2009
DOI: 10.1088/0004-637x/691/1/650
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NEAR-INFRARED PHOTOMETRY OF THE TYPE IIn SN 2005ip: THE CASE FOR DUST CONDENSATION

Abstract: Near-infrared photometric observations of the Type IIn SN 2005ip in NGC 2906 reveal large fluxes (>1.3 mJy) in the K s -band over more than 900 days. While warm dust can explain the late-time K s -band emission of SN 2005ip, the nature of the dust heating source is ambiguous. Shock heating of pre-existing dust by post-shocked gas is unlikely because the forward shock is moving too slowly to have traversed the expected dust-free cavity by the time observations first reveal the K s emission. While an infrared li… Show more

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Cited by 82 publications
(115 citation statements)
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References 42 publications
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“…Note that dust formation in a cool dense shell has been proposed for some interacting SNe (e.g., Pozzo et al 2004;Smith et al 2008Smith et al , 2009Mattila et al 2008;Fox et al 2009;Chugai 2009). The cool dense shell may be formed at the reverse-shocked region, and thus, the dust can be heated by the UV/X-ray radiation.…”
Section: Sn Dustmentioning
confidence: 91%
“…Note that dust formation in a cool dense shell has been proposed for some interacting SNe (e.g., Pozzo et al 2004;Smith et al 2008Smith et al , 2009Mattila et al 2008;Fox et al 2009;Chugai 2009). The cool dense shell may be formed at the reverse-shocked region, and thus, the dust can be heated by the UV/X-ray radiation.…”
Section: Sn Dustmentioning
confidence: 91%
“…As it was found in some CC SNe (e.g. SN 1998S, Pozzo et al 2004;SN 2005ip, Smith et al 2009and Fox et al 2009;SN 2006jc, Smith et al 2008aSN 2006tf, Smith et al 2008bSN 2007od, Andrews et al 2010, dust grains may condense in a cool dense shell (CDS) that is generated between the forward and reverse shock waves during the interaction of the SN ejecta and the preexisting circumstellar medium (CSM). The CDS may affect both the light curves and the spectral line profiles.…”
Section: Introductionmentioning
confidence: 92%
“…Given the maximum velocity of the ejecta of 10000 km s −1 , this constrains the distance of the inner radius of the CSM responsible for these profile peaks to Smith et al 2009, andFox et al 2009). The inner ±1500 km s −1 components may come from the forward shock created when the SN ejecta plowed into a central CSM ring, and the outer −5000 km s −1 components from the ejecta interacting with a blob of CSM out of the plane of the central ring.…”
Section: Spectral Evolutionmentioning
confidence: 99%