{"title":"夸克物质的光子E1和规则","authors":"D. Peaslee","doi":"10.1063/1.34904","DOIUrl":null,"url":null,"abstract":"Photoabsorption by nucleon E1 excitation is suggested as a means to test quark mobility in nuclear matter. To this end the E1 sum rules are exhibited for 3 non‐relativistic quarks in a harmonic oscillator model. An excellent fit is obtained to photopion production on free nucleons with an r.m.s. radius 〈r〉≊0.35 F and a constituent quark mass μ=0.37 GeV. Extension of this harmonic oscillator model without additional parameters leads to a Regge trajectory slope of dm2/dJ≊1.1 GeV2, which is just the empirically extracted value. Since γ‐γ scattering has not been observed on nuclear matter in the nucleon E1 region (Eγ=600–800 GeV), some discussion is presented of corresponding M1 measurements in the △ region (Eγ=200–400 MeV). In this discussion the γ‐γ backscattering contributions of individual nucleons are treated as incoherent.","PeriodicalId":240164,"journal":{"name":"Intersections Between Particles and Nuclear Physics","volume":"47 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1984-11-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Photon E1 sum rules for quark matter\",\"authors\":\"D. Peaslee\",\"doi\":\"10.1063/1.34904\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Photoabsorption by nucleon E1 excitation is suggested as a means to test quark mobility in nuclear matter. To this end the E1 sum rules are exhibited for 3 non‐relativistic quarks in a harmonic oscillator model. An excellent fit is obtained to photopion production on free nucleons with an r.m.s. radius 〈r〉≊0.35 F and a constituent quark mass μ=0.37 GeV. Extension of this harmonic oscillator model without additional parameters leads to a Regge trajectory slope of dm2/dJ≊1.1 GeV2, which is just the empirically extracted value. Since γ‐γ scattering has not been observed on nuclear matter in the nucleon E1 region (Eγ=600–800 GeV), some discussion is presented of corresponding M1 measurements in the △ region (Eγ=200–400 MeV). In this discussion the γ‐γ backscattering contributions of individual nucleons are treated as incoherent.\",\"PeriodicalId\":240164,\"journal\":{\"name\":\"Intersections Between Particles and Nuclear Physics\",\"volume\":\"47 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1984-11-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Intersections Between Particles and Nuclear Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.34904\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Intersections Between Particles and Nuclear Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.34904","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Photoabsorption by nucleon E1 excitation is suggested as a means to test quark mobility in nuclear matter. To this end the E1 sum rules are exhibited for 3 non‐relativistic quarks in a harmonic oscillator model. An excellent fit is obtained to photopion production on free nucleons with an r.m.s. radius 〈r〉≊0.35 F and a constituent quark mass μ=0.37 GeV. Extension of this harmonic oscillator model without additional parameters leads to a Regge trajectory slope of dm2/dJ≊1.1 GeV2, which is just the empirically extracted value. Since γ‐γ scattering has not been observed on nuclear matter in the nucleon E1 region (Eγ=600–800 GeV), some discussion is presented of corresponding M1 measurements in the △ region (Eγ=200–400 MeV). In this discussion the γ‐γ backscattering contributions of individual nucleons are treated as incoherent.