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PSR J1614−2230

PSR J1614–2230 is a pulsar in a binary system with a white dwarf in the constellation Scorpius. It was discovered in 2006 with the Parkes telescope in a survey of unidentified gamma ray sources in the Energetic Gamma Ray Experiment Telescope catalog.[3] PSR J1614–2230 is a millisecond pulsar, a type of neutron star, that spins on its axis roughly 317 times per second, corresponding to a period of 3.15 milliseconds. Like all pulsars, it emits radiation in a beam, similar to a lighthouse.[4] Emission from PSR J1614–2230 is observed as pulses at the spin period of PSR J1614–2230. The pulsed nature of its emission allows for the arrival of individual pulses to be timed. By measuring the arrival time of pulses, astronomers observed the delay of pulse arrivals from PSR J1614–2230 when it was passing behind its companion from the vantage point of Earth. By measuring this delay, known as the Shapiro delay, astronomers determined the mass of PSR J1614–2230 and its companion. The team performing the observations found that the mass of PSR J1614–2230 is 1.97 ± 0.04 M. This mass made PSR J1614–2230 the most massive known neutron star at the time of discovery, and rules out many neutron star equations of state that include exotic matter such as hyperons and kaon condensates.[1]

PSR J1614–2230
Observation data
Epoch J2000      Equinox J2000
Constellation Scorpius
Right ascension 16h 14m 36.5051s[1]
Declination −22° 30′ 31.081″[1]
Characteristics
Spectral type Pulsar
Astrometry
Distance1,200[1] pc
Details
Mass1.908[2] M
Radius13±2 km,[1] 1.87(29) × 10-5 R
Rotation3.1508076534271 ms[1]
Age5.2 × 109 years
Other designations
PSR J1614–22
Database references
SIMBADdata

In 2013, a slightly higher neutron star mass measurement was announced for PSR J0348+0432, 2.01 ± 0.04 M.[5] This confirmed the existence of such massive neutron stars using a different measuring technique.

After further high-precision timing of the pulsar, the mass measurement for J1614–2230 was updated to 1.908 ± 0.016 M in 2018.[2]

Background

 
Schematic view of a pulsar. The sphere in the middle represents the neutron star, the curves indicate the magnetic field lines and the protruding cones represent the emission beams.

Pulsars were discovered in 1967 by Jocelyn Bell and her adviser Antony Hewish using the Interplanetary Scintillation Array.[6] 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 M.[7][8] 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.[8] 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

The Energetic Gamma-Ray Experiment Telescope (EGRET) identified a half dozen known pulsars at gamma ray wavelengths. Many of the sources it detected had no known counterparts at other wavelengths. In order to see whether any of these sources were pulsars, Fronefield Crawford et al. used the Parkes telescope to conduct a survey of the EGRET sources located in the plane of the Milky Way that lacked a known counterpart. In the search, they discovered PSR J1614–2230, and concluded that it might be a counterpart to a gamma ray source near the same location.[3] The radio observations revealed that PSR J1614–2230 had a companion, likely a white dwarf. The observed orbital parameters of the system indicated a minimum companion mass of 0.4 M, and an orbital period of 8.7 days.[9]

Paul Demorest et al. used the Green Bank Telescope at the National Radio Astronomy Observatory to observe the system through a complete 8.7 day orbit, recording the pulse arrival times from PSR J1614–2230 over this period. After accounting for factors that would alter pulse arrival times from exactly matching its period of 3.1508076534271 milliseconds, including the orbital parameters of the binary system, the spin of the pulsar, and the motion of the system, Demorest et al. determined the delay in the arrival of pulses that resulted from the pulse having to travel past the companion to PSR J1614–2230 on its way to Earth. This delay is a consequence of general relativity known as the Shapiro delay, and the magnitude of the delay is dependent upon the mass of the white dwarf companion. The best fit companion mass was 0.500 ± 0.006 M. Knowing the companion mass and orbital elements then provided enough information to determine the mass of PSR J1614–2230 to be 1.97 ± 0.04 M.[1]

The measurement was later improved based on observations of the pulses over several years.[2]

Significance

The conditions in neutron stars are very different from those encountered on Earth, as a result of the high density and gravity of neutron stars; their masses are of order the mass of a star, but they have sizes around 10 to 13 kilometres (6 to 8 mi) in radius, which is comparable to the size of the center of large cities such as London.[4] Neutron stars also have the property that as they become more massive, their diameter decreases. The mass of PSR J1614–2230 is the second highest of all the known neutron stars. The existence of a neutron star with such a high mass constrains the composition and structure of neutron stars, both of which are poorly understood. The reason for this is that the maximum mass of a neutron star is dependent upon its composition. A neutron star composed of matter such as hyperons or kaon condensates would collapse to form a black hole before it could reach the observed mass of PSR J1614–2230, meaning neutron star models that include such matter are strongly constrained by this result.[1][10]

Notes

  1. ^ a b c d e f g h Demorest et al. (2010)
  2. ^ a b c Arzoumanian et al. (2018)
  3. ^ a b Crawford et al. (2006)
  4. ^ a b Jonathan Amos (October 28, 2010). "Neutron star packs two Suns' mass in London-sized space". BBC. Retrieved 2010-10-28.
  5. ^ Antoniadis et al. (2013)
  6. ^ Hewish et al. (1968)
  7. ^ Pacini (1968)
  8. ^ a b Gold (1968)
  9. ^ Hessels et al. (2005)
  10. ^ Zeeya Merali (October 27, 2010). "Massive neutron star is exactly that". Nature. Retrieved 2010-10-29.

References

  • Arzoumanian, Zaven; Brazier, Adam; Burke-Spolaor, Sarah; et al. (9 April 2018). "The NANOGrav 11-year Data Set: High-precision Timing of 45 Millisecond Pulsars". The Astrophysical Journal Supplement Series. 235 (2): 37. doi:10.3847/1538-4365/aab5b0. ISSN 1538-4365.
  • Crawford, F.; Roberts, M. S. E.; Hessels, J. W. T.; Ransom, S. M.; Livingstone, M.; Tam, C. R.; Kaspi, V. M. (2006). "A Survey of 56 Midlatitude EGRET Error Boxes for Radio Pulsars". The Astrophysical Journal. 652 (2): 1499–1507. arXiv:astro-ph/0608225. Bibcode:2006ApJ...652.1499C. doi:10.1086/508403. S2CID 522064.
  • Demorest, P. B.; Pennucci, T.; Ransom, S. M.; Roberts, M. S. E.; Hessels, J. W. T. (2010). "A two-solar-mass neutron star measured using Shapiro delay". Nature. 467 (7319): 1081–1083. arXiv:1010.5788. Bibcode:2010Natur.467.1081D. doi:10.1038/nature09466. PMID 20981094. S2CID 205222609.
  • Antoniadis, J.; Freire, P. C. C.; Wex, N.; Tauris, T. M.; Lynch, R. S.; Van Kerkwijk, M. H.; Kramer, M.; Bassa, C.; Dhillon, V. S.; Driebe, T.; Hessels, J. W. T.; Kaspi, V. M.; Kondratiev, V. I.; Langer, N.; Marsh, T. R.; McLaughlin, M. A.; Pennucci, T. T.; Ransom, S. M.; Stairs, I. H.; Van Leeuwen, J.; Verbiest, J. P. W.; Whelan, D. G. (2013). "A Massive Pulsar in a Compact Relativistic Binary". Science. 340 (6131): 1233232. arXiv:1304.6875. Bibcode:2013Sci...340..448A. doi:10.1126/science.1233232. PMID 23620056. S2CID 15221098.
  • Gold, T. (1968). "Rotating Neutron Stars as the Origin of the Pulsating Radio Sources". Nature. 218 (5143): 731–732. Bibcode:1968Natur.218..731G. doi:10.1038/218731a0. S2CID 4217682.
  • Hessels, J.; Ransom, S.; Roberts, M.; Kaspi, V.; et al. (January 11–17, 2004). "Three New Binary Pulsars Discovered With Parkes". In F. A. Rasio; I. H. Stairs (eds.). Binary Radio Pulsars. Vol. 328. Aspen, Colorado, USA: Astronomical Society of the Pacific (published 2005). arXiv:astro-ph/0404167. Bibcode:2005ASPC..328..395H.
  • Hewish, A.; Bell, S. J.; Pilkington, J. D. H.; Scott, P. F.; Collins, R. A. (1968). "Observation of a Rapidly Pulsating Radio Source". Nature. 217 (5130): 709. Bibcode:1968Natur.217..709H. doi:10.1038/217709a0. S2CID 4277613.
  • Pacini, F. (1968). "Rotating Neutron Stars, Pulsars and Supernova Remnants". Nature. 219 (5150): 145–146. arXiv:astro-ph/0208563. Bibcode:1968Natur.219..145P. doi:10.1038/219145a0. S2CID 4188947.

j1614, 2230, j1614, 2230, pulsar, binary, system, with, white, dwarf, constellation, scorpius, discovered, 2006, with, parkes, telescope, survey, unidentified, gamma, sources, energetic, gamma, experiment, telescope, catalog, j1614, 2230, millisecond, pulsar, . PSR J1614 2230 is a pulsar in a binary system with a white dwarf in the constellation Scorpius It was discovered in 2006 with the Parkes telescope in a survey of unidentified gamma ray sources in the Energetic Gamma Ray Experiment Telescope catalog 3 PSR J1614 2230 is a millisecond pulsar a type of neutron star that spins on its axis roughly 317 times per second corresponding to a period of 3 15 milliseconds Like all pulsars it emits radiation in a beam similar to a lighthouse 4 Emission from PSR J1614 2230 is observed as pulses at the spin period of PSR J1614 2230 The pulsed nature of its emission allows for the arrival of individual pulses to be timed By measuring the arrival time of pulses astronomers observed the delay of pulse arrivals from PSR J1614 2230 when it was passing behind its companion from the vantage point of Earth By measuring this delay known as the Shapiro delay astronomers determined the mass of PSR J1614 2230 and its companion The team performing the observations found that the mass of PSR J1614 2230 is 1 97 0 04 M This mass made PSR J1614 2230 the most massive known neutron star at the time of discovery and rules out many neutron star equations of state that include exotic matter such as hyperons and kaon condensates 1 PSR J1614 2230 Observation dataEpoch J2000 Equinox J2000Constellation ScorpiusRight ascension 16h 14m 36 5051s 1 Declination 22 30 31 081 1 CharacteristicsSpectral type PulsarAstrometryDistance1 200 1 pcDetailsMass1 908 2 M Radius13 2 km 1 1 87 29 10 5 R Rotation3 1508076534271 ms 1 Age5 2 109 yearsOther designationsPSR J1614 22Database referencesSIMBADdataIn 2013 a slightly higher neutron star mass measurement was announced for PSR J0348 0432 2 01 0 04 M 5 This confirmed the existence of such massive neutron stars using a different measuring technique After further high precision timing of the pulsar the mass measurement for J1614 2230 was updated to 1 908 0 016 M in 2018 2 Contents 1 Background 2 Observations 3 Significance 4 Notes 5 ReferencesBackground EditMain article Pulsar Schematic view of a pulsar The sphere in the middle represents the neutron star the curves indicate the magnetic field lines and the protruding cones represent the emission beams Pulsars were discovered in 1967 by Jocelyn Bell and her adviser Antony Hewish using the Interplanetary Scintillation Array 6 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 M 7 8 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 8 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 EditThe Energetic Gamma Ray Experiment Telescope EGRET identified a half dozen known pulsars at gamma ray wavelengths Many of the sources it detected had no known counterparts at other wavelengths In order to see whether any of these sources were pulsars Fronefield Crawford et al used the Parkes telescope to conduct a survey of the EGRET sources located in the plane of the Milky Way that lacked a known counterpart In the search they discovered PSR J1614 2230 and concluded that it might be a counterpart to a gamma ray source near the same location 3 The radio observations revealed that PSR J1614 2230 had a companion likely a white dwarf The observed orbital parameters of the system indicated a minimum companion mass of 0 4 M and an orbital period of 8 7 days 9 Paul Demorest et al used the Green Bank Telescope at the National Radio Astronomy Observatory to observe the system through a complete 8 7 day orbit recording the pulse arrival times from PSR J1614 2230 over this period After accounting for factors that would alter pulse arrival times from exactly matching its period of 3 1508076534271 milliseconds including the orbital parameters of the binary system the spin of the pulsar and the motion of the system Demorest et al determined the delay in the arrival of pulses that resulted from the pulse having to travel past the companion to PSR J1614 2230 on its way to Earth This delay is a consequence of general relativity known as the Shapiro delay and the magnitude of the delay is dependent upon the mass of the white dwarf companion The best fit companion mass was 0 500 0 006 M Knowing the companion mass and orbital elements then provided enough information to determine the mass of PSR J1614 2230 to be 1 97 0 04 M 1 The measurement was later improved based on observations of the pulses over several years 2 Significance EditThe conditions in neutron stars are very different from those encountered on Earth as a result of the high density and gravity of neutron stars their masses are of order the mass of a star but they have sizes around 10 to 13 kilometres 6 to 8 mi in radius which is comparable to the size of the center of large cities such as London 4 Neutron stars also have the property that as they become more massive their diameter decreases The mass of PSR J1614 2230 is the second highest of all the known neutron stars The existence of a neutron star with such a high mass constrains the composition and structure of neutron stars both of which are poorly understood The reason for this is that the maximum mass of a neutron star is dependent upon its composition A neutron star composed of matter such as hyperons or kaon condensates would collapse to form a black hole before it could reach the observed mass of PSR J1614 2230 meaning neutron star models that include such matter are strongly constrained by this result 1 10 Notes Edit a b c d e f g h Demorest et al 2010 a b c Arzoumanian et al 2018 a b Crawford et al 2006 a b Jonathan Amos October 28 2010 Neutron star packs two Suns mass in London sized space BBC Retrieved 2010 10 28 Antoniadis et al 2013 Hewish et al 1968 Pacini 1968 a b Gold 1968 Hessels et al 2005 Zeeya Merali October 27 2010 Massive neutron star is exactly that Nature Retrieved 2010 10 29 References EditArzoumanian Zaven Brazier Adam Burke Spolaor Sarah et al 9 April 2018 The NANOGrav 11 year Data Set High precision Timing of 45 Millisecond Pulsars The Astrophysical Journal Supplement Series 235 2 37 doi 10 3847 1538 4365 aab5b0 ISSN 1538 4365 Crawford F Roberts M S E Hessels J W T Ransom S M Livingstone M Tam C R Kaspi V M 2006 A Survey of 56 Midlatitude EGRET Error Boxes for Radio Pulsars The Astrophysical Journal 652 2 1499 1507 arXiv astro ph 0608225 Bibcode 2006ApJ 652 1499C doi 10 1086 508403 S2CID 522064 Demorest P B Pennucci T Ransom S M Roberts M S E Hessels J W T 2010 A two solar mass neutron star measured using Shapiro delay Nature 467 7319 1081 1083 arXiv 1010 5788 Bibcode 2010Natur 467 1081D doi 10 1038 nature09466 PMID 20981094 S2CID 205222609 Antoniadis J Freire P C C Wex N Tauris T M Lynch R S Van Kerkwijk M H Kramer M Bassa C Dhillon V S Driebe T Hessels J W T Kaspi V M Kondratiev V I Langer N Marsh T R McLaughlin M A Pennucci T T Ransom S M Stairs I H Van Leeuwen J Verbiest J P W Whelan D G 2013 A Massive Pulsar in a Compact Relativistic Binary Science 340 6131 1233232 arXiv 1304 6875 Bibcode 2013Sci 340 448A doi 10 1126 science 1233232 PMID 23620056 S2CID 15221098 Gold T 1968 Rotating Neutron Stars as the Origin of the Pulsating Radio Sources Nature 218 5143 731 732 Bibcode 1968Natur 218 731G doi 10 1038 218731a0 S2CID 4217682 Hessels J Ransom S Roberts M Kaspi V et al January 11 17 2004 Three New Binary Pulsars Discovered With Parkes In F A Rasio I H Stairs eds Binary Radio Pulsars Vol 328 Aspen Colorado USA Astronomical Society of the Pacific published 2005 arXiv astro ph 0404167 Bibcode 2005ASPC 328 395H Hewish A Bell S J Pilkington J D H Scott P F Collins R A 1968 Observation of a Rapidly Pulsating Radio Source Nature 217 5130 709 Bibcode 1968Natur 217 709H doi 10 1038 217709a0 S2CID 4277613 Pacini F 1968 Rotating Neutron Stars Pulsars and Supernova Remnants Nature 219 5150 145 146 arXiv astro ph 0208563 Bibcode 1968Natur 219 145P doi 10 1038 219145a0 S2CID 4188947 Retrieved from https en wikipedia org w index php title PSR J1614 2230 amp oldid 1136339964, wikipedia, wiki, book, books, library,

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