LIST OF PUBLICATIONS. Subject: "Pion absorption in the nucleus through the ; nn reaction". Carried
|
|
|
- Candace Heath
- 6 years ago
- Views:
Transcription
1 LIST OF PUBLICATIONS I. Ph.D. Thesis Subject: "Pion absorption in the nucleus through the ; nn reaction". Carried out under the supervision of Professor Judah M. Eisenberg, July II. Scientic Papers 1. Theoretical search for a stable ; NN bound state. J. of Phys. G5 (1979) Final state eects in the ; nn reaction. Nucl. Phys. A382 (1982) Intranuclear cascade calculation of pion-nucleus reactions in the resonance region. Z. Fraenkel, E. Piasetski and G. Kalbermann Phys. Rev. C26 (1982) Chiral-bag models and the n! n reaction. Phys. Rev. D28 (1983) Pion photoproduction in the (1232) region and chiral bag models. Phys. Rev. D28 (1983)71 6. Higher order pion eld eects in pion absorption on two nucleons. Phys. Rev. C28 (1983) Nonlinear eects in chiral bag models. 10th Int. Conf. on Few Body Problems, Vol. II, B. Zeitnitz, Editor (1983)621. 4
2 8. Nonlinear eects in chiral bag models. Proc. Work on Perspectives in Nucl. Phys., Trieste, S. Bo, Editor (1983) Application of chiral bag models to the Roper resonance. Phys. Rev. D29 (1984) The ABC eect and the chiral bag model form factor. Nucl. Phys. A426 (1984) Chiral soliton bag models with nonlinear pion elds. Phys. Lett. B138 (1984) Dirac phenomenology at low energies. B.C. Clark, S. Hama, E. Cooper, R.L. Mercer, In Neutron-Nucleus Collisions - A Probe of Nuclear Structure, Ed. J. Rapoport, AIP Conf. Proc. 124 (1984) Solitary waves in the Nambu Jona-Lasinio lagrangian. Phys. Rev. D31(1985) Equivalent local Dirac potentials B.C. Clark, S. Hama, E.D. Cooper and R.L. Mercer, Phys. Rev. Lett. 55 (1985) Relativistic impulse approximation for meson nucleus Scattering. B.C. Clark, S. Hama, R.L. Mercer, Phys. Rev. C31(1985) Solitary waves in a Skyrmion-quark lagrangian. Phys. Rev. D33 (1986)
3 17. The Lorentz-Lorenz eect and the Kemmer-Dun-Petiau equation. Phys. Rev. C33(1986) The proton-neutron mass dierence in the Skyrme model. Phys. Rev. C34(1986) Absence of attraction in the NN central potential derived from Skyrmions. J.M. Eisenberg, R.R Silbar, M.M Sternheim, Phys. Lett. B179(1986) The Kemmer-Dun-Petiau approach to pionic atoms. Phys. Rev. C34(1986) The Kemmer-Dun-Petiau Equation for pionic atoms and anomalous strong interaction eects. E. Friedman, G. Kalbermann and C.J. Batty, Phys. Rev. C34(1986) An improved approximation for the Skyrmion description of the NN system, Phys. Lett. B188(1987) Properties of Skyrmions of large baryon number. Jour. of Phys. G13(1987) The decay width and the energy shift of a metastable state. S. Gurvitz and Phys. Rev. Lett. 59(1987) Kemmer-Dun-Petiau equations from two-body Dirac equations. Phys. Rev. C37(1988) Relativistic deuteron-nucleus scattering in the Kemmer-Dun-Petiau formalism, 6
4 R. Kozack, B.C. Clark, S. Hama, R.L. Mercer and L. Ray, Phys. Rev. C37(1988) Strong interaction nite range eects in light pionic atoms. E. Friedman, A. Gal, C.J. Batty, Phys. Lett. B200(1988) Pair production in transport equations. J.M. Eisenberg and Phys. Rev. D37(1988) Properties of a nite temperature SUSY ensemble. G. Horwitz and Phys. Rev. D38(1988) Scale invariance and ination. B. Gradwohl and Phys. Lett. B208(1988) A search for ; NN bound states. Phys. Lett. B211(1988) Further investigation of the NN interaction in the Skyrme model. Jour. of Phys. G15(1989) NN interactions in the Skyrme model: Coupling to single-baryon vibrations. Nucl. Phys. A500(1989) The use of Skyrmions for two-nucleon systems. J.M. Eisenberg and Adv. in Part. and Nuc. 22(1989) Dilaton stars. B. Gradwohl and Nucl. Phys. B324(1989)215. 7
5 36. Baryon number ambiguities in the symmetrized product ansatz for the Skyrme model. M.M. Sternheim and Phys. Lett. B225(1989) Finite range eects in pionic atoms. E. Friedman, A. Gal and C. J. Batty, Nucl. Phys. A503(1989) Global strings and superuid vortices: dierences and similarities. B. A. Gradwohl, T. Piran and E. Bertschinger, Nucl. Phys. B338(1990) Baryon octet interactions in the Skyrme model. Phys. Lett. B235(1990) A non-linear constraint in scale-invariant theories. B.A. Gradwohl and Phys Rev. D41(1990) Skyrmions for two-baryon systems, J. M. Eisenberg and Nucl. Phys. A508(1990) Properties of the baryon octet in the SU(3) Skyrme model. Phys. Lett. B247(1990) Chiral invariance and scale invariance, G. Kalbermann. Phys. Rev. D42(1990) Radial vibrations in the SU(3) Skyrme model and the NN interaction. Phys. Lett. B257(1991) Consequences of an alternative Skyrmion stabilizing term for the NN force. 8
6 G. Pari and J. M. Eisenberg, Phys. Rev. C48(1991) Finite range eects in hadronic atoms, C. J. Batty, A. Gal, E. Friedman and Nucl. Phys. A535(1992) Baryon octet interactions in the Skyrme model with vibrations and rotations. Phys. Rev. D46(1992) Does the Skyrme model support color transparency? J. M. Eisenberg and Phys. Lett. B286(1992) A modied Skyrme model and the NN interaction, Phys. Rev. C48(1993) The two-nucleon problem in the Skyrme model, Nucl. Phys. A561(1993) The manifold of two Skyrmions, Phys. Lett. B319(1993) three-body forces in the Skyrme model, Phys. Lett. B304(1993) Changes in the radius of a nucleon in interaction with another nucleon, L. L. Frankfurt and J. M. Eisenberg, Phys. Lett. B329(1994) Proton spin content from Skyrmions. J. M. Eisenberg and A.Shaefer, Phys. Lett. B339(1994)211. 9
7 55. Spin content from skyrmions with parameters t to baryon properties. Nucl. Phys. A587(1995) An attractive nucleon-nucleon spin-orbit force from Skyrmions with dilatons, Phys. Lett. B349(1995) Massive topological solitons in electrodynamics, Proceedings of the conference: "The present status of the quantum theory of light", S. Jeers, S. Roy and J. P. Vigier, editors, Kluwer Academic publishers, Quarks and mesons in an SU(2) Skyrme model, preprint 1995, unpublished. 59. Hot nuclear matter with dilatons, J.M. Eisenberg and B. Svetitsky, Nucl. Phys. A600(1996) The nucleon-nucleon force from skyrmions, J.M. Eisenberg and Prog. Part. and Nuc. Phys. 36(1996) Two-baryon forces from skyrmions (April, 1996), J.M. Eisenberg and G. Kalbermann, in Int. Workshop on Hadron Physics 96 eds. E. Ferreira, R.A.M.S. Nazareth, V.L. Baltar, and J. de Sa Borges (World Scientic, Singapore, 1997) p The nucleon in the nucleus as given by skyrmions, J. M. Eisenberg and in Proc. Int. Conf. on Nuclear Physics at the Turn of the Millenium: Structure of Vacuum and Elementary Matters (World Scientic, Singapore),
8 63. Nuclear forces from Skyrmions, J. M. Eisenberg and Int. J. Mod. Phys. E5 (1996) A Skyrmion uid, Nucl. Phys. A., A612 (1997) Soliton tunneling, Physical Review E55, (rapid communications) 6360(1997) 66. Nuclei as skyrmion uids. Nuc. Phys. A (1998). 67. The soliton interacting as a particle Physics Letters A252, 37(1999). 68. Coherent Polychotomous waves from an attractive well Phys. Rev. A60, 2573 (1999). 69. The nucleus as a uid of Skyrmions: Energy levels and medium properties of a Skyrmion in the nucleus Journal of physics G, 26, 129 (2000). 70. Communication through an extra dimension G. Ka lbermann Int. Jour. Modern Physics A15, 3197(2000). 71. Nearness through extra dimensions G. Ka lbermann and H. Halevi, in ActionataDistance, A.Chubykalo and R. Smirnov Rueda, editors(2000). 72. Trapped states and bound states of a soliton in a well G. Ka lbermann Chaos solitons and fractals, 12, 625 (2001). 73. A model for soliton trapping in a well G. Ka lbermann Chaos solitons and fractals, 12-13, 2381 (2001). 11
9 74. Wave packet scattering from an attractive well Jour. of Phys. A34, 3841 (2001). 75. Diraction of wave packets in space and time, Jour. of Phys. A34, 6465 (2001). 76. A dierential equation for the Saman-Taylor nger G. Kalbermann, submitted to Journal of Physics A. 77. Stationary nger solutions in the Hele-Shaw cell, G. Kalbermann and R. Wallach, submitted to Journal of Physics A. 78. Diraction of wave packets in Kronig-Penney model, Jour. of Phys. A, 35, 1045 (2002). 79. Single slit and double slit scattering of wave packets Jour. of Phys. A35, 4599 (2002). 80. Wavepackets falling under a mirror, Jour. of Phys. A35, 9829 (2002). 81. A Helium nanodrop bouncing o a wall, Jour. of Phys. A (2004). 82. Ehrenfest theorem, Galilean invariance and nonlinear Schrodinger equations, Jour. of Phys. A (2004). 83. The Sine-Gordon Wobble, Jour. of Phys. A37, (2004). 84. Decay of a square pulse to Sine-Gordon breathers submitted to Physica D. 12
H-dibaryon in Holographic QCD. Kohei Matsumoto (M2, YITP) (in collaboration with Hideo Suganuma, Yuya Nakagawa)
H-dibaryon in Holographic QCD Kohei Matsumoto (M2, YITP) (in collaboration with Hideo Suganuma, Yuya Nakagawa) 1. Aug. 2016 1 Contents 1. Introduction 2. Chiral Soliton Model 3. Holographic QCD 4. Results
Interplay of kaon condensation and hyperons in dense matter EOS
NPCSM mini-workshop (YITP, Kyoto Univ., Kyoto, October 28(Fri), 2016) Interplay of kaon condensation and hyperons in dense matter EOS Takumi Muto (Chiba Inst. Tech.) collaborators : Toshiki Maruyama (JAEA)
Fractionized Skyrmions in Dense Compact-Star Matter
Fractionized Skyrmions in Dense Compact-Star Matter Yong-Liang Ma Jilin University Seminar @ USTC. Jan.07, 2016. Summary The hadronic matter described as a skyrmion matter embedded in an FCC crystal is
INTRODUCTION TO THE STRUCTURE OF MATTER
INTRODUCTION TO THE STRUCTURE OF MATTER A Course in Modern Physics John J. Brehm and William J. Mullin University of Massachusetts Amherst, Massachusetts Fachberelch 5?@8hnlsdie Hochschule Darmstadt! HochschulstraSa
In-medium properties of the nucleon within a pirho-omega model. Ju-Hyun Jung in collaboration with Hyun-Chul Kim and Ulugbek Yakhshiev
In-medium properties of the nucleon within a pirho-omega model Ju-Hyun Jung in collaboration with Hyun-Chul Kim and Ulugbek Yakhshiev Outline 1. In-medium modified π ρ ω mesonic Lagrangian 2. Structure
A.A. Godizov. Institute for High Energy Physics, Protvino, Russia
arxiv:1410.886v1 [hep-ph] 0 Oct 2014 QCD and nuclear physics. How to explain the coincidence between the radius of the strong interaction of nucleons and the characteristic scale of neutron-neutron electrostatic
Proton Structure and Prediction of Elastic Scattering at LHC at Center-of-Mass Energy 7 TeV
Proton Structure and Prediction of Elastic Scattering at LHC at Center-of-Mass Energy 7 TeV M. M. Islam 1, J. Kašpar 2,3, R. J. Luddy 1 1 Department of Physics, University of Connecticut, Storrs, CT 06269
PROTON STRUCTURE FROM HIGH ENERGY PROTON-PROTON AND ANTIPROTON-PROTON ELASTIC SCATTERING
PROTON STRUCTURE FROM HIGH ENERGY PROTON-PROTON AND ANTIPROTON-PROTON ELASTIC SCATTERING M. M. Islam 1, J. Kašpar 2,3, R. J. Luddy 1 1 Department of Physics, University of Connecticut, Storrs, CT 06269
L. David Roper
The Heavy Proton L. David Roper mailto:roperld@vt.edu 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
Proton. Hadron Charge: +1 Composition: 2 up quarks 1 down quark. Spin: 1/2
The proton radius puzzle Proton Hadron Charge: +1 Composition: 2 up quarks 1 down quark Spin: 1/2 1 How to measure the (rms) radius of the proton https://muhy.web.psi.ch/wiki/index.php/main/news Method
!-mesons produced in, p reactions. de Physique Nucleaire et de l'instrumentation Associee. Service de Physique Nucleaire
Quantum interference in the e + e, decays of - and!-mesons produced in, p reactions Madeleine Soyeur 1, Matthias Lutz 2 and Bengt Friman 2;3 1. Departement d'astrophysique, de Physique des Particules,
Physics 492 Lecture 28
Physics 492 Lecture 28 Main points of last lecture: Feynman diagrams. Main points of today s lecture:. Nuclear forces: charge exchange pion exchange Yukawa force deuteron charge independence, isospin symmetry
Introduction to Modern Physics Problems from previous Exams 3
Introduction to Modern Physics Problems from previous Exams 3 2007 An electron of mass 9 10 31 kg moves along the x axis at a velocity.9c. a. Calculate the rest energy of the electron. b. Calculate its
Effect of Λ(1405) on structure of multi-antikaonic nuclei
12th International Conference on Meson-Nucleon Physics and the Structure of the Nucleon, (May 31-June 4, 2010, College of William and Mary, Williamsburg, Virginia) Session 2B Effect of Λ(1405) on structure
Structure of Atomic Nuclei. Anthony W. Thomas
Structure of Atomic Nuclei Anthony W. Thomas JLab Users Meeting Jefferson Lab : June 2 nd 2015 The Issues What lies at the heart of nuclear structure? Start from a QCD-inspired model of hadron structure
MASTER OF SCIENCE IN PHYSICS
MASTER OF SCIENCE IN PHYSICS The Master of Science in Physics program aims to develop competent manpower to fill the demands of industry and academe. At the end of the program, the students should have
International workshop Strangeness Nuclear Physics 2017 March, 12th-14th, 2017, Osaka Electro-Communication University, Japan. quark mean field theory
International workshop Strangeness Nuclear Physics 2017 March, 12th-14th, 2017, Osaka Electro-Communication University, Japan The strangeness quark mean field theory Jinniu Hu School of Physics, Nankai
Nuclear Landscape not fully known
Nuclear Landscape not fully known Heaviest Elements? Known Nuclei Limit of proton rich nuclei? Fission Limit? Possible Nuclei Limit of Neutron Rich Nuclei? Nuclear Radii Textbooks: R = r 00 A 1/3 1/3 I.
16) Differential cross sections and spin density matrix elements for the reaction p p, M. Williams
Ralf W. Gothe, Professor of Physics University of South Carolina, Department of Physics and Astronomy Columbia, SC 29208 Phone: (803) 777-9025 Fax: (803) 777-3065 E-mail: gothe@sc.edu Publications (since
Can We Measure an Annihilation Range of the Nucleon-Antinucleon System?
Can We Measure an Annihilation Range of the Nucleon-Antinucleon System? The range of the annihilation of the nucleon-antinucleon system is intimately related to our idea of the internal structure of the
Critical lines and points. in the. QCD phase diagram
Critical lines and points in the QCD phase diagram Understanding the phase diagram Phase diagram for m s > m u,d quark-gluon plasma deconfinement quark matter : superfluid B spontaneously broken nuclear
PhD Thesis. Nuclear processes in intense laser eld. Dániel Péter Kis. PhD Thesis summary
PhD Thesis Nuclear processes in intense laser eld PhD Thesis summary Dániel Péter Kis BME Budapest, 2013 1 Background Since the creation of the rst laser light, there has been a massive progress in the
Neutron star properties from an NJL model modified to simulate confinement
Nuclear Physics B (Proc. Suppl.) 141 (25) 29 33 www.elsevierphysics.com Neutron star properties from an NJL model modified to simulate confinement S. Lawley a W. Bentz b anda.w.thomas c a Special Research
MODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont
MODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont McGRAW-HILL, INC. New York St. Louis San Francisco Auckland Bogota Caracas Lisbon London Madrid Mexico Milan Montreal New Delhi
arxiv: v1 [nucl-th] 17 Apr 2010
![arxiv: v1 [nucl-th] 17 Apr 2010](/thumbs/92/109009790.jpg "arxiv: v1 [nucl-th] 17 Apr 2010")
JLAB-THY-1-1165 Hypernuclei in the quark-meson coupling model K. Tsushima and P. A. M. Guichon Thomas Jefferson Lab., 12 Jefferson Ave., ewport ews, VA 2 366, USA SPh-DAPIA, CEA Saclay, F91191 Gif sur
Introduction to Modern Physics
SECOND EDITION Introduction to Modern Physics John D. McGervey Case Western Reserve University Academic Press A Subsidiary of Harcourt Brace Jovanovich Orlando San Diego San Francisco New York London Toronto
Search for the η-mesic Helium bound state with the WASA-at-COSY facility
Search for the η-mesic Helium bound state with the WASA-at-COSY facility Magdalena Skurzok 1, Wojciech Krzemień 2, Oleksandr Rundel 1 and Pawel Moskal 1 for the WASA-at-COSY Collaboration 1 M. Smoluchowski
Equation of state for hybrid stars with strangeness
Equation of state for hybrid stars with strangeness Tsuyoshi Miyatsu, Takahide Kambe, and Koichi Saito Department of Physics, Faculty of Science and Technology, Tokyo University of Science The 26th International
Homework 3: Group Theory and the Quark Model Due February 16
Homework 3: Group Theory and the Quark Model Due February 16 1. Lorentz Group. From the defining requirement that a Lorentz transformation implemented by a matrix Λ leave the metric invariant: Λ µ ρη ρσ
Predictions of High Energy Experimental Results
Predictions of High Energy Experimental Results Eliahu Comay Charactell Ltd., PO Box 39019, Tel-Aviv, 61390, Israel. E-mail: elicomay@post.tau.ac.il Eight predictions of high energy experimental results
Threshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab
hreshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab Introduction With the advent of higher energies at Jefferson Lab, the study of charmonium becomes possible. he threshold production of J/5
Photoabsorption and Photoproduction on Nuclei in the Resonance Region
Photoabsorption and Photoproduction on Nuclei in the Resonance Region Susan Schadmand Institut für Kernphysik First Workshop on Quark-Hadron Duality Frascati, June 6-8, 2005 electromagnetic probes Hadron
The EMC Effect Gerald A. Miller, Univ. of Washington
I NTERNATIONAL JOURNAL OF HIGH-ENERGY PHYSICS CERNCOURIER The EMC Effect Gerald A. Miller, Univ. of Washington V OLUME 53 NUMBER 4 M AY 2013 Deep in the nucleus: a puzzle revisited HEAVY IONS The key to
Lisheng Geng. Ground state properties of finite nuclei in the relativistic mean field model
Ground state properties of finite nuclei in the relativistic mean field model Lisheng Geng Research Center for Nuclear Physics, Osaka University School of Physics, Beijing University Long-time collaborators
arxiv:hep-ph/ v1 12 Oct 1994
A QCD ANALYSIS OF THE MASS STRUCTURE OF THE NUCLEON arxiv:hep-ph/9410274v1 12 Oct 1994 Xiangdong Ji Center for Theoretical Physics Laboratory for Nuclear Science and Department of Physics Massachusetts
NC photon production: nuclear models and pion electro- & photo-production
NC photon production: nuclear models and pion electro- & photo-production Xilin Zhang (Indiana U.& Ohio U.), Brian Serot (Indiana U.) Neutrino-Nucleus Interactions workshop, INT, Seattle, Dec. 2013 1 Outline
Particle Physics. All science is either physics or stamp collecting and this from a 1908 Nobel laureate in Chemistry
Particle Physics JJ Thompson discovered electrons in 1897 Rutherford discovered the atomic nucleus in 1911 and the proton in 1919 (idea of gold foil expt) All science is either physics or stamp collecting
arxiv: v1 [hep-ex] 22 Jun 2009
![arxiv: v1 [hep-ex] 22 Jun 2009](/thumbs/93/113032319.jpg "arxiv: v1 [hep-ex] 22 Jun 2009")
CPC(HEP & NP), 29, 33(X): 1 7 Chinese Physics C Vol. 33, No. X, Xxx, 29 Recent results on nucleon resonance electrocouplings from the studies of π + π p electroproduction with the CLAS detector V. I. Mokeev
Collaborators: Prof. W. Sandhas and members of his group (Bonn),
Few Body Systems A1 Integral Equations (AGS) A2 Integro-differential equations (Hyperspherical Harmonics) A3 Time evolution methods A4 Supersymmetric Quantum Mechanics (SUSY) and Few-Body systems A5 Astrophysics
Hypernuclei Production by K at rest
Hypernuclei Production by K at rest Germano Bonomi 1 Department of Mechanical and Industrial Engineering via Branze 38, Brescia, ITALY & INFN Pavia via Bassi 6, Pavia, ITALY The creation of a hypernucleus
Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation August Introduction to Nuclear Physics - 1
2358-19 Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation 6-17 August 2012 Introduction to Nuclear Physics - 1 P. Van Isacker GANIL, Grand Accelerateur National d'ions Lourds
Parity-Violating Asymmetry for 208 Pb
Parity-Violating Asymmetry for 208 Pb Matteo Vorabbi Dipartimento di Fisica - Università di Pavia INFN - Sezione di Pavia Rome - 2015 January 15 Matteo Vorabbi (Università di Pavia) Parity-Violating Asymmetry
Coherent and incoherent nuclear pion photoproduction
Coherent and incoherent nuclear pion photoproduction Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Gordon Conference on photonuclear reactions, August 2008
FYS3510 Subatomic Physics. Exam 2016
FYS3510 Subatomic Physics VS 2015 Farid Ould-Saada Exam 2016 In addition to the items marked in blue, don t forget all examples and related material given in the slides, including the ones presented during
DEPARTMENT OF PHYSICS
Department of Physics 1 DEPARTMENT OF PHYSICS Office in Engineering Building, Room 124 (970) 491-6206 physics.colostate.edu (http://www.physics.colostate.edu) Professor Jacob Roberts, Chair Undergraduate
Emission of Helium Nuclei in Relativistic Proton Interactions Leading to Total Break up of Ag and Br Nuclei. Z.Physik A 279, 407 (1976).
Emission of Helium Nuclei in Relativistic Proton Interactions Leading to Total Break up of Ag and Br Nuclei. Z.Physik A 279, 407 (1976). Inelastic Interactions of 69.0 GeV/c Protons with Emulsion Nuclei.
arxiv:hep-ph/ v1 1 Feb 2005
Vector Goldstone Boson and Lorentz Invariance arxiv:hep-ph/050011v1 1 Feb 005 Ling-Fong Li Department of Physics, Carnegie Mellon University, Pittsburgh, PA 1513 January 5, 018 Abstract Spontanous symmetry
PHYSICS-PH (PH) Courses. Physics-PH (PH) 1
Physics-PH (PH) 1 PHYSICS-PH (PH) Courses PH 110 Physics of Everyday Phenomena (GT-SC2) Credits: 3 (3-0-0) Fundamental concepts of physics and elementary quantitative reasoning applied to phenomena in
Origin of the Nuclear EOS in Hadronic Physics and QCD. Anthony W. Thomas
Origin of the Nuclear EOS in Hadronic Physics and QCD Anthony W. Thomas XXX Symposium on Nuclear Physics - Cocoyoc: Jan 5 th 2007 Operated by Jefferson Science Associates for the U.S. Department of Energy
The ATLAS Experiment and the CERN Large Hadron Collider
The ATLAS Experiment and the CERN Large Hadron Collider HEP101-2 January 28, 2013 Al Goshaw 1 HEP 101-2 plan Jan. 14: Introduction to CERN and ATLAS DONE Today: 1. Comments on grant opportunities 2. Overview
QCD Symmetries in eta and etaprime mesic nuclei
QCD Symmetries in eta and etaprime mesic nuclei Steven Bass Chiral symmetry, eta and eta physics: the masses of these mesons are 300-400 MeV too big for them to be pure Goldstone bosons Famous axial U(1)
Hadron Production in ultra relativistic nuclear collisions and the QCD phase boundary
Hadron Production in ultra relativistic nuclear collisions and the QCD phase boundary introductory remarks the thermal/statistical model results for AA collisions a note on thermal models in elementary
The ATLAS Experiment and the CERN Large Hadron Collider
The ATLAS Experiment and the CERN Large Hadron Collider HEP101-2 April 5, 2010 A. T. Goshaw Duke University 1 HEP 101 Plan March 29: Introduction and basic HEP terminology March 30: Special LHC event:
Hadron Physics & Quantum Chromodynamics Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora
Hadron Physics & Quantum Chromodynamics Adnan Bashir, IFM, UMSNH, Mexico August 2013 Hermosillo Sonora Hadron Physics & QCD Part 1: First Encounter With Hadrons: Introduction to Mesons & Baryons, The Quark
NUCLEAR FORCES. Historical perspective
NUCLEAR FORCES Figure 1: The atomic nucleus made up from protons (yellow) and neutrons (blue) and held together by nuclear forces. Nuclear forces (also known as nuclear interactions or strong forces) are
Nuclear Forces - Lecture 1 - R. Machleidt University of Idaho
CNS Summer School, Univ. of Tokyo, at Wako campus of RIKEN, Aug. 18-23, 2005 Nuclear Forces - Lecture 1 - R. Machleidt University of Idaho 1 Nuclear Forces - Overview of all lectures - Lecture 1: History,
Nuclear structure Anatoli Afanasjev Mississippi State University
Nuclear structure Anatoli Afanasjev Mississippi State University 1. Nuclear theory selection of starting point 2. What can be done exactly (ab-initio calculations) and why we cannot do that systematically?
A Superfluid Universe
A Superfluid Universe Lecture 2 Quantum field theory & superfluidity Kerson Huang MIT & IAS, NTU Lecture 2. Quantum fields The dynamical vacuum Vacuumscalar field Superfluidity Ginsburg Landau theory BEC
1 Geant4 to simulate Photoelectric, Compton, and Pair production Events
Syed F. Naeem, hw-12, Phy 599 1 Geant4 to simulate Photoelectric, Compton, and Pair production Events 1.1 Introduction An Aluminum (Al) target of 20cm was used in this simulation to see the eect of incoming
At this time the quark model consisted of three particles, the properties of which are given in the table.
*1 In 1961 Murray Gell-Mann predicted the existence of a new particle called an omega (Ω) minus. It was subsequently discovered in 1964. At this time the quark model consisted of three particles, the properties
DISCRETE SYMMETRIES IN NUCLEAR AND PARTICLE PHYSICS. Parity PHYS NUCLEAR AND PARTICLE PHYSICS
PHYS 30121 NUCLEAR AND PARTICLE PHYSICS DISCRETE SYMMETRIES IN NUCLEAR AND PARTICLE PHYSICS Discrete symmetries are ones that do not depend on any continuous parameter. The classic example is reflection
ESSENTIAL QUANTUM PHYSICS PETER LANDSHOFF. University of Cambridge ALLEN METHERELL. University of Central Florida GARETH REES. University of Cambridge
ESSENTIAL QUANTUM PHYSICS PETER LANDSHOFF University of Cambridge ALLEN METHERELL University of Central Florida GARETH REES University of Cambridge CAMBRIDGE UNIVERSITY PRESS Constants of quantum physics
On a non-cp-violating electric dipole moment of elementary. particles. J. Giesen, Institut fur Theoretische Physik, Bunsenstrae 9, D Gottingen
On a non-cp-violating electric dipole moment of elementary particles J. Giesen, Institut fur Theoretische Physik, Bunsenstrae 9, D-3773 Gottingen (e-mail: giesentheo-phys.gwdg.de) bstract description of
Cold and dense QCD matter
Cold and dense QCD matter GCOE sympodium Feb. 15, 2010 Yoshimasa Hidaka Quantum ChromoDynamics Atom Electron 10-10 m Quantum ChromoDynamics Atom Nucleon Electron 10-10 m 10-15 m Quantum ElectroDynamics
Complex 2D Matrix Model and Internal Structure of Resonances
Complex 2D Matrix Model and Internal Structure of Resonances Kanabu Nawa (RIKEN) In collaboration with Sho Ozaki, Hideko Nagahiro, Daisuke Jido and Atsushi Hosaka [arxiv:1109.0426[hep-ph]] CONTENTS * Nature
Coherent Neutrino Nucleus Scattering
1 Coherent Neutrino Nucleus Scattering E.A. Paschos a and A. Kartavtsev b (presented by E.A. Paschos) a Universität Dortmund, D 441 Dortmund, Germany b Rostov State University, Rostov on Don, Russia We
Hadronic Resonances in a Hadronic Picture. Daisuke Jido (Nuclear physics group)
Daisuke Jido (Nuclear physics group) Hadrons (particles interacting with strong interactions) are composite objects of quarks and gluons. It has been recently suggested that the structures of some hadrons
The Charged Higgs-like Bosons Have Already Been Observed by the ATLAS and CMS Collaborations
The Charged iggs-like Bosons ave Already Been Observed by the ATLAS and CMS Collaborations Mario Everaldo de Souza Departamento de Fisica, Universidade Federal de Sergipe, 491- São Cristovão, Sergipe,
Experimental Tests of Charge Symmetry Breaking in Hypernuclei
Experimental Tests of Charge Symmetry Breaking in Hypernuclei Institut für Kernphysik, Johannes Gutenberg-Universität, Mainz, Germany E-mail: achenbach@uni-mainz.de A pedagogical discussion of the charge
Is the relativistic distorted-wave impulse approximation useful to nuclear reaction?
Is the relativistic distorted-wave impulse approximation useful to nuclear reaction? K. Miyazaki Abstract e have reconsidered the nonrelativistic distorted-wave t-matrix approximation (NR-DTA) for proton
The balance function in azimuthal angle is a measure of the transverse flow
Physics Letters B 609 (2005) 247 251 www.elsevier.com/locate/physletb The balance function in azimuthal angle is a measure of the transverse flow Piotr Bożek The H. Niewodniczański Institute of Nuclear
arxiv:hep-ph/ v2 25 Mar 1995
Proton Spin in Chiral Quark Models H. J. Weber, X. Song Institute of Nuclear and Particle Physics, University of Virginia, Charlottesville, VA 901, USA arxiv:hep-ph/970166v 5 Mar 1995 and M. Kirchbach
Introduction to Elementary Particles
David Criffiths Introduction to Elementary Particles Second, Revised Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Preface to the First Edition IX Preface to the Second Edition XI Formulas and Constants
Relativistic EOS for Supernova Simulations
Relativistic EOS for Supernova Simulations H. Shen Nankai University, Tianjin, China 申虹 In collaboration with H. Toki RCNP, Osaka University, Japan K. Sumiyoshi Numazu College of Technology, Japan K. Oyamatsu
Spin Physics Experiments at SLAC
SLAC-PUB-9269 June, 2002 Spin Physics Experiments at SLAC P. Bosted, for the E155/E155x Collaborations 1 Stanford Linear Accelerator Center, Stanford CA 94309 and Physics Dept., University of Massachusetts,
How does the proton spin?
How does the proton spin? Steven Bass Proton spin problem: Where does the spin of the nucleon (proton and neutron) come from? E.g. The key difference between 3 He and 4 He in low temperature physics comes
PHYS 3446 Lecture #17
PHY 3446 Lecture #7 Monday, Nov. 6, 26 Dr.. Elementary Particle Properties Quantum Numbers trangeness Isospin Gell-Mann-Nishijima Relations Production and Decay of Resonances Monday, Nov. 6, 26 PHY 3446,
Highenergy Nuclear Optics of Polarized Particles
Highenergy Nuclear Optics of Polarized Particles Vladimir G. Baryshevsky Research Institute for Nuclear Problems Belarusian State University 1> World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI
QRPA Calculations of Charge Exchange Reactions and Weak Interaction Rates. N. Paar
Strong, Weak and Electromagnetic Interactions to probe Spin-Isospin Excitations ECT*, Trento, 28 September - 2 October 2009 QRPA Calculations of Charge Exchange Reactions and Weak Interaction Rates N.
Coupling of Angular Momenta Isospin Nucleon-Nucleon Interaction
Lecture 5 Coupling of Angular Momenta Isospin Nucleon-Nucleon Interaction WS0/3: Introduction to Nuclear and Particle Physics,, Part I I. Angular Momentum Operator Rotation R(θ): in polar coordinates the
An Introduction to the Standard Model of Particle Physics
An Introduction to the Standard Model of Particle Physics W. N. COTTINGHAM and D. A. GREENWOOD Ж CAMBRIDGE UNIVERSITY PRESS Contents Preface. page xiii Notation xv 1 The particle physicist's view of Nature
Nuclear equation of state for supernovae and neutron stars
Nuclear equation of state for supernovae and neutron stars H. Shen Nankai University, Tianjin, China 申虹 In collaboration with 南開大学 天津 H. Toki RCNP, Osaka University, Japan 中国 K. Sumiyoshi Numazu College
Antibaryons in massive heavy ion reactions: Importance of potentials
Antibaryons in massive heavy ion reactions: Importance of potentials C. Spieles, M. Bleicher, A. Jahns, R. Mattiello, H. Sorge, H. Stöcker, W. Greiner Institut für Theoretische Physik, J. W. Goethe Universität,
Symmetries and in-medium effects
Article available at http://www.epj-conferences.org or http://dx.doi.org/10.1051/epjconf/20147806003 EPJ Web of Conferences 78, 06003 ( 2014) DOI: 10.1051/ epjconf/ 20147806003 C Owned by the authors,
Clusters in Dense Matter and the Equation of State
Clusters in Dense Matter and the Equation of State Excellence Cluster Universe, Technische Universität München GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt in collaboration with Gerd Röpke
Transition Matrix Elements for Pion Photoproduction
Transition Matrix Elements for Pion Photoproduction Mohamed E. Kelabi 1 Abstract We have obtained the transition matrix elements for pion photoproduction by considering the number of gamma matrices involved.
Chiral Model in Nuclear Medium and Hypernuclear Production
WDS'10 Proceedings of ontributed Papers, Part III, 2 6, 2010. ISBN 978-80-7378-141-5 MATFYZPRESS hiral Model in Nuclear Medium and Hypernuclear Production V. Krejčiřík harles University, Faculty of Mathematics
Some new developments in relativistic point-coupling models
Some new developments in relativistic point-coupling models T. J. Buervenich 1, D. G. Madland 1, J. A. Maruhn 2, and P.-G. Reinhard 3 1 Los Alamos National Laboratory 2 University of Frankfurt 3 University
On Consistency in the Skyrme Topological Model
On Consistency in the Skyrme Topological Model Syed Afsar Abbas Centre for Theoretical Physics, JMI University, New Delhi - 11005, India and Jafar Sadiq Research Institute AzimGreenHome, NewSirSyed Nagar,
arxiv:hep-th/ v1 7 Nov 1998
SOGANG-HEP 249/98 Consistent Dirac Quantization of SU(2) Skyrmion equivalent to BFT Scheme arxiv:hep-th/9811066v1 7 Nov 1998 Soon-Tae Hong 1, Yong-Wan Kim 1,2 and Young-Jai Park 1 1 Department of Physics
Calculations of kaonic nuclei based on chiral meson-baryon coupled channel interaction models
Calculations of kaonic nuclei based on chiral meson-baryon coupled channel interaction models J. Hrtánková, J. Mare² Nuclear Physics Institute, eº, Czech Republic 55th International Winter Meeting on Nuclear
The Electric Charge Distribution of the Lambda Particle
427 Progress of Theoretical Physics, Vol. 90, No.2, August 1993 The Electric Charge Distribution of the Lambda Particle Seiichi Y ASUMOTO and Michihiro HIRATA Department of Physics, Hiroshima University,
Clebsch-Gordan Coefficients
Phy489 Lecture 7 Clebsch-Gordan Coefficients 2 j j j2 m m m 2 j= j j2 j + j j m > j m > = C jm > m = m + m 2 2 2 Two systems with spin j and j 2 and z components m and m 2 can combine to give a system
COMMENTS ON EXOTIC CHEMISTRY MODELS AND DEEP DIRAC STATES FOR COLD FUSION
COMMENTS ON EXOTIC CHEMISTRY MODELS AND DEEP DIRAC STATES FOR COLD FUSION R.A. Rice Y.E. Kim Department of Physics Purdue University West Lafayette, IN 47907 M. Rabinowitz Electric Power Research Institute
Xlr^A^lMAcVi^}/^ Chapter 1
Chapter 1 ^i.i...^.h..t.j-;^m-j:ivt-f-'.--ifi^'>-i-'->.i j-;.^,...(.»-.....^ - -. -.:.-j.j.ul-^.f,'. >.i^l-^m-i-)..l-j^hl». am'*i*
Low mass dileptons from Pb + Au collisions at 158 A GeV
PRAMANA cfl Indian Academy of Sciences Vol. 60, No. 5 journal of May 2003 physics pp. 1073 1077 Low mass dileptons from Pb + Au collisions at 158 A GeV SOURAV SARKAR 1, JAN-E ALAM 2;Λ and T HATSUDA 2 1
Selected Publications Wolfram Weise. B. Selected Publications last years (since 2005) status: December 2017 A. Monographs 256.
Selected Publications Wolfram Weise status: December 2017 A. Monographs Pions and Nuclei (with T.E.O. Ericson) International Series of Monographs in Physics Oxford University Press Clarendon, Oxford 1988
Nuclear equation of state for supernovae and neutron stars
Nuclear equation of state for supernovae and neutron stars H. Shen 申虹 In collaboration with Nankai University, Tianjin, China 南開大学 天津 中国 H. Toki RCNP, Osaka University, Japan K. Sumiyoshi Numazu College
DI-NEUTRON CORRELATIONS IN LOW-DENSITY NUCLEAR MATTER
1 DI-NEUTRON CORRELATIONS IN LOW-DENSITY NUCLEAR MATTER B. Y. SUN School of Nuclear Science and Technology, Lanzhou University, Lanzhou, 730000, People s Republic of China E-mail: sunby@lzu.edu.cn Based
FYS3510 Subatomic Physics. Exam 2016
FYS3510 Subatomic Physics VS 2015 Farid Ould-Saada Exam 2016 In addition to the items marked in blue, don t forget all examples and related material given in the slides, including the ones presented during