Hydrogen Lines in DA White Dwarfs: Improved Stark Broadening - PowerPoint PPT Presentation

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Hydrogen Lines in DA White Dwarfs: Improved Stark Broadening

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Spectroscopic Technique : Bergeron et al. (1992) Photosphere at 20,000 K ... Mike Seaton (1990) : MHD88 effects should also be included in line profiles calculations. ... – PowerPoint PPT presentation

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Title: Hydrogen Lines in DA White Dwarfs: Improved Stark Broadening


1
Hydrogen Lines in DA White Dwarfs Improved Stark
Broadening
Pier-Emmanuel Tremblay Pierre
BergeronUniversité de Montréal
E
-

2
Hydrogen-line (DA) white dwarfs
3
Spectroscopic Technique Bergeron et al. (1992)
4
Photosphere at 20,000 K
5
Mihalas, Hummer Däppen 1988Occupation
probability formalism
6
Mihalas, Hummer Däppen 1988Occupation
probability formalism
T10,000 K
T20,000 K
charged - neutral
7
W
WD0205250"old models" priorto 1992
8
Mike Seaton (1990) MHD88 effects should also be
included in line profiles calculations. Bergeron
(1993) ad-hoc parameter, used in all codes
(TLUSTY)
VCS ßcritx2
9
Stark Broadening - Hydrogen
10


Constant Electric FieldLinear Stark Effect
-




11
Microfield Distribution
  • ßE/Eo
  • P(ß)dß

MHD88 Holtsmark Nayfonov (1999) Hooper
12
rRdebye
Vidal, Cooper Smith (1973)Lemke (1997)
v
?(H)
e-
?
Constant Electric FieldLinear Stark Effect
H
?(e)
rRmin
13
Non-adiabatic quantum calculations
n5
n4
electronic collisions no-quenching
n3
n2
n1
t
14
V(r) qEz
Hydrogen Atom V(r)
V(z)
V(z)
z
z
Saddle point
?E
Energy of Nth level
15
Mihalas, Hummer Däppen 1988Occupation
probability formalism
Bound state
Free State
?E
16
ßcrit value not arbitrary!
  • ?crit

electronic collisions
17
Seaton (1990)
High Fields
Low Fields
Seaton (1990) first non-ideal profiles using
approximate electronic broadening
profiles Bergeron (1993) ad-hoc parameter.
18
This work
  • Vidal, Cooper Smith (1973) electron broadening
    theory.
  • Non-ideal correction for proton perturbations
    (MHD 88, Seaton 90).

19
This work
  • Non-ideal correction for electron perturbations
    (MHD 88).
  • It accounts for about 10 of the non-ideal
    effects.
  • Consistent implementation of the MHD88 Theory.

20
VCS This Work M. Seaton
(Lemke 1997)
T10,000 K Log Ne 17
21
Wiese et al. (1972)
22
(No Transcript)
23
0.7 M?
0.55 M?
0.7 M?
0.55 M?
24
0.7 M?
0.55 M?
0.7 M?
0.55 M?
25
(No Transcript)
26
?Teff 100 K ?log g 0.06
27
GD71
HZ43
This work VCS ßcritx2
28
Independent constraints
29
40 Eri B
30
Conclusion
  • Spectroscopic technique (Bergeron et al. 1992).
  • Current model atmospheres use MHD88 EOS and VCS
    Stark broadening profiles (Lemke 1997 tables)
  • Here we add MHD88 inside the VCS broadening
    theory in a consistent way for the first time.
  • We are currently looking at further implications
    at low and high Teff, UV lines and DO white
    dwarfs.
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