Mass & Radius of Compact Objects Fastest pulsar and its stellar EOS CHENGMIN ZHANG National Astronomical Observatories Chinese Academy of Sciences, Beijing.
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Transcript Mass & Radius of Compact Objects Fastest pulsar and its stellar EOS CHENGMIN ZHANG National Astronomical Observatories Chinese Academy of Sciences, Beijing.
Mass & Radius of Compact Objects
Fastest pulsar and its stellar EOS
CHENGMIN ZHANG
National Astronomical Observatories
Chinese Academy of Sciences, Beijing
Significance of Measuring Star mass
and radius – Neutron or Quark
we can measure physical
parameters of star, mass and
radius, probe the nuclear
physics and understand EOS
we can study the strong
gravitational field, where
Einstein GR might be tested
Neutron Stars ?
40+ NSs, M=1.4 M⊙ , R= 10 -30 km ?
Radio pulsars, X-ray NS, binary systems
(MT77)
(Stairs 2004)
(Lattimer & Prakash 2004,2006)
NS mass determined in Binary
system
MSP, PSR J0751+1807, M = 2.1(2) M⊙ ?; Nice et al. 2004
2A1822-371, M>0.97+-0.24 M⊙; Jonker et al 2003 ; (1.74 M⊙ ,2008)
DNS: M=1.25M⊙, M=1.34 M⊙ , double pulsars (2004)
PSR J0737-3039A/B Post-Keplerian Effects
R: Mass ratio
.
w: periastron advance
g: gravitational redshift
r & s: Shapiro delay
.
Pb: orbit decay
• Six measured
parameters – only two
independent
• Fully consistent with
general relativity (0.1%)
A: 1.34 M⊙ ; B: 1.25 M⊙
(Kramer et al. 2005)
No direct measure of radius !
Measured M-R relations
Apparent Radius: R∞=R/(1-Rs/R)1/2
Gravitational redshift: z=(1-Rs/R)-1/2 -1
Mass density: M/R3
g=~M/R2
1E1207.4-5209, Aql X-1 and EXO 0748-676
Rs=2GM: Schwarzschild radius
Photon Spectra: Key to Measuring Radius
For perfect Black Body:
Observed Total Flux: F =4 R∞2 SB T∞4/d2
Spectra are seldom
black body:
Neutron Stars have
atmospheres !
Composition and
Magnetic field shape
the spectra.
Other issues:
Is the surface
temperature and
radiation isotropic ?
RX J1856.5-3754 (Fred Walter’s Star !)
R
R
1- 2GM/Rc2
T 1- 2GM/Rc2 T
( 1- 2GM/Rc 2 (1 z) -1 )
The Mass-Radius
Exotic Stars
Gravitational Red-shift:
observation of spectral
lines (Cottam, et al 2002).
QPOs indicate ISCO
Typical twin kHz QPOs (24/35)
Z:
Sco x-1,
van der Klis et al 2006
Separation ~300 Hz
~Spin ?
Typically: Twin KHz QPO
Upper ν2 ~ 1000 (Hz)
Lower ν1 ~ 700 (Hz)
Twin 21/27 sources; ~290
Constrain star M_R by kHz QPOs
Inner boundary to emit kHz QPO: ISCO, R > MAX M, R
M<2.2 M⊙ (1kHz/freq)
R<19.5 km (1kHz/freq)
M/R3 relation known by model for twin kHz QPOs
SAXJ 1808.4: M/R3 by Burderi & King 1998
kHz QPOs from LMXBs: R-ISCO
Sco X-1
Excluded
kHz QPO maximum frequency constrains
NS equations of state
Striking case of RX J1856.5-3754
Truempet et al. 2004; Burwitz et al. 2003
This is an isolated neutron star (INS), valuable because:
We can see the surface
There are minimal magnetospheric complications
If we can see the surface, we can determine the angular diameter
The parallax gives the radius R
spectral lines give the surface composition, T, and g
R and g give M
M/R constrains the EOS of matter at nuclear densities
Gravitational light bending effect: R/M <~10 km/M⊙ ; Ransom et al 2004
Apparent radius R∞=16.5 km (d/117pc), Truempet 2005
True radius 14 km (1.4 M⊙), stiff EOS, rule out quark star
Relativistic precession model by Stella & Vietri 1999
M inferred from twin kHz QPOs
Max frequency – ISCO
ISCO Saturation
Einstein’s General Relativity: Perihelion precession
Precession Model for KHz QPO, Stella and Vietri, 1999
ν2 = νkepler
ν1 = νprecession
∆ν = ν2
= ν2 [1 – (1 – 3Rs/r)1/2]
- ν1 is not constant
M/R3 inferred from twin kHz QPOs
Max frequency – Star Surface R
Kepler frequency νk = (GM/4π2r3)0.5
νk = 1850 (Hz) A X3/2
ν1 = ν 2X (1- (1-X)1/2)1/2
A2=m/R63; X=R/r, m=M/M⊙ , R6 = R/106 cm
Zhang 2004, AA; Li & Zhang 2005
Maximum kHz QPO occurs at R or ISCO=3Rs
A> νk /1850 (Hz) and m < 2200 (Hz)/ νk
Miller et al 1998
Constraining M – R by R∞ and z
1E 1207.4-5209:
R∞=4.6 km, Bignami et al 2004
z=0.12-0.23; Sanwal et al 2002 ?
R 6 =R∞6 /(1+z)
M=f(z)R∞6 /(1+z)
F(z)=(20/3)z(1+z/2)/(1+z)2
Constraining M – R by R∞ and A~M/R3
Aql X-1 :
9 km<R∞<18 km, Rutledge et al 2001
one kHz QPO: 1040 Hz; van der Klis 2006
R6 =R∞6 /(1+0.15(A/0.7)2 R2∞6 )0.5
m=AR36
Constraining M – R by A=M/R^3 and z
EXo 0728-676:
z=0.35; Cottam et al 2002
One kHz QPO 695 Hz; Homan & van der Klis 2000
R6 =1.43f0.5(z)(0.7/A)
m=1.43f1.5(z)(0.7/A)
f(z)=(20/3)z(1+z/2)/(1+z)2
1E1207.4-5209,
Apparent radius, gravitational redshift
QUARK STAR ?
Aql X-1 ,
Apparent radius=14 km, single kHz QPO
EXO 0748-676 ,
gravitational redshift, kHz QPO
Measuring NS Mass & Radius
Mass-Radius relations
by kHz QPO, gravitational redshift and apparent radius
Apparent Radius: R∞=R/(1-Rs/R)1/2
Haensel 2001
Gravitational redshift: z=(1-Rs/R)-1/2 -1
Cottam et al 2003, z=0.35
Mass density: M/R3 (by kHz QPOs)
Zhang 2004
1E1207.4-5209, Aql X-1 and EXO 0748-676
Rs=2GM: Schwarzschild radius
Measuring STAR Mass-Radius
by kHz QPO, gravitational redshift and apparent radius
Zhang, Yin, Li, Xu, Zhang B, 2007
AqlX-1, EXO 0748-676 Samples
CN1/CN2: normal neutron matter, CS1/CS2: quark star
CPC: Bose-Einstein condensate of pions
How about the Sub-millisecond Pulsar
XTE J1739285, spin=1122 Hz
Spin=1122 Hz
Radio PSR, 716 Hz
Quark Star, FAST target
Cheng et al 1998,
Li 1999;
Xu, Qiao, Wang 2002
Horvath 2002
Harko, 2005
Zhang, ..Li, 2007
More……
ISCO condition, m ≤ 2200 (Hz)/spin
Keplerian at R, crust split
Max kHz QPO 1330 Hz
Ratio
difference
Zhang et al. 2006
Cir X-1
Spin Frequency - LMXBs
Spin frequency:
Max: 1122 Hz, Kaaret et al 2007
Min: 45 Hz Villarreal & Strohmayer 2004
23 Spin sources, Av ~ 400 Hz
Radio MSP:Max Spin=716 Hz
kHz QPO & spin relation
List of the Low-Mass X-Ray Binaries Simultaneously
Detected Twin Kilohertz QPO and Spin Frequencies
QPO (Hz) spin Dnu/spin
4U 160852 . . . . . . . . 802–1099 619
1.3
4U 163653 . . . . . . . . 971–1192 581
1.7
4U 170243 . . . . . . . . . 1055
330
3.2
4U 172834 . . . . . . . . . 582–1183 363
1.6
KS 1731260 . . . . . . . . 1169
524
2.2
4U 191505 . . . . . . . . . 514–1055 270
1.9
XTE J1807294 . . . . . . 353–587
191
1.8
SAX J1808.43658 . . . .694
401
1.7
QPO data, Belloni et al. (2005), van der Klis (2006)
Fastest Pulsar XTE J1739-285
spin = 1122 Hz M – R Kaaret et al. 2007
Quark Star =
sub-MSP ?
Quark Star ?
Summary
Conclusions: M-R relations
1.
Mass, measured
2.
Radius, not measured directly
3.
Spectra, MR relation
4.
Redshift, M/R
5.
kHz QPO, M/R^3, constraints
6.
Others… Ozel 2006
THANKS
Not clear: fuzzy in M-R
EOS: Quark or Neutron ?
Saturation of kHz QPO frequency ?
ISCO – Star Mass
4U1820-30, NASA
Swank 2004; Miller 2004
BH/ISCO: 3 Schwarzschild radius
Innermost stable circular orbit
NS/Surface: star radius, hard surface