Transcript Document

COOLING OF NEUTRON STARS
D.G. Yakovlev
Ioffe Physical Technical Institute, St.-Petersburg, Russia
1. Formulation of the Cooling Problem
2. Superlfuidity and Heat Capacity
3. Neutrino Emission
4. Cooling Theory versus Observations
• History
• Cooling stages
• Observations
• Tuning theory to explain observations
• Conclusions
Ladek Zdroj, February 2008,
PRE-PULSAR HISTORY
Stabler (1960) – PhD, First estimates of X-ray surface thermal
emission
Chiu (1964) – Estimates that neutron stars can be discovered
from observations of thermal X-rays
Morton (1964) , Chiu & Salpeter (1964), Bahcall & Wolf (1965) –
First simplified cooling calculations
Tsuruta & Cameron (1966) – Basic formulation of all elements
of the cooling theory
NEW HISTORY
Lattimer, Pethick, Prakash & Haensel (1991)
The possibility of direct Urca process in nucleon matter
Page & Applegate (1992)
Crucial importance of superfluidity for cooling
Schaab, Voskresensky, Sedrakian, Weber & Weigel (1997);
Page (1998)
The importance of Cooper pairing neutrino emission
THREE COOLING STAGES
After 1 minute of proto-neutron star stage of Sanjay Reddy
Stage
Duration
Physics
Relaxation
10—100 yr
Crust
Neutrino
10-100 kyr
Core, surface
Photon
infinite
Surface, core,
reheating
Analytical estimates
Thermal balance of
cooling star with
isothermal interior
dT
C (T )
  L (T )  L (Ts )  LHEAT
dt
L  4 R 2Ts4
L  L (1  rg /R )
Heat blanketing envelope: Ts  Ts (T )
T (t )  T (r , t ) exp( (r ))
Slow cooling via
Modified Urca
process
Fast cooling via
Direct Urca
process
tSLOW
1 year
~
T96
T ~ 1.5 108 K in t  105 yrs
tFAST
1 min
~
T94
T ~ 107 K in t  200 yrs
Spin
axis
OBSERVATIONS: MAIN PRINCIPLES
See lectures by Roberto Turolla
Isolated (cooling) neutron stars – no
additional heat sources:
Age t
Surface temperature Ts
MEASURING DISTANCES:
parallax; electron column density from radio data;
association with clusters and supernova remnants;
fitting observed spectra
MEASURING AGES:
pulsar spin-down age (from P and dP/dt);
association with stellar clusters and supernova remnants
MEASURING SURFACE TEMPERATURES:
fitting observed spectra
OBSERVATIONS
Chandra
image of
the Vela
pulsar
wind nebula
NASA/PSU
Pavlov et al
Chandra
XMM-Newton
MULTIWAVELENGTH SPECTRUM OF THE VELA PULSAR
t  (1.1  2.5) 104 yr
TS  0.65  0.71 MK
THERMAL RADIATION FROM ISOLATED NEUTRON STARS
OBSERVATIONS AND BASIC COOLING CURVE
Nonsuperfluid star
Nucleon core
Modified Urca
neutrino emission:
slow cooling
1=Crab
2=PSR J0205+6449
3=PSR J1119-6127
4=RX J0822-43
5=1E 1207-52
6=PSR J1357-6429
7=RX J0007.0+7303
8=Vela
9=PSR B1706-44
10=PSR J0538+2817
11=PSR B2234+61
12=PSR 0656+14
13=Geminga
14=RX J1856.4-3754
15=PSR 1055-52
16=PSR J2043+2740
17=PSR J0720.4-3125
MODIFIED AND DIRECT URCA PROCESSES
1=Crab
2=PSR J0205+6449
3=PSR J1119-6127
4=RX J0822-43
5=1E 1207-52
6=PSR J1357-6429
7=RX J0007.0+7303
8=Vela
9=PSR B1706-44
10=PSR J0538+2817
11=PSR B2234+61
12=PSR 0656+14
13=Geminga
14=RX J1856.4-3754
15=PSR 1055-52
16=PSR J2043+2740
17=PSR J0720.4-3125
M MAX  1.977 M
c  2.578 1015 g/cc
M D  1.358 M
c  8.17 1014 g/cc
From 1.1 M to 1.98 M with step M  0.01 M
MAIN PHYSICAL MODELS
Problems:
To discriminate between neutrino mechanisms
To broaden transition from slow to fast neutrino
emission
AN EXAMPLE OF SUPERFLUID BROADENING OF DIRECT URCA
THRESHOLD
Two models for proton superfluidity
Neutrino emissivity profiles
Superfluidity:
• Suppresses modified Urca process in the outer core
• Suppresses direct Urca just after its threshold (“broadens
the threshold”)
BASIC PHENOMENOLOGICAL CONCEPT
Neutrino emissivity function
Neutrino luminosity function
BASIC PARAMETERS:
QSLOW , QFAST , 1 , 2  LSLOW , LFAST , M 1 , M 2
MODIFIED AND DIRECT URCA PROCESSES:
SMOOTH TRANSITION
M VELA  1.61 M ?
MODIFIED AND DIRECT URCA PROCESSES:
SMOOTH TRANSITION -- II
Mass ordering is the same!
M VELA  1.47 M ?
TESTING THE LEVELS OF SLOW AND FAST NEUTRINO EMISSION
Slow neutrino emission:  Q(Mod Urca) / 30
Fast neutrino emission:  Q(Mod Urca)  30
Two other parameters are totally not
constrained
Summary of cooling regulators
Regulators of neutrino emission in neutron star cores
EOS, composition of matter
Superfluidity
Heat content and conduction in cores
Heat capacity
Thermal conductivity
Thermal conduction in heat blanketing envelopes
Thermal conductivity
Chemical composition
Magnetic field
Internal heat sources (for old stars and magnetars)
Viscous dissipation of rotational energy
Ohmic decay of magnetic fields, ect.
CONNECTION: Soft X-ray transients
Deep crustal heating: Brown, Bildsten, Rutledge (1998)
Energy release: Haensel & Zdunik (1990,2003), Gupta et al. (2007)
Levenfish, Haensel (2007)
SAX J1808.4-3658, talk by Craig Heinke
More in the next talk by Peter Jonker
CONNECTION: Magnetars
Kaminker et al. (2006)
SUMMARY OF CONNECTIONS
Sources: X-ray transients; magnetars; superbursts
Processes: quasistationary and transient
CONCLUSIONS
Today
Cooling neutron stars
Soft X-ray transients
• Constraints on slow and fast neutrino emission levels
• Mass ordering
Future
• New observations and good practical theories of dense matter
• Individual sources and statistical analysis
CONCLUSIONS
Ordinary cooling isolates neutron stars of age 1 kyr—1 Myr
• There is one basic phenomenological cooling concept
(but many physical realizations)
• Main cooling regulator: neutrino luminosity function
• Warmest observed stars are low-massive; their neutrino luminosity
should be < 1/30 of modified Urca
• Coldest observed stars are more massive; their neutrino luminosity
should be > 30 of modified Urca (any enhanced neutrino emission would do)
• Neutron star masses at which neutrino cooling is enhanced are not constrained
• The real physical model of neutron star interior is not selected
Connections
• Directly related to neutron stars in soft X-ray transients (assuming deep crustal
heating). From transient data the neutrino luminosity of massive stars
is enhanced by direct Urca or pion condensation
• Related to magnetars and superbusrts
Future
• New observations and accurate theories of dense matter
• Individual sources and statistical analysis
REFERENCES
C.J. Pethick. Cooling of neutron stars. Rev. Mod. Phys. 64, 1133, 1992.
D.G. Yakovlev, C.J. Pethick. Neutron Star Cooling. Annu. Rev. Astron.
Astrophys. 42, 169, 2004.
D. Page, U. Geppert, F. Weber. The cooling of compact stars. Nucl.
Phys. A 777, 497, 2006.