application of x-ray plasma diagnostics to nova winds

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(ESAC) European Space Astronomy Centre Jan-Uwe Ness Jan-Uwe Ness XMM-Newton Science Operations Centre XMM-Newton Science Operations Centre Application of X-ray Plasma Diagnostics to Nova Winds Chandra XMM-Newton Swift

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Talk presented by Jan-Uwe Ness (XMM-Newton Science Operations Centre) at the symposium "From atoms to stars: the impact of spectroscopy on astrophysics", Oxford, UK, 28-28 July 2011.

TRANSCRIPT

Page 1: Application of X-ray plasma diagnostics to nova winds

(ESAC)

European Space Astronomy Centre

Jan-Uwe NessJan-Uwe NessXMM-Newton Science Operations CentreXMM-Newton Science Operations Centre

Application of X-ray PlasmaDiagnostics to Nova Winds

ChandraXMM-Newton

Swift

Page 2: Application of X-ray plasma diagnostics to nova winds

The RS Oph system Recurrent Nova with 6 recorded outbursts since 1898

Page 3: Application of X-ray plasma diagnostics to nova winds
Page 4: Application of X-ray plasma diagnostics to nova winds

Accreted

material:H-rich!

Nuclear burning ignites

outburst

WD

Page 5: Application of X-ray plasma diagnostics to nova winds

Accreted

material:H-rich!

Nuclear burning ignites

outburst

enough radiativeenergy is producedto drive a wind with

v ≈ 1500 km s-1

WD

Page 6: Application of X-ray plasma diagnostics to nova winds

Pseudo Stellar

AtmosphereNuclear burning

Photosphere

Radiatively driven expansion

brightest in optical -> discovery

equivalent toa stellarradiation zone

R=100x106km

after 1 day

WD

Page 7: Application of X-ray plasma diagnostics to nova winds

WD

Nuclear burning

Photosphere

Density drops, outer layers go optically thin

=> Radius of Photosphere recedes to inner, hotter, layers

Pseudo Stellar

Atmosphere

Page 8: Application of X-ray plasma diagnostics to nova winds

Pseudo Stellar

AtmosphereNuclear burning

Photosphere

=> fades in optical but Lbol constant

=> spectrum shifts to higher energies ...

WD

Page 9: Application of X-ray plasma diagnostics to nova winds

Pseudo Stellar

AtmosphereNuclear burning

Photosphere

.... until the peak of the spectrum reaches soft X-rays

--> direct observations of nuclear burning

Super-Soft-SourceX-ray spectrum

⇒ SSS phaseWD

Page 10: Application of X-ray plasma diagnostics to nova winds

Lbol=1038 erg/s

WD WD WD

Constant Bolometric Luminosity phaseConstant Bolometric Luminosity phase

optical UV X-ray

Page 11: Application of X-ray plasma diagnostics to nova winds
Page 12: Application of X-ray plasma diagnostics to nova winds
Page 13: Application of X-ray plasma diagnostics to nova winds

Novae are powered by nuclear burning

The pressure is not high enough on a WD

surface to produce any elements heavier

than Helium

The CNO cycle changes the relative

abundances of C, N, and O

If the nova ejecta show any other

anomalies in composition, then either

- WD material has been dredged up

- The companion is anomalous

Page 14: Application of X-ray plasma diagnostics to nova winds

SSS Emission from hot white dwarf

Shock withstellar wind

+ giant in Symbiotic Novae

+ MS star in Classical Novae

Page 15: Application of X-ray plasma diagnostics to nova winds

Osborne et al. (2011)

shock phase SSS phase nebular phase

Swift observations of RS Oph

optical

Page 16: Application of X-ray plasma diagnostics to nova winds

Osborne et al. (2008)

shock phase SSS phase nebular phase

Swift observations of RS Oph

Ch

an

dra

/XM

M

XM

M-N

ew

ton

Ch

an

dra

XM

M-N

ew

ton

----

--- -

----

Ch

an

dra

Ch

an

dra

Page 17: Application of X-ray plasma diagnostics to nova winds

Swift spectra

Page 18: Application of X-ray plasma diagnostics to nova winds

grating spectra

Page 19: Application of X-ray plasma diagnostics to nova winds

RS Oph: 13.8 days after outburst H-like ionsHe-like ionsother lines(FeXVII - FeXXV)

simultaneousChandra and XMMspectra

Page 20: Application of X-ray plasma diagnostics to nova winds
Page 21: Application of X-ray plasma diagnostics to nova winds

Ness & Jordan (2008) MNRAS 385, 1691

Page 22: Application of X-ray plasma diagnostics to nova winds
Page 23: Application of X-ray plasma diagnostics to nova winds

3-T APEC model reproducesthe observations

==>Assumption of collisional

equilibrium may not be too bad

proper EMD analysis

Page 24: Application of X-ray plasma diagnostics to nova winds

f G T

Page 25: Application of X-ray plasma diagnostics to nova winds

N

O NeSi

MgS

Fe

Page 26: Application of X-ray plasma diagnostics to nova winds

f G T

Page 27: Application of X-ray plasma diagnostics to nova winds

f G T

Page 28: Application of X-ray plasma diagnostics to nova winds

N

O

Ne

Mg Si

S

Fe

Page 29: Application of X-ray plasma diagnostics to nova winds

solarabundance

0.46 x solar

Page 30: Application of X-ray plasma diagnostics to nova winds

N high=>CNO-cycledmaterial

Page 31: Application of X-ray plasma diagnostics to nova winds

RS Oph secondary has [N/Fe]=0.9:(Pavlenko et al. 2008)

=> 20-40% of N fromoutburst or companion

Page 32: Application of X-ray plasma diagnostics to nova winds

Sample of M giants bySmith & Lambert (1985/86)

RS Oph secondary has [N/Fe]=0.9:(Pavlenko et al. 2008)

=> 20-40% of N fromoutburst or companion

Page 33: Application of X-ray plasma diagnostics to nova winds

Sample of M giants by Rich et al. (2007)

Mg, Si not produced in outburst=> must come from WD or companion

Page 34: Application of X-ray plasma diagnostics to nova winds

The companion in Symbiotic Novae is a giant star that has similar abundance ano- malies as those expected in nova ejecta The abundances for RS Oph appear more anomalous than for typical stars of the same spectral type as the companion We might be seeing WD material

=> too many heavy elements for SN Ia But: The companion in symbiotics is stripped off the outer layers, exposing layers with different abundances.

Summary