RISS 학술연구정보서비스

검색

인기 검색어

    다국어 입력

    http://chineseinput.net/에서 pinyin(병음)방식으로 중국어를 변환할 수 있습니다.

    변환된 중국어를 복사하여 사용하시면 됩니다.

    예시)
    • 中文 을 입력하시려면 zhongwen을 입력하시고 space를누르시면됩니다.
    • 北京 을 입력하시려면 beijing을 입력하시고 space를 누르시면 됩니다.
    닫기

    Phenomenological Study of J/ψ Photoproduction on Nucleon = 핵자에서의 J/ψ 광생성에 대한 현상론적 연구

    한글로보기

    https://www.riss.kr/link?id=T17392865

    • 0

      상세조회
    • 0

      다운로드
    서지정보 열기
    • 내보내기
    • 내책장담기
    • 공유하기
    • 오류접수

    부가정보

    다국어 초록 (Multilingual Abstract) kakao i 다국어 번역

    We present a unified description of J/ψ photoproduction on the nucleon from threshold to W = 300 GeV by combining a dynamical hadronic model with diffractive Pomeron exchange. The hadronic sector is built from a phenomenological charm–nucleon potential vcN(r), formulated in Yukawa form and folded with the J/ψ wave function ΦJ/ψ(cc̄) obtained in a constituent quark model (CQM), yielding an effective J/ψ–nucleon interaction VJ/ψN(r). The photoproduction amplitude is computed from a cc̄ loop that couples the γ→cc̄ vertex to ΦJ/ψ, without invoking vector–meson dominance. This approach is crucial for accurately describing the behavior near threshold. The parameters of vcN(r) are constrained such that the long–range part of VJ/ψN(r) reproduces the Yukawa tail seen in lattice QCD, and are fitted to Jefferson Lab (JLab) total and differential cross sections with explicit final–state interactions (FSI). The resulting dσ/dt agree well with GlueX and Hall C data, and the analysis indicates that FSI dominate in the near–threshold region, providing sensitivity to the J/ψ–N scattering amplitude. With the same CQM inputs, we also predict ηc(1S) and ψ(2S) photoproduction cross sections, offering benchmarks for future measurements at JLab and the EIC. We further extend the framework to include coupled–channel (rescattering) effects through intermediate D̄0Λ+c and D̄∗0Λ+c states, consistently incorporating s–, t–, and u– channel mechanisms. These open–charm channels generate cusp–like enhancements in the total cross section near their respective thresholds, W ≃ 4.2–4.3 GeV, and account for the observed structure in the data. At higher energies, Pomeron exchange governs the cross section, while near threshold the interplay of FSI and coupled–channel dynamics is essential for a quantitative description.
    번역하기

    We present a unified description of J/ψ photoproduction on the nucleon from threshold to W = 300 GeV by combining a dynamical hadronic model with diffractive Pomeron exchange. The hadronic sector is built from a phenomenological charm–nucleon poten...

    We present a unified description of J/ψ photoproduction on the nucleon from threshold to W = 300 GeV by combining a dynamical hadronic model with diffractive Pomeron exchange. The hadronic sector is built from a phenomenological charm–nucleon potential vcN(r), formulated in Yukawa form and folded with the J/ψ wave function ΦJ/ψ(cc̄) obtained in a constituent quark model (CQM), yielding an effective J/ψ–nucleon interaction VJ/ψN(r). The photoproduction amplitude is computed from a cc̄ loop that couples the γ→cc̄ vertex to ΦJ/ψ, without invoking vector–meson dominance. This approach is crucial for accurately describing the behavior near threshold. The parameters of vcN(r) are constrained such that the long–range part of VJ/ψN(r) reproduces the Yukawa tail seen in lattice QCD, and are fitted to Jefferson Lab (JLab) total and differential cross sections with explicit final–state interactions (FSI). The resulting dσ/dt agree well with GlueX and Hall C data, and the analysis indicates that FSI dominate in the near–threshold region, providing sensitivity to the J/ψ–N scattering amplitude. With the same CQM inputs, we also predict ηc(1S) and ψ(2S) photoproduction cross sections, offering benchmarks for future measurements at JLab and the EIC. We further extend the framework to include coupled–channel (rescattering) effects through intermediate D̄0Λ+c and D̄∗0Λ+c states, consistently incorporating s–, t–, and u– channel mechanisms. These open–charm channels generate cusp–like enhancements in the total cross section near their respective thresholds, W ≃ 4.2–4.3 GeV, and account for the observed structure in the data. At higher energies, Pomeron exchange governs the cross section, while near threshold the interplay of FSI and coupled–channel dynamics is essential for a quantitative description.

    더보기

    목차 (Table of Contents)

    • 1 Introduction 1
    • 2 Meson-Baryon Reaction 6
    • 2.1 Lippmann–Schwinger Equation 7
    • 2.2 Cross Section Observable 9
    • 2.3 Matrix Element of the Potential 14
    • 1 Introduction 1
    • 2 Meson-Baryon Reaction 6
    • 2.1 Lippmann–Schwinger Equation 7
    • 2.2 Cross Section Observable 9
    • 2.3 Matrix Element of the Potential 14
    • 3 Pomeron Exchange Model 19
    • 3.1 The Pomerons 19
    • 3.2 Diffractive production of vector meson 23
    • 3.3 Pomeron-exchange Amplitude 27
    • 4 Dynamical Model 29
    • 4.1 General Formalism 30
    • 4.2 Final State Interaction 37
    • 4.3 Result 39
    • 4.3.1 1Y and 2Y comparison 40
    • 4.3.2 LQCD constraints 43
    • 4.3.3 Photo-production of ηc(1S) and ψ(2S) 50
    • 5 Coupled Channel Model 53
    • 5.1 General Formalism 54
    • 5.1.1 D̄0Λ+c Intermediate State 57
    • 5.1.2 D̄∗0Λ+c Intermediate State 60
    • 5.2 Result 62
    • 5.2.1 Comparison with data 63
    • 5.2.2 Comparison with Dynamical Model 67
    • 5.2.3 Open Charm Production 69
    • 6 Conclusions 71
    • Bibliography 73
    • Appendices 78
    • A Regge Phenomenology 79
    • B Numerical Calculation Method 85
    • C J/ψ→ e+e− Decay Width 89
    더보기

    분석정보

    View

    상세정보조회

    0

    Usage

    원문다운로드

    0

    대출신청

    0

    복사신청

    0

    EDDS신청

    0

    동일 주제 내 활용도 TOP

    더보기

    주제

    연도별 연구동향

    연도별 활용동향

    연관논문

    연구자 네트워크맵

    공동연구자 (7)

    유사연구자 (20) 활용도상위20명

    이 자료와 함께 이용한 RISS 자료

    나만을 위한 추천자료

    해외이동버튼