Eccentric Binary Millisecond Pulsars Paulo C. C. Freire arXiv:0907.3219v1.

Slides:



Advertisements
Similar presentations
Neutron Stars: Insights into their Formation, Evolution & Structure from their Masses and Radii Feryal Ozel University of Arizona In collaboration with.
Advertisements

Inspiraling Compact Objects: Detection Expectations
A New Relativistic Binary Pulsar: Gravitational Wave Detection and Neutron Star Formation Vicky Kalogera Physics & Astronomy Dept with Chunglee Kim (NU)
X-ray pulsars in wind-fed accretion systems 王 伟 (NAOC) July 2009, Pulsar Summer School Beijing.
The Neutron Star Equation of State- Electromagnetic Observations Frits Paerels Columbia University GWPAW, UW Milwaukee, January 26, 2011.
ASTR Fall Semester Joel E. Tohline, Alumni Professor Office: 247 Nicholson Hall [Slides from Lecture17]
Weighing in on Neutron Stars Varun Bhalerao California Institute of Technology Collaborators: F. Harrison, S. Kulkarni, Marten van Kerkwijk, and others.
Neutron Star masses and radii. NS Masses Stellar masses are directly measured only in binary systems Accurate NS mass determination for PSRs in relativistic.
Discovery of a Highly Eccentric Binary Millisecond Pulsar in a Gamma-Ray- Detected Globular Cluster Megan DeCesar (UWM) In collaboration with Scott Ransom.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
1. black hole - region of space where the pull of gravity is so great that even light cannot escape. Possible end of a very massive star.
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.
A brief review of double-pulsar system, PSR J
Neutron Stars and Black Holes
Pulsars – progress and puzzles 1 Jocelyn Bell Burnell University of Oxford Astrophysics & Mansfield College.
Magnetars origin and progenitors with enhanced rotation S.B. Popov, M.E. Prokhorov (Sternberg Astronomical Institute) (astro-ph/ )
Pulsar Timing with the GBT Scott Ransom National Radio Astronomy Observatory.
Thomas Klähn D. Blaschke R. Łastowiecki F. Sandin Thomas Klähn – Three Days on Quarkyonic Island.
Likely continuous sources for detection by ITF C. Palomba Slides based on a paper appeared in MNRAS, 2005 Isolated neutron stars “Standard” EOS (no quark.
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.
Vicky Kalogera with Bart Willems Mike Henninger Formation of Double Neutron Stars: Kicks and Tilts Department of Physics and Astronomy.
The 511 keV Annihilation Emission From The Galactic Center Department of Physics National Tsing Hua University G.T. Chen 2007/1/2.
The Milky Way. Structure of the Milky Way The Milky Way.
The birth-ultrafast-magnetic- field-decay model applied to isolated millisecond pulsars Ricardo Heras Preparatoria Abierta SEIEM Edo. Mexico.
Radio Pulsars R. N. Manchester Australia Telescope National Facility, CSIRO Sydney, Australia Summary Introduction to pulsar basics Multibeam searches.
25 Facts about Parkes, Pulsars and
Australian Telescope National Facility Marsfield, Sydney.
The mass ratio of the stellar components of a spectroscopic binary can be directly computed from their ratio in radial velocities. To derive the total.
Constraining Neutron Star Radii and Equations of State Josh Grindlay Harvard (collaboration with Slavko Bogdanov McGill Univ.)
Timing Relativistic Binary Pulsars to test Gravitation and measure NS masses Paulo C. C. Freire Arecibo Observatory / Cornell University.
Neutron Star (Mostly Pulsar) Masses Ingrid Stairs UBC Vancouver CAWONAPS TRIUMF Dec. 9, 2010.
PSR J1400 – 1410 Jessica Pal Rowan County Senior High School Introduction Data Analysis Summary Acknowledgements Results A pulsar is a rapidly rotating.
Star Clusters and their stars Open clusters and globular clusters General characteristics of globular clusters Globular cluster stars in the H-R diagram.
GENERAL RELATIVITY AND PRECISE MEASUREMENTS GENERAL RELATIVITY AND PRECISE MEASUREMENTS OF PULSAR MASSES D.G. Yakovlev Ioffe Physical Technical Institute,
Plasma universe Fluctuations in the primordial plasma are observed in the cosmic microwave background ESA Planck satellite to be launched in 2007 Data.
Radio Observations of X-ray Binaries : Solitary and Binary Millisecond Pulsars Jeong-Sook Kim 1 & Soon-Wook Kim 2  Department of Space Science and Astronomy.
Present and future of pulsar research: the Italian contribute Alessandro Corongiu LIGO-G Z Gravitational Waves Advanced Detectors Workshop La.
No Longer! The Double Pulsar Maura McLaughlin West Virginia University 5 April 2012 Collaborators: Kramer (MPiFR), Stairs (UBC), Perera (WVU), Kim (WVU),
Vicky Kaspi, McGill University CIFAR AGM Why Do We Need More Radio Pulsars?  Want to build a `Pulsar Timing Array’ (PTA) to detect gravitational.
18/04/2004New Windows on the Universe Jan Kuijpers Part 1: Gravitation & relativityPart 1: Gravitation & relativity J.A. Peacock, Cosmological Physics,
ON THE LOW LEVEL X-RAY EMISSION OF TRANSITIONAL PULSARS Enrico Bozzo University of Geneva.
THE PECULIAR EVOLUTIONARY HISTORY OF IGR J IN TERZAN 5 A. Patruno Reporter: Long Jiang ( 姜龙 )
The Radio Millisecond Pulsar PSR J : A Link to Low-Mass X-Ray Binaries Slavko Bogdanov.
Niharika Sravan Midwest Relativity Meeting October 27, 2013 IMPORTANCE OF TIDES FOR PERIASTRON PRECESSION IN ECCENTRIC NEUTRON STAR - WHITE DWARF BINARIES.
Historical SN and their properties Total energy released ~10 54 erg in a few hours.
Black Holes Accretion Disks X-Ray/Gamma-Ray Binaries.
Death of Stars II Physics 113 Goderya Chapter(s): 14
Binary Orbits. Orbits Binary Stellar Systems 1/3 to 2/3 of stars in binary systems Rotate around center of mass (barycenter) Period - days to years for.
Extra Solar Planet Detection by the Doppler Detection method The following slides are a summary of the classroom presentation annotating the Doppler Detection.
Binary stellar systems are interesting to study for many reasons. For example, most stars are members of binary systems, and so studies of binary systems.
Parsec-scale Constraints on the ISM From the Millisecond Pulsars in Terzan5 Scott Ransom (NRAO Charlottesville) Fernando Camilo (Columbia) Paulo Freire.
References: 1. Bhattacharya & van den Heuvel, Phys Reports, vol 203, 1, X-ray Binaries, edited by Lewin, van Paradijs, and van den Heuvel, 1995,
White dwarfs cool off and grow dimmer with time. The White Dwarf Limit A white dwarf cannot be more massive than 1.4M Sun, the white dwarf limit (or Chandrasekhar.
Formation of Redback and Black Widow Binary Millisecond Pulsars
Pulsar Timing Concepts to get across –Searching is only the beginning –By timing pulsars we extract most of the science –The principles involve some simple.
To find strange star with FAST R. X. Xu Renxin Xu ( 徐仁新 ) School of Physics, Peking University ( ) Frontiers in Radio Astronomy.
Black Widow Pulsars(BWP): the Price of Promiscuity A. R. King, M. B. Davies and M. E. Beer, 2003,MNRAS,345,678 Fu Lei
Neutron Stars and Black Holes
Experimental tests of the no-hair theorems of black holes
Signatures of formation mechanisms in the multiple-star statistics
Binary pulsars as probes of a Galactic dark matter disk
NANOGrav Long-term timing of two faint millisecond pulsars at Arecibo
Accretion in Binaries II
Binary Orbits.
8th Gravitational Wave Data Analysis Workshop
Star Clusters and their stars
Extrasolar planet detection: a view from the trenches
Neutron Star masses.
Center for Gravitational Wave Physics Penn State University
Final states of a star: 1. White Dwarf
Presentation transcript:

Eccentric Binary Millisecond Pulsars Paulo C. C. Freire arXiv: v1

INTRODUCTION The importance of the discovery of MSPs in eccentric orbits The context of this work Recent discovery of MSPs in eccentric binaries Prospects

FORMATION OF BINARY PULSARS

Spin Periods –companion mass (‘centi-second pulsar’ CSP, MSP) Magnetic fields –smaller surface magnetic diploe & cleaner rotation Masses –MSPs>CSPs?

How to measure the mass of a neutron star Keplerian orbits – Use doppler shift to measure the orbital velocity changes along the line-of-sight –Fit to determination the five Keplerian parameters: the orbital period P b project of the semi-major axis x the orbital eccentricity e the time of passage through periastron T 0 the longitude of periastron ω

Unknown parameters –two component masses m c, m p –the orbital inclination i The well-known mass function

Post-Keplerian parameters –the rate of advance of periastron ( dω/dt ) –the “Einstein delay” γ –the rate of orbital decay P b –“Shapiro” delay r and s

Use two PK parameters to solve for m p, m c and i test the self-consistency of GR Verification that there are no classical contributions to PK parameters e.g. DNS B –large e =0.617 and small P b =7 h 45 m –dω/dt = (7) ◦ yr −1, γ = (1)s –m p = (3) M ⊙, m c = (3) M ⊙ –dP b /dt = −2.4211(14)× 10 −12 ss −1

Neutron Star Masses –All precise NS mass measurements comes from CSPs located in DNS systems, ranges from (7)M ⊙ to (3) M ⊙ –Is such a narrow distribution of masses also observed for MSPs? small orbital eccentricities (2×10 −3 to 10 −7 ) of MSP-WD system makes the measurement of mass like B impossible(use dω/dt, γ ) dP b /dt will greatly amplified by a) a compact orbit, b) a large orbital eccentricity c) a massive companion Shapiro delay is also use to estimate for the pulsar mass ( of the order of a few µs in the T.O.A.s )

Eccentric binary MSPs in GCs –In GCs LMXB is 3 orders of magnitude more often than in the disk –Since 1987, 140 pulsars found in GCs Interactions with passing stars or even exchange encounters produce binary MSP with large e, and allow the measurement of dω/dt

Early results –The first measurement of dω/dt for a MSP was made in 2003 for PSR J0024−7204H dω/dt = (0.066 ± 0.001) ◦ yr −1 M =(1.61±0.04) M ⊙ m c >(f M 2 ) 1/3 for sin i ≤ 1 m p < 1.52 M ⊙ The maximum mass shows NS can be spun up to MS period with relatively small amounts of matter

J1909−3744 –because it has the narrowest pulse profile for any known pulsar (w50 =43µs); as a result, it is one of the most precisely timed MSPs –the orbital inclination is close to 90 ◦ –precise measurement of Shapiro delay provide m p = (1.438 ±0.024) M ⊙

Recent results

PSR J –a 2.15ms pulsar in a 95-day orbit with ∼ 1M ⊙ main- sequence star companion – e = 0.44 –it is possible that PSR J formed from a hierarchical triple system which the mass donor somehow eliminated –combine dω/dt and s measured give m p =(1.74 ± 0.04)M ⊙, m c = (1.028 ± 0.004)M ⊙

This is the first precisely measured NS mass larger than that of PSR B and the first significantly above the Chandrasekhar mass This pulsar proves that accretion can significantly increase the mass of MSPs compared to the NSs in DNS systems, i.e., the mass distribution for MSPs is definitely wider than the NS mass distribution in DNSs

Study of super-dense matter The precise measurement of MSP masses is so important because –Due to accretion they can be more massive than NSs in DNS systems –This can test our models of how matter behaves at the center of NSs –the mass measured for PSR J is higher than the maximum possible mass predicted by some EOS models

PROSPECTS The increased number of mass Probability distribution functions (pdfs) will assist the statistical studies of the MSP mass distribution. γof Ter 5 I is becoming detectable which we expect the pulsar to be massive (<1.96) Meanwhile, HST time has already been allocated for the study of the environs of these candidate super- massive pulsars The detection of their companions will be important to address the issue of whether the observed dω/dt is purely relativistic or not

Measurements of the spectral line widths of the companion might address once and for all the issue of whether the companion is rotating fast or not and whether it can contribute to the observed advance of periastron

Thanks