UV-NIR Observations of the Probable Luminous Supernova CSS 081009:002151-163204
ATel #1842; A. A. Miller, R. Chornock, N. R. Butler, D. A. Perley, W. Li, N. Smith, J. S. Bloom, A. V. Filippenko (UC Berkeley)
on 13 Nov 2008; 04:33 UT
Credential Certification: Weidong Li (weidong@astron.berkeley.edu)
Subjects: Infra-Red, Optical, Ultra-Violet, X-ray, Supernovae, Transient
Referred to by ATel #: 1860
We report on further observations of the SN candidate CSS081009:002151-163204
discovered by the Catalina Sky Survey (Drake et al., ATel #1823) which was
determined by Silverman et al. (ATel #1833) to be at redshift 0.285.
We triggered ToO observations with the Swift satellite starting on 2008 Nov. 11
at 04:10 UT. The transient was observed in all six ultraviolet and optical
filters on the UVOT. We reduced the observations following the calibration
methods described by Li et al. (2006, PASP, 118, 37) and Poole et al. (2008,
MNRAS, 383, 627). Our preliminary photometry is:
UVW2 = 19.60 ± 0.11
UVM2 = 19.20 ± 0.11
UVW1 = 19.02 ± 0.08
U = 18.67 ± 0.05
B = 19.25 ± 0.06
V = 18.58 ± 0.07
In addition, we observed the transient using the Peters Automated Infrared
Imaging Telescope (PAIRITEL) in J, H, and K_s nearly simultaneously with the
Swift observations. The transient is undetected in the K_s band, marginally
detected in the H band, but securely detected in the J band at a magnitude
(calibrated against 2MASS) of:
J = 18.5 ± 0.2
These magnitudes have not been corrected for the small component of Galactic
extinction along the line of sight or for the small contribution from a faint
presumed host galaxy seen in the DSS images.
The Swift observations also totaled 6.15 ks of exposure time with the XRT. The
source is not detected, with a 90% upper limit of F_x(0.3-10 keV) < 4e-14 erg
cm-2 s-1 assuming a power-law spectrum with
Gamma=2 and N_H=1e21 cm-2. At
the redshift of the source, this is an upper limit to the X-ray luminosity of
1e43 erg s-1. We note that the lack of an X-ray detection is consistent
with the interpretation of these super-luminous SNe as optically thick, shocked shells
(Smith & McCray 2007, ApJ, 671, L17).
The downturn in the UV continuum shape at short wavelengths, coupled with the
X-ray non-detection, is inconsistent with an AGN hypothesis for this transient.
Instead, the full SED can be approximately fit by a blackbody spectral shape,
with a characteristic temperature of ~10,500 K (in the rest frame). A direct
trapezoidal integration under the observed fluxes and an integration of
the blackbody fit give similar estimates for the bolometric luminosity of the
source of ~2e44 erg s-1. This extraordinary luminosity and blackbody
temperature are very similar to those of SN 2008es (Miller et al. 2008, arXiv:0808.2193;
Gezari et al. 2008, arXiv:0808.2812) at a similar age of about 30 rest-frame
days after discovery. Further spectroscopic observations are encouraged in
order to confirm the SN nature of this transient.
We thank the Swift PI Neil Gehrels for approving the requested ToO, and
the Swift staff for planning and executing the observations.