h50m00s, Decl. = -73o06'.0, and
R.A. = 0h53m53s, Decl. = -72o26'.7 (equinox 2000.0): "Pulsations
at 82.4 +/- 0.2 s from a previously unknown source were detected on
June 19 and 26, and pulsations at 46.4 +/- 0.1 s were detected on
June 5 and 19. Source positions were determined from four scans,
but accuracy is limited by the pulsations, which give variability
on the scan timescales. For the 82.4-s pulsar, we find R.A.(mean)
= 0h52m55s (standard deviation 2') and Decl.(mean) = -72o33'.0
(s.d. 8'), and so designate this source XTE J0052-725. The 46.4-s
pulsar's position is not near the scan centers and so is not well
determined, but it is unlikely to coincide with the apparently
inactive 46.6-s pulsar 1WGA J0053.8-7226 (IAUC 6788, 6789). The
intensity of XTE J0052-725 was approximately 1.5 mCrab (2-10 keV)
in all observations. The 46.4-s pulsar's collimator-response-
corrected intensity was poorly determined but was similar to that
of XTE J0052-725 on June 19."
1E 2259+586
V. M. Kaspi, McGill University and Massachusetts Institute of
Technology; F. P. Gavriil, McGill University; and P. M. Woods,
National Space Science and Technology Center, report on further
analysis of RXTE/PCA data from 1E 2259+586 (cf. IAUC 7924),
obtained during its outburst on June 18: "The pulsed flux in the
range 2-10 keV declined monotonically by a factor of 4 over the
15000 s in which the bursts were detected. The burst rate
decreased similarly. The pulse profile during the 15000 s was
significantly different than the long-term average profile, an
effect not seen in 5.8 yr of prior RXTE monitoring. These two
observations independently demonstrate that 1E 2259+586 is the
origin of the bursts, solidifying the common nature of anomalous
x-ray pulsars and soft-gamma-ray repeaters. Bursting in anomalous
x-ray pulsars was predicted in the magnetar model (Thompson and
Duncan 1996, Ap.J. 473, 322)."
Kaspi also reports (together with J. Jensen, F. Rigaut, and A.
Hatakeyama, Gemini Observatory; and P. M. Woods) that near-infrared
observations of 1E 2259+586 were obtained on June 21.614 UT with
the Gemini North 8-m reflector (+ NIRI + K_s filter). In a 30-min
exposure (seeing 0".7), the reported possible infrared counterpart
to the pulsar (Hulleman et al. 2000, A.Ap. 358, 605) was detected
with preliminary magnitude K_s = 20.36 +/- 0.15 (1.3 mag brighter
than the quiescent value), indicating that, about 3 days following
the bursts detected with RXTE/PCA (IAUC 7924), the source was a
factor of 3.4 brighter (5.4-sigma confidence limit), thus
confirming the infrared identification. Further infrared/optical
monitoring is advised.
1E 2259+586
V. M. Kaspi, McGill University and Massachusetts Institute of
Technology; and F. P. Gavriil, McGill University, report the
detection with the PCA aboard RXTE of short x-ray bursts from the
direction of the anomalous x-ray pulsar 1E 2259+586 (cf. IAUC
3745). The Chandra-determined position for this pulsar is R.A. =
23h01m08s.295, Decl. = +58o52'44".45 (equinox 2000.0; uncertainty
0".60 in radius, 99-percent confidence; Hulleman et al. 2001, Ap.J.
563, L49). The bursting behavior was detected during a routine
15000-s duration monitoring observation that began on June 18.652
UT. In this observation, about 45 bursts were detected, most of
which had duration < 1-2 s, reminiscent of those seen in soft
gamma-ray repeaters. The mean 1-s flux per burst is approximately
10**-8 erg cm**-2 s**-1 (2-20 keV). Observations at other
wavebands are encouraged.
4U 1543-47
J. M. Miller and R. A. Remillard, Massachusetts Institute of
Technology (MIT), for the RXTE ASM Team at MIT and NASA Goddard
Space Flight Center, report the detection of a new x-ray outburst
in the blackhole binary 4U 1543-47 (cf. IAUC 5520; archival optical
position R.A. = 15h47m08s.6, Decl. = -47o40'09", equinox 2000.0;
uncertainty +/- 1"). The first detections with the RXTE ASM
indicated a flux (2-12 keV) of 0.054 +/- 0.009 Crab on June 16.683
UT, rapidly increasing to 0.5 (June 17.122) and 1.65 Crab (June
17.552). The x-ray spectrum is very soft, implying that the
dominant component is thermal emission from the accretion disk.
Optical and radio measurements are strongly encouraged.
GX 339-4
D. M. Smith, University of California, Berkeley, on behalf of
a collaboration (including T. Belloni, W. A. Heindl, E. Kalemci, R.
Remillard, M. Nowak, J. H. Swank, and S. Corbel), reports that the
blackhole candidate GX 339-4, in outburst since Mar. 26, entered
the rare Very High State (VHS) of x-ray emission around May 6. The
energy spectrum is dominated by a disk blackbody but has a strong
power-law tail. The power spectrum of the fast variability
switches among at least three states: band-limited noise with a
broad quasiperiodic oscillation (QPO) near 9 Hz, red noise with a
narrower QPO near 6 Hz, and a quiet state with almost no
variability. RXTE/PCA observations are taking place at least twice
weekly. The RXTE ASM shows that the count rate has started to
decline from its peak. Monitoring in all other wavebands is
strongly encouraged; the VHS was last observed in 1988 (Miyamoto et
al. 1991, Ap.J. 383, 784).
SAX J1819.3-2525
C. B. Markwardt, University of Maryland and Goddard Space
Flight Center (GSFC); and J. H. Swank, GSFC, report that RXTE PCA
monitoring observations of the Galactic-center region on May 17.6
and 20.9 UT have shown that SAX J1819.3-2525 (IAUC 7119) = XTE
J1819-254 (IAUC 7120) = V4641 Sgr (IAUC 7277) is again active as an
x-ray source. This source was previously active in 1999 as a
"microquasar" and is a confirmed dynamical blackhole system (Orosz
et al. 2001, Ap.J. 555, 489). X-ray fluxes of 4.5 +/- 0.3 and 10.0
+/- 0.5 mCrab (in the band 2-10 keV) were detected at the two
observation epochs, at a position consistent with the source.
Follow-up RXTE observations are being scheduled.
XTE J0929-314
D. K. Galloway, E. H. Morgan, R. A. Remillard and D.
Chakrabarty, Massachusetts Institute of Technology, report: "We
have computed provisional orbital elements for XTE J0929-314 (cf.
IAUC 7897), using pulse frequency measurements from RXTE/PCA
observations between May 2.54 and 13.83 UT. Assuming a constant
pulsar spin frequency and a circular orbit, our preliminary orbital
solution has binary period 2614.75(15) s, projected semimajor axis
6.1(3) light-ms, and orbital epoch (time of 90 deg mean longitude)
2002 May 11.4941(2) TBD at the solar-system barycenter. The derived
barycentric pulsar spin frequency is 185.1052(1) Hz. The inferred
mass function of 2.7 x 10**-7 solar mass is the smallest measured
for any stellar binary. For a 1.4-solar-mass neutron star, the
minimum companion mass is 0.008 solar mass (or 8.5 Jupiter masses).
The x-ray source was active at a flux of 13 mCrab (2-10 keV) on May
15.69. RXTE observations are continuing."
XTE J0929-314
D. K. Galloway, E. H. Morgan, R. A. Remillard, and D.
Chakrabarty, Massachusetts Institute of Technology, write:
"Observations of the recently discovered 185-Hz accreting
millisecond pulsar XTE J0929-314 (cf. IAUC 7888, 7889, 7893, 7895)
with RXTE/PCA on May 9.5 UT indicate that the pulsar is still
active at a flux level of about 20 mCrab (2-10 keV), down from 30
mCrab on May 2. Orbital Doppler shifts of the pulse frequency were
clearly detected. Further RXTE observations are scheduled over the
next few days. Multiwavelength follow-up observations are strongly
encouraged."
XTE J0929-314
R. A. Remillard, Massachusetts Institute of Technology; and J.
Swank and T. Strohmayer, Goddard Space Flight Center, NASA, report
the discovery of 185-Hz pulsations in XTE J0929-314 (IAUC 7889).
This source was observed in a brief pointed observation with RXTE
on May 2, while the average flux was 28 mCrab (2-30 keV). A power
spectrum was computed for 800 s of PCA data, and a highly
significant pulsation is seen at 185.09 Hz, with a strong harmonic
at 370.18 Hz. This is the third known pulsar in which pulsations
faster than 10 ms can be seen in the persistent x-ray emission.
Rasters across the source give an improved position R.A. =
9h29m18s, Decl. = -31o23'.1 (equinox J2000.0; systematic
uncertainty 1'), consistent with the optical candidate (IAUC 7889).
M. P. Rupen, V. Dhawan, and A. J. Mioduszewski, National Radio
Astronomy Observatory, report the detection of a radio counterpart
to the x-ray transient XTE J0929-314 (IAUC 7888). Observations
with the Very Large Array (VLA) at 4.86 GHz show a source with flux
density 0.31 +/- 0.07 mJy on May 3, and 0.36 +/- 0.05 mJy on May 7,
at R.A. = 9h29m20s.194, Decl. = -31o23'03".41 (equinox J2000.0;
uncertainty +/- 0".3). This is 0".8 from the optical position
reported by Greenhill et al. (IAUC 7889) and provides strong
evidence that this optical identification is correct. Further
optical and x-ray observations are strongly encouraged.
P. Cacella, Brasilia, Brazil, reports that an unfiltered CCD
image taken with a 0.25-m reflector shows a variable (mag 18.3)
that is possibly the optical counterpart to XTE J0929-314 at
position end figures 20s.22, 03".6.
XTE J0929-31
R. A. Remillard, Massachusetts Institute of Technology (MIT),
for the RXTE ASM Team at MIT and Goddard Space Flight Center,
reports the discovery of a faint x-ray transient at R.A. = 9h29m22s,
Decl. = -31o22'.8 (equinox J2000.0; estimated uncertainty 3', 90-
percent confidence). The source is visible in sky maps computed
from 6-day intervals of ASM data. Average fluxes (2-12 keV): Apr.
13-18, 15 +/- 2 mCrab; Apr. 19-24, 20 +/- 2; Apr. 25-30, 26 +/- 1.
The error circle contains no noteworthy sources in the Simbad
catalogues. The ASM hardness ratios suggest an x-ray spectrum
similar to transients associated with weakly magnetic neutron stars
or some blackhole systems. Optical and radio observations are
encouraged.
eta CARINAE
M. F. Corcoran, Universities Space Research Association and
Goddard Space Flight Center, reports: "Recent observations of this
peculiar luminous star with the Proportional Counter Array on the
Rossi X-ray Timing Explorer show that the star has undergone an
especially strong x-ray flare in the band 2-10 keV. The flare
started on Mar. 12, apparently reached x-ray maximum on Apr. 21,
has not yet declined to the pre-flare brightness level. The peak
x-ray flux in the and 2-10 keV is 1.8 x 10**-10 erg s**-1 cm**-2;
eta Car has not been this bright in x-rays since 1997 May 29 (i.e.,
about 7 months prior to the x-ray eclipse)."
XTE J1901+014 and XTE J1751-305
R. A. Remillard, Massachusetts Institute of Technology (MIT);
and D. A. Smith, University of Michigan, for the RXTE ASM Team at
MIT and NASA Goddard Space Flight Center, report the discovery of
a fast x-ray transient. The detection was initially thought to be
a gamma-ray burst (cf. http://gcn.gsfc.nasa.gov/gcn/gcn3/1332.gcn3),
with a peak flux of 0.9 Crab (2-12 keV). The event began on Apr.
6.76268 UT, lasting > 2 min and < 3.15 hr (see
http://xte.mit.edu/xtej1901+104). The ASM data show rapid
evolution to a very hard spectrum during this outburst, but the IPN
instruments failed to detect the source above 15 keV (K. Hurley,
private communication). Furthermore, archival ASM data show a
previous outburst at the same position on 1997 June 21.215, which
was longer than 6 min and < 8 hr, with a peak flux of 0.4 Crab.
The combined ASM observations yield a best position R.A. =
19h01m36s, Decl. = +1 26'.4 (equinox J2000.0; estimated uncertainty
3' in R.A. and 2' in Decl.). The error box contains one very faint,
unidentified x-ray source from the Einstein Galactic Plane Survey:
2E 1859.1+0122 (R.A. = 19h01m40s.2, Decl. = +1 27'13", equinox
J2000.0; error radius 48"; Hertz and Grindlay 1988, A.J. 96, 233).
The time scales for these eruptions are reminiscent of the
microquasar and blackhole binary V4641 Sgr, so optical and radio
observations of XTE J1901+014 are strongly encouraged.
XTE J1751-305
Z. Wang and D. Chakrabarty, MIT, report that the candidate
infrared counterpart that they proposed for XTE J1751-305 (IAUC
7874) is now likely excluded. Further analysis of their J-band
images of the field from Apr. 9 UT have led to a revised
astrometric solution (0".5 rms) that places the candidate outside
the 0".6-radius Chandra x-ray error circle (IAUC 7876), lying 0".8
west and 0".4 north of its center. No stars are detected within
the error circle (limiting mag J = 20.5). The two detected stars
closest to the Chandra position are the former candidate (0".9
distant) and one (J = 18.0 +/- 0.5; blended with a neighbor to the
southwest having J = 13.5) that is 1".2 distant.
C. B. Markwardt, University of Maryland and Goddard Space
Flight Center, reports that XTE J1751-305 (IAUC 7867) has become
undetectable by the RXTE PCA instrument. Since discovery, RXTE
monitoring has shown a decrease in the x-ray flux, and as of Apr.
17.5 UT the 2-10-keV upper limit was approximately 1 mCrab (due
primarily to other nearby sources).
XTE J1751-305
C. B. Markwardt, University of Maryland and Goddard Space Flight
Center (GSFC); and J. H. Swank, GSFC, report that the orbital period of
the recently discovered pulsar XTE J1751-305 (IAUC 7867) is 2545.3(1)
s. RXTE PCA observations taken intermittently during Apr. 4.64-7.54
UT show doppler modulation of the pulsed signal, with a projected
semimajor axis of 10.06(6) light-ms. The barycentric mean spin frequency
of the pulsar is 435.31812(4) Hz, and the epoch of 90-deg mean
longitude is JD 2452369.1389(1). The mass function of the pulsar is
1.26 x 10**-6 solar mass, which gives a minimum mass for the companion of
0.014 solar mass (approximately 15 Jupiter masses). No x-ray eclipses or
absorption dips were observed, indicating that the source is not viewed
directly edge-on. A power-law fit to the x-ray spectrum has a photon
index of 1.9. The neutral-hydrogen-absorption column density for a
range of spectral models is 1 to 3 x 10**22 cm-2, indicating that the
optical counterpart will be heavily absorbed. The x-ray flux is
variable at the 1-to-2-percent level (r.m.s.), primarily on the timescale
of several orbital periods. The average x-ray flux has declined from
56 to 43 mCrab, corresponding to an exponential-decay constant of 10
days, thus justifying prompt follow-up observations.
XTE J1751-305
XTE J1751-305
C. B. Markwardt, University of Maryland and Goddard Space
Flight Center (GSFC); and J. H. Swank, GSFC, report that RXTE PCA
monitoring observations of the galactic-center region on Apr. 3.6
UT revealed a new millisecond pulsar, designated XTE J1751-305.
The best fitting source position is R.A. = 17h51m.5, Decl. =
-30o30' (equinox 2000.0), with an estimated position uncertainty of
about 5', due to nearby confusing sources (see item by in 't Zand
et al., below). In the first 200 s of a pointed RXTE PCA
observation on Apr. 4.65, x-ray pulsations were detected (with
10-sigma significance) at a barycentered frequency of 435.313 Hz
+/- 0.005 Hz. The r.m.s. pulsed amplitude in the band 2-10 keV was
2.5 percent. The approximate 2-10-keV x-ray fluxes on Apr. 3.6 and
4.6 were 55 +/- 1 and 60 +/- 2 mCrab, respectively. More
observations by RXTE are scheduled. This is only the second
accretion-powered millisecond pulsar. Further observations at
other wavelengths are encouraged.
J. J. M. in 't Zand, Astronomical Institute, Utrecht
University, and Space Research Organization Netherlands (SRON); P.
Lowes, SRON and BeppoSAX Science Operation Center, Rome; J. Heise,
SRON; and A. Bazzano and P. Ubertini, Istituto di Astrofisica
Spaziale e Fisica Cosmica, Rome, report that XTE J1751-305 was
detected in a BeppoSAX Wide Field Camera observation during Apr.
4.3-4.6 UT at a flux of 52 +/- 3 mCrab (2-28 keV) and localized at
R.A. = 17h51m16s, Decl. = -30o37'.5 (equinox 2000.0; uncertainty
1'.2, 99-percent confidence). No systematic flux trends were
observed at more than the 10-percent sensitivity, and no x-ray
bursts were detected.
XTE J1908+094
P. M. Woods, C. Kouveliotou, M. H. Finger, and E. Gogus,
National Space Science and Technology Center; and J. Swank, C.
Markwardt, and T. Strohmayer, Goddard Space Flight Center, report
the serendipitous discovery of a new x-ray transient, XTE J1908+094,
in RXTE PCA observations of the soft-gamma-ray repeater SGR 1900+14,
triggered following the burst activity on Feb. 17-18 (GCN 1253).
These observations failed to detect the 5.2-s SGR pulsations,
pointing towards a possible new source as the origin of the high
x-ray flux. An RXTE PCA scan of the region around SGR 1900+14 on
Feb. 21 was consistent with emission only from known sources (and
no new sources). However, the scans required SGR 1900+14 to be 20
times brighter than its quiescent flux level (GCN 1256). A
Director's Discretionary Time Chandra observation on Mar. 11 showed
that the SGR was quiescent and did not reveal any new source within
the Chandra ACIS field-of-view. A subsequent RXTE PCA scan on Mar.
17, taken in combination with the first scan, required that a new
source be included in the fit. The best-fit position is R.A. =
19h08m50s, Decl. = +9 22'.5 (equinox J2000.0; estimated 2'
systematic error radius), or approximately 24' away from the SGR
source. The source spectrum (2-30 keV) can be best fit with a
power-law function including photoelectric absorption (column
density N_h = 2.3 x 10**22, photon index = 1.55). Iron line
emission is present, but may be due to the Galactic ridge. Between
Feb. 19 and Mar. 17, the source flux (2-10 keV) has risen from 26
to 64 mCrab. The power spectrum is flat between 1 mHz and 0.1 Hz,
falling approximately as 1/f**0.5 up to 1 Hz. At 1 Hz is seen a
broad quasiperiodic oscillation peak and a break to a 1/f^2 power
law, which continues to 4 Hz. The fractional rms amplitude from 1
mHz to 4 Hz is 43 percent. No coherent pulsations are seen between
0.001 and 1024 Hz. The authors conclude that XTE J1908+094 is a
new blackhole candidate.
SAX J1805.5-2031
P. Lowes, National Institute for Space Research, Space
Research Organization Netherlands (SRON), Utrecht, and BeppoSAX
Science Operation Center (BSOC), Rome; J. J. M. in 't Zand,
Astronomical Institute, Utrecht University, and SRON; J. Heise,
SRON; M. Cocchi and L. Natalucci, Istituto di Astrofisica Spaziale
e Fisica Cosmica, Rome; G. Gennaro and M. Stornelli, BSOC, report
that on Mar. 5.5-5.9 UT, Wide Field Camera unit 1 on BeppoSAX
detected a new x-ray transient, designated SAX J1805.5-2031 and
located at R.A. = 18h05m34s, Decl. = -20o30'.8 (equinox 2000.0;
uncertainty 1'.8, 99-percent confidence). The flux was 0.04 Crab
units in the range 2-28 keV. No x-ray bursts were detected.
C. B. Markwardt, University of Maryland and Goddard Space
Flight Center (GSFC); and E. Smith and J. Swank, GSFC, report that
the source SAX J1805.5-2031 was observed by the RXTE PCA at 2-10
keV in monitoring scans of the Galactic bulge region around Mar.
2.97 UT (flux 51 +/- 2 mCrab) and in a 3100-s pointed PCA
observation starting Mar. 5.84 (flux 36 +/- 1 mCrab). The position
of the source in the PCA scans is consistent with the BeppoSAX WFC
position (cf. Lowes et al., above). The 2-20-keV spectrum is well
fitted with a combination of blackbody (kT = 0.9 keV) emission and
a power law (photon index -2.9) for a column density of 4 x 10**22
cm**-2. No strong pulsations of quasiperiodic oscillations are
detected; the total fractional r.m.s. variability of the source is
16 percent in the band 0.001-2048 Hz. Additional RXTE observations
are planned.
AQUILA X-1
J. H. Swank and E. A. Smith, Goddard Space Flight Center,
report: "Rossi X-Ray Timing Explorer observations indicate that
Aquila X-1 has begun an x-ray outburst. The ASM reported a level
of 33 mCrab during Feb. 12-15. On Feb. 15.6 UT, the flux began a
rise at the rate of 8.3 ASM counts/s (122 mCrab) per day. The PCA
watched as it rose from 75 to 120 mCrab during Feb. 16.03-16.25.
One x-ray burst was observed at the level of 1 Crab. Additional
RXTE observations are scheduled."
XTE J1550-564
XTE J1550-564
J. Swank, E. Smith, and C. Markwardt, Goddard Space Flight
Center, report: "Rossi X-Ray Timing Explorer observations indicate
that XTE J1550-564 is again at a flux of 50-100 mCrab, which it
reached in 2001 Jan. for about 3 weeks. Since 2001 Oct., the ASM
has indicated intermittent levels of a few ASM counts/s. In a
pointed observation on 2002 Jan. 10.875 UT, the PCA confirmed a
level 60 mCrab, with a very hard spectrum (power-law index 1.4 +/-
0.2, cutoff 30-60 keV), corresponding to a 2-50-keV luminosity of
3 x 10**36 erg/s at 2500 pc. The spectrum includes Fe K-shell line
emission, possibly in a reflection component, and about 10 percent
of the luminosity is in a component attributable to a disk. High-
amplitude fluctuations (33-percent rms) are again present, with
characteristic times of 20-100 s (cf. IAUC 7575). Based on recent
behavior, a full outburst is not likely; nevertheless, additional
RXTE observations are scheduled and coordinated observations at
other wavelengths are encouraged."
C. Bailyn, Yale University, adds: "YALO observations on Jan.
12.319 and 13.337 UT yield V = 18.36 and 18.33, respectively.
These values are near the peak optical flux from the last two
outbursts of this source."
2002 October 15 - 7993
July 5, 2002 - 7932
June 24, 2002 - 7926
June 19, 2002 - 7924
June 17, 2002 - 7920
May 29, 2002 - 7912
May 21, 2002 - 7906
May 16, 2002 - 7900
May 9, 2002 - 7897
May 7, 2002 - 7893
April 30, 2002 - 7888
April 29, 2002 - 7880
April 20, 2002 - 7880
April 08, 2002 - 7870
April 04, 2002 - 7867
March 21, 2002 - 7856
March 06, 2002 - 7843
February 16, 2002 - 7831
January 15, 2002 - 7792
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