Symmetry energy and density W. Trautmann GSI Helmholtzzentrum, Darmstadt view at Bormio 3000 M. Cevedale P. San Matteo.

Slides:



Advertisements
Similar presentations
Isospin dependence and effective forces of the Relativistic Mean Field Model Georgios A. Lalazissis Aristotle University of Thessaloniki, Greece Georgios.
Advertisements

Ilona Bednarek Ustroń, 2009 Hyperon Star Model.
ASY-EOS Past and future: PR Milano, 28/04/14. Fuchs and Wolter, EPJA 30 (2006) EOS of symmetric nuclear and neutron matter from Ab initio calculations.
Probing the Equation of State of Neutron-Rich Matter with Heavy-Ion Reactions Bao-An Li Arkansas State University 1.Equation of State and Symmetry Energy.
Nuclear equation of state in form suitable for quantum molecular dynamics model 1.Brief indroduction of the EOS prescription 2.New form for bullk and surface.
Systematics of Temperature Measurements with ALADIN ALADIN S114 Spring 1993.
The National Superconducting Cyclotron State University Betty Tsang Constraining neutron star matter with laboratory experiments 2005.
Constraining the properties of dense matter A.What is the EOS   1. Theoretical approaches   2. Example:T=0 with Skyrme   3. Present status   a)
P. Arumugam Centro de Física das Interacções Fundamentais and Departamento de Física, Instituto Superior Técnico, Lisbon, Portugal S.K. Patra, P.K. Sahu,
Overview of the experimental constraints on symmetry energy Betty Tsang, NSCL/MSU.
Constraining the symmetry energy of the EoS in relativistic heavy-ion reactions A. Krasznahorkay, ATOMKI, Debrecen.
Equation of State of Neutron-Rich Matter in the Relativistic Mean-Field Approach Farrukh J. Fattoyev My TAMUC collaborators: B.-A. Li, W. G. Newton My.
Probing properties of neutron stars with heavy-ion reactions Outline: Symmetry energy at sub-saturation densities constrained by heavy-ion collisions at.
Zbigniew Chajęcki National Superconducting Cyclotron Laboratory Michigan State University Probing reaction dynamics with two-particle correlations.
Constraining the EoS and Symmetry Energy from HI collisions Statement of the problem Demonstration: symmetric matter EOS Laboratory constraints on the.
A.What is the EOS?   0. Relationship to energy and to nuclear masses   1. Important questions   B. What observables are sensitive to the EOS and.
Department of Physics Kyoto University Tetsuya MURAKAMI HIMAC Pion Experiment and Pb Isotope Radius Measurements Pion Ratios and ESYM.
ASY-EOS experiment P. Russotto* for the ASY-EOS collaboration *LNS-INFN and Univ. of Catania, Italy /06/11.
Pornrad Srisawad Department of Physics, Naresuan University, Thailand Yu-Ming Zheng China Institute of Atomic Energy, Beijing China Azimuthal distributions.
Reaction mechanisms in transport theories: a test of the nuclear effective interaction Maria Colonna INFN - Laboratori Nazionali del Sud (Catania) NN2012.
Tensor force induced short-range correlation and high density behavior of nuclear symmetry energy Chang Xu ( 许 昌 ) Department of Physics, Nanjing Univerisity.
Effects of self-consistence violations in HF based RPA calculations for giant resonances Shalom Shlomo Texas A&M University.
Alex Brown PREX Aug Neutron Radii and the Neutron Equation of State.
Alex Brown UNEDF Feb Strategies for extracting optimal effective Hamiltonians for CI and Skyrme EDF applications.
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,
Maria Colonna Laboratori Nazionali del Sud (Catania) Testing the behavior of n-rich systems away from normal density Eurorib’ 10 June 6-11, Lamoura.
Probing the isospin dependence of nucleon effective mass with heavy-ion reactions Momentum dependence of mean field/ –Origins and expectations for the.
F. Sammarruca, University of Idaho Supported in part by the US Department of Energy. From Neutron Skins to Neutron Stars to Nuclear.
Neutral pion photoproduction and neutron radii Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Eurotag Meeting.
Pygmy Dipole Resonance in 64Fe
Pb Electroweak Asymmetry in Elastic Electron-Nucleus Scattering -- Weak charge form factor -- most weak charge is carried by neutrons PREX and.
Presentation by T. Gogami 2015/6/15 (Mon). Equation state of neutron matter.
BNU The study of dynamical effects of isospin on reactions of p Sn Li Ou and Zhuxia Li (China Institute of Atomic Energy, Beijing )
Equation of state of asymmetricic nuclear matter at supra- saturation densities CBM collaboration meeting April 15, 2010, Darmstadt, Germany Laboratory.
Measuring flow to constrain the symmetry energy of the nuclear equation of state Zoe Matthews for Liverpool University and the ASYEOS Collaboration QUATION.
Neutron enrichment of the neck-originated intermediate mass fragments in predictions of the QMD model I. Skwira-Chalot, T. Cap, K. Siwek-Wilczyńska, J.
The High-Density Symmetry Energy in Heavy Ion Collisions The High-Density Symmetry Energy in Heavy Ion Collisions Int. School on Nuclear Physics: Probing.
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.
Charge Equilibration Dynamics: The Dynamical Dipole Competition of Dissipative Reaction Mechanisms Neck Fragmentation M.Di Toro, PI32 Collab.Meeting, Pisa.
Probing the symmetry energy of neutron-rich matter Betty Tsang, NSCL/MSU IWNDT in Honor of Prof. Joe Natowitz Texas A&M University, College Station, Texas,
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.
ExperimentSpokesmanGoalRunning time Thesis? Scissors ModeTonchevAnalyze Scissors Mode excitations in actinide nuclei Pgymy DipoleTonchevAnalyze evolution.
Many-body theory of Nuclear Matter and the Hyperon matter puzzle M. Baldo, INFN Catania.
NEUTRON SKIN AND GIANT RESONANCES Shalom Shlomo Cyclotron Institute Texas A&M University.
Three-body force effect on the properties of asymmetric nuclear matter Wei Zuo Institute of Modern Physics, Lanzhou, China.
Nuclear Isovector Equation-of-State (EOS) and Astrophysics Hermann Wolter Dep. f. Physik, LMU Topics: 1.Phase diagram of strongly interacting matter and.
Congratulations and Thanks, Joe!. The density curvature parameter and high density behavior of the symmetry energy Lie-Wen Chen ( 陈列文 ) Department of.
Isovector reorientation of deuteron in the field of heavy target nuclei The 9th Japan-China Joint Nuclear Physics Symposium (JCNP 2015) Osaka, Japan, Nov.
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.
New Era of Nuclear Physics in the Cosmos, RIKEN, September 25-26, 2008 H. Sagawa, University of Aizu 1.Introduction 2.Incompressibility and ISGMR 3.Neutron.
Properties of clustered nuclear matter in nuclear reactions Maria Colonna INFN - Laboratori Nazionali del Sud (Catania) NUFRA October 2015 Kemer.
Symmetry energy in the neutron star equation of state and astrophysical observations David E. Álvarez C. Sept 2013 S. Kubis, D. Blaschke and T. Klaehn.
The symmetry energy at high density: new experimental results W. Trautmann GSI Helmholtzzentrum, Darmstadt, Germany Bormio th Meeting.
Tetsuya MURAKAMI For SAMURAI-TPC Collaboration Physics Using SAMURAI TPC.
Current status and future direction on symmetry energy determination using Heavy Ion Collisions How does this subfield intersect with other subfields?
Experimental determination of the symmetry energy W. Trautmann, GSI Helmholtzzentrum, Darmstadt, Germany Nuclear Equation of State for Compact Stars and.
Constraints on E sym (  )-L from RIB induced reactions…and more Zach Kohley NSCL/MSU NuSYM14 July 7, 2014.
W. Trautmann GSI Helmholtzzentrum, Darmstadt, Germany Symposium on applied nuclear physics and innovative technologies Kraków, June 5, 2013.
Electric Dipole Response, Neutron Skin, and Symmetry Energy
Density-dependence of nuclear symmetry energy
Transverse and elliptic flows and stopping
University of Liverpool, Liverpool, UK, July 7-9, 2014
BE and charge radii well described (mostly isoscalar)
and the nuclear equation of state
Workshop on Nuclear Structure and Astrophysical Applications
International Workshop on Nuclear Dynamics and Thermodynamics
Decomposition of sensitivity of the symmetry energy observables
Zbigniew Chajęcki Western Michigan University
Presentation transcript:

Symmetry energy and density W. Trautmann GSI Helmholtzzentrum, Darmstadt view at Bormio 3000 M. Cevedale P. San Matteo

----- ~ 8 solar masses source: Anna Watts, QM2014

Quelle: SciTechDaily neutron star merger (artists conception)

Nuclear Equation of State (EoS) remember talk of S. Gandolfi 0

Nuclear Physics and Astrophysics: E sym (ρ) 10 fm m 20 km m m 55 orders of magnitude in mass

from n-skins the world average: L = MeV Li and Han, PLB 727 (2013) neutron skins masses collective excitations isospin diffusion crust oscillations r-mode instabilities mass-radius analysis (L=3p 0 /ρ 0 )

"A way forward in the study of the symmetry energy..." Horowitz et al., JPhG 41 (2014) following NUSYM13 maximum sensitivity of structure data near 2/3 ρ 0 Zhang and Chen (PLB 726 (2013)) use Skyrme-Hartree-Fock to analyze isotope binding energy difference and neutron skin thickness of Sn isotopes; B.A. Brown (PRL 111 (2013)) uses Skyrme, properties of doubly-magic nuclei (binding energies, rms charge radii, and single-particle energies) and Δr np =0.16 – 0.24 fm for 208 Pb.

Brown, PRL 111 (2013) 13 Skyrme sets fitted to ground-state properties of doubly magic nuclei E sym determined at 0.1 fm -3 neutron skin determines slope at 0.1 fm -3 Brown, PRL 85 (2000)

pressure gauge for neutron-star matter neutron-over-charged particle elliptic-flow ratio in neutron-rich systems analysis with transport UrQMD (Li & Bleicher) Tübingen QMD (Cozma) differential squeeze-out

pressure gauge for neutron-star matter neutron-over-charged particle elliptic-flow ratio in neutron-rich systems analysis with transport UrQMD (Li & Bleicher) Tübingen QMD (Cozma) studied reactions: 197 Au A MeV 96 Ru A MeV 96 Zr A MeV

Asy-Eos experiment S394 in May 2011 studied reactions: 197 Au A MeV 96 Ru A MeV 96 Zr A MeV CHIMERA, ALADIN Tof-wall, μ-ball, for impact parameter orientation and modulus Constraining the Symmetry Energy at Supra-Saturation Densities with Measurements of Neutron and Proton Elliptic Flows Co-Spokespersons: R.C. Lemmon and P. Russotto

NeuLAND all plastic improved calorimetry 4 planes in RIKEN 5 planes at GSI more planes to come

NeuLAND all plastic improved calorimetry 4 planes in RIKEN 5 planes at GSI more planes to come existing LAND: 2 x 2 m 2 1 m deep 18 t

3,8 m Laboratori Nazionali del Sud Catania, Sicilia 4 double rings of CHIMERA, LNS Catania

spokespersons: P. Russotto (Catania) R. Lemmon (Daresbury)

L=72±13 MeV new data data: Leifels et al. PRL 71 (1993) differential flow: Russotto et al. PLB 697 (2011) see Bormio 2014

sensitivity to density Tübingen QMD and force developed by Das, Das Gupta, Gale, and Bao-An Li, Phys. Rev. C 67 (2003) of elliptic-flow ratio for 400 AMeV Dan Cozma et al.

calculate DEFR (ρ) Difference of Elliptic-Flow Ratio ρ sensitivity to density Tübingen QMD and force developed by Das, Das Gupta, Gale, and Bao-An Li, Phys. Rev. C 67 (2003) of elliptic-flow ratio for 400 AMeV Dan Cozma et al.

sensitivity to density Tübingen QMD and force developed by Das, Das Gupta, Gale, and Bao-An Li, Phys. Rev. C 67 (2003) of elliptic-flow ratio for 400 AMeV Dan Cozma et al. Difference of Elliptic-Flow Ratio ρ

ρ0ρ0 asymmetry pressure p 0 = 3.8 ± 0.7 MeV/fm 3 Steiner, Lattimer, and Brown, ApJ 765, L5 (2013)

FAIR civil construction 21

FAIR instrumentation 22 NeuLAND PLAWA Califa

GLAD GSI Large Acceptance Dipole superconducting iron free bending power 5 Tm

Athena+ X-ray Observatory ESA 2028 (proposed) quiescent Low-Mass X-ray Binaries

Athena+ X-ray Observatory ESA 2028 (proposed) coated silicon wafers millions of pores in hundreds of modules 2 m 2 active area

picotechnology launched Lagrange point reached

picotechnology launched Lagrange point reached lisa in 2034 neutron-star seismology with gravitational waves 72nd Winter Meeting...

backups

the symmetry energy from astrophysics radius Bob Rutledge (Mc Gill, Montreal) 8.2 – 10.4 km method: qLMXB‘s (Bormio 2015) Jim Lattimer (Stony Brook, USA) 11.2 – 12.8 km method: PRE-bursts and qLMXBs (Eur. Phys. J. A 2014) radii for neutron stars with 1.4 solar mass quiescent Low-Mass X-ray Binaries: radiate while accreting mass from a neighboring star Photospheric-Radius-Expansion bursts: X-ray bursts energetic enough to reach the so-called Eddington limit at which radiation pressure is sufficiently large to overcome gravity, leading to expansion of the star’s photosphere.

NICER on the ISS 2017 Neutron-star Interior Composition Explorer 56 X-ray telescopes Method: rotation-resolved spectroscopy with 100 nanosecond timing resolution Quelle:NASA

one number: L= 72 MeV corresponds to pressure 6, Pa at density 2, g/cm bar ?

more systematic parameter test with Tübingen QMD*) conclusion: super-soft not compatible with FOPI-LAND data elliptic flow ratio and difference Au A MeV *) V.S. Uma Maheswari, C. Fuchs, Amand Faessler, L. Sehn, D.S. Kosov, Z. Wang, NPA 628 (1998) M.D. Cozma et al., PRC 88, (2013) steps towards model invariance: tested in UrQMD: FP1 vs. FP2, i.e. momentum dep. of NNECS tested in T-QMD: soft vs. hard 190<K<280 MeV density dependence of NNECS asymmetry dependence of NNECS wave packet 2.5<L<7.0 fm 2 optical potential momentum dep. of isovector potential supersoftsuperstiff