Double white dwarfs and AM CVn binaries in the Galactic disc Gijs - - PowerPoint PPT Presentation

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Double white dwarfs and AM CVn binaries in the Galactic disc Gijs - - PowerPoint PPT Presentation

Double white dwarfs and AM CVn binaries in the Galactic disc Gijs Nelemans Institute of Astronomy, Cambridge Gijs Nelemans Outline Introduction Models for Galactic binaries Double white dwarfs Comparison of results, discussion,


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Double white dwarfs and AM CVn binaries in the Galactic disc

Gijs Nelemans

Institute of Astronomy, Cambridge

Gijs Nelemans

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Outline

  • Introduction
  • Models for Galactic binaries
  • Double white dwarfs

– Comparison of results, discussion, observations

  • AM CVn binaries

– Comparison of results, discussion, observations

  • Best guess LISA signals
  • What will we learn from LISA?
  • Conclusions

Gijs Nelemans

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Introduction

  • Most stars become white dwarfs and many are part of

(close) binary system

  • After GWR brings them together, stable mass transfer

may ensue: AM CVn systems

  • Close double white dwarfs and AM CVn systems are

low-frequency gravitational wave sources

  • Double white dwarfs are so numerous that they form an

unresolved noise for LISA

  • What do we know and what can we learn about these

populations?

Gijs Nelemans

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Models for Galactic binaries: ingredients

  • Description of stellar and binary evolution

– M, R, L, Mcore as function Mi, t – Recipe for effect of winds, mass transfer, supernova etc on orbit

  • Initial parameter distributions

– M (IMF), m/M, separation a, eccentricity e

  • Normalization and space distribution

– Star formation history – Binary fraction – Galactic distribution

Gijs Nelemans

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Double white dwarfs

  • Alternative description common envelope

Nelemans, Verbunt, & Yungelson, 2000, A&A, 360, 1011

  • IMF

Kroupa, Tout & Gilmore, MNRAS, 262, 545

  • Galactic model

Boissier & Prantzos, 1999, MNRAS, 307, 857

– Inside out disc formation – SFR(R, t) ∝ Σ1.5

G R−1

– Added bulge: mass consistent with dynamics and micro-lensing

Gijs Nelemans

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New double white dwarf observations, the SPY project

  • ESO VLT survey of ∼1500 white dwarfs for radial

velocity variations (PI Napiwotzki)

  • Current status:

– Surveyed 497 white dwarfs – 94 with radial velocity variations → 80 with white dwarf companion → 14 with main sequence companion – 9 double lined systems (see both white dwarfs) – 5 already have period determinations between 0.3 and 1.5 d

Gijs Nelemans

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Double white dwarfs - comparison with observations

  • Cooling models important

Nelemans, Yungelson, Portegies Zwart & Verbunt, 2001, A&A, 365, 491, with updates Gijs Nelemans

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Double white dwarfs - comparison with observations

  • Alternative common envelope description

Alternative Standard

Nelemans, Yungelson, Portegies Zwart & Verbunt, 2001, A&A, 365, 491, with updates Gijs Nelemans

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Double white dwarfs - comparison ITY97 Han98 NYPV01 HTP02 This talk P(M) ∝ M −2.5 MS79 MS79 KTG93 KTG93 P(m/M) cnst cnst cnst cnst cnst P(log a) cnst cnst cnst cnst cnst SFR(t) cnst cnst e−t/7Gyr cnst BP99 bin frac. (f) 1 1 0.5 1 0.5 f ×

  • SFR dt

7 1010 8.7 1010 4 1010 7.2 1010 4.1 1010 αλ (γ) αT Y = 1 ∼ 0.5 2 (1.75) 1.5 2 (1.75) ν (yr−1) 0.087 0.032 0.048 0.053 0.029 N (108) 3.5 1.0 2.5 ∼3? 2.3

ITY97 = Iben et al 1997, Han98 = Han, 1998, NYPV01 = Nelemans et al 2001, HTP02 = Hurley et al 2002 MS79 = Miller & Scalo 1979, KTG93 = Kroupa et al 1993, BP99 = Boissier & Prantzos 1999

Gijs Nelemans

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Double white dwarfs - discussion

  • Initial distributions

– ITY use different m/M and a distribution for close and wide binaries – With MS79 about 1.15 times more double white dwarfs than with KTG93

  • Binary evolution

– αT Y = 1 corresponds to roughly αλ = 5 – Han uses thermal energy of envelope in common envelope as well – Nelemans et al. alternative to common envelope give 1.7 times mode double white dwarfs – Minimum mass that evolves in age of Galaxy

Gijs Nelemans

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Double white dwarfs - discussion - BP99 model

  • 0.75 times lower birthrate (but similar total number)

5e+09 1e+10 "time ago" (yr) 5 10 15 SFR (Msun/yr) exponential SFR birth rate exponential BP99 + bulge birth rate BP99

Gijs Nelemans

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Double white dwarfs - discussion - BP99 model

  • More binaries in centre than with exponential disc

5 10 15 20 distance 0.1 0.2 0.3 0.4 0.5 0.6 fraction exponential disc BP99 + bulge

Gijs Nelemans

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AM CVn systems

  • AM CVn system are ultra-compact binaries with He rich

secondaries

  • Three formation channels

– From double white dwarfs that come into contact

Paczy´ nski 1967

– From Helium star + white dwarf binaries

Iben & Tutukov 1991

– From CV’s with evolved donors

Podsiadlowski et al 2002/3?

  • Large uncertainty in formation of AM CVn systems

Gijs Nelemans

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AM CVn systems - uncertainties

  • Double white dwarfs:

– Direct impact: large accretor size – Mass ratio of double white dwarfs

  • Helium star + white dwarf

– Edge lit detonation

  • CV’s with evolved donors

– Surface hydrogen – Small number at short periods

Gijs Nelemans

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AM CVn systems - stability mass transfer in double white dwarfs

Marsh, Nelemans & Steeghs, submitted Gijs Nelemans

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AM CVn systems - stability mass transfer in double white dwarfs

Marsh, Nelemans & Steeghs, submitted Gijs Nelemans

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AM CVn systems - stability mass transfer in double white dwarfs

AM CVn systems - uncertainties

  • Double white dwarfs:

– Direct impact: large accretor size – Mass ratio of double white dwarfs

  • Helium star + white dwarf

– Edge lit detonation

  • CV’s with evolved donors

– Surface hydrogen – Small number at short periods

Gijs Nelemans

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AM CVn systems - comparison with observations

Nelemans, Portegies Zwart, Verbunt, Yungelson, A&A, 368, 939 Gijs Nelemans

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AM CVn systems- comparison TY96 NYPV01 HTP02 This talk PHR023 f ×

  • SFR dt

7 1010 4 1010 7.2 1010 4.1 1010 6.9 1010 αλ (γ) αT Y = 1 2 (1.75) 1.5 2 (1.75) ∼ 0.5 ν (yr−1) 0.013 0.005 0.023 0.002 0.0007 N (107) 14 4.9 5.5 4.0

TY96 = Tutukov & Yungelson 1996, PHR02 = Podsiadlowski et al 2002

  • Large differences in birth rate (mass ratio’s)
  • Total numbers rather similar

Gijs Nelemans

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New and future AM CVn observations

  • Three new (possible) AM CVn systems (7 were known)

– V407 Vul (RX J1914.4+2456) P = 9.5 min, X-ray source

Cropper et al. 1998, Ramsay et al. 2002, Mash & Steeghs 2002

– KUV 01584-0939 P = 10.3 min

Warner & Woudt, 2002

– RX J0806.3+1527 P = 5.3 min, X-ray source

Israel et al. 2002, Ramsay et al. 2002 Gijs Nelemans

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Removing uncertainties with observations?

  • Stability of mass transfer in double white dwarfs

– From observed possible short period systems

  • Overall numbers

– Distances with HST – Survey for emission line systems

  • New systems from X-ray surveys?
  • Chemical abundances from accretion disc spectral

modelling

Gijs Nelemans

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Best guess LISA signals

  • Population synthesis including all binaries with compact
  • bjects
  • Gravitational waves from (all) compact binaries

Nelemans et al. 2001, A&A, 375, 890

  • No angular resolution included
  • Double white dwarf noise background
  • Many resolved binaries
  • Quite a few with measurable frequency change

Gijs Nelemans

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Best guess LISA signals

  • resolved systems: 12000 (wd, wd), 10000 AM CVn

Nelemans, 2002, LISA symposium proceedings Gijs Nelemans

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Best guess LISA signals

  • resolved systems

Type birth rate resolved systems with frequency (yr−1) change (wd, wd) 2.9×10−2 12163 560 AM CVn 1.8×10−3 10117 49 (ns, wd) 1.4×10−4 21 3 (ns, ns) 3.2×10−5 1 (bh, wd) 3.8×10−5 1 (bh, ns) 1.0×10−5 total 22303 614

Gijs Nelemans

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What can we learn from LISA?

  • Probe parameter space difficult to reach in other ways
  • Sensitive to (rare) short period systems
  • Overall Galactic distribution
  • Systems with changing frequency: mass limits
  • Including angular resolution could increase number of

detected (neutron star) binaries considerably

Gijs Nelemans

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What can we learn from LISA?

Gijs Nelemans

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Conclusions

  • Models not independent of observations
  • Improved statistics expected to improve models
  • LISA will resolve many thousands of Galactic white

dwarf binaries and some neutron star binaries

  • These will check parts of parameter space that are

inaccessible to other observations

  • Next step is to include LISA’s angular resolution

Gijs Nelemans