Electromagnetic Mass Difference of Lowest Lying Hadrons and Behavior Quarks in Hadrons
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概要
- 論文の詳細を見る
Electromagnetic mass difference of lowest lying hadrons are investigated in the quark model with Gaussian wave functions. The Fermi-Breit interactions for one photon exchange and one gluon exchange terms are calculated. To fit the electromagnetic mass differences of baryons (N,Σ,H) and mesons (π,K) with the common quark mass difference m_d-m_u, we must introduce different relative distances between quarks in a baryon due to spin-spin interactions This produces the negative change radius of neutron. The electromagnetic mass difference of the charmed meson D^+-D^0 is predicted to be 4.8 MeV in good agreement with experiments.
- 理論物理学刊行会の論文
- 1979-02-25
著者
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Minamikawa T
Department Of Physics Tokyo University Of Mercantile Marine
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Minamikawa Toshiyuki
Department Of Physics Tokyo University Of Mercantile Marine
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ITOH Chiaki
Department of Physics, Meiji-Gakuin University
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MIURA Kimio
Department of Physics, Nippon Ika University
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WATANABE Tsunetoshi
Department of Physics, Asia University
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Itoh Chiaki
Department Of Physics Meiji-gakuin University
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Miura Kimio
Department Of Physics Nippon Ika University
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Watanabe Tsunetoshi
Department Of Physics Asia University
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Minamikawa Toshiyuki
Department Of Physics Tokyo University Of Education
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ITOH Chiaki
Department of Physics, Meiji-Gakuen University
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Miura Kimio
Department of Mechanical Systems,Faculty of Computer Science and Systems Engineerig,Kyushu Institute of Technology
関連論文
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- Where Is the Σ_b? : Progress Letters
- Mass Differences of Baryon Isomultiplets and Σ^_c - Σ^0_c
- Electromagnetic Mass Difference of Lowest Lying Hadrons and Behavior Quarks in Hadrons
- One Gluon Exchange Contribution to Electromagnetic Mass Differences
- Electromagnetic Mass Diffrerences of Charmed Particles
- Charmed Mesons
- Massless Vector Gluons in a Unified Gauge Theory of Weak, Electromagnetic and Strong Interactions
- Electromagnetic mass difference and the Structure of Baryon and Boson
- On the Excitation of the J^P=3/2^+ Decuplet and J^P=3/2^- Octuplet in the Neutrino Reaction on the Quark and the Cloud Models
- Discrepancies between Additive Quark Model and Experiments of Baryon Magnetic Moments
- Proper Time Formulation with General Vertices
- SU(6), RP Invariance and Nonmesonic Decay of Hypernuclei
- SU(6) and RP Invariance in Nonleptonic Baryon Decays
- Weak Gamma Decays of Hyperons
- η_b, B_c and a Hybrid Potential(Particles and Fields)
- Relations between the Spectra of 2^+ and 2^- Mesons
- Finite Sums Containing Γ Functions and a Binomial Coefficient
- The 405 Multiplet Meson Decays
- Four-Body Semileptonic Decay of Hyperons and Algebra of Currents
- Nonleptonic Decays of Charmed Baryons in the Quark Model
- Nonleptonic Decays of Charmed Mesons in the Quark Model
- Compton Scattering at High Energies
- A Note on a Possible Avoidance of the Fixed Pole at J=0 in the Presence of the Ionization Point
- The p-n Mass Difference Based on the Reggeized Tadpole Model
- On the Application of the Veneziano Amplitude to Electromagnetic Mass Differences of πand K Mesons
- Regge Pole Model with the Diffractive Correction. II : pn and pp^^- Charge Exchange Scattering
- Regge Pole Model with the Diffractive Correction. I : The Charged Pion Photoproduction
- Pole Approximation and Unitary Symmetry in Nonleptonic Hyperon Decays
- Nonleptonic Hyperon Decay in the Quark Model
- Chiral Dynamics, Nonleptonic Decays of K Mesons and the Derivation of ΔI=1/2 Rule
- SU(3) Chiral Dynamics
- On the Electromagnetic Mass Differences of π and K
- Symmetry Breaking in the SU(3) Chiral Dynamics
- Electromagnetic Mass Difference and SU(3) Bootstrap Model
- Soft Meson Approximation and the Decays of Tensor Mesons
- The Electromagnetic Mass Difference of K Meson due to a Simplified Tadpole and πv→2γ