For more information about the facility visit: For more information about our group visit:

Slides:



Advertisements
Similar presentations
SYNTHESIS OF SUPER HEAVY ELEMENTS
Advertisements

Nuclear Symmetry energy and Intermediate heavy ion reactions R. Wada, M. Huang, W. Lin, X. Liu IMP, CAS.
Detector Design and Data Analysis for Heavy Ion Collision Experiments Peter, Chan Chak Fai SURE 2011 Supervisor: Prof Betty Tsang(NSCL, MSU)
The peculiarities of the production and decay of superheavy nuclei M.G.Itkis Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia.
1 Nuclear Physics 1 Section 11-1,2. 2 Electron Pressure From the total energy of a free electron gas we can calculate the electron pressure using.
Chapter 24 Nuclear Reactions and Their Applications.
Isospin Dependence of Intermediate Mass Fragments in 124Sn, 124Xe + 124Sn, 112Sn D. V. Shetty, A. Keksis, E. Martin, A. Ruangma, G.A. Souliotis, M. Veselsky,
Detecting Giant Monopole Resonances Peter Nguyen Advisors: Dr. Youngblood, Dr. Lui Texas A&M University Energy Loss Identifying The Particles Discovered.
Systematics of Temperature Measurements with ALADIN ALADIN S114 Spring 1993.
Neutron Number N Proton Number Z a sym =30-42 MeV for infinite NM Inclusion of surface terms in symmetry.
Dual-axis, Duo Lateral Position Sensitive Detectors Robin Dienhoffer State University of New York at Oswego Advisor: Dr. Sherry Yennello Cyclotron Institute,
The development of the NIMISiS Bias Control GUI by Christopher Crane Mentor Dr. Sherry Yennello.
EURISOL workshop, ECT* Trento, Jan Two-component (neutron/proton) statistical description of low-energy heavy-ion reactions E. Běták & M.
Clearly state goals and open questions. Questions Which exp. should we perform in order to know how far (how to measure this distance?) we are from eqil.(randomized)
Preliminary results from a study of isospin non-equilibrium E. Martin, A. Keksis, A. Ruangma, D. Shetty, G. Souliotis, M. Veselsky, E. M. Winchester, and.
The National Superconducting Cyclotron State University Betty Tsang Constraining neutron star matter with laboratory experiments 2005.
Radiation Detectors There are a variety of detectors that can be used to measure particles emitted from nuclear reactions. The various materials used in.
Using GEMINI to study multiplicity distributions of Light Particles Adil Bahalim Davidson College Summer REU 2005 – TAMU Cyclotron Institute.
Detecting Giant Monopole Resonances Peter Nguyen Advisors: Dr. Youngblood, Dr. Lui Texas A&M University.
Adil Bahalim Davidson College Dr. Joseph Natowitz (Advisor), Dr. Seweryn Kowalski (Mentor) Summer REU 2005 – TAMU Cyclotron Institute Reconstruction Main.
Detectors The energy loss of particles in matter can be used detect and identify those particles. There are different types of “detectors”: - Gas-filled.
NUCLEAR CHEMISTRY Nuclear Particles: Mass ChargeSymbol Mass ChargeSymbol PROTON 1 amu +1 H+, H, p NEUTRON 1 amu 0 n © Copyright R.J. Rusay.
Germany's United States 2 Germany 0 FIFA Women’s World Cup Semifinal.
E432a: Decay of Highly Excited Projectile-like Fragments Formed in dissipative peripheral collisions at intermediate energies 1.Understanding thermodynamic.
Zbigniew Chajęcki National Superconducting Cyclotron Laboratory Michigan State University Probing reaction dynamics with two-particle correlations.
- Mid-rapidity emission in heavy ion collisions at intermediate energies - Source reconstruction - Free nucleon multiplicities - Neutron/proton ratio of.
Isotopically resolved residues produced in the fragmentation of 136 Xe and 124 Xe projectiles Daniela Henzlova GSI-Darmstadt, Germany on leave from NPI.
Laura Francalanza Collaborazione EXOCHIM INFN Sezione di Catania - LNS.
The NSCL is funded in part by the National Science Foundation and Michigan State University. Determining the Impact Parameter and Cross-Section in Heavy.
Nuclear Reactions AP Physics B Montwood High School R. Casao.
The High Resolution Array The High Resolution Array is a detector designed to detect and identify light charged particles like protons, deuterium, triton,
J. Su( 苏军 ) and F.S. Zhang( 张丰收 ) College of Nuclear Science and Technology Beijing Normal University, Beijing, China Tel: ,
Summary of EOS working group Z. Chajecki,B. Tsang Additional contributions from: Garg, Brown, Pagano Neutron stars HICs, Structure Neutron skin Tan Ahn.
Probing the density dependence of symmetry energy at subsaturation density with HICs Yingxun Zhang ( 张英逊 ) China Institute of Atomic Energy JINA/NSCL,
Ln(R 12 ) N Alan McIntosh, Yennello Research Group, TAMU-CI. Nuclear Physics Town Meeting, Aug 2014, College Station, TX Asymmetry Dependence of Thermodynamic.
Isotope dependence of the superheavy nucleus formation cross section LIU Zu-hua( 刘祖华) (China Institute of Atomic Energy)
BNU The study of dynamical effects of isospin on reactions of p Sn Li Ou and Zhuxia Li (China Institute of Atomic Energy, Beijing )
Motivation Current status Outlook This work was supported in part by: The Robert A. Welch Foundation: Grant Number A-1266 and, The Department of Energy:
Dynamics effect and evolution of isoscaling on the Quantum Molecular Dynamics model Wendong TIAN, Yugang MA, Xiangzhou CAI, Jingen CHEN, Jinhui CHEN, Deqing.
Neutron enrichment of the neck-originated intermediate mass fragments in predictions of the QMD model I. Skwira-Chalot, T. Cap, K. Siwek-Wilczyńska, J.
Probing the symmetry energy with isospin ratio from nucleons to fragments Yingxun Zhang( 张英逊 ) China Institute of Atomic Energy The 11 th International.
Isospin study of projectile fragmentation Content 1 、 Isospin effect and EOS in asymmetry nuclei 2 、 Isotope Yields in projectile ragmentation 3 、 Summary.
The FAIR* Project *Facility for Antiproton and Ion Research Outline:  FAIR layout  Research programs Peter Senger, GSI USTC Hefei Nov. 21, 2006 and CCNU.
In-Medium Cluster Binding Energies and Mott Points in Low Density Nuclear Matter K. Hagel SSNHIC 2014 Trento, Italy 8-Apr-2014 Clustering and Medium Effects.
N/Z Dependence of Isotopic Yield Ratios as a Function of Fragment Kinetic Energy Carl Schreck Mentor: Sherry Yennello 8/5/2005 J. P. Bondorf et al. Nucl.
In Progress T-Rex TAMUTrap SASSYER Active Target Det RTC + chemistry Radioisotope production.
NEUTRON SKIN AND GIANT RESONANCES Shalom Shlomo Cyclotron Institute Texas A&M University.
Chapter 29:Nuclear Physics
Z.Q. Feng( 冯兆庆 ), W.F. Li( 李文飞 ), Z.Y. Ming( 明照宇 ), L.W. Chen( 陈列文 ), F. S. Zhang ( 张丰收 ) Institute of Low Energy Nuclear Physics Beijing Normal University.
Nuclear Changes Objectives: Students will:
Momentum distributions of projectile residues: a new tool to investigate fundamental properties of nuclear matter M.V. Ricciardi, L. Audouin, J. Benlliure,
Fragmentation of relativistic 9 Be and 14 N nuclei in nuclear track emulsion D. A. Artemenkov JINR, Dubna BECQUREL Collaboration web site:
In-medium properties of nuclear fragments at the liquid-gas phase coexistence International Nuclear Physics Conference INPC2007 Tokyo, Japan, June 3-8,
Search for a New State of Matter A state of matter not seen since the first few microseconds after the Big Bang is the object of study of P-25 physicists.
Chapter 4 Practice Questions. Which subatomic particle has a negative charge? 1.electron 2.proton 3.neutron 4.nucleus
March, 2006SERC Course1  Z>92 (Heaviest Element in Nature) and upto Z= achieved by n irradiation or p,  and d bombardment in Cyclotron ( )
Tetsuya MURAKAMI For SAMURAI-TPC Collaboration Physics Using SAMURAI TPC.
Romualdo de Souza Nuclear Chemistry- Studying the Behavior of Microscopic Droplets I.General Overview (What & Why) II.Particle Accelerator Labs (Where)
Production mechanism of neutron-rich nuclei in 238 U+ 238 U at near-barrier energy Kai Zhao (China Institute of Atomic Energy) Collaborators: Zhuxia Li,
Experimental Reconstruction of Primary Hot Fragment at Fermi Energy Heavy Ion collisions R. Wada, W. Lin, Z. Chen IMP, China – in JBN group.
Systematic Investigation of the Isotopic Distributions Measured in the Fragmentation of 124 Xe and 136 Xe Projectiles Daniela Henzlova GSI-Darmstadt, Germany.
Opportunities for statistical methods in nuclear reactions: Streamlining calibrations and improving sensitivity.
Detector Design and Data Analysis for Heavy Ion Collision Experiments
FAST IN-MEDIUM FRAGMENTATION OF PROJECTILE NUCLEI
Understanding the Isotopic Fragmentation of a Nuclear Collision
Shalom Shlomo Cyclotron Institute Texas A&M University
Energy Dependence of the Isotopic Composition in Nuclear Fragmentation
Cyclotron Institute, Texas A&M University
Reaction Dynamics in Near-Fermi-Energy Heavy Ion Collisions
Chemistry/Physical Setting
Presentation transcript:

For more information about the facility visit: For more information about our group visit: The properties of isospin asymmetric nuclear matter (that is matter with an excess of neutrons or protons) at densities higher or lower than normal nuclear matter can be studied using heavy ion reactions. These reactions are important for studying the structure, chemical composition and evolution of neutron stars and the dynamics of supernovae explosions. Predictions have been made that the decay of excited nuclear matter would be dependent on N/Z, due to the difference in the chemical potential of the neutrons and protons. These predictions indicated that a neutron-rich system would undergo a “distillation” that results in a low density (or gas) phase that receives much of the neutron richness and a high density (or liquid) phase that would become more isospin symmetric. The Yennello Research Group is involved in carrying out studies on isospin dependencies on the dynamical formation of excited systems, the process of isospin equilibration and the subsequent disintegration of these systems in heavy-ion reactions. The group is based at the Texas A&M University Cyclotron Institute and utilizes the K500 superconducting cyclotron, to accelerate our projectiles up to 40 percent the speed of light and collide it with a stationary target nuclei. These collisions create excited systems that decay by emitting fragments that are then collected using various detector arrays. These fragments can then provide information about the reactions that took place. We also collaborate with other groups in the U.S. and around the world. Some of our interesting results and equipment that we use are described below. F1 F2 B1 B2 Front1Back2 Front 2 Back 1 Charge collecting strips Dual-Axis Dual-Lateral Position Sensitive Silicon Detector This detector is a double sided p-on-n silicon structure with highly uniform resistive junction and ohmic layers with equipotential channels. The readout between two anodes is orthogonal with respect to the readout between the two cathodes. The position sensitivity is on the order of 200 um. Under fully reversed biased conditions, the lateral effect dominates over surface recombination for current distributions. On a given side, the lateral effect allows for linear position reconstruction without the necessity of software correction. Energy given by: Position Nuclear Equation of State From Atomic Nuclei to Neutron Stars Data favors a “ stiff ” form of the density dependence of the symmetry energy A constraint of E sym (r) = C(  /  o )  with C = 31 – 33 MeV and  = 0.6 – 1.05 is obtained by comparing with various other studies Density dependence of the symmetry energy in nuclear equation of state is largely unconstrained. FAUST has 68  E-E (Si-CsI) detector telescopes used for studying peripheral reactions. FAUST is mobile and can be used in any of the lines in the Cyclotron Institute. Its main use has been for peripheral heavy ion collisions. FAUST has been adapted to accept a Dual-Axis Dual Lateral Position Sensitive Silicon Detector to increase its position sensitivity 1000 fold. This detector is currently in development in the SJY group. FAUST Forward Array Using Silicon Technology NIMROD-ISiS is a 4pi (spherical) detector consisting of 228 detector modules covering from ~3-167 degrees. Each detector module consists of 1 or 2 silicon wafers and a CsI crystal. The combination of Si-Si and Si-CsI detectors yields elemental resolution for high Z’s as well as isotopic resolution for elements of Z = 1 - ~17. NIMROD- ISiS is coupled with the TAMU Neutron Ball. The Neutron Ball is composed of 6 tanks of Gd doped pseudocumine enveloping the NIMROD-ISiS array. This gives near 4  detection of neutrons for event neutron multiplicity estimation. The ability to collect quasi- complete events with isotopic resolution and neutron multiplicity makes the NIMROD-ISiS array useful for cutting edge nuclear experiments. Neutron and Ion Multidetector for Reaction Oriented Dynamic - Indian Silicon Sphere NIMROD-ISiS b = 6 48 Ca Sn at 32 MeV/nucleon t = 1 fm/ct = 20 fm/ct = 40 fm/ct = 60 fm/ct = 80 fm/ct = 100 fm/ct = 120 fm/ct = 140 fm/ct = 160 fm/ct = 180 fm/ct = 200 fm/c t = 220 fm/c Single component liquid Two component liquid 9 Be 10 Be 7 Be CsI Signal Si Signal Using Isoscaling to extract information about the symmetry energy. Phase Diagram of Nuclear Matter