Hard state neutron star and black hole X-ray binaries in the radio:X-ray luminosity plane
Motivated by the large body of literature around the phenomenological properties of accreting black hole (BH) and neutron star (NS) X-ray binaries in the radio:X-ray luminosity plane, we carry out a comparative regression analysis on 36 BHs and 41 NSs in hard X-ray states, with data over 7 dex in X-...
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description | Motivated by the large body of literature around the phenomenological properties of accreting black hole (BH) and neutron star (NS) X-ray binaries in the radio:X-ray luminosity plane, we carry out a comparative regression analysis on 36 BHs and 41 NSs in hard X-ray states, with data over 7 dex in X-ray luminosity for both. The BHs follow a radio to X-ray (logarithmic) luminosity relation with slope \(\beta=0.59\pm0.02\), consistent with the NSs' slope (\(\beta=0.44^{+0.05}_{-0.04}\)) within 2.5\(\sigma\). The best-fitting intercept for the BHs significantly exceeds that for the NSs, cementing BHs as more radio loud, by a factor \(\sim\)22. \This discrepancy can not be fully accounted for by the mass or bolometric correction gap, nor by the NS boundary layer contribution to the X-rays, and is likely to reflect physical differences in the accretion flow efficiency, or the jet powering mechanism. Once importance sampling is implemented to account for the different luminosity distributions, the slopes of the non-pulsating and pulsating NS subsamples are formally inconsistent (\(>3\sigma\)), unless the transitional millisecond pulsars (whose incoherent radio emission mechanism is not firmly established) are excluded from the analysis. We confirm the lack of a robust partitioning of the BH data set into separate luminosity tracks. |
doi_str_mv | 10.48550/arxiv.1805.01905 |
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The BHs follow a radio to X-ray (logarithmic) luminosity relation with slope \(\beta=0.59\pm0.02\), consistent with the NSs' slope (\(\beta=0.44^{+0.05}_{-0.04}\)) within 2.5\(\sigma\). The best-fitting intercept for the BHs significantly exceeds that for the NSs, cementing BHs as more radio loud, by a factor \(\sim\)22. \This discrepancy can not be fully accounted for by the mass or bolometric correction gap, nor by the NS boundary layer contribution to the X-rays, and is likely to reflect physical differences in the accretion flow efficiency, or the jet powering mechanism. Once importance sampling is implemented to account for the different luminosity distributions, the slopes of the non-pulsating and pulsating NS subsamples are formally inconsistent (\(>3\sigma\)), unless the transitional millisecond pulsars (whose incoherent radio emission mechanism is not firmly established) are excluded from the analysis. We confirm the lack of a robust partitioning of the BH data set into separate luminosity tracks.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1805.01905</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Beta rays ; Binary stars ; Bolometers ; Boundary layers ; Cementing ; Deposition ; Emission analysis ; Importance sampling ; Luminosity ; Millisecond pulsars ; Neutron stars ; Neutrons ; Physics - High Energy Astrophysical Phenomena ; Radio emission ; Regression analysis ; X ray binaries ; X ray stars ; X-rays</subject><ispartof>arXiv.org, 2018-05</ispartof><rights>2018. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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The BHs follow a radio to X-ray (logarithmic) luminosity relation with slope \(\beta=0.59\pm0.02\), consistent with the NSs' slope (\(\beta=0.44^{+0.05}_{-0.04}\)) within 2.5\(\sigma\). The best-fitting intercept for the BHs significantly exceeds that for the NSs, cementing BHs as more radio loud, by a factor \(\sim\)22. \This discrepancy can not be fully accounted for by the mass or bolometric correction gap, nor by the NS boundary layer contribution to the X-rays, and is likely to reflect physical differences in the accretion flow efficiency, or the jet powering mechanism. Once importance sampling is implemented to account for the different luminosity distributions, the slopes of the non-pulsating and pulsating NS subsamples are formally inconsistent (\(>3\sigma\)), unless the transitional millisecond pulsars (whose incoherent radio emission mechanism is not firmly established) are excluded from the analysis. We confirm the lack of a robust partitioning of the BH data set into separate luminosity tracks.</description><subject>Beta rays</subject><subject>Binary stars</subject><subject>Bolometers</subject><subject>Boundary layers</subject><subject>Cementing</subject><subject>Deposition</subject><subject>Emission analysis</subject><subject>Importance sampling</subject><subject>Luminosity</subject><subject>Millisecond pulsars</subject><subject>Neutron stars</subject><subject>Neutrons</subject><subject>Physics - High Energy Astrophysical Phenomena</subject><subject>Radio emission</subject><subject>Regression analysis</subject><subject>X ray binaries</subject><subject>X ray stars</subject><subject>X-rays</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj01Lw0AURQdBsNT-AFcOuE59mc_EnRS1hYKbLnQVXjITOjWdxJlE7L83bVxdHvfwuIeQuxSWIpMSHjH8up9lmoFcQpqDvCIzxnmaZIKxG7KI8QAATGkmJZ-RzzUGQ2OPvaXeDn1o_fkKFL2hZYPVF923jaUfScATLZ3H4GykztN-b2lA49qnqWuGo_NtdP2Jdg16e0uua2yiXfznnOxeX3ardbJ9f9usnrcJSiYSw5QUhtccVVbpEjWUOUrIeKptXuo6H6eyrEJeamWYNKquhBISRl5xyIHPyf309uJddMEdMZyKs39x8R-Jh4noQvs92NgXh3YIftxUMNBcpkwLwf8AaXRckQ</recordid><startdate>20180504</startdate><enddate>20180504</enddate><creator>Gallo, Elena</creator><creator>Degenaar, Nathalie</creator><creator>Jakob van den Eijnden</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20180504</creationdate><title>Hard state neutron star and black hole X-ray binaries in the radio:X-ray luminosity plane</title><author>Gallo, Elena ; 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The BHs follow a radio to X-ray (logarithmic) luminosity relation with slope \(\beta=0.59\pm0.02\), consistent with the NSs' slope (\(\beta=0.44^{+0.05}_{-0.04}\)) within 2.5\(\sigma\). The best-fitting intercept for the BHs significantly exceeds that for the NSs, cementing BHs as more radio loud, by a factor \(\sim\)22. \This discrepancy can not be fully accounted for by the mass or bolometric correction gap, nor by the NS boundary layer contribution to the X-rays, and is likely to reflect physical differences in the accretion flow efficiency, or the jet powering mechanism. Once importance sampling is implemented to account for the different luminosity distributions, the slopes of the non-pulsating and pulsating NS subsamples are formally inconsistent (\(>3\sigma\)), unless the transitional millisecond pulsars (whose incoherent radio emission mechanism is not firmly established) are excluded from the analysis. We confirm the lack of a robust partitioning of the BH data set into separate luminosity tracks.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1805.01905</doi><oa>free_for_read</oa></addata></record> |
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subjects | Beta rays Binary stars Bolometers Boundary layers Cementing Deposition Emission analysis Importance sampling Luminosity Millisecond pulsars Neutron stars Neutrons Physics - High Energy Astrophysical Phenomena Radio emission Regression analysis X ray binaries X ray stars X-rays |
title | Hard state neutron star and black hole X-ray binaries in the radio:X-ray luminosity plane |
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