Xia Zhou & Xiao-ping Zheng The deconfinement phase transition in the interior of neutron stars Huazhong Normal University May 21, 2009 CSQCD Ⅱ.

Slides:



Advertisements
Similar presentations
Stellar Structure Section 2: Dynamical Structure Lecture 3 – Limit on gravitational energy Limit on mean temperature inside stars Contribution of radiation.
Advertisements

1 Degenerate stars There is not a sharp transition between relativistically degenerate and non- relativistically degenerate gas. Similarly there is no.
Envelopes and thermal radiation of neutron stars with strong magnetic fields Alexander Y. Potekhin 1 in collaboration with D.G.Yakovlev, 1 A.D.Kaminker,
1 The structure and evolution of stars Lecture 2: The equations of stellar structure Dr. Stephen Smartt Department of Physics and Astronomy
Supported by DOE 11/22/2011 QGP viscosity at RHIC and LHC energies 1 Huichao Song 宋慧超 Seminar at the Interdisciplinary Center for Theoretical Study, USTC.
Questions and Probems. Matter inside protoneutron stars Hydrostatic equilibrium in the protoneutron star: Rough estimate of the central pressure is: Note.
Toshiki Maruyama (JAEA) Nobutoshi Yasutake (Chiba Inst. of Tech.) Minoru Okamoto (Univ. of Tsukuba & JAEA ) Toshitaka Tatsumi (Kyoto Univ.) Structures.
Phase transitions Qualitative discussion: the 1-component system water specific volume.
Hyperon Suppression in Hadron- Quark Mixed Phase T. Maruyama (JAEA), S. Chiba (JAEA), H.-J. Schhulze (INFN-Catania), T. Tatsumi (Kyoto U.) 1 Property of.
Hyperon-Quark Mixed Phase in Compact Stars T. Maruyama* (JAEA), T. Tatsumi (Kyoto U), H.-J. Schulze (INFN), S. Chiba (JAEA)‏ *supported by Tsukuba Univ.
Structured Mixed Phase of Nuclear Matter Toshiki Maruyama (JAEA) In collaboration with S. Chiba, T. Tatsumi, D.N. Voskresensky, T. Tanigawa, T. Endo, H.-J.
Objectives Determine the effect of mass on a star’s evolution.
The Phase Diagram of Nuclear Matter Oumarou Njoya.
LIGO- G Z August 18, 2004LIGO Scientific Collaboration 1 When do the pulsar upper limits get interesting? Ben Owen with Ian Jones.
AOSS 321, Winter 2009 Earth System Dynamics Lecture 10 2/10/2008 Christiane Jablonowski Eric Hetland
2008GRB_Nanjing1 Hyperaccretion disks around Neutron stars Dong Zhang & Zigao Dai Nanjing University.
Dr. Jie Zou PHY 1151G Department of Physics1 Chapter 17 Phases and Phase Changes.
Cooling of Hybrid Neutron Stars Hovik Grigorian Yerevan State University Dubna, JINR Ladek Zdroj2008.
Exam II Results Avg. 33.8=56%.
Stellar Structure Section 3: Energy Balance Lecture 4 – Energy transport processes Why does radiation dominate? Simple derivation of transport equation.
Metastability of Hadronic Compact Stars I. Vidaña & I. Bombaci, P. K. Panda, C. Providência “The Complex Physics of Compact Stars” Ladek Zdroj, Poland,
Thermal Evolution of Rotating neutron Stars and Signal of Quark Deconfinement Henan University, Kaifeng, China Miao Kang.
Stellar Structure Section 3: Energy Balance Lecture 5 – Where do time derivatives matter? (part 1)Time-dependent energy equation Adiabatic changes.
Stellar Structure Section 4: Structure of Stars Lecture 7 – Stellar stability Convective instability Derivation of instability criterion … … in terms of.
Phase Fluctuations near the Chiral Critical Point Joe Kapusta University of Minnesota Winter Workshop on Nuclear Dynamics Ocho Rios, Jamaica, January 2010.
Fluctuations and Correlations of Conserved Charges in QCD at Finite Temperature with Effective Models Wei-jie Fu, ITP, CAS Collaborated with Prof. Yu-xin.
Convection Convection: transfer of heat by a flowing liquid or gas
The structure of neutron star by using the quark-meson coupling model Heavy Ion Meeting ( ) C. Y. Ryu Soongsil University, Korea.
1 On the importance of nucleation for the formation of quark cores inside compact stars Bruno Werneck Mintz* Eduardo Souza Fraga Universidade Federal do.
The Interior of Stars I Overview Hydrostatic Equilibrium
Neutron stars swollen under strong magnetic fields Chung-Yeol Ryu Soongsil University, Seoul, Korea Vela pulsar.
QUARK MATTER SYMMETRY ENERGY AND QUARK STARS Peng-cheng Chu ( 初鹏程 ) (INPAC and Department of Physics, Shanghai Jiao Tong University.
Cooling of CasA With&without Quark Matter CSQCD-IV- Prepow my ‘cool’ co-authors: D. Blaschke, D. Voskresensky Hovik Grigorian : Yerevan State University,
Thermodynamic Self- Consistency and Deconfinement Transition Zheng Xiaoping Beijing 2009.
The Sun and other stars. The physics of stars A star begins simply as a roughly spherical ball of (mostly) hydrogen gas, responding only to gravity and.
Equation Of State and back bending phenomenon in rotating neutron stars 1 st Astro-PF Workshop – CAMK, 14 October 2004 Compact Stars: structure, dynamics,
THIN ACCRETION DISCS AROUND NEUTRON AND QUARK STARS T. Harko K. S. Cheng Z. Kovacs DEPARTMENT OF PHYSICS, THE UNIVERSITY OF HONG KONG, POK FU LAM ROAD,
Lecture 7: Matter and Energy. Last Time… forms of energy: forms of energy:  kinetic  potential  radiative Law of Conservation of Energy Law of Conservation.
THERMAL EVOLUION OF NEUTRON STARS: Theory and observations D.G. Yakovlev Ioffe Physical Technical Institute, St.-Petersburg, Russia Catania, October 2012,
COOLING OF NEUTRON STARS D.G. Yakovlev Ioffe Physical Technical Institute, St.-Petersburg, Russia Ladek Zdroj, February 2008, 1. Formulation of the Cooling.
Evan Knight and Adam Mali UCORE, Summer ‘07 Under Prof. James Imamura and Kathy Hadley.
Qun Wang University of Science and Technology of China
Hadron-Quark phase transition in high-mass neutron stars Gustavo Contrera (IFLP-CONICET & FCAGLP, La Plata, Argentina) Milva Orsaria (FCAGLP, CONICET,
Neutron star core-quakes caused by a transition to the mixed-phase EOS mixed-phase linear response theory stellar models M. Bejger, collaboration with.
COOLING OF NEUTRON STARS D.G. Yakovlev Ioffe Physical Technical Institute, St.-Petersburg, Russia Ladek Zdroj, February 2008, 1. Formulation of the Cooling.
Quark-Gluon Plasma Sijbo-Jan Holtman.
Write answers on sheet of paper – 13, 16, 17, 20 Write answers for Objective 5 on card! 26, 32, 34.
K S Cheng Department of Physics University of Hong Kong Collaborators: W.M. Suen (Wash. U) Lap-Ming Lin (CUHK) T.Harko & R. Tian (HKU)
In this lecture we look at: 1) Neutron stars in x-ray binaries 2) Mass-radius relationship 3) Strange star candidates 4) Quark deconfinement at T=0 5)
带强磁场奇异星的 中微子发射率 刘学文 指导老师:郑小平 华中师范大学物理科学与技术学院. Pulsar In 1967 at Cambridge University, Jocelyn Bell observed a strange radio pulse that had a regular period.
1 ASTR 8000 STELLAR ATMOSPHERES AND SPECTROSCOPY Introduction & Syllabus Light and Matter Sample Atmosphere.
Heat and Thermal Energy Sources 14 Key Ideas Thermal energy influences temperature, density, pressure, and a substance’s physical state. Thermal energy.
Clustered Quark Model Calculation of Strange Quark Matter Xuesen Na Department of Astronomy, School of Physics, PKU CSQCD II.
Compact Stars With a Dyson- Schwinger Quark Model 1 陈 欢 Collaborate with 魏金标( CUG ), M. Baldo, F. Burgio and H.-J. Schulze ( INFN ). 2015“ 中子星与核天体物理 ”
Department of Physics, Sungkyunkwan University C. Y. Ryu, C. H. Hyun, and S. W. Hong Application of the Quark-meson coupling model to dense nuclear matter.
Cosmology Scale factor Cosmology à la Newton Cosmology à la Einstein
1 NJL model at finite temperature and chemical potential in dimensional regularization T. Fujihara, T. Inagaki, D. Kimura : Hiroshima Univ.. Alexander.
OBJECTIVE 3 Students will identify that density is a fundamental property of matter. Changes in pressure and temperature can change the density of a material.
Quark deconfinement in compact stars:
Quark deconfinement in compact stars: University of Ferrara, Italy
Quark star RX J and its mass
Effects of rotochemical heating on the thermal evolution of superfluid neutron stars HuaZhong Normal University Chun-Mei Pi & Xiao-Ping Zheng.
Phase transitions in neutron stars with BHF
Cooling of Neutron Stars
Bayesian analysis for hybrid star
Symmetry energy with non-nucleonic degrees of freedom
Equation of State for Hadron-Quark Mixed Phase and Stellar Collapse
States of Matter: Solid: Particles are packed closely
Chemical Equilibrium Mass transfer takes place from higher chemical potential to lower chemical potential. If the chemical potential of reactants are.
Effects of the φ-meson on the hyperon production in the hyperon star
Presentation transcript:

Xia Zhou & Xiao-ping Zheng The deconfinement phase transition in the interior of neutron stars Huazhong Normal University May 21, 2009 CSQCD Ⅱ

Outline  Phase transition and energy release  The thermal evolution of neutron stars  Summary

Phase transition and energy release The total energy and baryon number densities for the mixed phase With the volume fraction, energy per baryon The derivative of e with respect to ρ

Phase transition and energy release Energy release per baryon with respect to total baryon number From S to F, the total release energy can be expressed as The energy release per baryon during phase transition

Construct the hybrid stars: Hadronic phase: relativistic mean field theory (RMF) Quark phase: MIT bag model Mixed phase: baryon number conservation and global charge neutrality Phase transition and energy release

The baryon number density dependence of releasing energy per converted baryon for different bag constants Phase transition and energy release

The baryon number density dependence of releasing energy per converted baryon for soft, moderate and stiff hadronic matter equation of state Phase transition and energy release

Latent heat: chemical balance The absorbed energy per baryon during phase transition Heating term M. Stejner et.al ApJ, 694:1019, 2009

Phase transition and energy release Heating luminosity of deconfinement heating Heating luminosity of latent heat it is less important and does not significantly change the thermal evolution ( M. Stejner et.al ApJ, 694:1019, 2009)

Hybrid stars: neutron star with quark phase or mixed phase interiors. The mixed phase of hadronic and quark matter construct with Gibbs conditions The cooling equation: Heating effect: released dissipation energy during varying pressure first-order phase transition (deconfinement heating) The thermal evolution of neutron stars

Cooling curves of rotating hybrid star with deconfinement heating The thermal evolution of neutron stars

Surface temperature due to rotochemical heating and deconfinement heating in quasi-equilibrium state as a function of stellar radius The thermal evolution of neutron stars O. Kargaltsev et.al ApJ, 602:327,2004

Summary  The deconfinement dissipation would significantly influence the thermal evolution of neutron stars  For the older pulsars with high thermal radiation, the deconfinement dissipation heating mechanism is more effect under the hybrid stars model  We need more observational data