The objective was a deep (40 ks) SIS/GIS pointing on the bright stellar X-ray source 31 Comae (G0 III) to record the 1-10 keV spectrum and obtain a lightcurve over the approx. 1 day duration of the observation

Ayres, Thomas R.

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Hertzsprung gap Coronae (NAG5-3327:
Investigator Program)
PRINCIPAL INVESTIGATOR :
ASCA Guest
Thomas R. Ayres
University of Colorado
Campus Box 389 [CASA]
Boulder, Colorado 80309-0389
Telephone: 303-492-4051
e-maih ayres@vulcan.colorado.edu
' /L, /:
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FINAL REPORT
SUMMARY.- ASCA Program: "HERTZSPRUNG GAP CORONAE"--Objective was a deep (40 ks)
SIS/GIS pointing on the bright stellar X-ray source 31 Comae (GO III) to record the 1-10 keV spectrum
and obtain a lightcurve over the ---1 day duration of the observation.
The following is the final report on an ASCA program to record the X-ray spectrum
and lightcurve of the bright X-ray source 31 Comae, an GO giant passing through the
Hertzsprung gap. The 40 ks pointing was conducted early in cycle 4. The source was
detected at a level of 0.3 cnts s -1. The SIS and GIS light curves were very stable during
the period of observation, indicating a lack of flare activity. The source was relatively
hard, indicating a mean coronal temperature in excess of ---,107 K.
The X-ray coronae of the fast-rotating Hertzsprung-gap giants (F0-G1 III) like 31 Co-
mae are among the hottest known (logT > 7.3 K); reminiscent of flaring gas in solar
active regions, or on RS CVn binaries and dMe stars. Yet, these giants as a class are not
noted for transient UV or X-ray outbursts; and indeed, they are X-ray-deficient with re-
spect to coronal proxies like Si IV A1400. The paradox--flare-temperature plasma, in the
face of X-ray deficiency and lack of overt flaring--bears on the nature of coronal heating
at the crucial evolutionary juncture where shallow convective envelopes first emerge; the
key transition between hot-star and cool-star X-ray activity.
We modeled the ASCA/SIS0 spectrum using a multi-spectral procedure we had devel-
oped previously for HST, EUVE, and ROSAT data. We constructed a differential volume
emission measure distribution, based primarily on the high-quality EUVE SW and MW
spectra, and introduced the other diagnostics as subsidiary constraints. ASCA provided
the crucial strong constraint on the high-temperature extension of the emission-measure
https://ntrs.nasa.gov/search.jsp?R=19980209649 2020-06-16T00:18:06+00:00Z
distribution, best-fit DVEM curve: the upper temperature extension (log T > 7.3 K)
was established by the ASCA/SIS0 spectrum (above 1.5 keV).
2T XSPEC simulations obtained a good fit for solar abundances, except for Mg: it
was raised to 1.7® to "fill in" a flux deficit near 1.3 keV. A similar effect has been noted
in other ASCA coronal spectra: it more likely is due to problems with the high-T emis-
sivities, than to a genuine compositional anomaly.
The puzzle of the Hertzsprung gap coronae is why they are very hot despite the high
ratio of C IV-to-X-ray emission which--in the context of solar loop scaling models--
implies a rather cool corona. If the solar models are to hold (i.e., imposing a physical
connectedness between the coronal and TZ emissions) the magnetic loops on the shal-
low convection zone giants must have fat footpoints and highly-constricted apexes. On
the other hand, these stars simply might support a dual population of coronal structures
that is very unlike the demographics of the solar case. The high-T emission might arise
in highly extended hot loops (whose large lengths would inhibit short-term variability);
whereas most of the TZ flux might arise in more compact structures (owing to pressure
scale height considerations) which have relatively cool T_ax's (say, < 10 _ K).
Based on ASCA and EUVE low-res spectra and HSTGHRS medium-res spectra of
31 Corn and related giants, we (myself and coauthor Alex Brown) developed a theory
to explain the presence of long, hot loops on the Hertzsprung gap stars. Our hypothe-
sis involves a remnant dipolar "magnetosphere" left over from the main sequence phase
(when the star was an A or B-type dwarf), which is energized by flows associated with
the shallow surface convection zone. but not yet disrupted by it. Later, the deepening
convection zone shreds the fossil dipolar field and replaces it with solar-like "dynamo"-
generated surface activity,. When at full strength, the large-scale dipolar field inhibits
mass loss by an ionized coronal wind. \¥hen the magnetosphere is removed, however, the
coronal wind becomes unconstrained, and the associated rapid loss of angular momentum
causes the star to spindown on a short timescale. The slowing of rotation debilitates the
spin-catalyzed dynamo, and the giants enter a low-activity phase of their coronal evolu-
tion. Our model nicely explains several of the curious features of the post-main sequence
development of coronae among the moderate-mass giants, but many details remain to be
worked out.
A preliminary version of the work was presented as a poster paper at the 1996 HEAD
meeting in San Diego. A detailed study, including also a cycle 5 ASCA observation of the
related star HR 9024 (G1 III), was presented as a poster at the 1997 HEAD meeting in
Estes Park. A formal publication is in preparation, pending additional modeling of the
SIS and GIS data sets.


Hertzsprung Gap Coronae: ASCA Guest Investigator Program

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