Strange Quark Stars with a Rotating Superfluid Core
The generation of a magnetic field and its distribution inside a rotating bare strange quark star are discussed. It is shown that the difference between the angular velocities of the superfluid and superconducting quark core Ω s and of the normal electron plasma Ω n increases because of spin-down of...
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Veröffentlicht in: | Astrophysics 2015-06, Vol.58 (2), p.216-232 |
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creator | Sedrakian, D. M. Hayrapetyan, M. V. Baghdasaryan, D. S. |
description | The generation of a magnetic field and its distribution inside a rotating bare strange quark star are discussed. It is shown that the difference between the angular velocities of the superfluid and superconducting quark core Ω
s
and of the normal electron plasma Ω
n
increases because of spin-down of the star and this leads to the generation of a magnetic field. The magnetic field distribution in a star is found for a stationary value of ∆Ω=Ω
s
- Ω
n
= const . The magnetic field in the superconducting quark core and in the normal electron shell is continuous along the star’s axis of rotation and has the same value
B
q
=
B
n
, while it is a dipole field outside the star. In all parts of the star this field is determined entirely by the total magnetic moment M of the star. It is also shown that the star’s magnetic moment M is proportional to ΔW, and for some models of compact stars it can vary from 10
31
-10
34
G·cm
3
. |
doi_str_mv | 10.1007/s10511-015-9377-6 |
format | Article |
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s
and of the normal electron plasma Ω
n
increases because of spin-down of the star and this leads to the generation of a magnetic field. The magnetic field distribution in a star is found for a stationary value of ∆Ω=Ω
s
- Ω
n
= const . The magnetic field in the superconducting quark core and in the normal electron shell is continuous along the star’s axis of rotation and has the same value
B
q
=
B
n
, while it is a dipole field outside the star. In all parts of the star this field is determined entirely by the total magnetic moment M of the star. It is also shown that the star’s magnetic moment M is proportional to ΔW, and for some models of compact stars it can vary from 10
31
-10
34
G·cm
3
.</description><identifier>ISSN: 0571-7256</identifier><identifier>EISSN: 1573-8191</identifier><identifier>DOI: 10.1007/s10511-015-9377-6</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Astronomy ; Astrophysics ; Astrophysics and Astroparticles ; Astrophysics and Cosmology ; Fluids ; Magnetic fields ; Magnetic moment ; Observations ; Observations and Techniques ; Physics ; Physics and Astronomy ; Quark stars ; Quarks ; Space Exploration and Astronautics ; Space Sciences (including Extraterrestrial Physics ; Stars ; Stars & galaxies ; Stellar rotation ; Superconductivity ; Superfluidity</subject><ispartof>Astrophysics, 2015-06, Vol.58 (2), p.216-232</ispartof><rights>Springer Science+Business Media New York 2015</rights><rights>COPYRIGHT 2015 Springer</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c553t-369684112696f2407412da032b1c2552edfea2af71a3ef25f5fe1fb4aa01f6d33</citedby><cites>FETCH-LOGICAL-c553t-369684112696f2407412da032b1c2552edfea2af71a3ef25f5fe1fb4aa01f6d33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s10511-015-9377-6$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s10511-015-9377-6$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Sedrakian, D. M.</creatorcontrib><creatorcontrib>Hayrapetyan, M. V.</creatorcontrib><creatorcontrib>Baghdasaryan, D. S.</creatorcontrib><title>Strange Quark Stars with a Rotating Superfluid Core</title><title>Astrophysics</title><addtitle>Astrophysics</addtitle><description>The generation of a magnetic field and its distribution inside a rotating bare strange quark star are discussed. It is shown that the difference between the angular velocities of the superfluid and superconducting quark core Ω
s
and of the normal electron plasma Ω
n
increases because of spin-down of the star and this leads to the generation of a magnetic field. The magnetic field distribution in a star is found for a stationary value of ∆Ω=Ω
s
- Ω
n
= const . The magnetic field in the superconducting quark core and in the normal electron shell is continuous along the star’s axis of rotation and has the same value
B
q
=
B
n
, while it is a dipole field outside the star. In all parts of the star this field is determined entirely by the total magnetic moment M of the star. It is also shown that the star’s magnetic moment M is proportional to ΔW, and for some models of compact stars it can vary from 10
31
-10
34
G·cm
3
.</description><subject>Astronomy</subject><subject>Astrophysics</subject><subject>Astrophysics and Astroparticles</subject><subject>Astrophysics and Cosmology</subject><subject>Fluids</subject><subject>Magnetic fields</subject><subject>Magnetic moment</subject><subject>Observations</subject><subject>Observations and Techniques</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quark stars</subject><subject>Quarks</subject><subject>Space Exploration and Astronautics</subject><subject>Space Sciences (including Extraterrestrial Physics</subject><subject>Stars</subject><subject>Stars & galaxies</subject><subject>Stellar rotation</subject><subject>Superconductivity</subject><subject>Superfluidity</subject><issn>0571-7256</issn><issn>1573-8191</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><recordid>eNqNkc9LwzAUx4MoOKd_gLeCFz105iVN0h7H8MdgIK56DlmbzM6unUmK-t-bMg-bKMg7PHh8vi-8fBA6BzwCjMW1A8wAYgwszqgQMT9AA2CCxilkcIgGmAmIBWH8GJ04t8IYZzzjA0Rzb1Wz1NFjp-xrlHtlXfRe-ZdIRfPWK181yyjvNtqauqvKaNJafYqOjKqdPvvuQ_R8e_M0uY9nD3fTyXgWF4xRH9PwQJoAkNANSbBIgJQKU7KAgjBGdGm0IsoIUFQbwgwzGswiUQqD4SWlQ3S53bux7VunnZfryhW6rlWj285JSCnjIkkp_gcKkKYkIz168QNdtZ1twiGBIikIRvgOtVS1llVj2vBPRb9UjhMGnNIM99ToFypUqddV0TbaVGG-F7jaCwTG6w-_VJ1zcprP91nYsoVtnbPayI2t1sp-SsCyly630mWQLnvpkocM2WZcYINWu3Pcn6EviFWpXw</recordid><startdate>20150601</startdate><enddate>20150601</enddate><creator>Sedrakian, D. 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S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c553t-369684112696f2407412da032b1c2552edfea2af71a3ef25f5fe1fb4aa01f6d33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Astronomy</topic><topic>Astrophysics</topic><topic>Astrophysics and Astroparticles</topic><topic>Astrophysics and Cosmology</topic><topic>Fluids</topic><topic>Magnetic fields</topic><topic>Magnetic moment</topic><topic>Observations</topic><topic>Observations and Techniques</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quark stars</topic><topic>Quarks</topic><topic>Space Exploration and Astronautics</topic><topic>Space Sciences (including Extraterrestrial Physics</topic><topic>Stars</topic><topic>Stars & galaxies</topic><topic>Stellar rotation</topic><topic>Superconductivity</topic><topic>Superfluidity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sedrakian, D. M.</creatorcontrib><creatorcontrib>Hayrapetyan, M. V.</creatorcontrib><creatorcontrib>Baghdasaryan, D. 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M.</au><au>Hayrapetyan, M. V.</au><au>Baghdasaryan, D. S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Strange Quark Stars with a Rotating Superfluid Core</atitle><jtitle>Astrophysics</jtitle><stitle>Astrophysics</stitle><date>2015-06-01</date><risdate>2015</risdate><volume>58</volume><issue>2</issue><spage>216</spage><epage>232</epage><pages>216-232</pages><issn>0571-7256</issn><eissn>1573-8191</eissn><abstract>The generation of a magnetic field and its distribution inside a rotating bare strange quark star are discussed. It is shown that the difference between the angular velocities of the superfluid and superconducting quark core Ω
s
and of the normal electron plasma Ω
n
increases because of spin-down of the star and this leads to the generation of a magnetic field. The magnetic field distribution in a star is found for a stationary value of ∆Ω=Ω
s
- Ω
n
= const . The magnetic field in the superconducting quark core and in the normal electron shell is continuous along the star’s axis of rotation and has the same value
B
q
=
B
n
, while it is a dipole field outside the star. In all parts of the star this field is determined entirely by the total magnetic moment M of the star. It is also shown that the star’s magnetic moment M is proportional to ΔW, and for some models of compact stars it can vary from 10
31
-10
34
G·cm
3
.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10511-015-9377-6</doi><tpages>17</tpages></addata></record> |
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subjects | Astronomy Astrophysics Astrophysics and Astroparticles Astrophysics and Cosmology Fluids Magnetic fields Magnetic moment Observations Observations and Techniques Physics Physics and Astronomy Quark stars Quarks Space Exploration and Astronautics Space Sciences (including Extraterrestrial Physics Stars Stars & galaxies Stellar rotation Superconductivity Superfluidity |
title | Strange Quark Stars with a Rotating Superfluid Core |
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