Isospin

Results: 90



#Item
31Valeriy Yazkov∗† SINP MSU E-mail: [removed] Measurement of π + π − and π K atom lifetimes allows to check prediction of Chiral Perturbation Theory for pion-pion scattering lengths with isospin 0 and

Valeriy Yazkov∗† SINP MSU E-mail: [removed] Measurement of π + π − and π K atom lifetimes allows to check prediction of Chiral Perturbation Theory for pion-pion scattering lengths with isospin 0 and

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Source URL: cds.cern.ch

Language: English - Date: 2011-09-06 04:23:24
32Eur. Phys. J. A[removed]: 18 DOI[removed]epja/i2011[removed]THE EUROPEAN PHYSICAL JOURNAL A

Eur. Phys. J. A[removed]: 18 DOI[removed]epja/i2011[removed]THE EUROPEAN PHYSICAL JOURNAL A

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Source URL: digital.csic.es

Language: English - Date: 2011-09-27 18:00:00
33The Heavy Proton L. David Roper mailto:[removed] Introduction The proton is the nucleus of the hydrogen atom, which has one orbiting electron. The proton is the least massive of the baryons. Its mass is[removed]

The Heavy Proton L. David Roper mailto:[removed] Introduction The proton is the nucleus of the hydrogen atom, which has one orbiting electron. The proton is the least massive of the baryons. Its mass is[removed]

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Source URL: www.roperld.com

Language: English - Date: 2014-01-26 07:41:03
34Quark Structure of Baryons: A 3D Harmonic Oscillator Model L. David Roper mailto:[removed] Introduction Baryons (Ref. 9) are constructed of three spin-½ positive-parity quarks. There are six different quarks (Ref

Quark Structure of Baryons: A 3D Harmonic Oscillator Model L. David Roper mailto:[removed] Introduction Baryons (Ref. 9) are constructed of three spin-½ positive-parity quarks. There are six different quarks (Ref

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Source URL: www.roperld.com

Language: English - Date: 2014-01-27 13:27:08
35Vittorio Lubicz∗ Università Roma Tre and INFN sezione di Roma Tre E-mail: [removed] I review lattice calculations and results for hadronic parameters relevant for kaon physics, in particular the vector fo

Vittorio Lubicz∗ Università Roma Tre and INFN sezione di Roma Tre E-mail: [removed] I review lattice calculations and results for hadronic parameters relevant for kaon physics, in particular the vector fo

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Source URL: pos.sissa.it

Language: English - Date: 2010-05-24 11:25:01
36Multi-hadron systems in lattice QCD Department of Physics, College of William and Mary, Williamsburg, VA 23185, USA Thomas Jefferson National Accelerator Facility, 12000 Jefferson Ave, Newport News, VA 23606, USA. E-mai

Multi-hadron systems in lattice QCD Department of Physics, College of William and Mary, Williamsburg, VA 23185, USA Thomas Jefferson National Accelerator Facility, 12000 Jefferson Ave, Newport News, VA 23606, USA. E-mai

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Source URL: pos.sissa.it

Language: English - Date: 2009-11-12 15:36:00
378. Naming scheme for hadrons[removed]NAMING SCHEME FOR HADRONS Revised 2004 by M. Roos (University of Finland) and C.G. Wohl (LBNL[removed]Introduction

8. Naming scheme for hadrons[removed]NAMING SCHEME FOR HADRONS Revised 2004 by M. Roos (University of Finland) and C.G. Wohl (LBNL[removed]Introduction

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Source URL: pdg.lbl.gov

Language: English - Date: 2014-08-21 16:38:33
388. Naming scheme for hadrons[removed]NAMING SCHEME FOR HADRONS Revised 2004 by M. Roos (University of Finland) and C.G. Wohl (LBNL[removed]Introduction

8. Naming scheme for hadrons[removed]NAMING SCHEME FOR HADRONS Revised 2004 by M. Roos (University of Finland) and C.G. Wohl (LBNL[removed]Introduction

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Source URL: pdg.lbl.gov

Language: English - Date: 2013-12-18 14:59:03
396. Symmetries in medium-light nuclei: at and beyond the N=Z line* 6.1. Introduction Symmetry is normally associated to the concept of beauty. In physics, symmetries help to better understand the world

6. Symmetries in medium-light nuclei: at and beyond the N=Z line* 6.1. Introduction Symmetry is normally associated to the concept of beauty. In physics, symmetries help to better understand the world

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Source URL: euroball.lnl.infn.it

Language: English - Date: 2006-09-06 11:40:27
40Chapter 6 Nucleon-Nucleon Interaction, Deuteron Protons and neutrons are the lowest-energy bound states of quarks and gluons. When we put two or more of these particles together, they interact, scatter and sometimes for

Chapter 6 Nucleon-Nucleon Interaction, Deuteron Protons and neutrons are the lowest-energy bound states of quarks and gluons. When we put two or more of these particles together, they interact, scatter and sometimes for

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Source URL: www.physics.umd.edu

Language: English - Date: 2007-04-26 22:13:24