Normal modes in magnetized two-fluid spin quantum plasmas
- Autores
- Gomez, Daniel Osvaldo; Kandus, Alejandra
- Año de publicación
- 2018
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- We extend the classical two-fluid magnetohydrodynamic (MHD) formalism to include quantum effects such as electron Fermi pressure, Bohm pressure, and spin couplings. At scales smaller than the electron skin-depth, the Hall effect and electron inertia must be taken into account, and can overlap with the quantum effects. We write down the full set of two-fluid quantumMHD(QMHD)and analyse the relative importance ofthese effects in the high-density environments of neutron star atmospheres and white dwarf interiors, finding that for a broad range of parameters all these effects are operative. Of all spin interactions we analyse only the spin-magnetic coupling, as it is linear in h(stroke) and consequently it is the strongest spin effect. We re-obtain the classical two-fluidMHD dispersion relations corresponding to the magnetosonic and Alfvén modes,modified by quantum effects. In the zero-spin case, for propagation parallel to the magnetic field, we find that the frequency of the fast mode is due to quantum effects modified by electron inertia, while the frequency of the Alfvén-slow sector has no quantum corrections. For perpendicular propagation, the fast-mode frequency is the same as for the parallel propagation plus a correction due only to classical two-fluid effects. When spin is considered, a whistler mode appears, which is due to two-fluid effects plus spin-magnetic interaction. There are no modifications due to spin for parallel propagation of magnetosonic and Alfvén waves, while for perpendicular propagation a dispersive term due to spin arises in the two-fluid expression for the fast magnetosonic mode.
Fil: Gomez, Daniel Osvaldo. Consejo Nacional de Investigaciónes Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Astronomía y Física del Espacio. - Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Astronomía y Física del Espacio; Argentina
Fil: Kandus, Alejandra. Universidade Estadual de Santa Cruz; Brasil - Materia
-
MHD
PLASMAS
STARS: NEUTRON
WHITE DWARFS - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
.jpg)
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/86355
Ver los metadatos del registro completo
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Normal modes in magnetized two-fluid spin quantum plasmasGomez, Daniel OsvaldoKandus, AlejandraMHDPLASMASSTARS: NEUTRONWHITE DWARFShttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1We extend the classical two-fluid magnetohydrodynamic (MHD) formalism to include quantum effects such as electron Fermi pressure, Bohm pressure, and spin couplings. At scales smaller than the electron skin-depth, the Hall effect and electron inertia must be taken into account, and can overlap with the quantum effects. We write down the full set of two-fluid quantumMHD(QMHD)and analyse the relative importance ofthese effects in the high-density environments of neutron star atmospheres and white dwarf interiors, finding that for a broad range of parameters all these effects are operative. Of all spin interactions we analyse only the spin-magnetic coupling, as it is linear in h(stroke) and consequently it is the strongest spin effect. We re-obtain the classical two-fluidMHD dispersion relations corresponding to the magnetosonic and Alfvén modes,modified by quantum effects. In the zero-spin case, for propagation parallel to the magnetic field, we find that the frequency of the fast mode is due to quantum effects modified by electron inertia, while the frequency of the Alfvén-slow sector has no quantum corrections. For perpendicular propagation, the fast-mode frequency is the same as for the parallel propagation plus a correction due only to classical two-fluid effects. When spin is considered, a whistler mode appears, which is due to two-fluid effects plus spin-magnetic interaction. There are no modifications due to spin for parallel propagation of magnetosonic and Alfvén waves, while for perpendicular propagation a dispersive term due to spin arises in the two-fluid expression for the fast magnetosonic mode.Fil: Gomez, Daniel Osvaldo. Consejo Nacional de Investigaciónes Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Astronomía y Física del Espacio. - Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Astronomía y Física del Espacio; ArgentinaFil: Kandus, Alejandra. Universidade Estadual de Santa Cruz; BrasilWiley Blackwell Publishing, Inc2018-12info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/86355Gomez, Daniel Osvaldo; Kandus, Alejandra; Normal modes in magnetized two-fluid spin quantum plasmas; Wiley Blackwell Publishing, Inc; Monthly Notices of the Royal Astronomical Society; 481; 3; 12-2018; 3988-39990035-8711CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/doi/10.1093/mnras/sty2537info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2026-08-25T14:47:58Zoai:ri.conicet.gov.ar:11336/86355instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982026-08-25 14:47:59.293CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
| dc.title.none.fl_str_mv |
Normal modes in magnetized two-fluid spin quantum plasmas |
| title |
Normal modes in magnetized two-fluid spin quantum plasmas |
| spellingShingle |
Normal modes in magnetized two-fluid spin quantum plasmas Gomez, Daniel Osvaldo MHD PLASMAS STARS: NEUTRON WHITE DWARFS |
| title_short |
Normal modes in magnetized two-fluid spin quantum plasmas |
| title_full |
Normal modes in magnetized two-fluid spin quantum plasmas |
| title_fullStr |
Normal modes in magnetized two-fluid spin quantum plasmas |
| title_full_unstemmed |
Normal modes in magnetized two-fluid spin quantum plasmas |
| title_sort |
Normal modes in magnetized two-fluid spin quantum plasmas |
| dc.creator.none.fl_str_mv |
Gomez, Daniel Osvaldo Kandus, Alejandra |
| author |
Gomez, Daniel Osvaldo |
| author_facet |
Gomez, Daniel Osvaldo Kandus, Alejandra |
| author_role |
author |
| author2 |
Kandus, Alejandra |
| author2_role |
author |
| dc.subject.none.fl_str_mv |
MHD PLASMAS STARS: NEUTRON WHITE DWARFS |
| topic |
MHD PLASMAS STARS: NEUTRON WHITE DWARFS |
| purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
| dc.description.none.fl_txt_mv |
We extend the classical two-fluid magnetohydrodynamic (MHD) formalism to include quantum effects such as electron Fermi pressure, Bohm pressure, and spin couplings. At scales smaller than the electron skin-depth, the Hall effect and electron inertia must be taken into account, and can overlap with the quantum effects. We write down the full set of two-fluid quantumMHD(QMHD)and analyse the relative importance ofthese effects in the high-density environments of neutron star atmospheres and white dwarf interiors, finding that for a broad range of parameters all these effects are operative. Of all spin interactions we analyse only the spin-magnetic coupling, as it is linear in h(stroke) and consequently it is the strongest spin effect. We re-obtain the classical two-fluidMHD dispersion relations corresponding to the magnetosonic and Alfvén modes,modified by quantum effects. In the zero-spin case, for propagation parallel to the magnetic field, we find that the frequency of the fast mode is due to quantum effects modified by electron inertia, while the frequency of the Alfvén-slow sector has no quantum corrections. For perpendicular propagation, the fast-mode frequency is the same as for the parallel propagation plus a correction due only to classical two-fluid effects. When spin is considered, a whistler mode appears, which is due to two-fluid effects plus spin-magnetic interaction. There are no modifications due to spin for parallel propagation of magnetosonic and Alfvén waves, while for perpendicular propagation a dispersive term due to spin arises in the two-fluid expression for the fast magnetosonic mode. Fil: Gomez, Daniel Osvaldo. Consejo Nacional de Investigaciónes Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Astronomía y Física del Espacio. - Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Astronomía y Física del Espacio; Argentina Fil: Kandus, Alejandra. Universidade Estadual de Santa Cruz; Brasil |
| description |
We extend the classical two-fluid magnetohydrodynamic (MHD) formalism to include quantum effects such as electron Fermi pressure, Bohm pressure, and spin couplings. At scales smaller than the electron skin-depth, the Hall effect and electron inertia must be taken into account, and can overlap with the quantum effects. We write down the full set of two-fluid quantumMHD(QMHD)and analyse the relative importance ofthese effects in the high-density environments of neutron star atmospheres and white dwarf interiors, finding that for a broad range of parameters all these effects are operative. Of all spin interactions we analyse only the spin-magnetic coupling, as it is linear in h(stroke) and consequently it is the strongest spin effect. We re-obtain the classical two-fluidMHD dispersion relations corresponding to the magnetosonic and Alfvén modes,modified by quantum effects. In the zero-spin case, for propagation parallel to the magnetic field, we find that the frequency of the fast mode is due to quantum effects modified by electron inertia, while the frequency of the Alfvén-slow sector has no quantum corrections. For perpendicular propagation, the fast-mode frequency is the same as for the parallel propagation plus a correction due only to classical two-fluid effects. When spin is considered, a whistler mode appears, which is due to two-fluid effects plus spin-magnetic interaction. There are no modifications due to spin for parallel propagation of magnetosonic and Alfvén waves, while for perpendicular propagation a dispersive term due to spin arises in the two-fluid expression for the fast magnetosonic mode. |
| publishDate |
2018 |
| dc.date.none.fl_str_mv |
2018-12 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
| format |
article |
| status_str |
publishedVersion |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/11336/86355 Gomez, Daniel Osvaldo; Kandus, Alejandra; Normal modes in magnetized two-fluid spin quantum plasmas; Wiley Blackwell Publishing, Inc; Monthly Notices of the Royal Astronomical Society; 481; 3; 12-2018; 3988-3999 0035-8711 CONICET Digital CONICET |
| url |
http://hdl.handle.net/11336/86355 |
| identifier_str_mv |
Gomez, Daniel Osvaldo; Kandus, Alejandra; Normal modes in magnetized two-fluid spin quantum plasmas; Wiley Blackwell Publishing, Inc; Monthly Notices of the Royal Astronomical Society; 481; 3; 12-2018; 3988-3999 0035-8711 CONICET Digital CONICET |
| dc.language.none.fl_str_mv |
eng |
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eng |
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info:eu-repo/semantics/altIdentifier/doi/10.1093/mnras/sty2537 |
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openAccess |
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https://creativecommons.org/licenses/by-nc-sa/2.5/ar/ |
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application/pdf application/pdf |
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Wiley Blackwell Publishing, Inc |
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Wiley Blackwell Publishing, Inc |
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reponame:CONICET Digital (CONICET) instname:Consejo Nacional de Investigaciones Científicas y Técnicas |
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Consejo Nacional de Investigaciones Científicas y Técnicas |
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CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas |
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dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar |
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