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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,


  1. Double white dwarfs and AM CVn binaries in the Galactic disc Gijs Nelemans Institute of Astronomy, Cambridge Gijs Nelemans

  2. 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

  3. 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

  4. Models for Galactic binaries: ingredients • Description of stellar and binary evolution – M , R , L , M core as function M i , 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

  5. 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 ) ∝ Σ 1 . 5 G R − 1 – Added bulge: mass consistent with dynamics and micro-lensing Gijs Nelemans

  6. 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

  7. Double white dwarfs - comparison with observations • Cooling models important Nelemans, Yungelson, Portegies Zwart & Verbunt, 2001, A&A, 365, 491, with updates Gijs Nelemans

  8. 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

  9. Double white dwarfs - comparison ITY97 Han98 NYPV01 HTP02 This talk ∝ M − 2 . 5 P ( M ) MS79 MS79 KTG93 KTG93 P ( m/M ) cnst cnst cnst cnst cnst P (log a ) cnst cnst cnst cnst cnst e − t/ 7 Gyr SFR ( t ) cnst cnst cnst BP99 bin frac. ( f ) 1 1 0.5 1 0.5 7 10 10 8.7 10 10 4 10 10 7.2 10 10 4.1 10 10 � f × SFR d t αλ ( γ ) α T 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 (10 8 ) 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

  10. 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 – α T 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

  11. Double white dwarfs - discussion - BP99 model • 0.75 times lower birthrate (but similar total number) 15 exponential SFR birth rate exponential BP99 + bulge birth rate BP99 10 SFR (Msun/yr) 5 0 5e+09 1e+10 "time ago" (yr) Gijs Nelemans

  12. Double white dwarfs - discussion - BP99 model • More binaries in centre than with exponential disc exponential disc 0.6 BP99 + bulge 0.5 0.4 fraction 0.3 0.2 0.1 0 0 5 10 15 20 distance Gijs Nelemans

  13. 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

  14. 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

  15. AM CVn systems - stability mass transfer in double white dwarfs Marsh, Nelemans & Steeghs, submitted Gijs Nelemans

  16. AM CVn systems - stability mass transfer in double white dwarfs Marsh, Nelemans & Steeghs, submitted Gijs Nelemans

  17. 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

  18. AM CVn systems - comparison with observations Nelemans, Portegies Zwart, Verbunt, Yungelson, A&A, 368, 939 Gijs Nelemans

  19. AM CVn systems- comparison TY96 NYPV01 HTP02 This talk PHR023 7 10 10 4 10 10 7.2 10 10 4.1 10 10 6.9 10 10 � f × SFR d t αλ ( γ ) α T 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 (10 7 ) 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

  20. 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

  21. 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

  22. Best guess LISA signals • Population synthesis including all binaries with compact objects • 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

  23. Best guess LISA signals • resolved systems: 12000 (wd, wd), 10000 AM CVn Nelemans, 2002, LISA symposium proceedings Gijs Nelemans

  24. Best guess LISA signals • resolved systems Type birth rate resolved systems with frequency (yr − 1 ) change 2.9 × 10 − 2 (wd, wd) 12163 560 1.8 × 10 − 3 AM CVn 10117 49 1.4 × 10 − 4 (ns, wd) 21 3 3.2 × 10 − 5 (ns, ns) 1 0 3.8 × 10 − 5 (bh, wd) 1 0 1.0 × 10 − 5 (bh, ns) 0 0 total 22303 614 Gijs Nelemans

  25. 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

  26. What can we learn from LISA? Gijs Nelemans

  27. 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

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