Three-Nucleon dynamics With BINA detector
|
|
|
- Roger Gilbert
- 5 years ago
- Views:
Transcription
1 INTERNATIONAL PHD PROJECTS IN APPLIED NUCLEAR PHYSICS AND INNOVATIVE TECHNOLOGIES This project is supported by the Foundation for Polish Science MPD program, co-financed by the European Union within the European Regional Development Fund Three-Nucleon dynamics With BINA detector By: Ghanshyam Khatri Supervisors: Prof. Stanisław Kistryn, (Jagiellonian University, Poland) Prof. Nasser Kalantar-Nayestanaki, (KVI & University of Groningen, The Netherlands) 22 May, 2012 PhD Jagiellonian University
2 Self Intro 2
3 Self Intro from a small city SURAT, not far from Mumbai! 3
4 Self Intro from a small city SURAT, not far from Mumbai! Before coming to UJ : 2007, B.Sc. - Navyug Sci. College (VNSGU) 2007, May-July, Summer BARC-Mumbai , Sci. Asst. Inst. for Plasma Research, India , Joint-European Master in Nuclear Ghent University, Belgium Nancy University, France Royal Institute of Technology, Sweden 2010-present 4
5 Outline Introduction Three-body(3N) dynamics BINA Detector Present and Future Summary 5
6 Introduction How many known forces in Nature? 1. Gravity (Newton s apple) 2. Electromagnetic (Sun light) 3. Weak Nuclear (Fukushima & Chernobyl) 4. Strong Nuclear (Reactor & Bombs) 6
7 Introduction How many known forces in Nature? 1. Gravity (Newton s apple) 2. Electromagnetic (Sun light) 3. Weak Nuclear (Fukushima & Chernobyl) 4. Strong Nuclear (Reactor & Bombs) 7
8 Photo Credit: Science Photo Library Introduction How many known forces in Nature? 1. Gravity (Newton s apple) 2. Electromagnetic (Sun light) 3. Weak Nuclear (Fukushima & Chernobyl) 4. Strong Nuclear (Reactor & Bombs) 1935 (Yukawa-theory): Meson exchange between two nucleon 8
9 Photo Credit : Wikipedia Photo Credit: Science Photo Library Introduction How many known forces in Nature? 1. Gravity (Newton s apple) 2. Electromagnetic (Sun light) 3. Weak Nuclear (Fukushima & Chernobyl) 4. Strong Nuclear (Reactor & Bombs) 1935 (Yukawa-theory): Meson exchange between two nucleon 1947 (Powell & his team ): Experimentally found Meson 9
10 Photo Credit : Wikipedia Photo Credit: Science Photo Library Introduction How many known forces in Nature? 1. Gravity (Newton s apple) 2. Electromagnetic (Sun light) 3. Weak Nuclear (Fukushima & Chernobyl) 4. Strong Nuclear (Reactor & Bombs) 1935 (Yukawa-theory): Meson exchange between two nucleon 1947 (Powell & his team ): Experimentally found Meson 10
11 Photo Credit : Wikipedia Photo Credit: Science Photo Library Introduction How many known forces in Nature? 1. Gravity (Newton s apple) 2. Electromagnetic (Sun light) 3. Weak Nuclear (Fukushima & Chernobyl) 4. Strong Nuclear (Reactor & Bombs) 1935 (Yukawa-theory): Meson exchange between two nucleon 1947 (Powell & his team ): Experimentally found Meson Smoking Meson??? 11
12 Introduction today after almost 6 decades! Modern phenomenological/meson exchange NN potentials: Nijmegen I Nijmegen II CD-Bonn Argonne V18 12
13 Introduction today after almost 6 decades! Modern phenomenological/meson exchange NN potentials: Nijmegen I Nijmegen II CD-Bonn Argonne V18 are able to explain the Interaction between two nucleons accurately e.g. np- & nn-scattering, deuteron ( 2 H) properties... Experiment Theory np-scattering High precision data from Los Alamos W. P. Abfalterer et al., PRL 81, 57 (1998) 13
14 Introduction today after almost 6 decades! Modern phenomenological/meson exchange NN potentials: Nijmegen I Nijmegen II CD-Bonn Argonne V18 are able to explain the Interaction between two nucleons accurately e.g. np- & nn-scattering, deuteron ( 2 H) properties... Experiment Theory np-scattering High precision data from Los Alamos W. P. Abfalterer et al., PRL 81, 57 (1998) Most of the present NN-scattering data can be reproduced solely with 2NF models with χ 2 /datum ~ 1, but 14
15 Introduction but FAILS to describe larger system (A>2)!... Experiment Theory np-scattering High precision data from Los Alamos W. P. Abfalterer et al., PRL 81, 57 (1998) 15
16 Introduction but FAILS to describe larger system (A>2)!... Experiment Theory even for the simplest A=3 e.g. 3 H and 3 He.unable to reproduce the data nd-scattering Model Nijm I 7.72 Nijm II 7.62 AV Reid Exp Triton B.E. [MeV] H. Witala et al. PRL 81, 1183 (1998) St. Kistryn et al. PRC 68, (2003) np-scattering High precision data from Los Alamos W. P. Abfalterer et al., PRL 81, 57 (1998) 16
17 Introduction.a new notion: Three-Nucleon Force (3NF) + = ~ V 12 +V 23 +V 31 =V theory 3NF = V 123 3N System 17
18 Introduction.a new notion: Three-Nucleon Force (3NF) + = ~ V 12 +V 23 +V 31 =V theory 3NF = V 123 3N System.adding 3NF in original 2NF helps! Model 3 H [MeV] 4 He [MeV] 2NF NF +3NF Experiment additional 3NF CD-Bonn+TM99 AV18+Urbana XI H. Witala et al. PRL 81, 1183 (1998) St. Kistryn et al. PRC 68, (2003) 18
19 Introduction Ab-initio calculations for light nuclei (+3NF) 19
20 Introduction Ab-initio calculations for light nuclei (+3NF) 20
21 3N dynamics why he said like this? 21
22 3N dynamics Three-body forces in nature; example 22
23 3N dynamics Three-body forces in nature; example 23
24 3N dynamics Three-body forces in a NUCLEAR system! N N H 3 i1 N 2 3 2mi i j1 v ij 24
25 25 3N dynamics Three-body forces in a NUCLEAR system! N N N j i ij i i v m H V v m H j i ij i i
26 3N dynamics Hot-Spot to see 3NF: intermediate energies?! 26
27 3N dynamics Hot-Spot to see 3NF: intermediate energies?! 3NF contribution 27
28 3N dynamics Theoretical models Faddeev framework (based on pairwise N-N interactions) provides exact treatment for the 3N system also allows to include 3NF 28
29 3N dynamics Theoretical models Faddeev framework (based on pairwise N-N interactions) provides exact treatment for the 3N system also allows to include 3NF Calculations from: Prof. Witała and Prof. Glöckle Main 2NF Models -Nijmegen I & II -CD Bonn (Charge Dependant) -Argonne V18-29
30 3N dynamics Theoretical models Faddeev framework (based on pairwise N-N interactions) provides exact treatment for the 3N system also allows to include 3NF Calculations from: Prof. Witała and Prof. Glöckle Main 2NF Models -Nijmegen I & II -CD Bonn (Charge Dependant) -Argonne V Additional 3NF Models -Tucson Melbourne (TM99) -Urbana IX - Illinois (IL2) - 30
31 3N dynamics Theoretical models Faddeev framework (based on pairwise N-N interactions) provides exact treatment for the 3N system also allows to include 3NF Calculations from: Prof. Witała and Prof. Glöckle Main 2NF Models -Nijmegen I & II -CD Bonn (Charge Dependant) -Argonne V Additional 3NF Models -Tucson Melbourne (TM99) -Urbana IX - Illinois (IL2) - Other Approaches: Coupled Channels with Δ-isobar excitation (Prof. Deltuva, Portugal) Chiral Perturbation Theory (ChPT) only upto NNLO (Prof. Epelbaum, Germany) 31
32 pd elastic scattering cross sections 3N dynamics Models vs. Data p d p d K. Ermisch et al., PRC 68, (2003), PRC 71, (2005) 32
33 pd elastic scattering cross sections 3N dynamics Models vs. Data p d p d K. Ermisch et al., PRC 68, (2003), PRC 71, (2005) 33
34 pd elastic scattering cross sections 3N dynamics Models vs. Data p d p d K. Ermisch et al., PRC 68, (2003), PRC 71, (2005) 34
35 pd elastic scattering cross sections 3N dynamics Models vs. Data p d p d K. Ermisch et al., PRC 68, (2003), PRC 71, (2005) 35
36 pd elastic scattering cross sections 3N dynamics Models vs. Data p d p d K. Ermisch et al., PRC 68, (2003), PRC 71, (2005) 36
37 pd elastic scattering cross sections 3N dynamics Models vs. Data p d p d K. Ermisch et al., PRC 68, (2003), PRC 71, (2005) 37
38 3N dynamics Are we done? No! 38
39 3N dynamics Are we done? No! 3NFs helped to improve theories, but still some discrepancy remains Do we understand the exact form of 3NFs!!? Include other ingredients? Can we consider the validity through complete phase-space of 3N dynamics? Urgent need for systematic and High-Precision data-base Next steps: dp-breakup, 4N-system detailed root-map to the 3N-system 39
40 3N dynamics Are we done? No! 3NFs helped to improve theories, but still some discrepancy remains Do we understand the exact form of 3NFs!!? Include other ingredients? Can we consider the validity through complete phase-space of 3N dynamics? Urgent need for systematic and High-Precision data-base Next steps: dp-breakup, 4N-system detailed root-map to the 3N-system Are there effects other than 3NFs? Yes 40
41 3N dynamics Are we done? No! 3NFs helped to improve theories, but still some discrepancy remains Do we understand the exact form of 3NFs!!? Include other ingredients? Can we consider the validity through complete phase-space of 3N dynamics? Urgent need for systematic and High-Precision data-base Next steps: dp-breakup, 4N-system detailed root-map to the 3N-system Are there effects other than 3NFs? Yes Coulomb and Relativistic (but importance is limited in certain region of phase-space) Recently coulomb effect was included successfully in the calculations with coupled channel calculations! [Prof. Deltuva, Portugal] Relativistic effects, recent work!! 4NF? (ChPT predicts 2NF>>3NF>>4NF) 41
42 3N dynamics 42
43 3N dynamics 43
44 BINA Detector Big Instrument for Nuclear-polarization Analysis (a 4π detector) 44
45 BINA Detector Big Instrument for Nuclear-polarization Analysis (a 4π detector)
46 BINA Detector Big Instrument for Nuclear-polarization Analysis (a 4π detector) MWPC ΔE E 46
![BINA Detector Wall covers θ=10-35 + Ball covers θ=up to 165 4π Phase-Space 150 phoswich Scintillators =Target chamber (~10-5 mbar) Wire chamber (MWPC) Three planes X, Y & U [118x118x148 wires] Thin](/docs-images/88/115982384/images/47-0.jpg "scintillators for particle identification (ΔE -wall) [1.8x10.8x0.1 cm 3 ] MWPC: CF4(80%) + Isobutene(20%) gas-mixture 20µm diameter tungsten wire Beam Ball: Triangular fast scint.")
47 BINA Detector Wall covers θ= Ball covers θ=up to 165 4π Phase-Space 150 phoswich Scintillators =Target chamber (~10-5 mbar) Wire chamber (MWPC) Three planes X, Y & U [118x118x148 wires] Thin scintillators for particle identification (ΔE -wall) [1.8x10.8x0.1 cm 3 ] MWPC: CF4(80%) + Isobutene(20%) gas-mixture 20µm diameter tungsten wire Beam Ball: Triangular fast scint. and slow phoswitch parts connected to PMT s through lightguide Forward scintillators (E-wall) [9x12x220 cm 3 ] 47
48 BINA Detector Liquid Target Liquid Hydrogen (and Deuterium) thin transparent CH 2 foil 48
49 BINA Detector Liquid Target Liquid Hydrogen (and Deuterium) thin transparent CH 2 foil Very tricky to handle it 49
50 BINA Detector Liquid Target Liquid Hydrogen (and Deuterium) thin transparent CH 2 foil Very tricky to handle it Hydrogen and Deuterium (gas-liquid phase few Kelvin) Balancing gas pressure within mechanical-stress limit of the target foil Filling in steps: insert a little gas which can be handle by the target foil and then cool it down to liquid (sudden pressure drop), repeat it 50
51 BINA Detector Liquid Target Liquid Hydrogen (and Deuterium) thin transparent CH 2 foil Very tricky to handle it Hydrogen and Deuterium (gas-liquid phase few Kelvin) Balancing gas pressure within mechanical-stress limit of the target foil Filling in steps: insert a little gas which can be handle by the target foil and then cool it down to liquid (sudden pressure drop), repeat it KVI Record: I m the only - handled the target system without breaking! 51
52 Present & Future Present Future 52
53 Present & Future Present Data Analysis of dp and E d =160 MeV from the last Experiment with BINA Results Planed for Poster ENPC-2012, Bucharest 2012: Giving new life to BCC (Bronowice Cyclotron Center), Krakow Future 53
54 Present & Future Present Data Analysis of dp and E d =160 MeV from the last Experiment with BINA Results Planed for Poster ENPC-2012, Bucharest 2012: Giving new life to BCC (Bronowice Cyclotron Center), Krakow Future BINA@BCC; new experiments with proton beam up-to 250 MeV, BINA@BCC; construction of polarized targets?? WASA@COSY ; Experiment in Jan-2013 (may be polarized beam?) Extend the study to larger nucleon system (A>3), 4NF? Look for exclusive channels and other observables Fine-tuning of models with inclusion of additional components in the dynamics e.g. coulomb and relativistic effects, N3LO for ChPT, different meson-exchanges 54
55 Summary 3NF definitely improves models: we are in right direction! Looking for effects beyond 2NF+3NF : coulomb, Relativistic, 4NF BINA gets residence permit in Poland! Make systematic and high-precision database to validate the models 3NF Experiments at : KVI, RIKEN, RCNP, IUCF, Julich and and now BINA@BCC in Krakow 55
56 Thank you for your attention!!! 56
Three- and Four-Nucleon Dynamics at Intermediate Energies
Three- and Four-Nucleon Dynamics at Intermediate Energies By: Ghanshyam Khatri 05 June, 2013 G. Khatri, MPD Symposium, Kraków 1 \ 20 Outline Motivation 3N dynamics Experiment with BINA: present work -
Experimental Investigation of Few-Nucleon Dynamics at Medium Energies
Experimental Investigation of Few-Nucleon Dynamics at Medium Energies by Ghanshyam Khatri 1 \ 22 Outline Introduction Three-body (3N) force Experimental tools BINA Detector and it s status at CCB (Krakow)
What have we learned about three-nucleon systems at intermediate energies?
What have we learned about three-nucleon systems at intermediate energies? Nasser Kalantar-Nayestanaki Kernfysisch Versneller Instituut (KVI), Univ. Of Groningen International Symposium on New Facet of
The three-nucleon system as a laboratory for nuclear physics: the need for 3N forces
FZJ-IKP(TH)-2007-10 HISKP-TH-0707 The three-nucleon system as a laboratory for nuclear physics: the need for 3N forces N. Kalantar-Nayestanaki 1, and E. Epelbaum 2,3, 1 Kernfysisch Versneller Instituut
Modern Theory of Nuclear Forces
Evgeny Epelbaum PAX Meeting, Stockholm, 15.06.2010 Modern Theory of Nuclear Forces Evgeny Epelbaum, Ruhr-Universität Bochum Outline Chiral EFT for nuclear forces Some hot topics (work in progress) Deuteron
LORENTZ BOOSTED NUCLEON-NUCLEON T-MATRIX AND THE TRITON BINDING ENERGY
October 7, 28 22:52 WSPC/INSTRUCTION FILE Modern Physics Letters A c World Scientific Publishing Company LORENTZ BOOSTED NUCLEON-NUCLEON T-MATRIX AND THE TRITON BINDING ENERGY H. KAMADA Department of Physics,
The light nuclei spin structure from the hadronic interactions at intermediate energies
The light nuclei spin structure from the hadronic interactions at intermediate energies P.K. Kurilkin on behalf JINR-Japan collaboration Hadron 2011, June 13-17, München, Germany Collaboration Joint Institute
Modern Theory of Nuclear Forces
Evgeny Epelbaum, FZ Jülich & University Bonn Lacanau, 29.09.2009 Modern Theory of Nuclear Forces Lecture 1: Lecture 2: Lecture 3: Introduction & first look into ChPT EFTs for two nucleons Nuclear forces
Three-nucleon potentials in nuclear matter. Alessandro Lovato
Three-nucleon potentials in nuclear matter Alessandro Lovato PRC 83, 054003 (2011) arxiv:1109.5489 Outline Ab initio many body method Nuclear Hamiltonian: 2- and 3- body potentials Density dependent potential
Evgeny Epelbaum. Forschungszentrum Jülich & Universität Bonn
Evgeny Epelbaum KHuK Jahrestagung, GSI, 25.10.2007 Evgeny Epelbaum Forschungszentrum Jülich & Universität Bonn Outline Motivation & Introduction Few nucleons in chiral EFT: where do we stand Work in progress:
Calculations of three-nucleon reactions
Calculations of three-nucleon reactions H. Witała Jagiellonian University, Kraków in collaboration with: J. Golak, R. Skibiński, K. Topolnicki, Kraków H. Kamada, Kyushu Institute of Technology E. Epelbaum,
Light hypernuclei based on chiral and phenomenological interactions
Mitglied der Helmholtz-Gemeinschaft Light hypernuclei based on chiral and phenomenological interactions Andreas Nogga, Forschungszentrum Jülich International Conference on Hypernuclear and Strange Particle
Cross sections for neutron-deuteron elastic scattering in the energy range MeV
Cross sections for neutron-deuteron elastic scattering in the energy range 135 250 MeV The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters.
Dedicated Arrays: MEDEA GDR studies (E γ = MeV) Highly excited CN E*~ MeV, 4 T 8 MeV
Dedicated Arrays: MEDEA GDR studies (E γ = 10-25 MeV) Highly excited CN E*~ 250-350 MeV, 4 T 8 MeV γ-ray spectrum intermediate energy region 10 MeV/A E beam 100 MeV/A - large variety of emitted particles
H. Kamada, A. Nogga, and W. Glockle, Institute fur Theoretische Physik 11, Ruhr-Universitat Bochum, D-44780
J Title: RECENT PROGRESS N THE 3N SYSTEM NCLUDNG THREE-NUCLEON FORCES Author(s): D. Hueber, T-5, MS-B283, Theoretical Division, Los Alamos National Laboratory, P.O. Box 1663, Los Alamos, NM 87545, USA
Poincaré Invariant Three-Body Scattering
Poincaré Invariant Three-Body Scattering Ch. Elster T. Lin W. Polyzou, W. Glöckle 10/9/008 Supported by: U.S. DOE, OSC, NERSC A Few-Body Theorist s view of the Nuclear Chart Bound State: 3 H - 3 He Scattering:
Nuclear Forces - Lecture 6 -
Physics Department, Tohoku University, June 30 July 2, 2014 Nuclear Forces - Lecture 6 - Nuclear many-body forces from chiral EFT R. Machleidt University of Idaho 1 Nuclear Forces - Overview of all lectures
Nuclear structure I: Introduction and nuclear interactions
Nuclear structure I: Introduction and nuclear interactions Stefano Gandolfi Los Alamos National Laboratory (LANL) National Nuclear Physics Summer School Massachusetts Institute of Technology (MIT) July
Investigation of the light nuclei spin structure from hadronic channels at Nuclotron
Investigation of the light nuclei spin structure from hadronic channels at Nuclotron P.K. Kurilkin on behalf of DSS collaboration Baldin ISHEPP-XXII, September 15-20, 2014, Dubna, Russia Outline Introduction
First Order Relativistic Three-Body Scattering. Ch. Elster
First Order Relativistic Three-Body Scattering Ch. Elster T. Lin, W. Polyzou W. Glöcle 4//7 Supported by: U.S. DOE, NERSC,OSC Nucleons: Binding Energy of H NN Model E t [MeV] Nijm I -7.7 Nijm II -7.64
The theory of nuclear forces: Is the never-ending ending story coming to an end? R. Machleidt University of Idaho
The theory of nuclear forces: Is the never-ending ending story coming to an end? University of Idaho What s left to say? Put the recent progress into a wider perspective. Fill in some missing details.
The 7th Asia-Pacific Conference on Few-Body Problems in Physics. Dp breakup reaction investigation using polarized and unpolarized deuteron beam
The 7th Asia-Pacific Conference on Few-Body Problems in Physics Dp breakup reaction investigation using polarized and unpolarized deuteron beam M. Janek on behalf of DSS collaboration (Russia-Japan-JINR-Romania-Bulgaria-Slovakia)
Nuclear structure from chiral-perturbation-theory two- plus three-nucleon interactions
Nuclear structure from chiral-perturbation-theory two- plus three-nucleon interactions Petr Navratil Lawrence Livermore National Laboratory* Collaborators: W. E. Ormand (LLNL), J. P. Vary (ISU), E. Caurier
THREE-BODY FORCE EFFECTS IN NEUTRON-DEUTERON SCATTERING AT 95 MeV
MENU 2007 11th InternationalC onference on M eson-nucleon Physics and the Structure ofthe Nucleon Septem ber10-14,2007 IKP,Forschungzentrum Jülich,Germ any THREE-BODY FORCE EFFECTS IN NEUTRON-DEUTERON
RG & EFT for nuclear forces
RG & EFT for nuclear forces Andreas Nogga, Forschungszentrum Jülich ECT* school, Feb/March 2006 Low momentum interactions: Using the RG to simplify the nuclear force for many-body calculations. Application
Spin structure of 3 He studied by deuteron and nucleon knockout processes
Spin structure of 3 He studied by deuteron and nucleon knockout processes S. Širca, U. of Ljubljana, Slovenia Electron-Nucleus Scattering XIII Marciana Marina, Isola d Elba 25 June 2014 1 Experiments covered
The nucleon-nucleon system in chiral effective theory
The nucleon-nucleon system in chiral effective theory Daniel Phillips Ohio University Research supported by the US Department of Energy Plan χet for nuclear forces: the proposal Leading order for S waves
ISOSPIN RESOLVED DOUBLE PION PRODUCTION AT CELSIUS
Vol. 29 (1998) ACTA PHYSICA POLONICA B No 11 ISOSPIN RESOLVED DOUBLE PION PRODUCTION AT CELSIUS M. Andersson a, Chr. Bargholtz a, E. Fumero a, K. Fransson a L. Holmberg a, K. Lindh a, L. Mårtensson a,
Quantum Monte Carlo calculations of medium mass nuclei
Quantum Monte Carlo calculations of medium mass nuclei Diego Lonardoni FRIB Theory Fellow In collaboration with: J. Carlson, LANL S. Gandolfi, LANL X. Wang, Huzhou University, China A. Lovato, ANL & UniTN
hg: Chiral Structure of Few-Nucleon Systems
Chiral Structure of Few-Nucleon Systems H. W. Grießhammer Center for Nuclear Studies, The George Washington University, Washington DC, USA D. R. Phillips: Chiral Dynamics with πs, Ns and s Done. hg: Chiral
Nuclear Physics from Lattice Effective Field Theory
Nuclear Physics from Lattice Effective Field Theory Dean Lee (NCSU/Bonn) work done in collaboration with Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Ulf-G. Meißner (Bonn/Jülich) Buḡra Borasoy (now
Meson production in pd fusion to ³HeX
Meson production in pd fusion to ³HeX with WASA-at-COSY Nils Hüsken for the WASA-at-COSY Collaboration Westfälische Wilhelms-Universität Münster, Institut für Kernphysik 25th International Nuclear Physics
Ab initio lattice EFT from light to medium mass nuclei Nuclear Lattice EFT Collaboration
Ab initio lattice EFT from light to medium mass nuclei Nuclear Lattice EFT Collaboration Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Timo Lähde (Jülich) Dean Lee (NC State) Thomas Luu (Jülich/Bonn)
Novel NN interaction and the spectroscopy of light nuclei
Physics Letters B 621 (2005) 96 101 www.elsevier.com/locate/physletb Novel NN interaction and the spectroscopy of light nuclei A.M. Shirokov a,j.p.vary b, A.I. Mazur c,s.a.zaytsev c,t.a.weber b a Skobeltsyn
XXIII International Baldin Seminar on High Energy Physics Problems
XXIII International Baldin Seminar on High Energy Physics Problems INVESTIGATION OF REACTIONS USING POLARIZED AND UNPOLARIZED DEUTERON BEAM AT NUCLOTRON: CURRENT STATE AND PERSPECTIVES M. Janek on behalf
Chiral effective field theory on the lattice: Ab initio calculations of nuclei
Chiral effective field theory on the lattice: Ab initio calculations of nuclei Nuclear Lattice EFT Collaboration Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Timo Lähde (Jülich) Dean Lee (NC State)
Research Activities at the RCNP Cyclotron Facility
Research Activities at the RCNP Cyclotron Facility Kichiji Hatanaka Research Center for Nuclear Physics Osaka University International Symposium on Nuclear Physics in Asia Convention Center of Beihang
Nuclear physics around the unitarity limit
Nuclear physics around the unitarity limit Sebastian König Nuclear Theory Workshop TRIUMF, Vancouver, BC February 28, 2017 SK, H.W. Grießhammer, H.-W. Hammer, U. van Kolck, arxiv:1607.04623 [nucl-th] SK,
Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation August Experimental Nuclear Physics: Part 2
2358-11 Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation 6-17 August 2012 Experimental Nuclear Physics: Part 2 E. Ricard McCutchan Brookhaven National Lab. USA Experimental
Nuclear structure III: Nuclear and neutron matter. National Nuclear Physics Summer School Massachusetts Institute of Technology (MIT) July 18-29, 2016
Nuclear structure III: Nuclear and neutron matter Stefano Gandolfi Los Alamos National Laboratory (LANL) National Nuclear Physics Summer School Massachusetts Institute of Technology (MIT) July 18-29, 2016
arxiv:nucl-th/ v2 28 May 2002
The ff particle based on modern nuclear forces A. Nogga, H. Kamada,W.Glöckle 3, B.R. Barrett Department of Physics, University of Arizona, Tucson,Arizona 857, USA Department of Physics, Faculty of Engineering,
Quantum Monte Carlo calculations of neutron and nuclear matter
Quantum Monte Carlo calculations of neutron and nuclear matter Stefano Gandolfi Los Alamos National Laboratory (LANL) Advances and perspectives in computational nuclear physics, Hilton Waikoloa Village,
Citation for published version (APA): Martinus, G. H. (1998). Proton-proton bremsstrahlung in a relativistic covariant model s.n.
University of Groningen Proton-proton bremsstrahlung in a relativistic covariant model Martinus, Gerard Henk IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you
Author(s) Fujiwara, Yoshikazu; Fukukawa, Kenj. Citation Few-Body Systems (2013), 54(1-4): 4.
Title Nucleon Deuteron Breakup Differenti Derived from the Quark-Model NN Int Author(s) Fujiwara, Yoshikazu; Fukukawa, Kenj Citation Few-Body Systems (), (-): Issue Date - URL http://hdl.handle.net//699
arxiv: v1 [nucl-th] 23 Feb 2016
![arxiv: v1 [nucl-th] 23 Feb 2016](/thumbs/87/96519857.jpg "arxiv: v1 [nucl-th] 23 Feb 2016")
September 12, 2018 Threshold pion production in proton-proton collisions at NNLO in chiral EFT arxiv:1602.07333v1 [nucl-th] 23 Feb 2016 V. Baru, 1, 2 E. Epelbaum, 1 A. A. Filin, 1 C. Hanhart, 3 H. Krebs,
Few- and many-nucleon systems with semilocal coordinate-space regularized chiral nucleon-nucleon forces
Few- and many-nucleon systems with semilocal coordinate-space regularized chiral nucleon-nucleon forces S. Binder,, 2 A. Calci, 3 E. Epelbaum, 4 R.J. Furnstahl, 5 J. Golak, 6 K. Hebeler, 7 T. Hüther, 7
Theory Challenges for describing Nuclear Reactions
Theory Challenges for describing Nuclear Reactions Ch. Elster 06/20/2014 Supported by: U.S. Department of Energy Astrophysics: Stellar Evolution Nuclear Physics: Nuclear Synthesis Indirect Methods: Nuclear
The heavy ion irradiation facility at KVI-CART
The heavy ion irradiation facility at KVI-CART Brian N. Jones 1, Marc-Jan van Goethem 1,2, Rob Kremers 1, Harry Kiewiet 1, Emiel van der Graaf 1, Sytze Brandenburg 1 1 University of Groningen, KVI-Center
RG & EFT for nuclear forces
RG & EFT for nuclear forces Andreas Nogga, Forschungszentrum Jülich ECT* school, Feb/March 2006 Low momentum interactions: Using the RG to simplify the nuclear force for many-body calculations. Application
p-d radiative capture and mesonic effects Ingo Sick
/erice07/erice. p-d radiative capture and mesonic effects Ingo Sick 3-body system as ideal test-system for understanding of nuclei exact calculations for ground- and continuum state several independent
Ab initio nuclear structure from lattice effective field theory
Ab initio nuclear structure from lattice effective field theory Nuclear Lattice EFT Collaboration Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Timo Lähde (Jülich) Thomas Luu (Jülich) Dean Lee (NC State)
ABC Effect in Double Pionic Fusion
Fachbereich Physik CERN Courier September 2011 BLINDBILD ABC Effect in Double Pionic Fusion Facets of Strong-Interaction Physics Hirschegg Jan. 15 21, 2012 Heinz Clement Outline Two-Pion Production in
Nuclear Physics with polarized beams and targets
Nuclear Physics with polarized beams and targets Indranil Mazumdar TIFR-Mumbai SLENA-2008 SINP 20 th Feb. 2008 Plan of the talk Low energy Nuclear Physics with polarized beams» Reasons for polarized beam/target
Lattice Simulations with Chiral Nuclear Forces
Lattice Simulations with Chiral Nuclear Forces Hermann Krebs FZ Jülich & Universität Bonn July 23, 2008, XQCD 2008, NCSU In collaboration with B. Borasoy, E. Epelbaum, D. Lee, U. Meißner Outline EFT and
Electric Dipole Moment of Light Nuclei. Iraj R. Afnan. (The Flinders University of South Australia) Happy Birthday Tony
Electric ipole Moment of Light Nuclei Iraj R. Afnan (The Flinders University of South Australia) Happy Birthday Tony Collaborator: Benjamin F. Gibson, Los Alamos National Laboratory. 1 How I met Tony ate:
Elastic nucleon-deuteron scattering and breakup with chiral forces
Elastic nucleon-euteron scattering an breakup with chiral orces H.Witała, J.Golak, R.Skibiński, K.Topolnicki JAGIELLONIAN UNIVERSITY LENPIC Collaboration Jagiellonian University, Kraków Ruhr-Universität,
Carbon-12 in Nuclear Lattice EFT
Carbon-12 in Nuclear Lattice EFT Nuclear Lattice EFT Collaboration Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Timo A. Lähde (Jülich) Dean Lee (NC State) Thomas Luu (Jülich) Ulf-G. Meißner (Bonn/Jülich)
Neutron-Deuteron Breakup:
Neutron-Deuteron Breakup: A Probe of the Neutron-Neutron Interaction Triangle Universities Nuclear Laboratory (TUNL) T.B. Clegg A.H. Couture A.S. Crowell C.R. Howell J. Deng J.H. Esterline University of
THE THREE NUCLEON SYSTEM AT LEADING ORDER OF CHIRAL EFFECTIVE THEORY
THE THREE NUCLEON SYSTEM AT LEADING ORDER OF CHIRAL EFFECTIVE THEORY Young-Ho Song(RISP, Institute for Basic Science) Collaboration with R. Lazauskas( IPHC, IN2P3-CNRS) U. van Kolck (Orsay, IPN & Arizona
Few- Systems. Selected Topics in Correlated Hyperspherical Harmonics. Body. A. Kievsky
Few-Body Systems 0, 11 16 (2003) Few- Body Systems c by Springer-Verlag 2003 Printed in Austria Selected Topics in Correlated Hyperspherical Harmonics A. Kievsky INFN and Physics Department, Universita
Muon Capture With Improved Chiral Forces
, Jacek Golak, Kacper Topolnicki, Henryk Witała M. Smoluchowski Institute of Physics, Jagiellonian University, PL-30059 Kraków, Poland E-mail: roman.skibinski@uj.edu.pl Muon capture on the 2 H, 3 H and
Nucleon-nucleon interaction in covariant chiral effective field theory
Guilin, China The Seventh Asia-Pacific Conference on Few-Body Problems in Physics Nucleon-nucleon interaction in covariant chiral effective field theory Xiu-Lei Ren School of Physics, Peking University
Local chiral NN potentials and the structure of light nuclei
Local chiral NN potentials and the structure of light nuclei Maria Piarulli @ELBA XIV WORKSHOP June 7-July 1 16, Marciana Marina, Isola d Elba PHYSICAL REVIEW C 91, 43(15) Minimally nonlocal nucleon-nucleon
Correlations derived from modern nucleon-nucleon potentials
Correlations derived from modern nucleon-nucleon potentials H. Müther Institut für Theoretische Physik, Universität Tübingen, D-72076 Tübingen, Germany A. Polls Departament d Estructura i Costituents de
Neutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321
Neutron Interactions Part I Rebecca M. Howell, Ph.D. Radiation Physics rhowell@mdanderson.org Y2.5321 Why do we as Medical Physicists care about neutrons? Neutrons in Radiation Therapy Neutron Therapy
Three- and four-particle scattering
Three- and four-particle scattering A. Deltuva Centro de Física Nuclear da Universidade de Lisboa Few-particle scattering Three-particle scattering equations Three-nucleon system Three-body direct nuclear
Nuclear electric dipole moment in the Gaussian expansion method
Nuclear electric dipole moment in the Gaussian expansion method Nodoka Yamanaka (ithes Group, RIKEN) In collaboration with E. Hiyama (RIKEN), T. Yamada (Kanto-Gakuin Univ.), Y. Funaki (RIKEN) 2015/10/12
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
Four-nucleon scattering
Four-nucleon scattering A. Deltuva Centro de Física Nuclear da Universidade de Lisboa Hamiltonian H + i> j 4N scattering v i j 1 v 12 4 3 2 Wave function: Schrödinger equation (HH + Kohn VP) [M. Viviani,
arxiv:nucl-th/ v1 16 Jul 2002
Evolution of Nuclear Spectra with Nuclear Forces R. B. Wiringa[*] and Steven C. Pieper[ ] Physics Division, Argonne National Laboratory, Argonne, IL 60439 (Dated: February 8, 2008) We first define a series
Nuclear Structure and Reactions using Lattice Effective Field Theory
Nuclear Structure and Reactions using Lattice Effective Field Theory Dean Lee North Carolina State University Nuclear Lattice EFT Collaboration Frontiers of Nuclear Physics Kavli Institute for Theoretical
LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration
LCS2014 International Workshop LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration Outline Overview of the LEPS&LEPS2 beamlines Recent results from LEPS Search
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,
José Antonio Briz Monago, M. Carmona-Gallardo and. M.J.G. Borge, A. Perea, O. Tengblad, M. Turrión
GEANT4 SIMULATIONS FOR THE R3B CALORIMETER José Antonio Briz Monago, M. Carmona-Gallardo and M.J.G. Borge, A. Perea, O. Tengblad, M. Turrión Outline Introduction: FAIR at GSI (Germany) R3B Experiment Requirements
Nuclear Energy; Effects and Uses of Radiation
Nuclear Energy; Effects and Uses of Radiation Nuclear Reactions and the Transmutation of Elements A nuclear reaction takes place when a nucleus is struck by another nucleus or particle. Compare with chemical
MICROSCOPIC OPTICAL POTENTIAL FROM NN CHIRAL POTENTIALS. Carlotta Giusti Università and INFN, Pavia. Matteo Vorabbi (TRIUMF) Paolo Finelli (Bologna)
MICROSCOPIC OPTICAL POTENTIAL FROM NN CHIRAL POTENTIALS Carlotta Giusti Università and INFN, Pavia Matteo Vorabbi (TRIUMF) Paolo Finelli (Bologna) Nuclear ab initio Theories and Neutrino Physics: INT Seattle
Role of Spin in NN NNπ
Spin Physics (SPIN2014) International Journal of Modern Physics: Conference Series Vol. 40 (2016) 1660061 (6 pages) c The Author(s) DOI: 10.1142/S2010194516600612 Role of Spin in NN NNπ Vadim Baru Institut
Recent results in lattice EFT for nuclei
Recent results in lattice EFT for nuclei Dean Lee (NC State) Nuclear Lattice EFT Collaboration Centro de Ciencias de Benasque Pedro Pascua Bound states and resonances in EFT and Lattice QCD calculations
Light Nuclei from chiral EFT interactions
Light Nuclei from chiral EFT interactions Petr Navratil Lawrence Livermore National Laboratory* Collaborators: V. G. Gueorguiev (UCM), J. P. Vary (ISU), W. E. Ormand (LLNL), A. Nogga (Julich), S. Quaglioni
Momentum Transfer Dependence of Spin Isospin Modes in Quasielastic Region (RCNP E131 Collaboration) Tomotsugu WAKASA RCNP Osaka University
Momentum Transfer Dependence of Spin Isospin Modes in Quasielastic Region (RCNP E131 Collaboration) Tomotsugu WAKASA RCNP Osaka University Overview Motivations Experiment Definition of Experimental Spin
SFB Teilprojekt C2 Few Nucleon Systems
SFB 634 - Teilprojekt C2 Few Nucleon Systems Thorsten Kröll / Peter von Neumann-Cosel SFB 634 Programme Basic properties of the nucleon Polarizability of the nucleon Charge radius of the proton Electron-beam
PoS(Baldin ISHEPP XXII)042
Multifragmentation of nuclei by photons: new approaches and results Institute for Nuclear Research RAS Prospect 60-let Octabra, 7A, 117312 Moscow, Russia E-mail: vladimir@cpc.inr.ac.ru A review on multifragmentation
Chapter IX: Nuclear fusion
Chapter IX: Nuclear fusion 1 Summary 1. General remarks 2. Basic processes 3. Characteristics of fusion 4. Solar fusion 5. Controlled fusion 2 General remarks (1) Maximum of binding energy per nucleon
NN-Correlations in the spin symmetry energy of neutron matter
NN-Correlations in the spin symmetry energy of neutron matter Symmetry energy of nuclear matter Spin symmetry energy of neutron matter. Kinetic and potential energy contributions. A. Rios, I. Vidaña, A.
High-resolution Study of Gamow-Teller Transitions
High-resolution Study of Gamow-Teller Transitions Yoshitaka Fujita, Osaka Univ. @CNS-SS, 04.Aug.17-20 Nucleus : 3 active interactions out of 4 Strong, Weak, EM Comparison of Analogous Transitions High
Physics Program at COSY-Jülich with Polarized Hadronic Probes
Mitglied der Helmholtz-Gemeinschaft Physics Program at COSY-Jülich with Polarized Hadronic Probes Forschungszentrum Jülich October 9, 2008 Andro Kacharava (JCHP/IKP, FZ-Jülich) Overview COSY (Cooler Synchrotron)
arxiv: v1 [nucl-th] 7 May 2010
![arxiv: v1 [nucl-th] 7 May 2010](/thumbs/83/88958658.jpg "arxiv: v1 [nucl-th] 7 May 2010")
Polarization observables and spin-aligned fusion rates in 2 H(d,p) 3 H and 2 H(d,n) 3 He reactions A. Deltuva and A. C. Fonseca Centro de Física Nuclear da Universidade de Lisboa, P-1649-3 Lisboa, Portugal
Cross-Section Measurement of 2 H(n,np)n at 16 MeV in Symmetric Constant Relative Energy Configurations
Cross-Section Measurement of 2 H(n,np)n at 16 MeV in Symmetric Constant Relative Energy Configurations Alexander Hoff Couture A dissertation submitted to the faculty of the University of North Carolina
N-d 3-body scattering and NN interactions
N- 3-boy scattering an NN interactions Collaboration o: H. Witała, J. Golak, R. Skibiński, K. Topolnicki, Jagiellonian University, Kraków W. Gloeckle, E. Epelbaum, H. Krebs, Bochum Ul-G. Meibner, A.Nogga,
energy loss Ionization + excitation of atomic energy levels Mean energy loss rate de /dx proportional to (electric charge) 2 of incident particle
Lecture 4 Particle physics processes - particles are small, light, energetic à processes described by quantum mechanics and relativity à processes are probabilistic, i.e., we cannot know the outcome of
INTRODUCTION TO MAGNETIC NUCLEAR FUSION
INTRODUCTION TO MAGNETIC NUCLEAR FUSION S.E. Sharapov Euratom/CCFE Fusion Association, Culham Science Centre, Abingdon, Oxfordshire OX14 3DB, UK With acknowledgments to B.Alper for use of his transparencies
Neutral Pion Photoproduction in the Threshold Region
Neutral Pion Photoproduction in the Threshold Region Testing Chiral Perturbation Theory David Hornidge MOUNT ALLISON UNIVERSITY A2, CB, and TAPS Collaborations Mainzer Mikrotron 07 August 2012 2 Collaboration
Measurements of liquid xenon s response to low-energy particle interactions
Measurements of liquid xenon s response to low-energy particle interactions Payam Pakarha Supervised by: Prof. L. Baudis May 5, 2013 1 / 37 Outline introduction Direct Dark Matter searches XENON experiment
Coulomb effects in pionless effective field theory
Coulomb effects in pionless effective field theory Sebastian König in collaboration with Hans-Werner Hammer Helmholtz-Institut für Strahlen- und Kernphysik (Theorie) and Bethe Center for Theoretical Physics,
STUDY OF nn-interaction IN nd- AND dd-reactions
INTERNATIONAL SEMINAR ISINN- 2017 Dubna, Russia, May 22 26, 2017 STUDY OF nn-interaction IN nd- AND dd-reactions E.Konobeevski 1, A.Kasparov 1, V.Lebedev 2, M.Mordovskoy 1, A.Spassky 2, S.Zuyev 1 1 Institute
R. P. Redwine. Bates Linear Accelerator Center Laboratory for Nuclear Science Department of Physics Massachusetts Institute of Technology
Pion Physics in the Meson Factory Era R. P. Redwine Bates Linear Accelerator Center Laboratory for Nuclear Science Department of Physics Massachusetts Institute of Technology Bates Symposium 1 Meson Factories
From few-body to many-body systems
From few-body to many-body systems Nasser Kalantar-Nayestanaki, KVI-CART, University of Groningen Few-Body Physics: Advances and Prospects in Theory and Experiment 614. WE-Heraeus-Seminar, Bad Honnef April
Four-, Five-, and. Double Strangeness
Four-, Five-, and Six-Body Calculations of Double Strangeness s-shell Hypernuclei H. Nemura Institute of Particle and Nuclear Studies, KEK This talk is based on the work S= 2 world nucl-th/0407033 in collaboration
Measurement of 59 Ni(n, p) 59 Co Reaction Cross-section through Surrogate Technique for Fusion Technology Applications
Measurement of 59 Ni(n, p) 59 Co Reaction Cross-section through Surrogate Technique for Fusion Technology Applications Presented By Jyoti Pandey Department of Physics G.B. Pant University, Pantnagar Uttarakhand,
The No-Core Shell Model
The No-Core Shell Model New Perspectives on P-shell Nuclei - The Shell Model and Beyond Erich Ormand Petr Navratil Christian Forssen Vesselin Gueorguiev Lawrence Livermore National Laboratory Collaborators: