Spectroscopic overlaps between states in 16 C and 15 C IV (with WBT and NuShell)

Nuclear structure and stellar weak interaction rates of nuclei below the 132 Sn core

Nuclear structure and stellar weak interaction rates of nuclei below the 132 Sn core Nuclear and Atomic Physics Division, Saha Institute of Nuclear Physics, Kolkata 700064, INDIA E-mail: maitrayee.sahasarkar@saha.ac.in

Statistical Theory for the Beta-Delayed Neutron and Gamma-Ray Emission

Statistical Theory for the Beta-Delayed Neutron and Gamma-Ray Emission T. Kawano, P Möller Theoretical Division, Los Alamos National Laboratory LA-UR-13-21895 Slide 1 Combining QRPA Calculation and Statistical

Evidence for an l = 0 ground state in 9 He

26 April 2001 Physics Letters B 505 (2001) 21 26 www.elsevier.nl/locate/npe Evidence for an l = 0 ground state in 9 He L. Chen a,b,b.blank a,1,b.a.brown a,b,m.chartier a,c,1,a.galonsky a,b, P.G. Hansen

Structure of neutron-rich Mg isotopes explored by beta-decay of spin-polarized Na isotopes

Structure of neutron-rich Mg isotopes explored by beta-decay of spin-polarized Na isotopes K. Tajiri, T. Shimoda, K. Kura, M. Kazato, M. Suga, A. Takashima, T. Masue, T. Hori, T. Suzuki, T. Fukuchi, A.

Physics Letters B 695 (2011) Contents lists available at ScienceDirect. Physics Letters B.

Physics Letters B 695 (2011) 507 511 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Configuration interactions constrained by energy density functionals B.

Alpha decay. Introduction to Nuclear Science. Simon Fraser University Spring NUCS 342 February 21, 2011

Alpha decay Introduction to Nuclear Science Simon Fraser University Spring 2011 NUCS 342 February 21, 2011 NUCS 342 (Lecture 13) February 21, 2011 1 / 27 Outline 1 The Geiger-Nuttall law NUCS 342 (Lecture

Robert Charity Washington University in St. Louis, USA. Rewriting Nuclear Physics Textbooks 30 years with radioactive Ion Beam Physics

Resonance phenomena: from compound nucleus decay to proton radioactivity Robert Charity Washington University in St. Louis, USA Rewriting Nuclear Physics Textbooks 30 years with radioactive Ion Beam Physics

Theoretical Analysis of Neutron Double-Differential Cross Section of n + 19 F at 14.2 MeV

Commun. Theor. Phys. (Beijing, China) 47 (2007) pp. 102 106 c International Academic Publishers Vol. 47, No. 1, January 15, 2007 Theoretical Analysis of Neutron Double-Differential Cross Section of n +

2 Give the compound nucleus resulting from 6-MeV protons bombarding a target of. my notes in the part 3 reading room or on the WEB.

Lecture 15 Krane Enge Cohen Williams Reaction theories compound nucleus 11.10 13.7 13.1-3 direct reactions 11.11 13.11/12 ch 14 Admixed Wave functions residual interaction 5.1-4 Admixed Wave functions

PRAMANA c Indian Academy of Sciences Vol. 85, No. 3 journal of September 2015 physics pp

PRAMANA c Indian Academy of Sciences Vol. 85, No. 3 journal of September 2015 physics pp. 03 13 136 Sn and three-body forces M SAHA SARKAR 1, and S SARKAR 2 1 Saha Institute of Nuclear Physics, Bidhan

Semi-Classical perturbation theory Coulomb only First-order most used

direct reactions Models for breakup Semi-Classical perturbation theory Coulomb only First-order most used TDSE (Time Dependent Schrodinger Equation) Coulomb + Nuclear Semi-classical orbit needed DWBA (Distorted

Physics of neutron-rich nuclei

Physics of neutron-rich nuclei Nuclear Physics: developed for stable nuclei (until the mid 1980 s) saturation, radii, binding energy, magic numbers and independent particle. Physics of neutron-rich nuclei

Probing the shell model using nucleon knockout reactions

Probing the shell model using nucleon knockout reactions J A Tostevin Department of Physics, School of Electronics and Physical Sciences, University of Surrey, Guildford GU2 7XH, United Kingdom, and Graduate

Charge exchange reactions and photo-nuclear reactions

Charge exchange reactions and photo-nuclear reactions σ( 7 Li, 7 Be) and σ(γ,n) S. Nakayama (Univ of Tokushima) Determination of σ(γ,n) from CE reactions (CE reaction = Charge Exchange reaction) Application

Structure of Sn isotopes beyond N =82

Structure of Sn isotopes beyond N =8 L. Coraggio, A. Covello, A. Gargano, and N. Itaco Dipartimento di Scienze Fisiche, Università di Napoli Federico II, and Istituto Nazionale di Fisica Nucleare, Complesso

Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia

Commun. Theor. Phys. (Beijing, China) 43 (005) pp. 709 718 c International Academic Publishers Vol. 43, No. 4, April 15, 005 Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia

Resonant Reactions direct reactions:

Resonant Reactions The energy range that could be populated in the compound nucleus by capture of the incoming projectile by the target nucleus is for direct reactions: for neutron induced reactions: roughly

Interaction cross sections for light neutron-rich nuclei

PHYSICAL REVIEW C, VOLUME 65, 014612 Interaction cross sections for light neutron-rich nuclei B. A. Brown and S. Typel Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory,

Centrifugal Barrier Effects and Determination of Interaction Radius

Commun. Theor. Phys. 61 (2014) 89 94 Vol. 61, No. 1, January 1, 2014 Centrifugal Barrier Effects and Determination of Interaction Radius WU Ning ( Û) Institute of High Energy Physics, P.O. Box 918-1, Beijing

Nuclear Physics (13 th lecture)

uclear Physics ( th lecture) Cross sections of special neutron-induced reactions UCLR FISSIO Mechanism and characteristics of nuclear fission. o The fission process o Mass distribution of the fragments

Direct reactions methodologies for use at fragmentation beam energies

1 Direct reactions methodologies for use at fragmentation beam energies TU Munich, February 14 th 2008 Jeff Tostevin, Department of Physics Faculty of Engineering and Physical Sciences University of Surrey,

STRUCTURE FEATURES REVEALED FROM THE TWO NEUTRON SEPARATION ENERGIES

NUCLEAR PHYSICS STRUCTURE FEATURES REVEALED FROM THE TWO NEUTRON SEPARATION ENERGIES SABINA ANGHEL 1, GHEORGHE CATA-DANIL 1,2, NICOLAE VICTOR AMFIR 2 1 University POLITEHNICA of Bucharest, 313 Splaiul

Part II Particle and Nuclear Physics Examples Sheet 4

Part II Particle and Nuclear Physics Examples Sheet 4 T. Potter Lent/Easter Terms 018 Basic Nuclear Properties 8. (B) The Semi-Empirical mass formula (SEMF) for nuclear masses may be written in the form

Central density. Consider nuclear charge density. Frois & Papanicolas, Ann. Rev. Nucl. Part. Sci. 37, 133 (1987) QMPT 540

Central density Consider nuclear charge density Frois & Papanicolas, Ann. Rev. Nucl. Part. Sci. 37, 133 (1987) Central density (A/Z* charge density) about the same for nuclei heavier than 16 O, corresponding

Lecture 14 Krane Enge Cohen Williams Nuclear Reactions Ch 11 Ch 13 Ch /2 7.5 Reaction dynamics /4 Reaction cross sections 11.

Lecture 14 Krane Enge Cohen Williams Nuclear Reactions Ch 11 Ch 13 Ch 13 7.1/2 7.5 Reaction dynamics 11.2 13.2 7.3/4 Reaction cross sections 11.4 2.10 Reaction theories compound nucleus 11.10 13.7 13.1-3

Chapter VIII: Nuclear fission

Chapter VIII: Nuclear fission 1 Summary 1. General remarks 2. Spontaneous and induced fissions 3. Nucleus deformation 4. Mass distribution of fragments 5. Number of emitted electrons 6. Radioactive decay

Nuclear Science Seminar (NSS)

Nuclear Science Seminar (NSS) Nov.13, 2006 Weakly-bound and positive-energy neutrons in the structure of drip-line nuclei - from spherical to deformed nuclei 6. Weakly-bound and positive-energy neutrons

The astrophysical reaction 8 Li(n,γ) 9 Li from measurements by reverse kinematics

J. Phys. G: Nucl. Part. Phys. 25 (1999) 1959 1963. Printed in the UK PII: S0954-3899(99)00382-5 The astrophysical reaction 8 Li(n,γ) 9 Li from measurements by reverse kinematics Carlos A Bertulani Instituto

Lowest excited states of 13 O

PHYSICAL REVIEW C 75, 2467 (27) Lowest excited states of 13 O B. B. Skorodumov, 1,* G. V. Rogachev, 2 P. Boutachkov, 1 A. Aprahamian, 1 V. Z. Goldberg, 3 A. Mukhamedzhanov, 3 S. Almaraz, 1 H. Amro, 4 F.

arxiv:nucl-th/ v1 14 Nov 2005

Nuclear isomers: structures and applications Yang Sun, Michael Wiescher, Ani Aprahamian and Jacob Fisker Department of Physics and Joint Institute for Nuclear Astrophysics, University of Notre Dame, Notre

Quantum Theory of Many-Particle Systems, Phys. 540

Quantum Theory of Many-Particle Systems, Phys. 540 Questions about organization Second quantization Questions about last class? Comments? Similar strategy N-particles Consider Two-body operators in Fock

Compound Nucleus Reactions

Compound Nucleus Reactions E CM a Q CN Direct CN decays Time. Energy. Two-step reaction. CN forgets how it was formed. Decay of CN depends on statistical factors that are functions of E x, J. Low energy

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics PHY-30 Dr. E. Rizvi Lecture 5 - Quantum Statistics & Kinematics Nuclear Reaction Types Nuclear reactions are often written as: a+x Y+b for accelerated projectile a colliding

Measurements of B(E2) transition rates in neutron rich carbon isotopes, 16 C- 20 C.

Measurements of B(E2) transition rates in neutron rich carbon isotopes, 16 C- 20 C. Paul Fallon Lawrence Berkeley National Laboratory Marina Petri, R. M. Clark, M. Cromaz, S. Gros, H. B. Jeppesen, I-Y.

Exotic Nuclei. Ingo Wiedenhöver, National Nuclear Physics Summer School 7/16/2007 Tallahassee, Florida

Exotic Nuclei Outline Shell Structure Collective Structure: Experimental methods: Coulomb excitation Knockout reactions Magic Numbers in exotic nuclei New modes of collectivity? Ingo Wiedenhöver, National

Isoscaling, isobaric yield ratio and the symmetry energy: interpretation of the results with SMM

Isoscaling, isobaric yield ratio and the symmetry energy: interpretation of the results with SMM P. Marini, A. Botvina, A. Bonasera, Z. Kohley, L. W. May, R. Tripathi, S. Wuenschel, and S. J. Yennello

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

Spectroscopy of Single-Particle States in Oxygen Isotopes via (p, 2p) Reaction

Spectroscopy of Single-Particle States in Oxygen Isotopes via (p, 2p) Reaction Shoichiro KAWASE Center for Nuclear Study, the University of Tokyo (p,2p) reaction as a spectroscopic tool Simple reaction

Nuclear structure input for rp-process rate calculations in the sd shell

Nuclear structure input for rp-process rate calculations in the sd shell W A RICHTER ITHEMBA LABS UNIVERSITY OF THE WESTERN CAPE B A BROWN NSCL, MICHIGAN STATE UNIVERSITY This work is supported by the

Physics 102: Lecture 26. X-rays. Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1

Physics 102: Lecture 26 X-rays Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1 X-Rays Photons with energy in approx range 100eV to 100,000eV. This large energy means they

Surrogate reactions: the Weisskopf-Ewing approximation and its limitations

International Conference on Nuclear Data for Science and Technology 2007 DOI: 10.1051/ndata:07537 Invited Surrogate reactions: the Weisskopf-Ewing approximation and its limitations J. Escher 1,a, L.A.

The many facets of breakup reactions with exotic beams

Angela Bonaccorso The many facets of breakup reactions with exotic beams G Blanchon, DM Brink, F Carstoiu, A Garcia-Camacho, R Kumar, JMargueron, N Vinh Mau JAPAN-ITALY EFES Workshop on Correlations in

KNOCKOUT REACTIONS WITH RARE-ISOTOPE BEAMS

KNOCKOUT REACTIONS WITH RARE-ISOTOPE BEAMS Spectroscopic factors and single-particle (unit) cross sections Single-nucleon knockout: Bound and continuum states Two-nucleon knockout: A new direct reaction

Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy.

Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy Hiroshi Watanabe Outline Prospects for decay spectroscopy of neutron-rich

Introduction to Nuclear Science

Introduction to Nuclear Science PIXIE-PAN Summer Science Program University of Notre Dame 2006 Tony Hyder, Professor of Physics Topics we will discuss Ground-state properties of the nucleus Radioactivity

Determining Compound-Nuclear Reaction Cross Sections via Surrogate Reactions: Approximation Schemes for (n,f) Reactions

Determining Compound-Nuclear Reaction Cross Sections via Surrogate Reactions: Approximation Schemes for (n,f) Reactions Jutta E. Escher and Frank S. Dietrich Lawrence Livermore National Laboratory P.O.

Quantum mechanics of many-fermion systems

Quantum mechanics of many-fermion systems Kouichi Hagino Tohoku University, Sendai, Japan 1. Identical particles: Fermions and Bosons 2. Simple examples: systems with two identical particles 3. Pauli principle

SURROGATE REACTIONS. An overview of papers by Jason Burke from LLNL

SURROGATE REACTIONS An overview of papers by Jason Burke from LLNL Compound Nuclear Reaction cross sections Cross sections for compound-nuclear reactions are required input for astrophysical models and

SPIN-PARITIES AND HALF LIVES OF 257 No AND ITS α-decay DAUGHTER 253 Fm

NUCLEAR PHYSICS SPIN-PARITIES AND HALF LIVES OF 5 No AND ITS α-decay DAUGHTER 5 Fm P. ROY CHOWDHURY, D. N. BASU Saha Institute of Nuclear Physics, Variable Energy Cyclotron Centre, /AF Bidhan Nagar, Kolkata

Statistical Approach to Nuclear Level Density

Statistical Approach to Nuclear Level Density R. A. Sen kov,v.g.zelevinsky and M. Horoi Department of Physics, Central Michigan University, Mount Pleasant, MI 889, USA Department of Physics and Astronomy

Pairing and ( 9 2 )n configuration in nuclei in the 208 Pb region

Pairing and ( 9 2 )n configuration in nuclei in the 208 Pb region M. Stepanov 1, L. Imasheva 1, B. Ishkhanov 1,2, and T. Tretyakova 2, 1 Faculty of Physics, Lomonosov Moscow State University, Moscow, 119991

Shape coexistence and beta decay in proton-rich A~70 nuclei within beyond-mean-field approach

Shape coexistence and beta decay in proton-rich A~ nuclei within beyond-mean-field approach A. PETROVICI Horia Hulubei National Institute for Physics and Nuclear Engineering, Bucharest, Romania Outline

Chapter VI: Beta decay

Chapter VI: Beta decay 1 Summary 1. General principles 2. Energy release in decay 3. Fermi theory of decay 4. Selections rules 5. Electron capture decay 6. Other decays 2 General principles (1) The decay

Down and Up Along the Proton Dripline Proton Radioactivity Centrifugal (l=5) ) V 20 Coulomb Me( Radius (fm) Nuclear

V (MeV) V (MeV) Michael Thoennessen, Physics, August -17, 02 Down and U Along the Proton Driline Proton Radioactivity Heavy ne-proton Emitter Light ne-proton Emitter Light Two-Proton Emitter Heavy Two

Radioactivity at the limits of nuclear existence

Radioactivity at the limits of nuclear existence Zenon Janas Institute of Experimental Physics University of Warsaw Chart of nuclei - stable - β + - β - - α - fission - p p and 2p radioactivty proton radioactivity

Stability of heavy elements against alpha and cluster radioactivity

CHAPTER III Stability of heavy elements against alpha and cluster radioactivity The stability of heavy and super heavy elements via alpha and cluster decay for the isotopes in the heavy region is discussed

Beta-delayed neutron emission: New experimental study of angular properties.

Beta-delayed neutron emission: New experimental study of angular properties. N. J. Stone Russbach Winter School March 2014 (with acknowledgements to Robert Grzywacz and Jirina Stone) Outline History First

Decay studies of 170,171 Au, Hg, and 176 Tl

PHYSICAL REVIEW C 69, 054323 (2004) Decay studies of 170,171 Au, 171 173 Hg, and 176 Tl H. Kettunen, T. Enqvist, T. Grahn, P. T. Greenlees, P. Jones, R. Julin, S. Juutinen, A. Keenan, P. Kuusiniemi, M.

Charge density distributions and charge form factors of some even-a p-shell nuclei

International Journal of ChemTech Research CODEN (USA): IJCRGG, ISSN: 974-49, ISSN(Online):455-9555 Vol.1 No.6, pp 956-963, 17 Charge density distributions and charge form factors of some even-a p-shell

Calculations of Compound Nucleus Spin-Parity Distributions Populated via the (p,t) Reaction in Support of Surrogate Neutron Capture Measurements

Calculations of Compound Nucleus Spin-Parity Distributions Populated via the (p,t) Reaction in Support of Surrogate Neutron Capture Measurements J.Benstead 1,2,a, J.A.Tostevin 2, J.E.Escher 3, J.T.Burke

[2] State in what form the energy is released in such a reaction.... [1]

(a) The following nuclear reaction occurs when a slow-moving neutron is absorbed by an isotope of uranium-35. 0n + 35 9 U 4 56 Ba + 9 36Kr + 3 0 n Explain how this reaction is able to produce energy....

BETA-RAY SPECTROMETER

14 Sep 07 β-ray.1 BETA-RAY SPECTROMETER In this experiment, a 180, constant-radius magnetic spectrometer consisting of an electromagnet with a Geiger-Muller detector, will be used to detect and analyze

Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation August Introduction to Nuclear Physics - 2

2358-20 Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation 6-17 August 2012 Introduction to Nuclear Physics - 2 P. Van Isacker GANIL, Grand Accelerateur National d'ions Lourds

Bogdan Fornal. Institute of Nuclear Physics, Polish Academy of Sciences Krakow, Poland

Bogdan Fornal Institute of Nuclear Physics, Polish Academy of Sciences Krakow, Poland Collaboration: IFJ PAN Krakow - ANL Argonne - ANU Canberra The Nuclear Structure Workshop at the Weizmann Institute,

More Energetics of Alpha Decay The energy released in decay, Q, is determined by the difference in mass of the parent nucleus and the decay products, which include the daughter nucleus and the particle.

The IC electrons are mono-energetic. Their kinetic energy is equal to the energy of the transition minus the binding energy of the electron.

1 Lecture 3 Nuclear Decay modes, Nuclear Sizes, shapes, and the Liquid drop model Introduction to Decay modes (continued) Gamma Decay Electromagnetic radiation corresponding to transition of nucleus from

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics PHY-302 Dr. E. Rizvi Lecture 13 - Gamma Radiation Material For This Lecture Gamma decay: Definition Quantum interpretation Uses of gamma spectroscopy 2 Turn to γ decay

Neutrino-nucleus reactions on 12 Cand 16 O. Abstract

Neutrino-nucleus reactions on 12 Cand 16 O N. Auerbach 1,N.VanGiai 2 and O.K. Vorov 1 1 School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel 2 Division de Physique Théorique, Institut

Properties of Nuclei deduced from the Nuclear Mass

Properties of Nuclei deduced from the Nuclear Mass -the 2nd lecture- @Milano March 16-20, 2015 Yoshitaka Fujita Osaka University Image of Nuclei Our simple image for Nuclei!? Nuclear Physics by Bohr and

SECTION A Quantum Physics and Atom Models

AP Physics Multiple Choice Practice Modern Physics SECTION A Quantum Physics and Atom Models 1. Light of a single frequency falls on a photoelectric material but no electrons are emitted. Electrons may

Investigation of the Nuclear Structure for Some p-shell Nuclei by Harmonic Oscillator and Woods-Saxon Potentials

Investigation of the Nuclear Structure for Some p-shell Nuclei by Harmonic Oscillator and Woods-Saxon Potentials Ahmed N. Abdullah Department of Physics, College of Science, University of Baghdad, Baghdad-Iraq.

Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

The Bohr Atom Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. What is the energy of the emitted photon when an electron drops from the third

Alpha decay, ssion, and nuclear reactions

Alpha decay, ssion, and nuclear reactions March 11, 2002 1 Energy release in alpha-decay ² Consider a nucleus which is stable against decay by proton or neutron emission { the least bound nucleon still

Monte Carlo Simulation for Statistical Decay of Compound Nucleus

CNR20, Prague, Czech Republic, Sep. 9 23, 20 Monte Carlo Simulation for Statistical Decay of Compound Nucleus T. Kawano, P. Talou, M.B Chadwick Los Alamos National Laboratory Compound Nuclear Reaction,

General Physics (PHY 2140)

General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics Radioactivity Nuclear reactions http://www.physics.wayne.edu/~apetrov/phy2140/ Chapter 29 1 Lightning Review Last lecture: 1. Nuclear

Radioactivity and energy levels

Radioactivity and energy levels Book page 497-503 Review of radioactivity β ; Free neutron proton β- decay is continuous β : Proton in nucleus neutron antineutrino neutrino Summary of useful equations

Physics 102: Lecture 26. X-rays. Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1

Physics 102: Lecture 26 X-rays Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1 But first a quick review of the periodic table http://www.youtube.com/watch?v=smwlzwgmmwc

The liquid drop model

The liquid drop model Introduction to Nuclear Science Simon Fraser University Spring 2011 NUCS 342 January 10, 2011 NUCS 342 (Tutorial 0) January 10, 2011 1 / 33 Outline 1 Total binding energy NUCS 342

Introduction to Nuclear Physics Physics 124 Solution Set 4

Introduction to Nuclear Physics Physics 14 Solution Set 4 J.T. Burke January 3, 000 1 Problem 14 In making a back of the envelope calculation we must simplify the existing theory and make appropriate assumptions.

Nuclear Shell Model. Experimental evidences for the existence of magic numbers;

Nuclear Shell Model It has been found that the nuclei with proton number or neutron number equal to certain numbers 2,8,20,28,50,82 and 126 behave in a different manner when compared to other nuclei having

FINAL-STATE INTERACTIONS IN QUASIELASTIC ELECTRON AND NEUTRINO-NUCLEUS SCATTERING: THE RELATIVISTIC GREEN S FUNCTION MODEL

FINAL-STATE INTERACTIONS IN QUASIELASTIC ELECTRON AND NEUTRINO-NUCLEUS SCATTERING: THE RELATIVISTIC GREEN S FUNCTION MODEL Carlotta Giusti and Andrea Meucci Università and INFN, Pavia Neutrino-Nucleus

arxiv: v2 [nucl-th] 28 Aug 2014

Pigmy resonance in monopole response of neutron-rich Ni isotopes? Ikuko Hamamoto 1,2 and Hiroyuki Sagawa 1,3 1 Riken Nishina Center, Wako, Saitama 351-0198, Japan 2 Division of Mathematical Physics, arxiv:1408.6007v2

Atomic and nuclear physics

Chapter 4 Atomic and nuclear physics INTRODUCTION: The technologies used in nuclear medicine for diagnostic imaging have evolved over the last century, starting with Röntgen s discovery of X rays and Becquerel

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

EXPERIMENTAL METHODS

S. H. Liu, 1 J. H. Hamilton, 1 A. V. Ramayya, 1 A. Covello, 2 A. Gargano, 2 N. Itaco, 2 Y. X. Luo, 1,3 J. O. Rasmussen, 3 S. J. Zhu, 4 J. K. Hwang, 1 A.V.Daniel, 1,5 G.M.Ter-Akopian, 5 Y. Oganessian 5,

α particles, β particles, and γ rays. Measurements of the energy of the nuclear

.101 Applied Nuclear Physics (Fall 004) Lecture (1/1/04) Nuclear ecays References: W. E. Meyerhof, Elements of Nuclear Physics (McGraw-Hill, New York, 1967), Chap 4. A nucleus in an excited state is unstable

1p1/2 0d5/2. 2s1/2-0.2 Constant Bound Wave Harmonic Oscillator Bound Wave Woods-Saxon Bound Wave Radius [fm]

Development of the Multistep Compound Process Calculation Code Toshihiko KWNO Energy Conversion Engineering, Kyushu University 6- Kasuga-kouen, Kasuga 86, Japan e-mail: kawano@ence.kyushu-u.ac.jp program

Many-Body Resonances of Nuclear Cluster Systems and Unstable Nuclei

Many-Body Resonances of Nuclear Cluster Systems and Unstable Nuclei Contents of the lecture 1. Resonances and complex scaling method 2. Many-body resonances of He-isotopes and their mirror nuclei 3. Coulomb

Theory and Calculation of Two-nucleon Transfer Reactions

Theory and Calculation of Two-nucleon Transfer Reactions Ian Thompson Nuclear Theory and Modeling, L-414, P. O. Box 808, Livermore, CA 94551! This work performed under the auspices of the U.S. Department

The Nuclear Many-Body problem. Lecture 3

The Nuclear Many-Body problem Lecture 3 Emergent phenomena at the drip lines. How do properties of nuclei change as we move towards the nuclear driplines? Many-body open quantum systems. Unification of

PHY492: Nuclear & Particle Physics. Lecture 6 Models of the Nucleus Liquid Drop, Fermi Gas, Shell

PHY492: Nuclear & Particle Physics Lecture 6 Models of the Nucleus Liquid Drop, Fermi Gas, Shell Liquid drop model Five terms (+ means weaker binding) in a prediction of the B.E. r ~A 1/3, Binding is short

Cross Sections of Gadolinium Isotopes in Neutron Transmission Simulated Experiments with Low Energy Neutrons up to 100 ev

Cross Sections of Gadolinium Isotopes in Neutron Transmission Simulated Experiments with Low Energy Neutrons up to 100 ev C. Oprea, A. Oprea Joint Institute for Nuclear Research (JINR) Frank Laboratory

arxiv: v1 [nucl-th] 7 Nov 2018

Matrix Model With a Phase Transition Arun Kingan and Larry Zamick Department of Physics and Astronomy Rutgers University, Piscataway, New Jersey 08854 arxiv:1811.02562v1 [nucl-th] 7 Nov 2018 November 8,

BETA DECAY. Q = m x m y. Q = m x m y 2m e. + decay, a. + Decay : X! Y e

BETA DECAY In -decay processes, the mass number A is constant, but the proton and neutron numbers change as the parent decays to a daughter that is better bound with lower mass. In decay, a neutron transforms

Some (more) High(ish)-Spin Nuclear Structure. Lecture 2 Low-energy Collective Modes and Electromagnetic Decays in Nuclei

Some (more) High(ish)-Spin Nuclear Structure Lecture 2 Low-energy Collective Modes and Electromagnetic Decays in Nuclei Paddy Regan Department of Physics Univesity of Surrey Guildford, UK p.regan@surrey.ac.uk

An α decay is a nuclear transformation in which a nucleus reduces its energy by emitting an α-particle. Z 2 X N He 2, A X X + α.

Chapter 14 α Decay Note to students and other readers: This Chapter is intended to supplement Chapter 8 of Krane s excellent book, Introductory Nuclear Physics. Kindly read the relevant sections in Krane

Bohr s Correspondence Principle

Bohr s Correspondence Principle In limit that n, quantum mechanics must agree with classical physics E photon = 13.6 ev 1 n f n 1 i = hf photon In this limit, n i n f, and then f photon electron s frequency

I. 1. Nuclear Structure Study of 50 Mn by Charge-exchange (p,n) Reaction on 50 Cr

CYRIC Annual Report 2002 I. 1. Nuclear Structure Study of 50 Mn by Charge-exchange (p,n) Reaction on 50 Cr Kamurai G., Orihara H., Terakawa A., Yamamoto A., Suzuki H., Mizuno H., Kikuchi Y., Kumagai K.,

Beta and gamma decays

Beta and gamma decays April 9, 2002 Simple Fermi theory of beta decay ² Beta decay is one of the most easily found kinds of radioactivity. As we have seen, this result of the weak interaction leads to

Density dependence of the symmetry energy and the nuclear equation of state : A dynamical and statistical model perspective

Density dependence of the symmetry energy and the nuclear equation of state : A dynamical and statistical model perspective D. V. Shetty, S. J. Yennello, and G. A. Souliotis The density dependence of the