PSR J0348+0432

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PSR J0348+0432
Artist’s impression of the pulsar PSR J0348+0432 and its white dwarf companion.jpg
Artist’s impression of the pulsar PSR J0348+0432 and its white dwarf companion.
Observation data
Epoch J2000      Equinox J2000
Constellation Taurus
Right ascension 03h 48m 43.639s[1]
Declination +04° 32′ 11.458″[1]
Characteristics
Spectral type Pulsar
Astrometry
Radial velocity (Rv) -1 ± 20[1] km/s
Proper motion (μ) RA: +4.04[1] mas/yr
Dec.: +3.5[1] mas/yr
Parallax (π) 0.47 mas
Distance 2,100[1] pc
Orbit
Primary PSR J0348+0432
Companion White dwarf
Period (P) 0.102424062722(7) day[1]
Semi-major axis (a) 0.832  × 109 m
Inclination (i) 40.2(6)°
Details
Pulsar
Mass 2.01[1] M
Radius 13±2 km,[1] 1.87(29) × 10-5 R
Rotation 39.1226569017806 ms[1]
Age 2.6 × 109 years
White dwarf
Mass 0.172[1] M
Radius 0.065 (5) R
Other designations
PSR J0348+0432

PSR J0348+0432 is a neutron star in a binary system with a white dwarf. It was discovered in 2007 with the Green Bank Telescope in a drift-scan survey.[2]

In 2013, a mass measurement for this neutron star was announced: 2.01 \pm 0.04 M_\odot .[1] This measurement was done with a combination of radio timing and precise spectroscopy of the white dwarf companion. This is slightly higher, but statistically indistinguishable, from the mass of PSR J1614–2230, which was measured using the Shapiro delay.[3] This measurement confirmed the existence of such massive neutron stars using a different measuring technique.

The notable feature of this binary pulsar is its combination of high neutron star mass and short orbital period: 2 hours and 27 minutes. This allowed a measurement of the orbital decay due to the emission of gravitational waves, as observed for PSR B1913+16 and PSR J0737-3039.

Background

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Pulsars were discovered in 1967 by Jocelyn Bell and her adviser Antony Hewish using the Interplanetary Scintillation Array.[4] Franco Pacini and Thomas Gold quickly put forth the idea that pulsars are highly magnetized rotating neutron stars, which form as a result of a supernova at the end of the life of stars more massive than about 10 times the mass of the Sun (M).[5][6] The radiation emitted by pulsars is caused by interaction of the plasma surrounding the neutron star with its rapidly rotating magnetic field. This interaction leads to emission "in the pattern of a rotating beacon," as emission escapes along the magnetic poles of the neutron star.[6] The "rotating beacon" property of pulsars arises from the misalignment of their magnetic poles with their rotational poles. Historically, pulsars have been discovered at radio wavelengths where emission is strong, but space telescopes that operate in the gamma ray wavelengths have also discovered pulsars.

Observations

In 2007 the Green Bank Telescope underwent track repair, and was unable to track for several months. An international team of astronomers was nevertheless able to record the data from the antenna, letting the Earth do the job of moving the beam of the telescope across the sky, a process known as a drift scan survey. They found a total of 35 new pulsars, including 7 new millisecond pulsars and PSR J0348+0432.[2]

In 2011 John Antoniadis studied the white dwarf companion with the European Southern Observatory's Very Large Telescope, in Chile, and determined its mass and the mass of the pulsar. Radio timing of the pulsar with the 305-m radio telescope at the Arecibo Observatory and the Effelsberg 100-m Radio Telescope soon detected the orbital decay of the system due to the emission of gravitational waves. This matched the rate predicted by general relativity.[1][7][8]

Significance

The combination of a large neutron star mass, low white dwarf mass (mass ratio ~ 1:11.7) and short orbital period (2 hours and 27 minutes) allows astronomers to test general relativity in a regime of extreme gravitational fields, where it has never been tested before. The result also has implications for the direct detection of gravitational waves and for understanding of stellar evolution.[7] The measured mass of 2.01 \pm 0.04 M_\odot puts an empirical lower bound on the value of the Tolman–Oppenheimer–Volkoff limit.

Notes

  1. 1.00 1.01 1.02 1.03 1.04 1.05 1.06 1.07 1.08 1.09 1.10 1.11 1.12 Antoniadis et al. (2013)
  2. 2.0 2.1 Lynch et al. (2013)
  3. Demorest et al. (2010)
  4. Hewish et al. (1968)
  5. Pacini (1968)
  6. 6.0 6.1 Gold (1968)
  7. 7.0 7.1 Lua error in package.lua at line 80: module 'strict' not found.
  8. Lua error in package.lua at line 80: module 'strict' not found.

References

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