The Wolf–Rayet + Black Hole Binary NGC 300 X-1: What is the Mass of the Black Hole?
We present new X-ray and UV observations of the Wolf–Rayet + black hole (BH) binary system NGC 300 X-1 with the Chandra X-ray Observatory and the Hubble Space Telescope Cosmic Origins Spectrograph. When combined with archival X-ray observations, our X-ray and UV observations sample the entire binary...
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Veröffentlicht in: | The Astrophysical journal 2021-03, Vol.910 (1), p.74 |
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creator | Binder, Breanna A. Sy, Janelle M. Eracleous, Michael Christodoulou, Dimitris M. Bhattacharya, Sayantan Cappallo, Rigel Laycock, Silas Plucinsky, Paul P. Williams, Benjamin F. |
description | We present new X-ray and UV observations of the Wolf–Rayet + black hole (BH) binary system NGC 300 X-1 with the Chandra X-ray Observatory and the Hubble Space Telescope Cosmic Origins Spectrograph. When combined with archival X-ray observations, our X-ray and UV observations sample the entire binary orbit, providing clues to the system geometry and interaction between the BH accretion disk and the donor star wind. We measure a binary orbital period of 32.7921 ± 0.0003 hr, in agreement with previous studies, and perform phase-resolved spectroscopy using the X-ray data. The X-ray light curve reveals a deep eclipse, consistent with inclination angles of
i
= 60°–75°, and a pre-eclipse excess consistent with an accretion stream impacting the disk edge. We further measure radial velocity variations for several prominent far-UV spectral lines, most notably H
ii
λ
1640 and C
iv
λ
1550. We find that the He
ii
emission lines systematically lag the expected Wolf–Rayet star orbital motion by a phase difference of Δ
ϕ
∼ 0.3, while C
iv
λ
1550 matches the phase of the anticipated radial velocity curve of the Wolf–Rayet donor. We assume the C
iv
λ
1550 emission line follows a sinusoidal radial velocity curve (semi-amplitude = 250 km s
−1
) and infer a BH mass of 17 ± 4
M
⊙
. Our observations are consistent with the presence of a wind-Roche lobe overflow accretion disk, where an accretion stream forms from gravitationally focused wind material and impacts the edge of the BH accretion disk. |
doi_str_mv | 10.3847/1538-4357/abe6a9 |
format | Article |
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i
= 60°–75°, and a pre-eclipse excess consistent with an accretion stream impacting the disk edge. We further measure radial velocity variations for several prominent far-UV spectral lines, most notably H
ii
λ
1640 and C
iv
λ
1550. We find that the He
ii
emission lines systematically lag the expected Wolf–Rayet star orbital motion by a phase difference of Δ
ϕ
∼ 0.3, while C
iv
λ
1550 matches the phase of the anticipated radial velocity curve of the Wolf–Rayet donor. We assume the C
iv
λ
1550 emission line follows a sinusoidal radial velocity curve (semi-amplitude = 250 km s
−1
) and infer a BH mass of 17 ± 4
M
⊙
. Our observations are consistent with the presence of a wind-Roche lobe overflow accretion disk, where an accretion stream forms from gravitationally focused wind material and impacts the edge of the BH accretion disk.</description><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.3847/1538-4357/abe6a9</identifier><language>eng</language><publisher>Philadelphia: IOP Publishing</publisher><subject>Accretion disks ; Astrophysics ; Binary stars ; Black holes ; Emission lines ; Hubble Space Telescope ; Inclination angle ; Light curve ; Line spectra ; Orbits ; Overflow ; Radial velocity ; Space telescopes ; Spectroscopy ; Velocity curve ; Wind ; X ray telescopes</subject><ispartof>The Astrophysical journal, 2021-03, Vol.910 (1), p.74</ispartof><rights>Copyright IOP Publishing Mar 01, 2021</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c2949-322e75f9aacb67497fb38ecb66db164517ce571a4c4250756623cac37cc62b953</citedby><cites>FETCH-LOGICAL-c2949-322e75f9aacb67497fb38ecb66db164517ce571a4c4250756623cac37cc62b953</cites><orcidid>0000-0002-7652-2206 ; 0000-0003-1415-5823 ; 0000-0002-7502-0597 ; 0000-0002-3719-940X ; 0000-0003-0267-8432 ; 0000-0002-8427-0766 ; 0000-0002-4955-0471</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Binder, Breanna A.</creatorcontrib><creatorcontrib>Sy, Janelle M.</creatorcontrib><creatorcontrib>Eracleous, Michael</creatorcontrib><creatorcontrib>Christodoulou, Dimitris M.</creatorcontrib><creatorcontrib>Bhattacharya, Sayantan</creatorcontrib><creatorcontrib>Cappallo, Rigel</creatorcontrib><creatorcontrib>Laycock, Silas</creatorcontrib><creatorcontrib>Plucinsky, Paul P.</creatorcontrib><creatorcontrib>Williams, Benjamin F.</creatorcontrib><title>The Wolf–Rayet + Black Hole Binary NGC 300 X-1: What is the Mass of the Black Hole?</title><title>The Astrophysical journal</title><description>We present new X-ray and UV observations of the Wolf–Rayet + black hole (BH) binary system NGC 300 X-1 with the Chandra X-ray Observatory and the Hubble Space Telescope Cosmic Origins Spectrograph. When combined with archival X-ray observations, our X-ray and UV observations sample the entire binary orbit, providing clues to the system geometry and interaction between the BH accretion disk and the donor star wind. We measure a binary orbital period of 32.7921 ± 0.0003 hr, in agreement with previous studies, and perform phase-resolved spectroscopy using the X-ray data. The X-ray light curve reveals a deep eclipse, consistent with inclination angles of
i
= 60°–75°, and a pre-eclipse excess consistent with an accretion stream impacting the disk edge. We further measure radial velocity variations for several prominent far-UV spectral lines, most notably H
ii
λ
1640 and C
iv
λ
1550. We find that the He
ii
emission lines systematically lag the expected Wolf–Rayet star orbital motion by a phase difference of Δ
ϕ
∼ 0.3, while C
iv
λ
1550 matches the phase of the anticipated radial velocity curve of the Wolf–Rayet donor. We assume the C
iv
λ
1550 emission line follows a sinusoidal radial velocity curve (semi-amplitude = 250 km s
−1
) and infer a BH mass of 17 ± 4
M
⊙
. Our observations are consistent with the presence of a wind-Roche lobe overflow accretion disk, where an accretion stream forms from gravitationally focused wind material and impacts the edge of the BH accretion disk.</description><subject>Accretion disks</subject><subject>Astrophysics</subject><subject>Binary stars</subject><subject>Black holes</subject><subject>Emission lines</subject><subject>Hubble Space Telescope</subject><subject>Inclination angle</subject><subject>Light curve</subject><subject>Line spectra</subject><subject>Orbits</subject><subject>Overflow</subject><subject>Radial velocity</subject><subject>Space telescopes</subject><subject>Spectroscopy</subject><subject>Velocity curve</subject><subject>Wind</subject><subject>X ray telescopes</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNpFkE1OwzAQhS0EEqWwZ2mJJQq1Pf6J2SAalRapgIRatTvLMY6aEpoSp4vuuAM35CQkBMFq3ozem9F8CJ1TcgUxVwMqII44CDWwqZdWH6De3-gQ9QghPJKglsfoJIR12zKte2g-W3m8KIvs6-Pz2e59jS_xsLDuFU_KwuNhvrHVHj-OEwyE4GVEr_FiZWucB1w3yQcbAi6zH_0fuzlFR5ktgj_7rX00vxvNkkk0fRrfJ7fTyDHNdQSMeSUyba1LpeJaZSnEvtHyJaWSC6qcF4pa7jgTRAkpGTjrQDknWaoF9NFFt3dble87H2qzLnfVpjlpmoBUEmJQjYt0LleVIVQ-M9sqf2v-MpSYFp5pSZmWlOngwTcqO18h</recordid><startdate>20210301</startdate><enddate>20210301</enddate><creator>Binder, Breanna A.</creator><creator>Sy, Janelle M.</creator><creator>Eracleous, Michael</creator><creator>Christodoulou, Dimitris M.</creator><creator>Bhattacharya, Sayantan</creator><creator>Cappallo, Rigel</creator><creator>Laycock, Silas</creator><creator>Plucinsky, Paul P.</creator><creator>Williams, Benjamin F.</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-7652-2206</orcidid><orcidid>https://orcid.org/0000-0003-1415-5823</orcidid><orcidid>https://orcid.org/0000-0002-7502-0597</orcidid><orcidid>https://orcid.org/0000-0002-3719-940X</orcidid><orcidid>https://orcid.org/0000-0003-0267-8432</orcidid><orcidid>https://orcid.org/0000-0002-8427-0766</orcidid><orcidid>https://orcid.org/0000-0002-4955-0471</orcidid></search><sort><creationdate>20210301</creationdate><title>The Wolf–Rayet + Black Hole Binary NGC 300 X-1: What is the Mass of the Black Hole?</title><author>Binder, Breanna A. ; Sy, Janelle M. ; Eracleous, Michael ; Christodoulou, Dimitris M. ; Bhattacharya, Sayantan ; Cappallo, Rigel ; Laycock, Silas ; Plucinsky, Paul P. ; Williams, Benjamin F.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2949-322e75f9aacb67497fb38ecb66db164517ce571a4c4250756623cac37cc62b953</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Accretion disks</topic><topic>Astrophysics</topic><topic>Binary stars</topic><topic>Black holes</topic><topic>Emission lines</topic><topic>Hubble Space Telescope</topic><topic>Inclination angle</topic><topic>Light curve</topic><topic>Line spectra</topic><topic>Orbits</topic><topic>Overflow</topic><topic>Radial velocity</topic><topic>Space telescopes</topic><topic>Spectroscopy</topic><topic>Velocity curve</topic><topic>Wind</topic><topic>X ray telescopes</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Binder, Breanna A.</creatorcontrib><creatorcontrib>Sy, Janelle M.</creatorcontrib><creatorcontrib>Eracleous, Michael</creatorcontrib><creatorcontrib>Christodoulou, Dimitris M.</creatorcontrib><creatorcontrib>Bhattacharya, Sayantan</creatorcontrib><creatorcontrib>Cappallo, Rigel</creatorcontrib><creatorcontrib>Laycock, Silas</creatorcontrib><creatorcontrib>Plucinsky, Paul P.</creatorcontrib><creatorcontrib>Williams, Benjamin F.</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Binder, Breanna A.</au><au>Sy, Janelle M.</au><au>Eracleous, Michael</au><au>Christodoulou, Dimitris M.</au><au>Bhattacharya, Sayantan</au><au>Cappallo, Rigel</au><au>Laycock, Silas</au><au>Plucinsky, Paul P.</au><au>Williams, Benjamin F.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Wolf–Rayet + Black Hole Binary NGC 300 X-1: What is the Mass of the Black Hole?</atitle><jtitle>The Astrophysical journal</jtitle><date>2021-03-01</date><risdate>2021</risdate><volume>910</volume><issue>1</issue><spage>74</spage><pages>74-</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>We present new X-ray and UV observations of the Wolf–Rayet + black hole (BH) binary system NGC 300 X-1 with the Chandra X-ray Observatory and the Hubble Space Telescope Cosmic Origins Spectrograph. When combined with archival X-ray observations, our X-ray and UV observations sample the entire binary orbit, providing clues to the system geometry and interaction between the BH accretion disk and the donor star wind. We measure a binary orbital period of 32.7921 ± 0.0003 hr, in agreement with previous studies, and perform phase-resolved spectroscopy using the X-ray data. The X-ray light curve reveals a deep eclipse, consistent with inclination angles of
i
= 60°–75°, and a pre-eclipse excess consistent with an accretion stream impacting the disk edge. We further measure radial velocity variations for several prominent far-UV spectral lines, most notably H
ii
λ
1640 and C
iv
λ
1550. We find that the He
ii
emission lines systematically lag the expected Wolf–Rayet star orbital motion by a phase difference of Δ
ϕ
∼ 0.3, while C
iv
λ
1550 matches the phase of the anticipated radial velocity curve of the Wolf–Rayet donor. We assume the C
iv
λ
1550 emission line follows a sinusoidal radial velocity curve (semi-amplitude = 250 km s
−1
) and infer a BH mass of 17 ± 4
M
⊙
. Our observations are consistent with the presence of a wind-Roche lobe overflow accretion disk, where an accretion stream forms from gravitationally focused wind material and impacts the edge of the BH accretion disk.</abstract><cop>Philadelphia</cop><pub>IOP Publishing</pub><doi>10.3847/1538-4357/abe6a9</doi><orcidid>https://orcid.org/0000-0002-7652-2206</orcidid><orcidid>https://orcid.org/0000-0003-1415-5823</orcidid><orcidid>https://orcid.org/0000-0002-7502-0597</orcidid><orcidid>https://orcid.org/0000-0002-3719-940X</orcidid><orcidid>https://orcid.org/0000-0003-0267-8432</orcidid><orcidid>https://orcid.org/0000-0002-8427-0766</orcidid><orcidid>https://orcid.org/0000-0002-4955-0471</orcidid><oa>free_for_read</oa></addata></record> |
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source | IOP Publishing Free Content; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; Alma/SFX Local Collection |
subjects | Accretion disks Astrophysics Binary stars Black holes Emission lines Hubble Space Telescope Inclination angle Light curve Line spectra Orbits Overflow Radial velocity Space telescopes Spectroscopy Velocity curve Wind X ray telescopes |
title | The Wolf–Rayet + Black Hole Binary NGC 300 X-1: What is the Mass of the Black Hole? |
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