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The Pulsar Mass Distribution
John Antoniadis
Marcel Grossmann Meeting, Rome July 13th
NS mass measurements - Overview
• Information on masses for about 70 binary systems

• Excluding marginal detections, strongly model-dependent measurements, probabilistic arguments,

then we have 35 precision measurements, all of them for DNS and millisecond binary pulsars

• 10 additional systems with constraints on the total mass

• Only few extrema, recent measurements
Triple
MSCompanion
WDCompanion
NSCompanion
Eclipsing
XBs
Pulsar Timing Measurements
TOA residual
model
fold fold
Session i Session j
KP: Orbital Period
Eccentricity
Inclination
Epoch of periastron
Longitude of periastron
Longitude of ascension
Projected semi-major axis
PK: Precession of periastron
‘‘Einstein” delay
Shapiro-delay “range”
Shapiro-delay “shape”
Spin precession
Orbital decay
D. Champion
Pulsar Timing Measurements
PK = f(K; mp, mc)
Parametrized post-Keplerian formalism

For a wide class of gravity theories:
(Damour 1988, Damour & Taylor 1992 )
˙!
E
˙Pb
˙! = 3
✓
Pb
2⇡
◆ 5/3
(T M)2/3
(1 e2
) 1
E = e
✓
Pb
2⇡
◆1/3
T
2/3
M 4/3
mc(mp + 2mc)
˙Pb =
192⇡
5
✓
1 +
73
24
e2
+
37
96
e4
◆
(1 e2
) 7/2
T
5/3
mpmcM 1/3
r = T mc s = sin i
In General Relativity:
Caveats
• Highest precision achieved for millisecond pulsars, but those are found in binaries
with extremely small eccentricity

• Impossible to measure precession of periastron, thus mass measurements possible
only through Shapiro delay in high inclination systems 

Optical Spectroscopy to the Rescue!!!
mc
Pb
.
Pb
.
mc
qq
JA et al. 2012
Extrema
PSR J1614-2230
Demorest et al. 2010
• Binary MSP with 8.7 days orbital period

• Edge on inclination

• Pulsar mass 1.97(4) solar masses
Revised value based on the 9-year NanoGrav dataset:

(Arzurmanian et al. 2015; Arxiv:1505.07540)
1.928(17) Solar Masses
Extrema
PSR J0348+0432
• Relativistic binary MSP system with 2.5 hours orbital period

• Low Mass White-Dwarf Companion

• Pulsar mass 2.01(4) solar masses based on optical spectroscopy
MWD MWD
P
.
b
P
.
b qq
JA et al. 2013
Extrema
PSR J0348+0432
JA et al. 2013
P
.
bP
.
b
MWD MWD
q q
PSR J0348+0432
April 2014
• Relativistic binary MSP system with 2.5 hours orbital period

• Low Mass White-Dwarf Companion

• Pulsar mass 2.01(4) solar masses based on optical spectroscopy
Potential Extrema
• Example I: PSR J1748-2021B - GC MSP in eccentric orbit around low-mass
companion. Total mass of the system 2.92(20) Solar Masses

• Example II: PSR J1012+0537 - Estimate based on revised WD models: 1.83(11) Msol

• Example III: B1957+20 - MPSR = 2.40(12) Msol
Constraints on the EoS
Courtesy: N. Wex
Possible Complementary Constraints
Eccentric Millisecond Pulsars: A new class of binaries
Pulsar P (ms) Porb [days] Mc [Msol] eccentricity Companion Ref.
J1946+3417 3.1 27 0.24 0.13 ? Barr et al. 2013
J2234+0611 3.6 32 0.23 0.13 WD Deneva et al. 2013
J1950+2414 4.3 32 0.24 0.08 ? Knispel et al.
J1618-3921 12 23 0.20 0.027 ? Bailes et al. 2010
Scenario A (exciting!)

Rotationally-delayed Accretion Induced Collapse of a Massive WD (Freire & Tauris 2014)
Eccentric MSPS: Possible Formation Scenarios
If correct, then all MSPs should have masses very close to the Chandrasekhar mass 

…but mass measurements give a direct constraint on the gravitational binding energy
Scenario Β (exciting!)

Phase transition from neutron star to strange quark star (Long et al. 2015)
Eccentric MSPS: Possible Formation Scenarios
Core Density in LMXBs reaches
threshold for quark
deconfinement ->
Transformation to Strange Quark
Star

Again similar masses(?) 

Constraints on binding energy
Scenario C (boring…)

Interaction of the proto-WD with a circumbinary disk (JA, 2014, ApJL)
Eccentric MSPS: Possible Formation Scenarios
Mass distribution should be identical to those of regular MSPs
Eccentric MSPS: Possible Formation Scenarios
• White Dwarf has been detected in optical for PSR J2234+0611

• Measurement of the advance of periastron (+ Shapiro delay or optical) will
yield very precise masses for all of these systems

• At least one of them is massive ( > 1.85 Solar Masses), making A unlikely :-(
The MSP mass distribution
• ~15% of MSPs are massive 

• Past studies infer a normal distribution for MSPs with M~1.45 and ΔΜ~0.2 Solar Masses

(or less than 2% of MSPs above 1.9 Solar Masses)

• Distribution highly skewed or bimodal
Massive Pulsars May Not Be Outliers After All!!!
Ozel et al. 2012
Pulsar Mass [Solar Masses]
The MSP mass distribution
Evidence for Bimodality
• Binormal distribution is highly favoured
compared to alternatives 

(e.g. comparing in terms of a penalized
likelihood, > 95% more likely)

• Peaks at m1,2 =1.4, 1.8 solar masses with
Δm1 = 0.08, Δm2 = 0.2

• Expected from stellar evolution if there is
a difference between stars burning
carbon radiatively/convectively 

(Timmes et al. 1996)
350 MSPs
3σ
2σ
1σ
500 MSPs
3σ
2σ
1σ
Implications for EoS constraints
The MSP mass distribution
At least 350 MSP masses in the future 

with SKA phase-II, GAIA, LSST…
Summary
So far 20 precision mass measurements for MSPs of which 4 have a mass > 1.8 Msol
There seem to be clear ways to distinguish between AIC, strange stars and “normal”
NSs in (some) binary systems
Massive Neutron Stars are not as rare as previously thought [15-20% are massive]
Millisecond Pulsar Mass Distribution is most likely bimodal
Strong constraints on the EoS, Mmax > 1.94 Msol (99.9% CL), but we will do better in
the future
Double NS mass distribution (not discussed) also extremely interesting (check talk
by Joey Martinez at BN3)

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The Pulsar Mass Distribution

  • 1. The Pulsar Mass Distribution John Antoniadis Marcel Grossmann Meeting, Rome July 13th
  • 2. NS mass measurements - Overview • Information on masses for about 70 binary systems • Excluding marginal detections, strongly model-dependent measurements, probabilistic arguments,
 then we have 35 precision measurements, all of them for DNS and millisecond binary pulsars • 10 additional systems with constraints on the total mass • Only few extrema, recent measurements Triple MSCompanion WDCompanion NSCompanion Eclipsing XBs
  • 3. Pulsar Timing Measurements TOA residual model fold fold Session i Session j KP: Orbital Period Eccentricity Inclination Epoch of periastron Longitude of periastron Longitude of ascension Projected semi-major axis PK: Precession of periastron ‘‘Einstein” delay Shapiro-delay “range” Shapiro-delay “shape” Spin precession Orbital decay D. Champion
  • 4. Pulsar Timing Measurements PK = f(K; mp, mc) Parametrized post-Keplerian formalism For a wide class of gravity theories: (Damour 1988, Damour & Taylor 1992 ) ˙! E ˙Pb ˙! = 3 ✓ Pb 2⇡ ◆ 5/3 (T M)2/3 (1 e2 ) 1 E = e ✓ Pb 2⇡ ◆1/3 T 2/3 M 4/3 mc(mp + 2mc) ˙Pb = 192⇡ 5 ✓ 1 + 73 24 e2 + 37 96 e4 ◆ (1 e2 ) 7/2 T 5/3 mpmcM 1/3 r = T mc s = sin i In General Relativity:
  • 5. Caveats • Highest precision achieved for millisecond pulsars, but those are found in binaries with extremely small eccentricity • Impossible to measure precession of periastron, thus mass measurements possible only through Shapiro delay in high inclination systems Optical Spectroscopy to the Rescue!!! mc Pb . Pb . mc qq JA et al. 2012
  • 6. Extrema PSR J1614-2230 Demorest et al. 2010 • Binary MSP with 8.7 days orbital period • Edge on inclination • Pulsar mass 1.97(4) solar masses Revised value based on the 9-year NanoGrav dataset:
 (Arzurmanian et al. 2015; Arxiv:1505.07540) 1.928(17) Solar Masses
  • 7. Extrema PSR J0348+0432 • Relativistic binary MSP system with 2.5 hours orbital period • Low Mass White-Dwarf Companion • Pulsar mass 2.01(4) solar masses based on optical spectroscopy MWD MWD P . b P . b qq JA et al. 2013
  • 8. Extrema PSR J0348+0432 JA et al. 2013 P . bP . b MWD MWD q q PSR J0348+0432 April 2014 • Relativistic binary MSP system with 2.5 hours orbital period • Low Mass White-Dwarf Companion • Pulsar mass 2.01(4) solar masses based on optical spectroscopy
  • 9. Potential Extrema • Example I: PSR J1748-2021B - GC MSP in eccentric orbit around low-mass companion. Total mass of the system 2.92(20) Solar Masses • Example II: PSR J1012+0537 - Estimate based on revised WD models: 1.83(11) Msol • Example III: B1957+20 - MPSR = 2.40(12) Msol
  • 10. Constraints on the EoS Courtesy: N. Wex
  • 11. Possible Complementary Constraints Eccentric Millisecond Pulsars: A new class of binaries Pulsar P (ms) Porb [days] Mc [Msol] eccentricity Companion Ref. J1946+3417 3.1 27 0.24 0.13 ? Barr et al. 2013 J2234+0611 3.6 32 0.23 0.13 WD Deneva et al. 2013 J1950+2414 4.3 32 0.24 0.08 ? Knispel et al. J1618-3921 12 23 0.20 0.027 ? Bailes et al. 2010
  • 12. Scenario A (exciting!)
 Rotationally-delayed Accretion Induced Collapse of a Massive WD (Freire & Tauris 2014) Eccentric MSPS: Possible Formation Scenarios If correct, then all MSPs should have masses very close to the Chandrasekhar mass …but mass measurements give a direct constraint on the gravitational binding energy
  • 13. Scenario Β (exciting!)
 Phase transition from neutron star to strange quark star (Long et al. 2015) Eccentric MSPS: Possible Formation Scenarios Core Density in LMXBs reaches threshold for quark deconfinement -> Transformation to Strange Quark Star Again similar masses(?) 
 Constraints on binding energy
  • 14. Scenario C (boring…)
 Interaction of the proto-WD with a circumbinary disk (JA, 2014, ApJL) Eccentric MSPS: Possible Formation Scenarios Mass distribution should be identical to those of regular MSPs
  • 15. Eccentric MSPS: Possible Formation Scenarios • White Dwarf has been detected in optical for PSR J2234+0611 • Measurement of the advance of periastron (+ Shapiro delay or optical) will yield very precise masses for all of these systems • At least one of them is massive ( > 1.85 Solar Masses), making A unlikely :-(
  • 16. The MSP mass distribution • ~15% of MSPs are massive • Past studies infer a normal distribution for MSPs with M~1.45 and ΔΜ~0.2 Solar Masses
 (or less than 2% of MSPs above 1.9 Solar Masses) • Distribution highly skewed or bimodal Massive Pulsars May Not Be Outliers After All!!! Ozel et al. 2012 Pulsar Mass [Solar Masses]
  • 17. The MSP mass distribution Evidence for Bimodality • Binormal distribution is highly favoured compared to alternatives 
 (e.g. comparing in terms of a penalized likelihood, > 95% more likely)
 • Peaks at m1,2 =1.4, 1.8 solar masses with Δm1 = 0.08, Δm2 = 0.2
 • Expected from stellar evolution if there is a difference between stars burning carbon radiatively/convectively 
 (Timmes et al. 1996)
  • 18. 350 MSPs 3σ 2σ 1σ 500 MSPs 3σ 2σ 1σ Implications for EoS constraints The MSP mass distribution At least 350 MSP masses in the future 
 with SKA phase-II, GAIA, LSST…
  • 19. Summary So far 20 precision mass measurements for MSPs of which 4 have a mass > 1.8 Msol There seem to be clear ways to distinguish between AIC, strange stars and “normal” NSs in (some) binary systems Massive Neutron Stars are not as rare as previously thought [15-20% are massive] Millisecond Pulsar Mass Distribution is most likely bimodal Strong constraints on the EoS, Mmax > 1.94 Msol (99.9% CL), but we will do better in the future Double NS mass distribution (not discussed) also extremely interesting (check talk by Joey Martinez at BN3)