Boron Abundances in Rapidly Rotating Early-B Stars.
Models of rotation in early-B stars predict that rotationally driven mixing should deplete surface boron abundances during the main-sequence lifetime of many stars. However, recent work has shown that many boron depleted stars are intrinsically slow rotators for which models predict no depletion should have occurred, while observations of nitrogen in some more rapidly rotating stars show less mixing than the models predict. Boron can provide unique information on the earliest stages of mixing in B stars, but previous surveys have been biased towards narrow-lined stars because of the difficulty in measuring boron abundances in rapidly rotating stars. The two targets observed as part of our Cycle 13 SNAP program 10175, just before STIS failed, demonstrate that it is possible to make useful boron abundance measurements for early-B stars with Vsin(i) above 100 km/s. We propose to extend that survey to a large enough sample of stars to allow statistically significant tests of models of rotational mixing in early-B stars.
Targets are all bright B0 to B2, class III-V stars, with projected rotational velocities, V sin(i), between 65 and 165 km/s.
Acquisitions for stars fainter than V=4.5 use the F28X50OIII filter with exposure times calculated to give S/N=300, and a peak pixel with about 43,000 e- or about 30% of the full well. For brighter stars, the F28X50ND5 filter is used with an exposure time set to give S/N=120, and a peak pixel with about 6800 e-. Note special ACQ sequence for visit 23 to ensure observation of the correct star.
All visits then take dithered CR-SPLIT=NO, GAIN=4 exposures with the STIS CCD G230MB grating (R=6000) at the 1995 CENWAVE setting with the 52X0.2 aperture, using a 6 point centered STIS along-the-slit pattern with 0.431035" (8.5 pixel) spacing. This spectral range covers 1917 to 2073 Angstroms and includes, among other things, the B III resonance doublet at 2065/2068 angstroms, a strong C III multiplet near 1923 angstroms, and numerous blended Fe III and Fe IV lines. The spectra will also include ISM lines from Zn II and Cr II.
Exposure times for each subexposure are calculated based on the measured TD1 flux in the 1965 angstrom band. Where this is not available, estimates based on IUE LGAP fluxes or stellar models are used instead. For stars with FLAM(1965) greater than about 6e-10 ergs/cm2/Angstrom/sec, the exposure time is choosen to give a Poisson S/N of 500:1 per resolution element per exposure. Stars fainter than this use a fixed time of 120 s per exposure. The faintest target should still give S/N=170 in each exposure. Actual S/N achieved will depend on how good the pixel-to-pixel flat fields are. The six individual exposures at the different dither positions will be coadded and cosmic-ray rejected using customized software.
Sample exposure time calculations at 2065 angstroms. S/N given per 2-pixel wide resolution element summed over 7 pixel high extraction box:
Target 1: Kurucz B1V model normalized to FLAM(1965)=1.2e-10 gives S/N=250 per 120 s exposure.
Target 14: Kurucz B1V model normalized to FLAM(1965)=7.55e-10, gives S/N=500 per 76.1 s exposure.
Target 41: Kurucz B1V model normalized to FLAM(1965)=5.7e-11 gives S/N=170 per 120 s exposure.
The shortest visit requires a visibility of about 20 minutes. The 27 longest visits with 120 s exposure times each require about 31 minutes of visibility.
Auto-wavecals have been replaced with GO-specified wavecals at the end of each visit.
Three of the targets in this program, HD160578, HD143275, and HD144217 have GHRS Echelle B data close to the wavelength of the B III line. However, for two of these stars, the data don’t actually reach both B III lines, while for the third, HD143275, the S/N does not appear to be adequate for our purposes. Note that these potential duplications for HD143275 and HD144217 were discussed in our phase 1 proposal, while for HD 160578, the GHRS data don't cover either boron line at all!
HOT STARS
0
false
0.0
0.0
false
false
false
false
false
AVAILABLE
STAR
B0-B2 V-IV
SPEC=B1V; B-V=-0.084; FLAM(1965)=1.19800e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B1.5V; B-V=-0.058; FLAM(1965)=1.50100e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B0.5V; B-V=-0.199; FLAM(1965)=3.23700e-09
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B1.5IV; B-V=-0.031; FLAM(1965)=1.09900e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2V; B-V=-0.192; FLAM(1965)=2.36600e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B1.5V; B-V=-0.142; FLAM(1965)=8.50000e-11
J2000
00 00 0.0000
+00 00 0.00
J2000
STAR
B0-B2 V-IV
SPEC=B1.5IV; B-V=-0.216; FLAM(1965)=2.34000e-10
J2000
00 00 0.0000
+00 00 0.00
J2000
STAR
B0-B2 V-IV
SPEC=B2IV-V; B-V=-0.156; FLAM(1965)=2.31300e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV-V; B-V=-0.195; FLAM(1965)=3.27700e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2V; B-V=-0.175; FLAM(1965)=3.90000e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 III-I
SPEC=B2III; B-V=-0.164; FLAM(1965)=9.95000e-11
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B0.5IV; B-V=0.0330; FLAM(1965)=1.07000e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV/V; B-V=-0.170; FLAM(1965)=1.33300e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV/Ve; B-V=-0.150; FLAM(1965)=7.55000e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2Ve; B-V=-0.190; FLAM(1965)=1.15300e-10
J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B1V; B-V=-0.151; FLAM(1965)=3.39600e-10
J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B1.5IV; B-V=-0.151; FLAM(1965)=2.19300e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B1.5Vp; B-V=-0.228; FLAM(1965)=8.15000e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B1IV; B-V=-0.195; FLAM(1965)=1.20000e-09
J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B0Vp; B-V=-0.220; FLAM(1965)=6.50000e-09
J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV; B-V=-0.193; FLAM(1965)=4.21400e-09
J2000
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J2000
STAR
B0-B2 V-IV
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J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B1V; B-V=-0.210; FLAM(1965)=2.50000e-08
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV-V; B-V=-0.176; FLAM(1965)=4.14200e-09
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2V; B-V=-0.178; FLAM(1965)=2.49200e-09
J2000
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J2000
STAR
B0-B2 V-IV
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J2000
00 00 0.0000
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J2000
STAR
B0-B2 III-I
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J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV; B-V=-0.225; FLAM(1965)=2.32800e-09
J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV-Ve; B-V=-0.170; FLAM(1965)=1.85600e-09
J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
00 00 0.0000
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J2000
STAR
B0-B2 III-I
SPEC=B2III; B-V=-0.177; FLAM(1965)=7.73000e-10
J2000
00 00 0.0000
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J2000
STAR
B0-B2 III-I
SPEC=B2III; B-V=-0.184; FLAM(1965)=4.20300e-09
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
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J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B0.2IV; B-V=-0.117; FLAM(1965)=4.31200e-09
J2000
00 00 0.0000
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J2000
STAR
B0-B2 V-IV
SPEC=B2V; B-V=-0.024; FLAM(1965)=1.7e-10
J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 III-I
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 III-I
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B2IV-V; B-V=-0.132; FLAM(1965)=3.27200e-10
J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
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J2000
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J2000
STAR
B0-B2 V-IV
SPEC=B1V...; B-V=-0.071; FLAM(1965)=2.90200e-10
J2000
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J2000
STIS/CCD
Spectroscopic
No
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G230MB
1995
POS-TARG
DITHER
0.431035
LINE
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true
6
90.0
STIS-ALONG-SLIT
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true
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true
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true
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The scheduling data was generated by CASM 17.2.
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true
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The scheduling data was generated by CASM 17.2.
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true
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The scheduling data was generated by CASM 17.2.
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true
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The scheduling data was generated by CASM 17.2.
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false
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The scheduling data was generated by CASM 17.2.
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true
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The scheduling data was generated by CASM 17.2.
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true
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The scheduling data was generated by CASM 17.2.
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true
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Copy of visit 20
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false
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The scheduling data was generated by CASM 17.2.
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true
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The scheduling data was generated by CASM 17.2.
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true
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Copy of visit 22
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false
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The scheduling data was generated by CASM 17.2.
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The target for visit 23, HD 108249 is only 4" from the slightly brighter star HD 108248 (target 22). A slightly bigger than expected pointing error could put both stars in the ACQ subarray, causing the wrong one to be observed, but our knowledge of the relative offset isn't good enough to do a blind offset from the brighter to the fainter one, and an offset followed by a peakup would take more time than we want to spend.
So instead, we will first do an ACQ on the brighter of the two stars. This should cancel out any pointing errors due to the guide star coordinate accuarcy, and ensure that the second ACQ image only contains the fainter target HD 108249.
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true
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true
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Copy of visit 24
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false
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The scheduling data was generated by CASM 17.2.
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true
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Copy of visit 25
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false
1
0
The scheduling data was generated by CASM 17.2.
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