1 / 10

Trends in the Chandra X-Ray Spectra of O and Early B Stars

Trends in the Chandra X-Ray Spectra of O and Early B Stars. June 24, 2008. Spectra of Stars. We know that spectra result from physical processes within stars. They often reflect physical properties of the stars that created them. ex. Optical Spectra. X-Ray Spectra of O and Early B Stars.

tyne
Télécharger la présentation

Trends in the Chandra X-Ray Spectra of O and Early B Stars

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Trends in the Chandra X-Ray Spectra of O and Early B Stars June 24, 2008

  2. Spectra of Stars • We know that spectra result from physical processes within stars. • They often reflect physical properties of the stars that created them. ex. Optical Spectra

  3. X-Ray Spectra of O and Early B Stars • The spectra on the left are a representative sampling of O and early B star spectra, with earlier spectral types at top. • The spectra were taken on the Chandra X-Ray telescope using the high energy transmission grating (HETG) on the advanced camera for imaging spectroscopy (ACIS). • Nolan Walborn suggested in a 2006 paper that these spectra may reveal a temperature trend similar to that observed for optical spectra. • I will be looking for evidence that tends to confirm or disprove this hypothesis.

  4. X-Ray Production in Hot Stars • X-Ray emission arises in the stellar winds of these stars. • The stellar winds are radiatively driven. • The line-driven stellar winds are inherently unstable. • Shocks in the wind arise from the instability and produce x-rays.

  5. X-Ray Spectra and Temperature • Line strength ratios • Differential Emission Measure dEM= nenH dV In a plasma with a single well-defined temperature, or D(T)= ne(T)nH(T)(dV/d logT) in a plasma with a temperature distribution.

  6. Delta Orionis O9.5 II + B0.5 III Teff = 33000 K R= 17 Rsun M=23 Msun vinf = 2000 km/s dM/dt = 1.07 * 10-6 Msun/yr HD93129AB O2 If* + (2x) O3.5 V((f+)) Teff = 50000 K R= 20 Rsun M=120 Msun vinf = 3200 km/s dM/dt = 1.8 * 10-5 Msun/yr Xi Persei O7.5 III(n)((f)) Teff = 36000 K R= 12 Rsun M=34 Msun vinf = 2450 km/s dM/dt = 2.0 * 10-6 Msun/yr Stars and Parameters

  7. HD93129AB Xi Persei Delta Orionis 0.05 ± 0.02 0.05 ± 0.02 0.21 ± 0.06 Silicon XIV/Silicon XIII Ratios

  8. HD93129AB Xi Persei Delta Orionis 0.27 ± 0.04 0.12 ± 0.02 0.24 ± 0.03 Magnesium XIV/Magnesium XIII Ratios

  9. Conclusions (for now) • Line ratios of stars in our sample seem to have little to do with effective temperature. • This tends to disprove Walborn’s suggestion that the trend in the spectrum is temperature-related. • However, there does appear to be some slight tendency for individual lines to become broader and more blueshifted in the hotter stars.

  10. Some Directions for Research • Continue to measure line ratios in more stars. • Possibly explore measuring line ratios for other elements. • Look into measuring emission measures for our sample stars as another probe of temperature.

More Related