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[vsnet-history 745] SN 1993J (Filippenko)




Date:    Fri, 16 Apr 93 08:33:01 PDT
From: alex%avf.hepnet@Lbl.Gov (ALEX FILIPPENKO, UC BERKELEY, 510-642-1813)
Subject: SN 1993J updates

  4-16-93
SN 1993J'ers:
   Here are three messages about various topics:

  (1) From Kurt Weiler (kweiler@shimmer.nrl.navy.mil)

Subj:	SN1993J Radio Information Update

N. Panagia, Space Telescope Science Institute and University of
Catania; S. D. Van Dyk and K. W. Weiler, Naval Research Laboratory
report that the available radio observations of SN 1993J are already
sufficient for initial modelling of the progenitor star and projection
of the likely evolution of the radio emission.  Applying the Chevalier
mini-shell model which has been shown appropriate for other radio
supernovae (Weiler, et al. 1986, ApJ 301, 790) with the usual
assumptions for the stellar wind from the red supergiant progenitor
star and assigning a normal spectral index of -0.7 and an index for the
emission decay rate of -0.7, the model yields a presupernova mass loss
rate of about 2 x 10 ^-6 Msun/yr.  The stellar evolution models of
Maeder & Meynet (1988, A&AS, 76, 411) then imply a ZAMS mass
for the progenitor of SN1993J of <15 Msun.  Comparison with other
known radio supernovae, however, indicate that SN1993J is quite
similar in radio properties to SN1980K and SN1981K, and may
represent the lower end of the mass range of stars which can explode
as Type II supernovae.  This relative consistency of properties may
indicate a relatively firm lower limit to the radio properties of Type
II supernovae, and therefore a possible minimum distance indicator. 
Our modelling also results in predictions of the radio flux density to
be expected from SN1993J at various frequencies to assist planning
observations at other telescopes.  Taking 26 March 1993 as Day = 1,
the expected peak flux density at different radio frequencies is ~20
mJy on Day 20 (14 April) at 23 GHz, ~20 mJy on Day 25 (19 April)
at 15 GHz, ~25 mJy on Day 40 (4 May) at 8.4 GHz, ~30 mJy on Day
55 (19 May) at 5 GHz, and ~35 mJy on Day 130 (2 August) at 1.4
GHz.  After peak, the flux density at each frequency should decline
approximately as t^-0.7.

****

  (2) From Janet Mattei (aavso@cfa0.harvard.edu)

CONSISTENT COMPARISON STAR MAGNITUDE MEASUREMENTS DESPERATELY NEEDED 
for SN 1993J in NGC 3031

Photoelectric (V) and preferably also B, R, I measurements of the comparison
stars shown on the Thompson-Bryan and AAVSO preliminary charts are
desperately needed in order to obtain homogeneous brightness estimates of 
Supernova 1993J in NGC 3031.  This need was also pointed out by Dr. Gerard 
de Vaucouleurs earlier.  

Presently there are the following finder charts of the NGC 3031 field:

1.  AAVSO PRELIMINARY CHART, indicated with designation 0947+69.  Made
in 1979 by T. Fetterman, an active AAVSO observer and supernova searcher.
In the absence of a chart of this galaxy for visual observers, it was
developed to aid observers identify the field stars and to provide approximate
brightness estimates for these stars.  The bright magnitudes (brighter than
about 9.0 to 9.5) are from the SAO Catalog, in which magnitudes come from 
various sources and so are often not homogeneous.  The faint magnitudes are 
visual eye estimates by T. Fetterman.  These visual eye estimates may have a 
zero point problem and/or inconsistancies.  Due to uncertainties in the 
magnitudes of the comparison stars, this chart was indicated by the AAVSO as 
preliminary and thus subject to revision.  The circulation of this chart was 
very limited.

2.  THOMPSON-BRYAN CHART.  Published by Cambridge University Press, 
well-drafted field of NGC 3031, printed with white stars on black background.  
The comparison star magnitudes come from the following sources:
  a. Photoelectric sequences
       i. One set [underlined] is from A. R. Sandage (Astron. Journ. 89, 621,
1984), and includes mostly stars northeast of NGC 3031.  Observers have 
reported that these magnitudes are consistent within themselves.
      ii. One set [overlined] is from H. G. Corwin, and includes stars in 
the field of the galaxy and close to the supernova.  Observers have reported 
brightness differences for some of the stars in this set.
  b. Visual magnitudes
        From AAVSO preliminary chart 0947+69 [double-underlined].  Not all 
the stars on the preliminary chart are entered on the Thompson-Bryan chart.
  c. Source(s) unknown
       Also on this Thompson-Bryan chart are magnitudes for which the source 
is not indicated.  These stars do not have any markings (e.g., underlining or 
overlining).  

Thompson and Bryan circulated a limited number of an early edition of their 
finder chart, with stars indicated as black dots on a white background.  The 
chart of SN 1993J distributed with AAVSO Alert Notice 169 is this chart. 
Regrettably, we noticed after distribution that this early version is 
different from the published one, in that some comparison star magnitudes in 
the early version are different from the ones in the published chart.  Why 
these magnitudes were changed and what their source is are not known to me.

3. GUIDE STAR CATALOG CHART.  Magnitudes were independently obtained by the
Space Telescope Science Institute.  For some stars shown in this field, the 
GSC magnitudes are quite different from photoelectric magnitudes mentioned
above.


Thus, in the finder charts mentioned above, there are at least five sources 
of comparison star magnitudes.  These magnitudes are not always consistent 
within and between sources.  

In order to revise the brightness estimates reported by visual observers and 
those doing differential photometry, and to follow the optical behavior of
this supernova, photoelectric measurements of ALL comparison stars with 
magnitudes on the Thompson-Bryan chart need to be made as soon as possible.

Also, it is essential that all observers report what comparison stars they 
have used and are using in making magnitude estimates.

Janet A. Mattei
AAVSO Director

****

  (3) From Roberta Humphreys (roberta@aps1.spa.umn.edu)

      Notes on the Progenitor:  Reddening, Variability, and Luminosity 

           Roberta Humphreys, Greg Aldering, and Kris Davidson
                University of Minnesota

    1. Nature of progenitor:
  
          Determining the nature of the progenitor obviously depends on
       whether we can resolve a single image,and if not, fit the observed
       energy distribution with a single composite spectrum.
 
          The energy distribution from the UBVR photometry we reported in
       IAU Circ # 5739 can be fit by an unreddened late F -type
       supergiant,  an early F-type supergiant with Av 1.2 mag or an early A
       type supergiant with Av about 2 mag.  Taken at face value our colors
       are consistent with a late A or early F-type supergiant with
        Av 1.2 -1.5 mag.

       The BVR colors reported by Perelmuter ( Mar 1990) are consistent with an 
       unreddened late G-type supergiant or a reddened mid to late F -type
       supergiant with Av 1 -1.5 mag.

        If we look only at the V-R colors and assume no reddening then a late
        K-type supergiant is possible. But with any reddening even the V-R
        color becomes too blue for a red supergiant.    
 
        Most people are reporting V and V-R photometry for the possible
        progenitor but multicolor photometry ( especially B and U) is
        needed to constrain the nature of the progenitor and to determine
        the reddening.

        Also the progenitor image is being described as stellar. With our
        digitized scans we have been careful to isolate what appears to be
        a stellar image from possible background contamination and nearby
        stars, and on each plate we measured an image that was basically
        stellar with the same x,y center to 0.15 arcsec with respect to
        a reference grid. Evenso the image on the blue plate was more 
        elliptical. Thus, at the distance of M81 it is probable that
        this image is not single. 

        We have now scanned additional plates of M81 including a short 
        exposure J (blue) and F (red) plates from March 21 1985.
        The plates were scanned in multi-level isodensity thresholds.
        On the J plate the image separates into at least two components.
        One appears to still be blended and the other agrees in position
        to within 0.13 arcsec with the centroid of the short R image
        ( which did not resolve into separate images). This positional
        agreement corresponds to 2 parsecs at the distance of M81. At
        the highest isodensity levels, the B and R images have diameters
        20 microns which is 6 parsecs in M81. Thus these images may 
        still be blended. The corresponding magnitudes for the images on
        these short exposure plates are B=21.8 and R=19.9 mag. 
        If V-R =0.8mag ( see #3 below), then the corresponding V is
        20.7 mag and B-V = 1.1 mag.

        [ The scale of these 4-meter plates is 18.6 arcsec/mm. The 
          encoders on the APS read to 0.366 micron with a 
          repeatability of 1 micron.]

         Observers with CCD images may  be able to deconvolve their
         images.

        Not surprisingly, it is possible to fit the observed energy
        distribution of the progenitor by a wide range of composite spectra
        from a mid K star ( the latest) plus an early B star (the earliest)
        to a late G star plus an early A star. These fits assume no reddening. 
        Increased reddening restricts the range of allowed composite spectra
        by decreasing any contribution from a red supergiant.
   
        However the possible variability may put important constraints on
        any proposed composite. 

     2. Reddening: 
       
       As Richmond reported in IAU Circ 5739 there is high reddening across
       the face of M81, as indicated from the UV images- Av 1.5 mag ( Hill et 
       al 1992); the radio and Halpha measurements by Kaufman et al (1987) 
       show an average reddening of 1.1 mag +/- 0.4 with no gradient from
       the nucleus. In a study of the red supergiants Humphreys et al (1986)
       found Av from 1 -1.5 mag. Thus there is significant reddening
       throughout M81.

       SN1993J may be in a hole, but given its location in a spiral arm
       near a prominent dust lane this seems unlikely. Reddening should
       be considered when discussing the luminosity of the supernova and
       the possible progenitor.


     3. Variability:

        The photometry reported for the possible progenitor shows considerable
      evidence for variability with the R mag posssibly ranging from 20.7 to
      19.0. 

      Summary of photometry for possible progenitor:

Date               V         V-R  (R)      B-V       U-B              Source

Mar 21-23 1982    20.8       0.9  19.9    0.6       0.3          4-meter plates

Jan 21 1985       21.5       0.8  20.7                        CCD Pal 1.5-meter
                  (transformed from r,g-r) 

Mar 21  1985     (20.7)           19.9    1.1                   4-meter plates

Mar  1990         20.0       0.7  19.3    1.1                  CCD KPNO

Jan 24 1992       19.7:      0.8  19.0:                    CCD Hiltner 2.5 meter

Oct 2 1992                        20.0                    CCD KPNO 0.9 meter 

Mar 16-23 1993                    20.0                    Haute-Provence CCD 

    
     There are several very important points about the variability:

     1. The V-R color has remained essentially constant at 0.8 +/- 0.1 mag.
        This is very remarkable. All luminous irregular variables show
        changes in color coinciding with the expansion and contraction
        of their atmospheres. This is also true for M supergiants.

        No change in color with this much variation in magnitude means
        a real change in the total luminosity of the star. 

        This could be explained by the ejection of shells.

     2. An R mag of about 20 appears three or more times in this list.
        If the star is varying between max. and min., one would not expect 
        random measurements to give the same magnitude. This may mean 
        that an R of 20 and a corresponding V of 20.8 represent some
        kind of quiescent state for the star, and are indicative of 
        the star's true luminosity.

     3. In a 1984 paper Sandage ( AJ,89,621) lists the magnitudes for
        several irregular blue variables in M81 for the period 1910
        to about 1955. One of these I2 is quite close to SN1993J. He
        lists variations for this star of a few 0.1's. Thus if the 
        progenitor was varying at that time by one or more magnitudes,
        I think he would have noticed it.

      4. Finally, the variablity may not be real and only due to differences
         in reduction. Because the object is obviously in a crowded region,
         the magnitudes may depend on where the background is set.  

    4. Luminosity:
 

      Using the unreddened distance modulus for M81 of 27.5 - 27.7 and no
     reddening for the progenitor then Mv is -7.6 at visual max.

      But with 1 -1.5 mag Av, then Mv becomes -8.6 to -9.1 and the star
    is in the regime of the cool hypergiants near the upper luminosity
    boundary in the HRD.

       The above luminosities are all for the brightest observed
    mv of near 20 mag. A V mag near 20.8mag may be more representative
    of the progenitor's true luminosity. If V=20.8 then Mv is -6.8 or
    about -7.8 with 1 mag of reddening. 

       For the SN, if max light was mv 10.3 the Mv was   -17.3 or
   withh reddening Mv -18.3 to -18.8.

    5. Needed:

       There are numerous photographic plates of M81 as well as CCD images
    of this famous galaxy. It is critical to measure as many as possible
    to document this stars variability. According to a paper by Sandage
    (1984) plates exist as far back as 1910!

       Zickgraf et al (1990 PASP,102,925) have published a faint UBVR
   CCD sequence for M81 and Sandage (1984 AJ 89,621) has a BV photoelectric
   sequence that can be used for calibration. 


       It is especially important to measure magnitudes in B and U.

       Efforts should be made to deconvolve the image.


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