An ultraluminous X-ray source powered by an accreting neutron star

The majority of ultraluminous X-ray sources are point sources that are spatially offset from the nuclei of nearby galaxies and whose X-ray luminosities exceed the theoretical maximum for spherical infall (the Eddington limit) onto stellar-mass black holes. Their X-ray luminosities in the 0.5–10 kilo...

Full description

Bibliographic Details
Main Authors: Bachetti, M., Harrison, Fiona A., Walton, D. J., Grefenstette, Brian W., Fürst, F., Barret, D., Beloborodov, A., Boggs, S. E., Christensen, F. E., Craig, W. W., Fabian, A. C., Hailey, Charles J., Hornschemeier, A., Kaspi, Victoria, Kulkarni, S. R., Maccarone, T. J., Miller, J. M., Rana, V., Stern, D., Tendulkar, S. P., Tomsick, J., Webb, N. A., Zhang, W. W., Chakrabarty, Deepto
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:en_US
Published: Nature Publishing Group 2015
Online Access:http://hdl.handle.net/1721.1/98042
https://orcid.org/0000-0001-8804-8946
_version_ 1826213203362709504
author Bachetti, M.
Harrison, Fiona A.
Walton, D. J.
Grefenstette, Brian W.
Fürst, F.
Barret, D.
Beloborodov, A.
Boggs, S. E.
Christensen, F. E.
Craig, W. W.
Fabian, A. C.
Hailey, Charles J.
Hornschemeier, A.
Kaspi, Victoria
Kulkarni, S. R.
Maccarone, T. J.
Miller, J. M.
Rana, V.
Stern, D.
Tendulkar, S. P.
Tomsick, J.
Webb, N. A.
Zhang, W. W.
Chakrabarty, Deepto
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Bachetti, M.
Harrison, Fiona A.
Walton, D. J.
Grefenstette, Brian W.
Fürst, F.
Barret, D.
Beloborodov, A.
Boggs, S. E.
Christensen, F. E.
Craig, W. W.
Fabian, A. C.
Hailey, Charles J.
Hornschemeier, A.
Kaspi, Victoria
Kulkarni, S. R.
Maccarone, T. J.
Miller, J. M.
Rana, V.
Stern, D.
Tendulkar, S. P.
Tomsick, J.
Webb, N. A.
Zhang, W. W.
Chakrabarty, Deepto
author_sort Bachetti, M.
collection MIT
description The majority of ultraluminous X-ray sources are point sources that are spatially offset from the nuclei of nearby galaxies and whose X-ray luminosities exceed the theoretical maximum for spherical infall (the Eddington limit) onto stellar-mass black holes. Their X-ray luminosities in the 0.5–10 kiloelectronvolt energy band range from 10[superscript 39] to 10[superscript 41] ergs per second. Because higher masses imply less extreme ratios of the luminosity to the isotropic Eddington limit, theoretical models have focused on black hole rather than neutron star systems. The most challenging sources to explain are those at the luminous end of the range (more than 10[superscript 40] ergs per second), which require black hole masses of 50–100 times the solar value or significant departures from the standard thin disk accretion that powers bright Galactic X-ray binaries, or both. Here we report broadband X-ray observations of the nuclear region of the galaxy M82 that reveal pulsations with an average period of 1.37 seconds and a 2.5-day sinusoidal modulation. The pulsations result from the rotation of a magnetized neutron star, and the modulation arises from its binary orbit. The pulsed flux alone corresponds to an X-ray luminosity in the 3–30 kiloelectronvolt range of 4.9 × 10[superscript 39] ergs per second. The pulsating source is spatially coincident with a variable source that can reach an X-ray luminosity in the 0.3–10 kiloelectronvolt range of 1.8 × 10[superscript 40] ergs per second. This association implies a luminosity of about 100 times the Eddington limit for a 1.4-solar-mass object, or more than ten times brighter than any known accreting pulsar. This implies that neutron stars may not be rare in the ultraluminous X-ray population, and it challenges physical models for the accretion of matter onto magnetized compact objects.
first_indexed 2024-09-23T15:45:24Z
format Article
id mit-1721.1/98042
institution Massachusetts Institute of Technology
language en_US
last_indexed 2024-09-23T15:45:24Z
publishDate 2015
publisher Nature Publishing Group
record_format dspace
spelling mit-1721.1/980422022-09-29T15:56:06Z An ultraluminous X-ray source powered by an accreting neutron star Bachetti, M. Harrison, Fiona A. Walton, D. J. Grefenstette, Brian W. Fürst, F. Barret, D. Beloborodov, A. Boggs, S. E. Christensen, F. E. Craig, W. W. Fabian, A. C. Hailey, Charles J. Hornschemeier, A. Kaspi, Victoria Kulkarni, S. R. Maccarone, T. J. Miller, J. M. Rana, V. Stern, D. Tendulkar, S. P. Tomsick, J. Webb, N. A. Zhang, W. W. Chakrabarty, Deepto Massachusetts Institute of Technology. Department of Physics Chakrabarty, Deepto The majority of ultraluminous X-ray sources are point sources that are spatially offset from the nuclei of nearby galaxies and whose X-ray luminosities exceed the theoretical maximum for spherical infall (the Eddington limit) onto stellar-mass black holes. Their X-ray luminosities in the 0.5–10 kiloelectronvolt energy band range from 10[superscript 39] to 10[superscript 41] ergs per second. Because higher masses imply less extreme ratios of the luminosity to the isotropic Eddington limit, theoretical models have focused on black hole rather than neutron star systems. The most challenging sources to explain are those at the luminous end of the range (more than 10[superscript 40] ergs per second), which require black hole masses of 50–100 times the solar value or significant departures from the standard thin disk accretion that powers bright Galactic X-ray binaries, or both. Here we report broadband X-ray observations of the nuclear region of the galaxy M82 that reveal pulsations with an average period of 1.37 seconds and a 2.5-day sinusoidal modulation. The pulsations result from the rotation of a magnetized neutron star, and the modulation arises from its binary orbit. The pulsed flux alone corresponds to an X-ray luminosity in the 3–30 kiloelectronvolt range of 4.9 × 10[superscript 39] ergs per second. The pulsating source is spatially coincident with a variable source that can reach an X-ray luminosity in the 0.3–10 kiloelectronvolt range of 1.8 × 10[superscript 40] ergs per second. This association implies a luminosity of about 100 times the Eddington limit for a 1.4-solar-mass object, or more than ten times brighter than any known accreting pulsar. This implies that neutron stars may not be rare in the ultraluminous X-ray population, and it challenges physical models for the accretion of matter onto magnetized compact objects. United States. National Aeronautics and Space Administration (Contract NNG08FD60C) 2015-08-06T12:12:00Z 2015-08-06T12:12:00Z 2014-10 Article http://purl.org/eprint/type/JournalArticle 0028-0836 1476-4687 http://hdl.handle.net/1721.1/98042 Bachetti, M., F. A. Harrison, D. J. Walton, B. W. Grefenstette, D. Chakrabarty, F. Fürst, D. Barret, et al. “An Ultraluminous X-Ray Source Powered by an Accreting Neutron Star.” Nature 514, no. 7521 (October 8, 2014): 202–204. https://orcid.org/0000-0001-8804-8946 en_US http://dx.doi.org/10.1038/nature13791 Nature Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. application/pdf Nature Publishing Group arXiv
spellingShingle Bachetti, M.
Harrison, Fiona A.
Walton, D. J.
Grefenstette, Brian W.
Fürst, F.
Barret, D.
Beloborodov, A.
Boggs, S. E.
Christensen, F. E.
Craig, W. W.
Fabian, A. C.
Hailey, Charles J.
Hornschemeier, A.
Kaspi, Victoria
Kulkarni, S. R.
Maccarone, T. J.
Miller, J. M.
Rana, V.
Stern, D.
Tendulkar, S. P.
Tomsick, J.
Webb, N. A.
Zhang, W. W.
Chakrabarty, Deepto
An ultraluminous X-ray source powered by an accreting neutron star
title An ultraluminous X-ray source powered by an accreting neutron star
title_full An ultraluminous X-ray source powered by an accreting neutron star
title_fullStr An ultraluminous X-ray source powered by an accreting neutron star
title_full_unstemmed An ultraluminous X-ray source powered by an accreting neutron star
title_short An ultraluminous X-ray source powered by an accreting neutron star
title_sort ultraluminous x ray source powered by an accreting neutron star
url http://hdl.handle.net/1721.1/98042
https://orcid.org/0000-0001-8804-8946
work_keys_str_mv AT bachettim anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT harrisonfionaa anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT waltondj anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT grefenstettebrianw anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT furstf anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT barretd anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT beloborodova anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT boggsse anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT christensenfe anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT craigww anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT fabianac anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT haileycharlesj anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT hornschemeiera anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT kaspivictoria anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT kulkarnisr anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT maccaronetj anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT millerjm anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT ranav anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT sternd anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT tendulkarsp anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT tomsickj anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT webbna anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT zhangww anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT chakrabartydeepto anultraluminousxraysourcepoweredbyanaccretingneutronstar
AT bachettim ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT harrisonfionaa ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT waltondj ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT grefenstettebrianw ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT furstf ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT barretd ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT beloborodova ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT boggsse ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT christensenfe ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT craigww ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT fabianac ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT haileycharlesj ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT hornschemeiera ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT kaspivictoria ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT kulkarnisr ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT maccaronetj ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT millerjm ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT ranav ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT sternd ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT tendulkarsp ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT tomsickj ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT webbna ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT zhangww ultraluminousxraysourcepoweredbyanaccretingneutronstar
AT chakrabartydeepto ultraluminousxraysourcepoweredbyanaccretingneutronstar