A Test for the Disruption of Magnetic Braking in Cataclysmic Variable Evolution P. Davis 1, U. Kolb 1, B. Willems 2, B. T. Gänsicke 3 1 Department of Physics.

Slides:



Advertisements
Similar presentations
The Secondary Stars of Cataclysmic Variables Christian Knigge arXiv: v2 reporter:ShaoYong.
Advertisements

Open Clusters: At The Interface of Stellar Evolution and Stellar Dynamics Robert D. Mathieu University of Wisconsin - Madison.
SDSS finds the period minimum spike Boris Gänsicke John Southworth John Thorstensen M Dillon, P Rodríguez-Gil, A Aungwerojwit, TR Marsh, P Szkody, SCC.
Mass Transfer in Double White Dwarf Binaries Juhan Frank Theoretical Astrophysics Group at Louisiana State University JPL 65th Birthday Conference Trzebieszowice.
Small is Beautiful: Cataclysmic Variables from the SDSS John Southworth Boris Gänsicke Tom Marsh + many others.
Christian Knigge University of Southampton School of Physics & Astronoy P. Marenfeld and NOAO/AURA/NSF Christian Knigge University of Southampton Low-Mass.
Christian Knigge University of Southampton School of Physics & Astronoy Disk Stability vs Close Binary Evolution Rob Hynes (LSU) Christian Knigge University.
Accretion Processes in GRBs Andrew King Theoretical Astrophysics Group, University of Leicester, UK Venice 2006.
Accretion in Binaries Two paths for accretion –Roche-lobe overflow –Wind-fed accretion Classes of X-ray binaries –Low-mass (BH and NS) –High-mass (BH and.
On the Roche Lobe Overflow Reporter: Wang Chen 12/02/2014 Reference: N. Ivanova, v1.
AS 3004 Stellar Dynamics Mass transfer in binary systems Mass transfer occurs when –star expands to fill Roche-lobe –due to stellar evolution –orbit, and.
Vicky Kalogera Jeremy Sepinsky with Krzysztof Belczynski X-Ray Binaries and and Super-Star Clusters Super-Star Clusters.
Magnetars origin and progenitors with enhanced rotation S.B. Popov, M.E. Prokhorov (Sternberg Astronomical Institute) (astro-ph/ )
Mass Loss and Evolution of Low-Mass X-ray Binaries Xiang-Dong Li Department of Astronomy Nanjing University
X-ray Binaries in Nearby Galaxies Vicky Kalogera Northwestern University with Chris Belczynski (NU) Andreas Zezas and Pepi Fabbiano (CfA)
Understanding LMXBs in Elliptical Galaxies Vicky Kalogera.
VLT spectroscopy of SDSS cataclysmic variables John Southworth Boris Gänsicke Tom Marsh.
Population synthesis with dynamics Natasha Ivanova MODEST-6 August 2005 or the problems that we face.
Two stories from the life of binaries: getting bigger and making magnetars Sergei Popov, Mikhail Prokhorov (SAI MSU) This week SAI celebrates its 175 anniversary.
Mike Shara Department of Astrophysics American Museum of Natural History STAR CLUSTER DYNA MIC S Or: BINARY EVOLUTION on STEROIDS.
Secular Evolution of Pre-Main Sequence Triples Erez Michaely Advisor : Prof. Hagai Perets Israel Institute of Technology, Haifa.
Properties of stars during hydrogen burning Hydrogen burning is first major hydrostatic burning phase of a star: Hydrostatic equilibrium: a fluid element.
Variability of Be Stars: A Key to the Structure of their Circumstellar Environments Anatoly Miroshnichenko University of Toledo Variable Star Meeting 2004.
Interesting News… Regulus Age: a few hundred million years Mass: 3.5 solar masses Rotation Period:
ASTR377: A six week marathon through the firmament by Orsola De Marco Office: E7A 316 Phone: Week 6, May 24-27, 2009.
Mass Determinations of Short Period CV Donors Authors: Christopher D.J. Savoury*, S.P Littlefair*, V.S. Dhillion*, T.R. Marsh #, B.T. Gänsicke #, *The.
J. Cuadra – Accretion of Stellar Winds in the Galactic Centre – IAU General Assembly – Prague – p. 1 Accretion of Stellar Winds in the Galactic Centre.
Spin angular momentum evolution of the long-period Algols Dervişoğlu, A.; Tout, Christopher A.; Ibanoğlu, C. arXiv:
He star evolutionary channel to intermediate-mass binary pulsars with a short-orbital-period Chen Wen-Cong School of Physics, Peking University Department.
Basics of Cataclysmic Variables iPTF Summer School August 28, 2014 Paula Szkody U of Washington.
INAF, Osservatorio Astronomico di Roma XI Advanced School of Astrophysics, Brazil, 1-6 September 2002.
The SW Sextantis stars and the evolution of cataclysmic variables
Christian Knigge University of Southampton School of Physics & Astronoy The Secondary Stars of Cataclysmic Variables P. Marenfeld and NOAO/AURA/NSF Christian.
Lars Bildsten Kavli Institute for Theoretical Physics University of California Santa Barbara Unusual Binaries made via Interactions.
CV and pre-CV populations in the SDSS era Ulrich Kolb with Phil Davis (OU), Bart Willems (NWU)
The Brightest point X-ray sources in elliptical galaxies and the mass spectrum of accreting black holes N. Ivanova, V. Kalogera astro-ph/
Qingkang Li Department of Astronomy Beijing Normal University The Third Workshop of SONG, April, 2010 Disks of Be Stars & Their Pulsations &
INTRODUCTION OVERVIEW  Classical Novae (CNe) are thought to occur in binary systems known as Cataclysmic Variables (CV’s).  CV’s are close, interacting.
Where are the Accreting Helium White Dwarfs?? Drawing by T. Piro.
Population of dynamically formed triples in dense stellar systems Natalia Ivanova Fred Rasio, Vicky Kalogera, John Fregeau, Laura Blecha, Ryan O'Leary.
Models of Blue Stragglers part I A talk for Hans Zinnecker (sort of). Alison Sills, McMaster University.
Do accretion discs regulate the momentum of young stars? S.P. Littlefair 1,2, T. Naylor 2, R.D. Jeffries 3, B. Burningham 2, E. Saunders 2 1 Dept of Physics.
Comprehensive analytic formulae for stellar evolution as a function of mass and metallicity Author : Jarrod R. Hurley , Onno R. Pols and Christopher A.
White Dwarf Binaries in Globular Clusters Fred Rasio (Northwestern)
Two planets orbiting the post-common envelope binary NN Serpentis Evidence for planets orbiting the post-common envelope binary NN Serpentis Stefan Dreizler.
From an evolutionary point of view Selma de Mink Utrecht University Lorentz Center Workshop “Stellar Mergers” Ines Brott (Utrecht), Matteo Cantiello (Utrecht),
Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:
1. INTRODUCTION As the brightest dwarf nova and one of the brightest cataclysmic variables of any kind, SS Cygni has been extensively observed. Its outbursts,
Constraining close binaries evolution with SDSS/SEGUE: a representative sample of white dwarf/main sequence binaries Matthias Schreiber ESO, May 4th, 2006.
Introduction Star itself Ejecta, Great Eruption in 1840 formed the Homunculus The 5.52 yr periodicity Binary vs shell D = 2.3 kpc.
Orbital evolution of compact Black-hole binaries and white dwarf binaries Wencong Chen Astro-ph/ Astro-ph/
PCEBs from the SDSS testing disrupted magnetic braking Matthias Schreiber Tucson, March-2009 Boris T. Gaensicke, John Southworth, S. Stylianos (Warwick)
The Empirical Mass Distribution of Hot B Subdwarfs derived by asteroseismology and other means Valerie Van Grootel (1) G. Fontaine (2), P. Brassard (2),
Cataclysmic Variables: A Perfect Testbed for Variability Brokering Paula Szkody University of Washington Santa Barbara May 13, 2015.
Evolutionary Sequences For Low- And-Intermediate-Mass X-Ray Binaries Ph. Podsiadlowski S. Rappaport E. D. Pfahl.
Classical Novae on a Helium White Dwarf Irit Idan (Technion) Lars Bildsten ((KITP, UCSB) Ken Shen (UCSB)
L 3 - Stellar Evolution I: November-December, L 3: Collapse phase – theoretical models Background image: courtesy ESO - B68 with.
Be/X-Ray 双星中的中子星自传演化 成忠群 南京大学 Contents 1. Introduction (1) Observed period gap for BeXBs (2) Possible interpretation by the authors 2. What.
The mass of the neutron star in SMC X-1 A.K.F Val Baker, A.J. Norton & H. Quaintrell Department of Physics and Astronomy, The Open University, Walton Hall,
Formation of Redback and Black Widow Binary Millisecond Pulsars
Einstein 2005 July 21, 2005 Relativistic Dynamical Calculations of Merging Black Hole-Neutron Star Binaries Joshua Faber (NSF AAPF Fellow, UIUC) Stu Shapiro.
Binary Origin of Blue Stragglers Xuefei CHEN Yunnan Observatory, CHINA.
Black Widow Pulsars(BWP): the Price of Promiscuity A. R. King, M. B. Davies and M. E. Beer, 2003,MNRAS,345,678 Fu Lei
FOUR NEW ECLIPSING CATACLYSMIC VARIABLES FROM THE SDSS John Southworth and Boris Gänsicke Department of Physics, University of Warwick, UK
Matteo Cantiello Astronomical Institute Utrecht Binary star progenitors of long GRBs M. Cantiello, S.-C. Yoon, N. Langer, and M. Livio A&A 465, L29-L33.
The Minimum Mass Ratio for Contact Close Binary
Evolution of X-ray Binaries and the Formation of Binary Pulsars
Delay time distribution of type Ia supernovae
Delay time distribution of type Ia supernovae
Center for Gravitational Wave Physics Penn State University
Presentation transcript:

A Test for the Disruption of Magnetic Braking in Cataclysmic Variable Evolution P. Davis 1, U. Kolb 1, B. Willems 2, B. T. Gänsicke 3 1 Department of Physics & Astronomy, Open University, Walton Hall, Milton Keynes, MK7 6AA, UK 2 Department of Physics & Astronomy, Northwestern University, 2131 Tech Drive, Evanston, Illinois, USA 3 Department of Physics, University of Warwick, Coventry, UK MNRAS, 2008, 389,

Talk Overview ■ The period gap ■ The disrupted magnetic braking hypothesis ■ Our method ■ Summary of results ■ Future work: the SDSS ■ Conclusions

The Period Gap & The Disrupted Magnetic Braking Hypothesis

Ritter & Kolb (2003), Edition 7.9 (2008)

Donor fully convective → magnetic braking ceases System becomes “dCV” Mass transfer resumes ~ 2 h Evolution driven by gravitational radiation. Rappaport, Verbunt & Joss (1983) Spruit & Ritter (1983) Magnetic braking drives rapid mass transfer  donor star swells

Method

■ Calculate present day populations of: ● “detached CVs” (dCVs) ● “gap post-common envelope binaries” (gPCEBs)  0.17 < M 2 / M sun < 0.36 ■ BiSEPS (Binary System Evolution and Population Synthesis) ● Stellar evolution package: Hurley, Pols & Tout 2000 ● Binary Evolution based on Hurley, Tout & Pols 2002 ● Open University developed code (Willems & Kolb 2002, 2004) ● Significant modifications: □ Realistic treatment of mass transfer in CVs □ Reaction of donor star due to mass loss □ Evolution of dCV across period gap

Primary mass ? Initial Mass Ratio Distribution Common Envelope ejection efficiency, α CE α CE = constant = 0.1 – 5.0 (e.g. Willems & Kolb 2004) α CE = (M 2 /M sun ) p, p = 0.5, 1, 2 (Politano & Weiler 2007) Magnetic Braking Strength + Hurley, Pols & Tout (2002) Rappaport, Verbunt & Joss (1983) R 3 Ω 3 (M env /M) R 2 Ω 3 M R 4 Ω 3 M Angular momentum loss rate Calibrate strength  ~10 -9 M sun yr -1 at 3 hr (e.g. McDermot & Taam 1989) Disrupting Magnetic Braking ■ Gap width of ~ 1 hour ■ R 2 ~ 1.3R MS at 3 hr ■ Disrupt magnetic braking once M 2 = 0.17M sun ■  lower edge at ~ 2 hr

Results

Excess of dCVs over PCEBs in the period gap → “Mirror Gap” ■ Flat initial mass ratio distribution (Goldberg, Lazeh & Latham 2003 ■ α CE = 1 gPCEB dCV Total

“Mirror Gap” α CE = 0.6 α CE = 0.1 ■ Flat initial mass ratio distribution (Goldberg, Lazeh & Latham 2003) ■ Significant Mirror Gap. Ratio dCV/gPCEB in gap: ● ~ 13 for α CE = 0.1 ● ~ 4 for α CE = 0.6 Iben & Livio 1993

■ The ratio dCV:gPCEB  indicator of size of mirror gap

How about… ■ Different Magnetic braking strengths? ■ Narrower period gap? From a weaker magnetic braking law? (Ivanova & Taam 2003) Gap width of ½ hr  dCV:gPCEB ~ 2.1  mirror gap still expected. ■ CVs from thermal timescale mass transfer Contribute an extra ~40% to calculated dCV population (Kolb & Willems 2005) dCV:gPCEB =3.5 dCV:gPCEB =5.5 dCV:gPCEB =6.0  Still obtain a mirror gap with a significant peak height, irrespective of MB law

■ ~ 50 PCEBs identified with determined orbital periods. ~10 from SDSS (Rebassa-Mansergas et al 2008, Schreiber et al. 2008) ■ 3 dCV candidates so far identified. □ At 164.2, and 130 minutes ■ Require few hundred white dwarf-main sequence binaries to adequately resolve mirror gap. SDSS

Conclusions ■ Dearth of CVs with P orb ≈ 2 and 3 hours. ■ Standard explanation  disrupted magnetic explanation… ■ Test: Orbital period distribution of gPCEB and dCV population  “Mirror Gap”  excess of dCV over gPCEBs there. ■ Expect dCV:gPCEB ~ 4 to 13  mirror gap with a significant peak height ■ Observationally feasible  SDSS

References ■ Goldberg D., Mazeh T., Latham D. W., 2003, ApJ, 591, 397 ■ Hurley J. R., Pols O. R., Tout C. A., 2000, MNRAS, 315, 543 ■ Hurley J. R., Tout C. A., Pols O. R., 2002, MNRAS, 329, 897 ■ Iben I. J., Livio M., 1993, PASP, 105, 1357 ■ Ivanova N., Taam R. E., 2003, ApJ, 599, 516 ■ Jones B. F., Fischer D. A., Stauffer J. R., 1996, AJ, 112, 1562 ■ Knigge C., 2006, MNRAS, 373, 484 ■ Kolb U., Willems B., 2005, ASP Conf. Ser., 330, 17 ■ Politano M., Weiler K. P., 2007, ApJ, 665, 663 ■ Rappaport S., Verbunt F., Joss P. C., 1983, ApJ, 275, 713 ■ Rebassa-Mansergas A., et al., 2007, MNRAS, 382, 1377 ■ Rebassa-Mansergas A., et al., 2008, MNRAS, 390, 1635 ■ Ritter H., Kolb U., 2003, A&A, 404, 301 ■ Schreiber M. R., et al., 2008, A&A, 484, 441 ■ Spruit H. C., Ritter H., 1983, A&A, 124, 267 ■ Willems B., Kolb U., 2002, MNRAS, 337, 1004 ■ Willems B., Kolb U., 2004, A&A, 419, 1057