Quark deconfinement in compact stars and GRBs structure Alessandro Drago University of Ferrara.

Slides:



Advertisements
Similar presentations
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,
Advertisements

Questions and Probems. Matter inside protoneutron stars Hydrostatic equilibrium in the protoneutron star: Rough estimate of the central pressure is: Note.
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.
Ilona Bednarek Ustroń, 2009 Hyperon Star Model.
Strangeness barrierhttp://vega.bac.pku.edu.cn/rxxu R. X. Xu Renxin Xu School of Physics, Peking University ( ) 1 st bilateral meeting on “Quark and Compact.
Internal structure of Neutron Stars. Artistic view.
The neutron radius of 208 Pb and neutron star structure. guitar nebula, neutron star bow wave.
Cosmology The Origin and Future of the Universe Part 2 From the Big Bang to Today.
Cooling of Compact Stars with Color Superconducting Quark Matter Tsuneo Noda (Kurume Institute of Technology) Collaboration with N. Yasutake (Chiba Institute.
Thomas Klähn D. Blaschke R. Łastowiecki F. Sandin Sept 2, 2011Thomas Klähn – Symposium on NeD, Heraklion.
Symmetry energy in the era of advanced gravitational wave detectors Hyun Kyu Lee Hanyang University Heavy Ion Meeting , Asan Science Hall, Korea.
Thomas Klähn D. Blaschke R. Łastowiecki F. Sandin Thomas Klähn – Three Days on Quarkyonic Island.
Black holes: Introduction. 2 Main general surveys astro-ph/ Neven Bilic BH phenomenology astro-ph/ Thomas W. Baumgarte BHs: from speculations.
Xia Zhou & Xiao-ping Zheng The deconfinement phase transition in the interior of neutron stars Huazhong Normal University May 21, 2009 CSQCD Ⅱ.
Metastability of Hadronic Compact Stars I. Vidaña & I. Bombaci, P. K. Panda, C. Providência “The Complex Physics of Compact Stars” Ladek Zdroj, Poland,
The high density QCD phase transition in compact stars Giuseppe Pagliara Institut für Theoretische Physik Heidelberg, Germany Excited QCD 2010, Tatra National.
Thermal Evolution of Rotating neutron Stars and Signal of Quark Deconfinement Henan University, Kaifeng, China Miao Kang.
Constraining neutron star properties with perturbative QCD Aleksi Vuorinen University of Helsinki University of Oxford Main reference: Kurkela,
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.
Dark Matter begin. Definition Dark Matter is matter that we cannot see. It neither emits nor reflects any light. If we can’t see it, how do we know it.
Internal structure of Neutron Stars. Artistic view.
1 On the importance of nucleation for the formation of quark cores inside compact stars Bruno Werneck Mintz* Eduardo Souza Fraga Universidade Federal do.
Dense Stellar Matter Strange Quark Matter driven by Kaon Condensation Hyun Kyu Lee Hanyang University Kyungmin Kim HKL and Mannque Rho arXiv:
Neutron stars swollen under strong magnetic fields Chung-Yeol Ryu Soongsil University, Seoul, Korea Vela pulsar.
Internal structure of Neutron Stars. Artistic view.
Institut d’Astronomie et d’Astrophysique Université Libre de Bruxelles Structure of neutron stars with unified equations of state Anthea F. FANTINA Nicolas.
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,
Hypernucleus In A Two Frequency Model Yiharn Tzeng, S.Y.Tsay Tzeng, T.T.S.Kuo.
Origins: Dark Matter & Dark Energy WWK: Students will understand the theories of Dark Matter & Dark Energy and how they’re thought to affect the Universe.
Chiral phase transition and chemical freeze out Chiral phase transition and chemical freeze out.
Phase transition induced collapse of Neutron stars Kim, Hee Il Astronomy Program, SNU 13th Haengdang Symposium, 11/30/2007.
Many-body theory of Nuclear Matter and the Hyperon matter puzzle M. Baldo, INFN Catania.
Neutrino mass and DM direct detection Daijiro Suematsu (Kanazawa Univ.) Erice Sept., 2013 Based on the collaboration with S.Kashiwase PRD86 (2012)
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)
Asymmetric Neutrino Reaction in Magnetized Proto-Neutron Stars in Fully Relativistic Approach Tomoyuki Maruyama BRS, Nihon Univ. (Japan) Tomoyuki Maruyama.
Gamma-Ray-Bursts in Nuclear Astrophysics Giuseppe Pagliara Dip. Fisica Politecnico di Torino INFN-Ferrara XI Convegno su Problemi di Fisica Nucleare Teorica.
Nuclear Isovector Equation-of-State (EOS) and Astrophysics Hermann Wolter Dep. f. Physik, LMU Topics: 1.Phase diagram of strongly interacting matter and.
Holographic QCD in the medium
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.
CEBAF - Continuous Electron Beam Accelerator Facility.
Hybrid proto-neutron stars within a static approach. O. E. Nicotra Dipartimento di Fisica e Astronomia Università di Catania and INFN.
Some theoretical aspects of Magnetars Monika Sinha Indian Institute of Technology Jodhpur.
Clustered Quark Model Calculation of Strange Quark Matter Xuesen Na Department of Astronomy, School of Physics, PKU CSQCD II.
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.
Maximum Mass of Neutron Stars with Hadron-Quark Transient Core □Introduction □Universal 3-body force □Approach by 3-Window Model □Some results
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 ”
Nuclear Fission and Fusion Chapter 10.2 Notes. Nuclear Forces Protons and neutrons are tightly packed inside the nucleus Remember that unstable nuclei.
By the end of this presentation, you should be able to: Select and use Coulomb’s law to determine the force of repulsion, and Newton’s law of gravitation.
Matter-antimatter coexistence method for finite density QCD
The nuclear EoS at high density
Neutron star radii and the EOS of neutron-rich matter
Correspondence of Many-flavor Limit and Kaluza-Klein Degrees of Freedom in the Description of Compact Stars Szilvia KARSAI Wigner Research Centre for Physics.
Microscopic Equations of State
Quark deconfinement in compact stars:
Quark deconfinement in compact stars: University of Ferrara, Italy
EOS discussion.
Quark star RX J and its mass
Internal structure of Neutron Stars
Stellar core collapse with QCD phase transition
The quark-deconfinement model of Gamma-Ray-Bursts
Hyperon mixing and universal many-body repulsion in neutron stars
INFN Sezione di Catania
Phase transitions in neutron stars with BHF
Internal structure of Neutron Stars
Internal structure of Neutron Stars
Symmetry energy with non-nucleonic degrees of freedom
Early Universe.
Internal structure of Neutron Stars
Effects of the φ-meson on the hyperon production in the hyperon star
Presentation transcript:

Quark deconfinement in compact stars and GRBs structure Alessandro Drago University of Ferrara

Outline What do we learn from the existence of stars of 2 M s ? Are hyperons excluded? Are hybrid quark-hadron stars excluded? Are quark stars excluded? Are radii smaller than about 10 km excluded by theory? – Two families co-existence hypothesis : hadronic stars and quark stars A. D., A. Lavagno and G. Pagliara; arXiv: A few observational facts about long GRBs – Quiescent times: an open problem – The «quark deconfinement» interpretation The magnetar model for GRBs ( Usov92, Thompson 94, Metzger, Bucciantini et al) and how it can incorporate quark deconfinement to explain long quiescent times

What do we learn from the existence of stars of 2 M s ?

Strangeness production In heavy ion experiments strangeness can be produced only by strong- interaction and therefore via associated production (weak interaction does not have time to take place). The typical fraction of strangeness is less than 10% In a compact star strangeness is mainly produced by weak interaction. Hyperons «normally» start appearing at densities above (2.5 – 3) r 0 Hyperons can significantly soften the EoS: is it possible to have a 2 M s compact star with hyperons? Yes, but…

Hyperons in b -stable matter

Hyperonic stars in a non-relativistic BHF with parametrised 3-body forces between hyperons Vidana et al. Europhys.Lett. 94 (2011) body forces are not sufficent to reach two solar masses The central density is very large, 5 – 9 r 0 A relativistic approach could be needed stiffer and softer pure nucleonic EoS (curves 1 and 2) stiffer and softer hyperonic stars (curves 3 and 4) Radius of a purely nucleonic star about 12 km

Borrowed from I. Vidana Radii for a 1.4 M s hyperonic star are about km

Basic questions Threshold for L : m n = m L Possibilities: – to reduce the mass of the nucleon, since m n = (m n * 2 + K f 2 ) ½ + … – to increase the chemical potential of the L 1.How much can the mass of the nucleon be reduced? 2.How strongly repulsive can be the YNN, YYN, YYY three-body forces? Can it be much more repulsive than NNN three-body force at high density?

Struggling with hybrid stars Ippolito et al. Phys.Rev. D77 (2008) Zdunik and Haensel A&A, 551 (2013) A61 It is not impossible to satisfy the 2 M s limit with a hybrid star but special limits on the parameters’ values have to be imposed Radius of a 1.4 M s hybrid star: km

Cold quark matter: a perturbative QCD approach Kurkela, Romatschke, Vuorinen ; Phys.Rev. D81 (2010) “ … equations of state including quark matter lead to hybrid star masses up to 2M s, in agreement with current observations. For strange stars, we find maximal masses of 2.75M s and conclude that confirmed observations of compact stars with M > 2M s would strongly favor the existence of stable strange quark matter”

Passing the test with quark stars Weissenborn et al.; Astrophys.J. 740 (2011) L14 It is not particularly difficult to reach masses larger than 2 M s in the case of quark stars. In principle even larger masses can be obtained.

A remark concerning «history» M.Alford, D.Blaschke, A.Drago, T.Klaehn, G.Pagliara, J.Schaffner-Bielich Nature, 445 (2007) E7 Based on papers published before 2006 Radii for a 1.4 M s star larger than 11 km

About masses and radii Hebeler, Lattimer, Pethick, Schwenk ApJ773(2013)11 Analysis based on politropic expansion: R 1.4 > 10 km Explicit model calculations indicate a even slightly larger limit If a 2.4 M s star will be discovered, then R 1.4 > 12 km !

First «conclusion» It is possible to reach two solar masses with hyperonic and with hybrid stars, although tight limits on the parameters’ space have to be imposed. The two solar mass constraint can be satisfied more easily with quark stars (but it is unlikely that ALL compact stars are quark stars). The radii of a 1.4 M s star are larger than about (10 ― 10.5) km if all compact stars are either nucleonic or hadronic or hybrid stars. If a 2.4 M s star exists then radii smaller than about 12 km are ruled out if all compact stars belong to one family.

Are radii smaller than 10 km ruled out by microphysics? (and what if a 2.4 M s will be discovered?)

Analysis of 5 QLMXBs Guillot et al. ApJ772(2013)7 Lattimer and Steiner

Guillot et al. ApJ772(2013)7 analysis of 5 QLMXBs

The role of delta resonances Schurhoff, Schramm, Dexheimer ApJ 724 (2010) L74 The delta-nucleon mass splitting at nuclear matter saturation can be tested via electron-nucleus scattering and therefore cannot be increased almost arbitrary as for the Lambda-nucleon mass splitting. It could therefore be difficult to eliminate delta resonances (and the associate softening) from compact stars!

How to have small radii and large masses with two types of compact stars A.D., A. Lavagno, G. Pagliara arXiv: The hadronic star will not transform into a quark star till the moment in which hyperons start appearing, or slightly later. In this way stars with radii of the order of 10 km or smaller are possible and those stars are mainly made of nucleons and Δ-resonances. The most heavy stars would instead be quark stars. Stars with a mass smaller than about 1.5 M s would be composed of nucleons and of D resonances. Their properties concerning e.g. stability under rapid rotation would be similar to purely nucleonic stars. They would also have a crust. Most of the features of supermassive stars would instead differ from those of normal neutron stars.

Signatures of a two family scenario The energy released in the conversion from hadrons to quarks is typically of the order of erg, large enough to produce a neutrino flux able to revitalize a failed SN explosion. A few GRBs could be associated with the conversion from hadrons to quarks. In particular GRBs not associated with a SN can exist. Also suggests GRBs with «two» active periods. The radius of the most massive stars is expected to be large instead of relatively small. The most massive stars should be anomalous concerning e.g.: – «crust» vibration – Cooling – Caracteristic of an outburst associated with mass accretion – … A few (rare) stars with small masses and small radii can exist Stars with a mass significantly larger than 2 M s can exist

What can we learn from measuring the radii of compact stars? If all measured radii will be of the order of about 12 km we will be able to exclude certain solutions (e.g. the ones based on very stiff phenomenological EOSs at low-moderate densities). – «Exotica» will likely be present in at least the more heavy stars. – There will be no need to speculate about the existence of quark stars. If instead at least a few stars will be found to have radii of the order of 10 km or smaller, than most likely there are two families of compact stars – The most heavy objects will be quark stars. – Stars of normal mass will not contain significant amount of hyperons or strange quarks. They will behave similarly to nucleonic stars. LOFT and NICER should be able to distinguish between these two possibilities

Conclusions The possible co-existence of two families of compact stars is suggested by recent analysis of their masses and radii, but better data for the radii are needed. The transition from a hadronic star to a quark star releases about erg, mainly in neutrinos. This energy (together with the one associated with the rotation of the star) can be sufficient to power a GRB. The time structure of long GRBs suggests the existence of long quiescent times (from seconds up to a few hundred seconds) separating «two» active periods. Quark deconfinement in the compact star can be at the origin of the second active period. Possibility to integrate this mechanism into the proto-magnetar model. Also the possible existence of GRBs not associated with a SN can be explained by the mechanism based on quark deconfinement.

M-R relations and parameters’ value Kosov, Fuchs, Marmyanov, Faessler, PLB 421 (1998) 37

Composition of matter without and with D -resonances D -resonances can take the place of hyperons, pushing the hyperons’ threshold to larger densities