Relativistic one boson exchange model for the nucleon nucleon interaction
Nucleon-nucleon data below 300-MeV laboratory energy are described by a manifestly covariant wave equation in which one of the intermediate nucleons is restricted to its mass shell. Antisymmetrization of the kernel yields an equation in which the two nucleons are treated in an {ital exactly} symmetr...
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Veröffentlicht in: | Physical review. C, Nuclear physics Nuclear physics, 1991-10, Vol.45 |
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container_title | Physical review. C, Nuclear physics |
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creator | Gross, Franz Van Orden, Jay Holinde, Karl |
description | Nucleon-nucleon data below 300-MeV laboratory energy are described by a manifestly covariant wave equation in which one of the intermediate nucleons is restricted to its mass shell. Antisymmetrization of the kernel yields an equation in which the two nucleons are treated in an {ital exactly} symmetric manner, and in which all amplitudes satisfy the Pauli principle {ital exactly}. The kernel is modeled by the sum of one boson exchanges, and four models, all of which fit the data very well ({chi}{sup 2}{congruent}3 per data point) are discussed. Two models require the exchange of {ital only} the {pi}, {sigma}, {rho}, and {omega}, but also require an admixture of {gamma}{sup 5} coupling for the pion, while two other models restrict the pion coupling to pure {gamma}{sup 5}{gamma}{sup {mu}}, but require the exchange of {ital six} mesons, including the {eta}, and a light scalar-isovector meson referred to as {sigma}{sub 1}. Deuteron wave functions resulting from these models are obtained. Th |
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Antisymmetrization of the kernel yields an equation in which the two nucleons are treated in an {ital exactly} symmetric manner, and in which all amplitudes satisfy the Pauli principle {ital exactly}. The kernel is modeled by the sum of one boson exchanges, and four models, all of which fit the data very well ({chi}{sup 2}{congruent}3 per data point) are discussed. Two models require the exchange of {ital only} the {pi}, {sigma}, {rho}, and {omega}, but also require an admixture of {gamma}{sup 5} coupling for the pion, while two other models restrict the pion coupling to pure {gamma}{sup 5}{gamma}{sup {mu}}, but require the exchange of {ital six} mesons, including the {eta}, and a light scalar-isovector meson referred to as {sigma}{sub 1}. Deuteron wave functions resulting from these models are obtained. Th</description><identifier>ISSN: 0556-2813</identifier><identifier>EISSN: 1089-490X</identifier><language>eng</language><publisher>United States</publisher><subject>AMPLITUDES ; BOSONS ; DEUTERONS ; KERNELS ; MESONS ; NUCLEONS ; PAULI PRINCIPLE ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; PIONS ; WAVE EQUATIONS ; WAVE FUNCTIONS</subject><ispartof>Physical review. 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C, Nuclear physics</title><description>Nucleon-nucleon data below 300-MeV laboratory energy are described by a manifestly covariant wave equation in which one of the intermediate nucleons is restricted to its mass shell. Antisymmetrization of the kernel yields an equation in which the two nucleons are treated in an {ital exactly} symmetric manner, and in which all amplitudes satisfy the Pauli principle {ital exactly}. The kernel is modeled by the sum of one boson exchanges, and four models, all of which fit the data very well ({chi}{sup 2}{congruent}3 per data point) are discussed. Two models require the exchange of {ital only} the {pi}, {sigma}, {rho}, and {omega}, but also require an admixture of {gamma}{sup 5} coupling for the pion, while two other models restrict the pion coupling to pure {gamma}{sup 5}{gamma}{sup {mu}}, but require the exchange of {ital six} mesons, including the {eta}, and a light scalar-isovector meson referred to as {sigma}{sub 1}. Deuteron wave functions resulting from these models are obtained. Th</description><subject>AMPLITUDES</subject><subject>BOSONS</subject><subject>DEUTERONS</subject><subject>KERNELS</subject><subject>MESONS</subject><subject>NUCLEONS</subject><subject>PAULI PRINCIPLE</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>PIONS</subject><subject>WAVE EQUATIONS</subject><subject>WAVE FUNCTIONS</subject><issn>0556-2813</issn><issn>1089-490X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1991</creationdate><recordtype>article</recordtype><recordid>eNqNjL0KwjAURoMoWH_eIT5AIW3S0s6i6CoObiW93tpIvBeaKD6-HXT3LGc4H99EJJmq6tTU6jIViSqKMs2rTM_FIoS7GtG6TMTxhN5G93IhOpBMKFsOTBLf0Fu6oXzwFb3seJCxR0lP8Djmnx1FHCxEx7QSs876gOuvl2Kz3523h5TH6yaAiwg9MBFCbOrC5MbofzYf-BQ98w</recordid><startdate>19911001</startdate><enddate>19911001</enddate><creator>Gross, Franz</creator><creator>Van Orden, Jay</creator><creator>Holinde, Karl</creator><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>19911001</creationdate><title>Relativistic one boson exchange model for the nucleon nucleon interaction</title><author>Gross, Franz ; Van Orden, Jay ; Holinde, Karl</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-osti_scitechconnect_9542443</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1991</creationdate><topic>AMPLITUDES</topic><topic>BOSONS</topic><topic>DEUTERONS</topic><topic>KERNELS</topic><topic>MESONS</topic><topic>NUCLEONS</topic><topic>PAULI PRINCIPLE</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>PIONS</topic><topic>WAVE EQUATIONS</topic><topic>WAVE FUNCTIONS</topic><toplevel>online_resources</toplevel><creatorcontrib>Gross, Franz</creatorcontrib><creatorcontrib>Van Orden, Jay</creatorcontrib><creatorcontrib>Holinde, Karl</creatorcontrib><creatorcontrib>Thomas Jefferson Lab National Accelerator Facility</creatorcontrib><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Physical review. C, Nuclear physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gross, Franz</au><au>Van Orden, Jay</au><au>Holinde, Karl</au><aucorp>Thomas Jefferson Lab National Accelerator Facility</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Relativistic one boson exchange model for the nucleon nucleon interaction</atitle><jtitle>Physical review. C, Nuclear physics</jtitle><date>1991-10-01</date><risdate>1991</risdate><volume>45</volume><issn>0556-2813</issn><eissn>1089-490X</eissn><abstract>Nucleon-nucleon data below 300-MeV laboratory energy are described by a manifestly covariant wave equation in which one of the intermediate nucleons is restricted to its mass shell. Antisymmetrization of the kernel yields an equation in which the two nucleons are treated in an {ital exactly} symmetric manner, and in which all amplitudes satisfy the Pauli principle {ital exactly}. The kernel is modeled by the sum of one boson exchanges, and four models, all of which fit the data very well ({chi}{sup 2}{congruent}3 per data point) are discussed. Two models require the exchange of {ital only} the {pi}, {sigma}, {rho}, and {omega}, but also require an admixture of {gamma}{sup 5} coupling for the pion, while two other models restrict the pion coupling to pure {gamma}{sup 5}{gamma}{sup {mu}}, but require the exchange of {ital six} mesons, including the {eta}, and a light scalar-isovector meson referred to as {sigma}{sub 1}. Deuteron wave functions resulting from these models are obtained. Th</abstract><cop>United States</cop><oa>free_for_read</oa></addata></record> |
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source | American Physical Society Journals |
subjects | AMPLITUDES BOSONS DEUTERONS KERNELS MESONS NUCLEONS PAULI PRINCIPLE PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PIONS WAVE EQUATIONS WAVE FUNCTIONS |
title | Relativistic one boson exchange model for the nucleon nucleon interaction |
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