Solar neutrinos and the principle of equivalence
We study the proposed solution of the solar neutrino problem which requires a flavor nondiagonal coupling of neutrinos to gravity. We adopt a phenomenological point of view and investigate the consequences of the hypothesis that the neutrino weak interaction eigenstates are linear combinations of th...
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Veröffentlicht in: | Physical Review, D D, 1995-08, Vol.52 (4), p.1770-1779 |
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description | We study the proposed solution of the solar neutrino problem which requires a flavor nondiagonal coupling of neutrinos to gravity. We adopt a phenomenological point of view and investigate the consequences of the hypothesis that the neutrino weak interaction eigenstates are linear combinations of the gravitational eigenstates which have slightly different couplings to gravity, {ital f}{sub 1}{ital G} and {ital f}{sub 2}{ital G}, {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{much_lt}1, corresponding to a difference in redshift between electron and muon neutrinos, {Delta}{ital z}/(1+{ital z}){similar_to}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}. Our {chi}{sup 2} analysis of the available solar neutrino data on observed event rates rules out most of the relevant parameter space, allowing only {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{similar_to}3{times}10{sup {minus}14} for small values of the mixing angle [2{times}10{sup {minus}3}{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}10{sup {minus}2}] and 10{sup {minus}16}{approx_lt}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{approx_lt}10{sup {minus}15} for large mixing [0.6{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}0.9]. We show that the recoil-electron spectrum measured by the Kamiokande II Collaboration can be used to exclude part of the allowed regions obtained above. We analyze the prospects of using future spectral measurements of solar neutrinos to distinguish the oscillation mechanism due to the violation of the equivalence principle from more conventional mechanisms which require neutrinos to have nondegenerate masses. We find that, for small mixing angles, the flavor nondiagonal coupling to gravity leads to predictions regarding the shape of the {sup 8}B-neutrino spectrum which will be distinguishable in the upcoming SNO and Super-Kamiokande experiments and which are independent of solar models. |
doi_str_mv | 10.1103/PhysRevD.52.1770 |
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We adopt a phenomenological point of view and investigate the consequences of the hypothesis that the neutrino weak interaction eigenstates are linear combinations of the gravitational eigenstates which have slightly different couplings to gravity, {ital f}{sub 1}{ital G} and {ital f}{sub 2}{ital G}, {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{much_lt}1, corresponding to a difference in redshift between electron and muon neutrinos, {Delta}{ital z}/(1+{ital z}){similar_to}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}. Our {chi}{sup 2} analysis of the available solar neutrino data on observed event rates rules out most of the relevant parameter space, allowing only {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{similar_to}3{times}10{sup {minus}14} for small values of the mixing angle [2{times}10{sup {minus}3}{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}10{sup {minus}2}] and 10{sup {minus}16}{approx_lt}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{approx_lt}10{sup {minus}15} for large mixing [0.6{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}0.9]. We show that the recoil-electron spectrum measured by the Kamiokande II Collaboration can be used to exclude part of the allowed regions obtained above. We analyze the prospects of using future spectral measurements of solar neutrinos to distinguish the oscillation mechanism due to the violation of the equivalence principle from more conventional mechanisms which require neutrinos to have nondegenerate masses. We find that, for small mixing angles, the flavor nondiagonal coupling to gravity leads to predictions regarding the shape of the {sup 8}B-neutrino spectrum which will be distinguishable in the upcoming SNO and Super-Kamiokande experiments and which are independent of solar models.</description><identifier>ISSN: 0556-2821</identifier><identifier>DOI: 10.1103/PhysRevD.52.1770</identifier><identifier>PMID: 10019404</identifier><language>eng</language><publisher>United States</publisher><subject>COUPLING ; EIGENSTATES ; ELECTRON NEUTRINOS ; EQUIVALENCE PRINCIPLE ; FLAVOR ; MUON NEUTRINOS ; PHYSICS ; QUANTUM GRAVITY ; SOLAR NEUTRINOS ; SPECTRA</subject><ispartof>Physical Review, D, 1995-08, Vol.52 (4), p.1770-1779</ispartof><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c364t-a6fcb7af2f5a3cace2d7643b995bc75e5f07b12e653be0645bcea9d76f85b4123</citedby><cites>FETCH-LOGICAL-c364t-a6fcb7af2f5a3cace2d7643b995bc75e5f07b12e653be0645bcea9d76f85b4123</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,881,2863,2864,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/10019404$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/90562$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Bahcall, JN</creatorcontrib><creatorcontrib>Krastev, PI</creatorcontrib><creatorcontrib>Leung, CN</creatorcontrib><creatorcontrib>Univ. of North Carolina, Chapel Hill, NC (United States)</creatorcontrib><title>Solar neutrinos and the principle of equivalence</title><title>Physical Review, D</title><addtitle>Phys Rev D Part Fields</addtitle><description>We study the proposed solution of the solar neutrino problem which requires a flavor nondiagonal coupling of neutrinos to gravity. We adopt a phenomenological point of view and investigate the consequences of the hypothesis that the neutrino weak interaction eigenstates are linear combinations of the gravitational eigenstates which have slightly different couplings to gravity, {ital f}{sub 1}{ital G} and {ital f}{sub 2}{ital G}, {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{much_lt}1, corresponding to a difference in redshift between electron and muon neutrinos, {Delta}{ital z}/(1+{ital z}){similar_to}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}. Our {chi}{sup 2} analysis of the available solar neutrino data on observed event rates rules out most of the relevant parameter space, allowing only {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{similar_to}3{times}10{sup {minus}14} for small values of the mixing angle [2{times}10{sup {minus}3}{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}10{sup {minus}2}] and 10{sup {minus}16}{approx_lt}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{approx_lt}10{sup {minus}15} for large mixing [0.6{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}0.9]. We show that the recoil-electron spectrum measured by the Kamiokande II Collaboration can be used to exclude part of the allowed regions obtained above. We analyze the prospects of using future spectral measurements of solar neutrinos to distinguish the oscillation mechanism due to the violation of the equivalence principle from more conventional mechanisms which require neutrinos to have nondegenerate masses. We find that, for small mixing angles, the flavor nondiagonal coupling to gravity leads to predictions regarding the shape of the {sup 8}B-neutrino spectrum which will be distinguishable in the upcoming SNO and Super-Kamiokande experiments and which are independent of solar models.</description><subject>COUPLING</subject><subject>EIGENSTATES</subject><subject>ELECTRON NEUTRINOS</subject><subject>EQUIVALENCE PRINCIPLE</subject><subject>FLAVOR</subject><subject>MUON NEUTRINOS</subject><subject>PHYSICS</subject><subject>QUANTUM GRAVITY</subject><subject>SOLAR NEUTRINOS</subject><subject>SPECTRA</subject><issn>0556-2821</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1995</creationdate><recordtype>article</recordtype><recordid>eNpNkM1LAzEQxXNQbK3ePUmOXrbmY5N0j1KtCgXFj3NI0gld2SbtZrfQ_96UreBchhl-78F7CN1QMqWU8Pv39SF9wP5xKtiUKkXO0JgIIQs2Y3SELlP6IXmY5BdoRAmhVUnKMSKfsTEtDtB3bR1iwiascLcGvM2nq7cN4Ogx7Pp6bxoIDq7QuTdNguvTnqDvxdPX_KVYvj2_zh-WheOy7AojvbPKeOaF4c44YCslS26rSlinBAhPlKUMpOAWiCzzF0yVGT8TtqSMTxAefGPqap1c3YFbuxgCuE5XRMgjcjcg2zbuekid3tTJQdOYALFPms5ExQRVOfMEkQF1bUypBa9zvo1pD5oSfaxP_9WnBdPH-rLk9uTe2w2s_gmG7vgvbBVugw</recordid><startdate>19950815</startdate><enddate>19950815</enddate><creator>Bahcall, JN</creator><creator>Krastev, PI</creator><creator>Leung, CN</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>19950815</creationdate><title>Solar neutrinos and the principle of equivalence</title><author>Bahcall, JN ; Krastev, PI ; Leung, CN</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c364t-a6fcb7af2f5a3cace2d7643b995bc75e5f07b12e653be0645bcea9d76f85b4123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1995</creationdate><topic>COUPLING</topic><topic>EIGENSTATES</topic><topic>ELECTRON NEUTRINOS</topic><topic>EQUIVALENCE PRINCIPLE</topic><topic>FLAVOR</topic><topic>MUON NEUTRINOS</topic><topic>PHYSICS</topic><topic>QUANTUM GRAVITY</topic><topic>SOLAR NEUTRINOS</topic><topic>SPECTRA</topic><toplevel>online_resources</toplevel><creatorcontrib>Bahcall, JN</creatorcontrib><creatorcontrib>Krastev, PI</creatorcontrib><creatorcontrib>Leung, CN</creatorcontrib><creatorcontrib>Univ. of North Carolina, Chapel Hill, NC (United States)</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Physical Review, D</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bahcall, JN</au><au>Krastev, PI</au><au>Leung, CN</au><aucorp>Univ. of North Carolina, Chapel Hill, NC (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Solar neutrinos and the principle of equivalence</atitle><jtitle>Physical Review, D</jtitle><addtitle>Phys Rev D Part Fields</addtitle><date>1995-08-15</date><risdate>1995</risdate><volume>52</volume><issue>4</issue><spage>1770</spage><epage>1779</epage><pages>1770-1779</pages><issn>0556-2821</issn><abstract>We study the proposed solution of the solar neutrino problem which requires a flavor nondiagonal coupling of neutrinos to gravity. We adopt a phenomenological point of view and investigate the consequences of the hypothesis that the neutrino weak interaction eigenstates are linear combinations of the gravitational eigenstates which have slightly different couplings to gravity, {ital f}{sub 1}{ital G} and {ital f}{sub 2}{ital G}, {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{much_lt}1, corresponding to a difference in redshift between electron and muon neutrinos, {Delta}{ital z}/(1+{ital z}){similar_to}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}. Our {chi}{sup 2} analysis of the available solar neutrino data on observed event rates rules out most of the relevant parameter space, allowing only {vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{similar_to}3{times}10{sup {minus}14} for small values of the mixing angle [2{times}10{sup {minus}3}{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}10{sup {minus}2}] and 10{sup {minus}16}{approx_lt}{vert_bar}{ital f}{sub 1}{minus}{ital f}{sub 2}{vert_bar}{approx_lt}10{sup {minus}15} for large mixing [0.6{approx_lt}sin{sup 2}(2{theta}{sub {ital G}}){approx_lt}0.9]. We show that the recoil-electron spectrum measured by the Kamiokande II Collaboration can be used to exclude part of the allowed regions obtained above. We analyze the prospects of using future spectral measurements of solar neutrinos to distinguish the oscillation mechanism due to the violation of the equivalence principle from more conventional mechanisms which require neutrinos to have nondegenerate masses. We find that, for small mixing angles, the flavor nondiagonal coupling to gravity leads to predictions regarding the shape of the {sup 8}B-neutrino spectrum which will be distinguishable in the upcoming SNO and Super-Kamiokande experiments and which are independent of solar models.</abstract><cop>United States</cop><pmid>10019404</pmid><doi>10.1103/PhysRevD.52.1770</doi><tpages>10</tpages><oa>free_for_read</oa></addata></record> |
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subjects | COUPLING EIGENSTATES ELECTRON NEUTRINOS EQUIVALENCE PRINCIPLE FLAVOR MUON NEUTRINOS PHYSICS QUANTUM GRAVITY SOLAR NEUTRINOS SPECTRA |
title | Solar neutrinos and the principle of equivalence |
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