Fine structure of giant resonances in Calcium isotopes

Slides:



Advertisements
Similar presentations
N. Pietralla and K. Sonnabend for the SFB 634
Advertisements

Kerstin Sonnabend, IKP, TU Darmstadt S-DALINAC - Nuclear Astrophysics Nuclear Astrophysics at the Darmstadt superconducting electron linear accelerator.
RIKEN Seminar, September 8th, Complete Electric Dipole Response and Neutron Skin in 208 Pb A. Tamii Research Center for Nuclear Physics, Osaka University.
Photo-Nuclear Physics Experiments by using an Intense Photon Beam Toshiyuki Shizuma Gamma-ray Nondestructive Detection Research Group Japan Atomic Energy.
Giant resonances, exotic modes & astrophysics
Spectroscopy at the Particle Threshold H. Lenske 1.
CEA DSM Irfu Shell evolution towards 100 Sn Anna Corsi CEA Saclay/IRFU/SPhN.
n_TOF meeting November 2007, BARI.
Gamma-Ray Spectra _ + The photomultiplier records the (UV) light emitted during electronic recombination in the scintillator. Therefore, the spectrum collected.
| Institut für Kernphysik | Project C2 | Anna Maria Heilmann | 1 Construction of a Neutron Ball for Exclusive Electron Scattering Experiments.
Dipole Strengths in 112,120 Sn and Systematics of the Pygmy Dipole Resonance at Z=50 Shell Closure BANU ÖZEL 1,2, J. ENDERS 1, Y. KALMYKOV 1, P. von NEUMANN-COSEL.
Soft Electric Dipole Modes in Heavy Nuclei: Some Selected Examples S-DALINAC TU DARMSTADT Soft E1 modes: the case of 208 Pb * Supported by DFG under contracts.
John Daoutidis October 5 th 2009 Technical University Munich Title Continuum Relativistic Random Phase Approximation in Spherical Nuclei.
Yoshitaka FUJITA (Osaka Univ.) Hirschegg Workshop /2006, Jan GT (  ) : Important weak response GT transitions of Astrophysics Interest.
Scint. Al Internal reflection External reflection ↑ ↑ ↑ Decay Detector Development for Giant Resonance Studies By: Gus Olson Mentor: Dr. D.H.Youngblood.
Study of e + e  collisions with a hard initial state photon at BaBar Michel Davier (LAL-Orsay) for the BaBar collaboration TM.
Proton polarization measurements in π° photo-production --On behalf of the Jefferson Lab Hall C GEp-III and GEp-2γ collaboration Wei Luo Lanzhou University.
CMD-2 and SND results on the  and  International Workshop «e+e- Collisions from  to  » February 27 – March 2, 2006, BINP, Novosibirsk, Russia.
Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.
Α - capture reactions using the 4π γ-summing technique Α. Lagoyannis Institute of Nuclear Physics, N.C.S.R. “Demokritos”
Study of 58Ni excited states by (p, p’) inelastic scattering
Isotopically resolved residues produced in the fragmentation of 136 Xe and 124 Xe projectiles Daniela Henzlova GSI-Darmstadt, Germany on leave from NPI.
Soft collective excitations in weakly bound nuclei studied with ELI-NP A.Krasznahorkay Inst. of Nuclear Research of the Hung. Acad. of Sci. (ATOMKI)
AUJOURD’ HUI…..et…. DEMAIN Keep contact with experimentalists, work together Beyond mean-field, but via Particle- Vibration Coupling.
XII Nuclear Physics Workshop Maria and Pierre Curie: Nuclear Structure Physics and Low-Energy Reactions, Sept , Kazimierz Dolny, Poland Self-Consistent.
Effects of self-consistence violations in HF based RPA calculations for giant resonances Shalom Shlomo Texas A&M University.
Motivation. Why study ground state hyperon electroproduction? CLAS detector and analysis. Analysis results. Current status and future work. M. Gabrielyan.
Gamma-ray strength functions obtained with the Oslo method Ann-Cecilie Larsen July 8, 2008 Workshop on Statistical Nuclear Physics and Applications in.
Giant Resonances - Some Challenges from Recent Experiments
Systematic study of isovector dipole mode up to A=50 KEK 研究会「原子核・ハドロン物理 : 横断研究会」 KEK, 2007 年 11 月 19 日 -21 日 稲倉恒法 中務孝 矢花一浩 ( 筑波大学 ) ( 理研 ) ( 筑波大学 )
E1 strength distribution in even-even nuclei studied with the time-dependent density functional calculations Takashi NAKATSUKASA Theoretical Nuclear Physics.
Low-lying dipole strength in unstable nuclei. References: N. Ryezayeva et al., Phys. Rev. Lett. 89 (2002) P. Adrich, A. Kimkiewicz et al., Phys.Rev.
Level Densities and Gamma Strength Functions from the Fine Structure of Giant Resonances S-DALINAC TU DARMSTADT Spin- and parity-resolved level densities.
Pygmy Dipole Resonance in 64Fe
Measurements of the cross sections and Ay for D(p,n) inclusive breakup reaction at 170 MeV Y. Maeda Y. Maeda, T. Saito, H. Miyasako (Univ. of Miyazaki)
1 The results of the study of dp-elastic scattering at the energies from 500 to 1000 MeV/nucleon A.A Terekhin et al. Joint Institute for Nuclear Research,
Nuclear Structure, Safety, and Applications I. Usman, J. Carter, E. Sideras-Haddad, G.R.J. Cooper, L. Donaldson, M. Latif, N. Botha, R. Neveling, F. D.
Dott. Antonio Botrugno Ph.D. course UNIVERSITY OF LECCE (ITALY) DEPARTMENT OF PHYSICS.
09/10/2005NSTAR Graal collaboration1 The Graal collaboration results and prospects Presented by Carlo Schaerf Università di Roma “Tor Vergata” and.
Some aspects of reaction mechanism study in collisions induced by Radioactive Beams Alessia Di Pietro.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
Nuclear Structure SnSn P,n p n (  )‏ ( ,Xn)‏ M1E1 p,nn X λ ?E1 ExEx  Study of the pygmy dipole resonance as a function of deformation.
NEUTRON SKIN AND GIANT RESONANCES Shalom Shlomo Cyclotron Institute Texas A&M University.
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
Oct 6, 2008Amaresh Datta (UMass) 1 Double-Longitudinal Spin Asymmetry in Non-identified Charged Hadron Production at pp Collision at √s = 62.4 GeV at Amaresh.
Study on ν-A Reaction Cross Sections within CRPA Jeong-Yeon LEE and Yeong-Duk KIM Sejong University, KOREA.
09/10/2005NSTAR Graal collaboration1 The Graal collaboration results and prospects Presented by Carlo Schaerf Università di Roma “Tor Vergata” and.
Beginning of 0˚ mode for K600 at iTL
00 Cooler CSB Direct or Extra Photons in d+d  0 Andrew Bacher for the CSB Cooler Collaboration ECT Trento, June 2005.
LOMONOSOV MOSCOW STATE UNIVERSITY, SKOBELTSYN INSTITUTE OF NUCLEAR PHYSICS Multi-particle photodisintegration of heavy nuclei A.N. Ermakov, B.S. Ishkhanov,
Search for low spin states at high excitation energies in 20 Ne with the p,t reaction iThemba LABS & Stellenbosch University Energy Postgraduate Conference.
24 Nov 2006 Kentaro MIKI University of Tsukuba “electron / photon flow” Elliptic flow measurement of direct photon in √s NN =200GeV Au+Au collisions at.
The experimental evidence of t+t configuration for 6 He School of Physics, Peking University G.L.Zhang Y.L.Ye.
100MeV/u 12 C+ 12 C Scattering at RCNP Weiwei Qu 、 Gaolong Zhang 、 Satoru Terashima 、 Isao Tanihata 、 Chenlei Guo 、 Xiaoyun Le 、 Hoo Jin Ong 、 Harutaka.
SFB 634 *Supported by the DFG within SFB 634 and 446 JAP 113/267/0-2 Complete Dipole Strength Distributions from High-Resolution Polarized Proton Scattering.
Jun Chen Department of Physics and Astronomy, McMaster University, Canada For the McMaster-NSCL and McMaster-CNS collaborations (5.945, 3+ : **) (5.914,
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Nature of Mixed-Symmetry 2 + States in 94 Mo from High-Resolution Electron and Proton Scattering and Line Shape of the First Excited 1/2 + State in 9 Be.
Exploring the alpha cluster structure of nuclei using the thick target inverse kinematics technique for multiple alpha decays. The 24 Mg case Marina Barbui.
Young Researchers Session in IFIN-HH 2016
School of Physics and Nuclear Energy Engineering
Large-scale shell-model study of E1 strength function and level density Yutaka Utsuno Advanced Science Research Center, Japan Atomic Energy Agency Center.
Giant Monopole Resonance
Event Reconstruction and Data Analysis in R3BRoot Framework
of secondary light ion beams
of secondary light ion beams
Kaons Propagation Through Nuclei
Nuclear excitations in relativistic nuclear models
E19 result Ryuta Kiuchi (SNU)
Daniela Henzlova GSI-Darmstadt, Germany
Presentation transcript:

Fine structure of giant resonances in Calcium isotopes Iyabo Usman University of the Witwatersrand On behalf of iThemba/Wits/UCT/RCNP/IKP-TU-Darmstadt K600 Group *Project Funded By South African National Research Foundation (Grant No: 85730) German DFG under contracts SFB 634, NE 679/2-2 HST15 RCNP Osaka University 16 – 19 November 2015

Outline Fine structure of Giant Resonances High energy-resolution experiments with K600 Magnetic Spectrometer of iThemba LABS Isoscalar Giant Quadrupole Resonance in 40Ca Isovector Giant Dipole Resonance in 40,42,44,48Ca Energy Scales and Comparison with Theoretical Calculations Level density extraction from (p,p′) data

Fine Structure of Giant Resonances Have been established as a Global phenomenon in - nuclei across the periodic table - other resonances Dominant processes of the decay? Global phenomenon have been established in nuclei across the periodic table as well as other resonances. However, dominant damping mechanisms as well as spin and parity resolved level densities are yet to be elucidated Spin- and parity-resolved level densities at energies above thresholds?

K600 Magnetic Spectrometer Scintillator paddles1 and 2 drift-chambers Dipole magnet 1 Scattering chamber Best resolution = 25 keV @ 200 MeV on Au target Best resolution = 9 keV @ 66 MeV on Pb target Largest angle so far = 87o Smallest angle = 21o with external beamstop Smallest angle = 7o with internal beamstop 2 VDC: high accuracy horizontal position determination in focal plane 1 HDC: high accuracy vertical position determination 2 plastic scintillators (BC-408) acting as trigger detectors for particle identification

K600 magnetic spectrometer at 0o Ion-optics values is included mainly for completeness Contact person: neveling@tlabs.ac.za

Fine structure of ISGQR in 40Ca ∆E = 35 - 40 keV (FWHM) Fine structures in the region of the ISGQR are clearly visible. Excitation energy spectra in 40Ca at angles below, at and above the maximum of the ISGQR.

Fine structure of the IVGDR in 42,44,48Ca M. Latif, PhD Thesis (in preparation) University of the Witwatersrand ∆E = 34 - 41 keV (FWHM) Excitation energy spectra in 42,44,48Ca at zero-degree

Wavelet Analysis Wavelet coefficients Morlet: Complex Morlet: position scale spectrum wavelet Morlet: Complex Morlet: Complex Lorentzian:

Characteristic Energy Scales 40Ca ISGQR ISGQR is not mainly concentrated in a well-defined peak in light nuclei but completely fragmented e.g. 40Ca, 28Si & 12C Wavelet Coefficients Pronounced fine structure is observed up to

Comparison with Theoretical Calculations To understand the origin and physical nature of different scales, comparison of experimental results with model calculations is important. Theoretical models for ISGQR and IVGDR in 40,42,44,48Ca - Random Phase Approximation (RPA) - Second-RPA (SRPA) - (R-QRPA) - Relativistic Quasiparticle Time Blocking Approximation (RQTBA)

Comparison with Theoretical Calculations RPA and SRPA in 40Ca ISGQR Experimental Scales (150, 240, 460) keV; (1.05, 2.0, 3.9) MeV; Observed fragmentation is attributed to mixing of the 1p–1h states with more complex configurations, including collective phonons RPA only accounts for Landau damping I. Usman, Z. Buthelezi, J. Carter, G. R. J. Cooper, R. W. Fearick, S. V. Fortsch, H. Fujita, Y. Fujita, Y. Kalmykov, P. von Neuman-Cosel, R. Neveling, P. Papakonstantinou, A. Richter, R. Roth, A. Shevchenko, E. Sideras-Haddad, F.D. Smit, Physics Letters B 698 (2011) 191-195.

Comparison with Theoretical Calculations QRPA and RQTBA 48Ca IVGDR M. Latif, PhD Thesis (in preparation) University of the Witwatersrand E. Litvinova, P. Ring and V. Tselyaev, Phys. Rev. C 78 (2008) 014312. E. Litvinova, Phys. Rev. C 91 (2015) 034332.

Extraction of spin- and parity-dependent Level densities Level densities of Jπ = 2+and 1- states extracted from high energy-resolution (p,p′) experiments in the region above particle thresholds Continuum background determination using Quasi-free calculations and model-independent method of Discrete Wavelet Transform (DWT) Self consistent procedure to extract level densities based on fluctuation analysis and Autocorrelation functions

Fluctuation Analysis Measure of cross section fluctuations with respect to a stationary mean value. Assumptions: Procedure: Background subtraction from the experimental spectrum Smoothing by convolution with a Gaussian function of width larger than ∆E Folding with a Gaussian function with a width smaller than ∆E Create a stationary spectrum Mean level width Mean level spacing Energy resolution Sum of normalised variances

Autocorrelation Function Mean level spacing proportional to the variance of Intensity fluctuations in can be autocorrelated at energies E and E + ε can be extracted from ε = energy increment C(ε) = Autocorrelation function

Level density: Background Subtraction and Autocorrelation Function DWT Background subtraction Fluctuation Analysis Autocorrelation Quasi-free Background subtraction Limited contribution from quasi-free in the ISGQR region

Spin-parity-resolved Level Densities I. Usman et.al., PRC 84 (2011) 054322 M. Jingo, PhD Thesis (2014) University of the Witwatersrand Experimental (filled symbol) BSFG-Rauscher (red); BSFG-von Egidy (Green); HF-BCS (Blue); HFB (Orange);

Ongoing work: Fine structure of the ISGMR in 40Ca 𝟒𝟎 𝑪𝒂 𝜶, 𝜶 ′ @ 𝟎 𝒐 Preliminary data analysis !!! Level density of J𝝅 = 0+ states to be extracted !!!

Summary The Fine structure conforms to the global character of phenomenon in ISGQR and IVGDR Theoretical calculations: RPA, SRPA, R-QRPA and R-QTBA reveal good agreements with the experimental energy scales Spin-parity dependent level densities extraction as important ingredients used as input for calculations in nuclear astrophysics

Thank you