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Insights from Radio Wavelengths into Supernova Progenitors Laura Chomiuk Jansky Fellow, Michigan State University
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Supernova Types: I vs. II Type I: No Hydrogen Thermonuclear WD explosions (Ia) and Core collapse of massive stars stripped of H envelopes (Ib/c) Type II: Show Hydrogen Core collapse of massive stars with H envelope
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Supernova Types: A Continuum of H-richness Ic (No H) (No He) Ib (No H) IIb (H goes away) II (some H) IIn (Lots of H)
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(Smartt 2009) A diverse, complicated zoo of massive stars and core- collapse SNe + SNe Ia
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Searching for SN progenitors directly with optical imaging SN 2005gl Before During After
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Or, constraining SN progenitors indirectly- - in the radio Soderberg et al (2008)
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1970 SN 1970G: The first SN detected in the radio (Gottesman et al. 1972, Goss et al. 1973)
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1970 1982
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shell
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SN 1994I @ 20 cm Weiler et al. (2011) absorbed (either free-free or synchrotron) synchrotron τ ≈ 1 fading because blast decelerates and CSM decreases in density
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v w ≈ 30 km/s v sn ≈ 10,000 km/s SN blast probes ~1 year of mass loss in one day!
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What makes a SN bright at radio wavelengths? A fast blastwave Expansion into dense surroundings
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1970 1982 1986 Radio bolsters a division in Type I SNe: Type Ib/c: Show radio emission, core collapse Type Ia: No radio emission, thermonuclear (Panagia et al. 1986)
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1970 1982 1986 1998 Relativistic SN 1998bw associated with GRB 980425 (Kulkarni et al. 1998, Wieringa et al. 1999)(Galama et al. 1998)
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1970 1982 1986 1998 2006 A diversity of mass loss histories SN 2003bg (Soderberg et al. 2006)
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Shells, Spirals, and Shelves SN 1993J (Weiler et al. 2007) SN 2007bg (Salas et al. 2012) (Ryder et al. 2004) SN 2001ig
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SNe Ib/c: WR stars or interacting binaries?
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Mdot/v wind = 10 -10 10 -9 10 -8 10 -7 10 -6 M yr -1 / km s -1 1970 1982 1986 1998 2006 SNe Ib/c show mass loss rates consistent with WR stars.
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Still no radio emission from SNe Ia (Panagia et al. 2006) Time Since Explosion (Days) Radio Luminosity (erg/s/Hz) 1970 1982 1986 1998 2006
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WD + Giant WD + Sub- giant or Main Sequence WD + WD (NASA/Swift/ Aurore Simonnet, Sonoma State Univ.) Different progenitor models predict different circumbinary environments.
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1970 1982 1986 1998 2006 2011
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...And still no radio emission from SNe Ia! Assumes v w = 50 km/s VLA JVLA n ISM = 1 cm -3 M = 10 -8 M yr -1. 1970 1982 1986 1998 2006 2011
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Strong limits on the environment of SN 2011fe from EVLA (Chomiuk et al. 2012, Horesh et al. 2011) SN 2011fe assumes v w = 50 km/s n ISM = 1 cm -3 M = 10 -8 M yr -1.
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Chomiuk et al. (2012), Margutti et al. (2012) Strong limits on the environment of SN 2011fe from EVLA
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1970 1982 1986 1998 2006 2011 SN 2009ip: Watching an LBV explode (Mauerhan et al. 2012)
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SN 2009ip: No longer an impostor since ~Sept 15 No radio detection yet; VLA monitoring ongoing
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1970 1982 1986 1998 2006 2011 SN 1970G revisited 33.7 ± 4.3 μJy @ 5 GHz (Dittman et al. in prep)
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SN 1970G consistently challenges our radio facilities (Stockdale et al. 2001, Dittman et al. in prep)
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SN 1970G: Decline in Radio + Rise in X- rays = Compact Object? (Dittman et al. in prep)
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Radio light curves of SNe trace mass loss histories of progenitors. 1970 1982 1986 1998 2006 2011 Discovery of first radio SN Theory of radio SN Type I SNe split into Ia and Ib/c Long GRB associated with a relat-ivistic SN Diversity of mass loss histories Ib/c mass loss consistent with WR No Ia radio detections Jansky VLA Era: Sensitivity Bonanza! Relativistic SNe w/o GRBs Still no Ia radio detections
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A continuum in blast wave velocities between normal SNe Ib/c and GRBs (Soderberg et al. 2010, more in prep) 1970 1982 1986 1998 2006 2011
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