Generation of helical magnetic field in a viable scenario of inflationary magnetogenesis
We study the generation of helical magnetic fields in a model of inflationary magnetogenesis which is free from the strong coupling and backreaction problems. To generate helical magnetic fields, we add an f2F˜μνFμν term to the Lagrangian of the Ratra model. The strong coupling and backreaction prob...
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Veröffentlicht in: | Physical review. D 2018-04, Vol.97 (8), p.083503, Article 083503 |
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description | We study the generation of helical magnetic fields in a model of inflationary magnetogenesis which is free from the strong coupling and backreaction problems. To generate helical magnetic fields, we add an f2F˜μνFμν term to the Lagrangian of the Ratra model. The strong coupling and backreaction problems are avoided if we take a particular behavior of coupling function f, in which f increases during inflation and decreases postinflation to reheating. The generated magnetic field is fully helical and has a blue spectrum, dρB/dlnk∝k4. This spectrum is obtained when coupling function f∝a2 during inflation. The scale of reheating in our model has to be lower than 4000 GeV to avoid backreaction postinflation. The generated magnetic field spectrum satisfies the γ-ray bound for all the possible scales of reheating. The comoving magnetic field strength and its correlation length are ∼4×10−11 G and 70 kpc respectively, if reheating takes place at 100 GeV. For reheating at the QCD scales of 150 MeV, the field strength increases to ∼ nano gauss, with coherence scale of 0.6 Mpc. |
doi_str_mv | 10.1103/PhysRevD.97.083503 |
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R.</creator><creatorcontrib>Sharma, Ramkishor ; Subramanian, Kandaswamy ; Seshadri, T. R.</creatorcontrib><description>We study the generation of helical magnetic fields in a model of inflationary magnetogenesis which is free from the strong coupling and backreaction problems. To generate helical magnetic fields, we add an f2F˜μνFμν term to the Lagrangian of the Ratra model. The strong coupling and backreaction problems are avoided if we take a particular behavior of coupling function f, in which f increases during inflation and decreases postinflation to reheating. The generated magnetic field is fully helical and has a blue spectrum, dρB/dlnk∝k4. This spectrum is obtained when coupling function f∝a2 during inflation. The scale of reheating in our model has to be lower than 4000 GeV to avoid backreaction postinflation. The generated magnetic field spectrum satisfies the γ-ray bound for all the possible scales of reheating. The comoving magnetic field strength and its correlation length are ∼4×10−11 G and 70 kpc respectively, if reheating takes place at 100 GeV. For reheating at the QCD scales of 150 MeV, the field strength increases to ∼ nano gauss, with coherence scale of 0.6 Mpc.</description><identifier>ISSN: 2470-0010</identifier><identifier>EISSN: 2470-0029</identifier><identifier>DOI: 10.1103/PhysRevD.97.083503</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Coupling ; Field strength ; Heating ; Magnetic fields ; Magnetism</subject><ispartof>Physical review. 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D</title><description>We study the generation of helical magnetic fields in a model of inflationary magnetogenesis which is free from the strong coupling and backreaction problems. To generate helical magnetic fields, we add an f2F˜μνFμν term to the Lagrangian of the Ratra model. The strong coupling and backreaction problems are avoided if we take a particular behavior of coupling function f, in which f increases during inflation and decreases postinflation to reheating. The generated magnetic field is fully helical and has a blue spectrum, dρB/dlnk∝k4. This spectrum is obtained when coupling function f∝a2 during inflation. The scale of reheating in our model has to be lower than 4000 GeV to avoid backreaction postinflation. The generated magnetic field spectrum satisfies the γ-ray bound for all the possible scales of reheating. The comoving magnetic field strength and its correlation length are ∼4×10−11 G and 70 kpc respectively, if reheating takes place at 100 GeV. 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R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c341t-66782c53f8f92d04d2934456b483a33d0194328c009fe7e4dd56dc3a5cc5f6f13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Coupling</topic><topic>Field strength</topic><topic>Heating</topic><topic>Magnetic fields</topic><topic>Magnetism</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sharma, Ramkishor</creatorcontrib><creatorcontrib>Subramanian, Kandaswamy</creatorcontrib><creatorcontrib>Seshadri, T. R.</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. D</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sharma, Ramkishor</au><au>Subramanian, Kandaswamy</au><au>Seshadri, T. R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Generation of helical magnetic field in a viable scenario of inflationary magnetogenesis</atitle><jtitle>Physical review. D</jtitle><date>2018-04-04</date><risdate>2018</risdate><volume>97</volume><issue>8</issue><spage>083503</spage><pages>083503-</pages><artnum>083503</artnum><issn>2470-0010</issn><eissn>2470-0029</eissn><abstract>We study the generation of helical magnetic fields in a model of inflationary magnetogenesis which is free from the strong coupling and backreaction problems. To generate helical magnetic fields, we add an f2F˜μνFμν term to the Lagrangian of the Ratra model. The strong coupling and backreaction problems are avoided if we take a particular behavior of coupling function f, in which f increases during inflation and decreases postinflation to reheating. The generated magnetic field is fully helical and has a blue spectrum, dρB/dlnk∝k4. This spectrum is obtained when coupling function f∝a2 during inflation. The scale of reheating in our model has to be lower than 4000 GeV to avoid backreaction postinflation. The generated magnetic field spectrum satisfies the γ-ray bound for all the possible scales of reheating. The comoving magnetic field strength and its correlation length are ∼4×10−11 G and 70 kpc respectively, if reheating takes place at 100 GeV. For reheating at the QCD scales of 150 MeV, the field strength increases to ∼ nano gauss, with coherence scale of 0.6 Mpc.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevD.97.083503</doi></addata></record> |
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title | Generation of helical magnetic field in a viable scenario of inflationary magnetogenesis |
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