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Chiral Symmetry Restoration by Parity Doubling and the Structure of Neutron Stars
Chiral symmetry restoration by parity doubling and the structure of neutron stars Micha l Marczenko,1 David Blaschke,1, 2, 3 Krzysztof Redlich,1, 4 and Chihiro Sasaki1 1Institute of Theoretical Physics, University of Wroc law, PL-50204 Wroc law, Poland 2Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, 141980 Dubna, Russia 3National Research Nuclear University, 115409 Moscow, Russia 4Extreme Matter Institute EMMI, GSI, D-64291 Darmstadt, Germany (Dated: November 14, 2018) We investigate the equation of state for the recently developed hybrid quark-meson-nucleon model under neutron star conditions of β−equilibrium and charge neutrality. The model has the character- istic feature that, at increasing baryon density, the chiral symmetry is restored within the hadronic phase by lifting the mass splitting between chiral partner states, before quark deconfinement takes place. Most important for this study are the nucleon (neutron, proton) and N(1535) states. We present different sets for two free parameters, which result in compact star mass-radius relations in accordance with modern constraints on the mass from PSR J0348+0432 and on the compactness from GW170817. We also consider the threshold for the direct URCA process for which a new relationship is given, and suggest as an additional constraint on the parameter choice of the model that this process shall become operative at best for stars with masses above the range for binary radio pulsars, M > 1:4 M . I. INTRODUCTION neutron stars. However, already before this occurs, a strong phase transition manifests itself by the appearance The investigation of the equation of state (EoS) of com- of an almost horizontal branch on which the hybrid star pact star matter became rather topical within the past solutions lie, as opposed to the merely vertical branch of few years, mainly due to the one-to-one correspondence pure neutron stars. -
Convective Urca Process and Cooling in Dense Stellar Matter
Convective Urca Process and cooling in dense stellar matter M. Schoenberg: The name Urca was given by us to the process which accompanies the emission of neutrino in supernova because of the following curious situation: In Rio de Janeiro, we went to play at the Casino-da-Urca and Gamow was very impressed with the table in which there was a roulette, in which money disappeared very quickly. With a sense of humor, he said: ‘Well, the energy is being lost in the centre of supernova with almost the same rapidity as money does from these tables!’ (from Grib, Novello: “Gamow in rio and the discovery of the URCA process”, Astronom & Astrophys. Trans. 2000, Vol 19) Feb 10 2010, Advisor-Seminar WS09/10 by Fabian Miczek Urca reactions Urca pairs consist of mother (M) and daughter (D) nuclei Urca reactions A A − - beta decay: Z1M Z De e A − A - electron capture: Z De Z 1Me Central questions: Is a continuous cycling between mother and daugter possible? Both reactions emit a neutrino => possible cooling mechanism? 2 electron captures require a threshold energy Eth=EM−ED−me c beta decays release the threshold energy M We're interested in degenerate stellar matter (ideal gas of ions, Fermi gas of electrons) E th threshold energy can be provided by e- mc2 the Fermi energy of the electrons D Example (E = 4.4 MeV) 23 23 − th Na Nee e 23 − 23 Nee Nae Electron captures in degenerate matter Fermi energy > threshold energy assume zero temperature ( kT << E ) F A − A Z De Z 1 M e energy heat M neutrino Fermi electron threshold e- mc2 density of states D -
On the Theory of Gamma-Ray and Fast Radio Bursts
On the Theory of Gamma-ray and Fast Radio Bursts D. Skripachov Abstract Gamma-ray bursts are characterized by energy comparable to the rest mass of stars and duration comparable to the time of passage of light of several diameters of star. It means GRBs signal the flares occur when stars fall on supermassive neutron collapsars (SMNC) located at the centers of galaxies. Long, short, very short and weak GRBs are matched the fall of main sequence stars, white dwarfs, neutron stars (NS) and rogue planets, respectively. GRB is the result of heating of star caused by the action of three factors: transverse compression of angular convergence to SMNC, friction of light matter (LM), and volumetric compression of the entry into gravitationally distended space. GRB is a circular flare in the stellar corona. GRB lasts until the star will be hidden under the π- horizon, on which the angle of gravitational deflection of beams is 180°. Multiple peaks are caused by the fall of binary stars and stars with planets, as well as by consecutive bursts of stellar core and overlying layers. Early afterglow is due to the annihilation, and later (x-ray and radio) due to aurora and remanence of LM. FRB precedes very short GRB. Milliseconds before GRB, "magnetic lightning" arises, which is a reconnection of magnetic field lines from NS anterior pole to SMNC. Magnetic dipoles of LM nuclei are aligned along the magnetic lines of force. This is accompanied by radio emission generated strictly perpendicular magnetic tube connecting NS and SMNC. Gravitation bends the plane of FRB in the hyperboloid with the cone angle of 40°. -
Arxiv:1901.01410V3 [Astro-Ph.HE] 1 Feb 2021 Mental Information Is Available, and One Has to Rely Strongly on Theoretical Predictions for Nuclear Properties
Origin of the heaviest elements: The rapid neutron-capture process John J. Cowan∗ HLD Department of Physics and Astronomy, University of Oklahoma, 440 W. Brooks St., Norman, OK 73019, USA Christopher Snedeny Department of Astronomy, University of Texas, 2515 Speedway, Austin, TX 78712-1205, USA James E. Lawlerz Physics Department, University of Wisconsin-Madison, 1150 University Avenue, Madison, WI 53706-1390, USA Ani Aprahamianx and Michael Wiescher{ Department of Physics and Joint Institute for Nuclear Astrophysics, University of Notre Dame, 225 Nieuwland Science Hall, Notre Dame, IN 46556, USA Karlheinz Langanke∗∗ GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany and Institut f¨urKernphysik (Theoriezentrum), Fachbereich Physik, Technische Universit¨atDarmstadt, Schlossgartenstraße 2, 64298 Darmstadt, Germany Gabriel Mart´ınez-Pinedoyy GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany; Institut f¨urKernphysik (Theoriezentrum), Fachbereich Physik, Technische Universit¨atDarmstadt, Schlossgartenstraße 2, 64298 Darmstadt, Germany; and Helmholtz Forschungsakademie Hessen f¨urFAIR, GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany Friedrich-Karl Thielemannzz Department of Physics, University of Basel, Klingelbergstrasse 82, 4056 Basel, Switzerland and GSI Helmholtzzentrum f¨urSchwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany (Dated: February 2, 2021) The production of about half of the heavy elements found in nature is assigned to a spe- cific astrophysical nucleosynthesis process: the rapid neutron capture process (r-process). Although this idea has been postulated more than six decades ago, the full understand- ing faces two types of uncertainties/open questions: (a) The nucleosynthesis path in the nuclear chart runs close to the neutron-drip line, where presently only limited experi- arXiv:1901.01410v3 [astro-ph.HE] 1 Feb 2021 mental information is available, and one has to rely strongly on theoretical predictions for nuclear properties. -
Arxiv:2008.04340V2 [Astro-Ph.HE] 7 Dec 2020
SLAC-PUB-17548 Exciting Prospects for Detecting Late-Time Neutrinos from Core-Collapse Supernovae Shirley Weishi Li,1, 2, 3, ∗ Luke F. Roberts,4, y and John F. Beacom1, 2, 5, z 1Center for Cosmology and AstroParticle Physics (CCAPP), Ohio State University, Columbus, OH 43210 2Department of Physics, Ohio State University, Columbus, OH 43210 3SLAC National Accelerator Laboratory, Menlo Park, CA, 94025 4National Superconducting Cyclotron Laboratory and Department of Physics and Astronomy, Michigan State University, East Lansing, MI 48824 5Department of Astronomy, Ohio State University, Columbus, OH 43210 (Dated: December 7, 2020) The importance of detecting neutrinos from a Milky Way core-collapse supernova is well known. An under-studied phase is proto-neutron star cooling. For SN 1987A, this seemingly began at about 2 s, and is thus probed by only 6 of the 19 events (and only theν ¯e flavor) in the Kamiokande-II and IMB detectors. With the higher statistics expected for present and near-future detectors, it should be possible to measure detailed neutrino signals out to very late times. We present the first comprehensive study of neutrino detection during the proto-neutron star cooling phase, considering a variety of outcomes, using all flavors, and employing detailed detector physics. For our nominal model, the event yields (at 10 kpc) after 10 s|the approximate duration of the SN 1987A signal| far exceed the entire SN 1987A yield, with '250ν ¯e events (to 50 s) in Super-Kamiokande, '110 νe events (to 40 s) in DUNE, and '10 νµ; ντ ; ν¯µ; ν¯τ events (to 20 s) in JUNO. -
Participant List Xiamen-CUSTIPEN Workshop, Xiamen, January 3 to 7, 2019
Participant list Xiamen-CUSTIPEN Workshop, Xiamen, January 3 to 7, 2019 No. Name Affiliation Email 01 Shunke Ai 艾舜轲 Beijing Normal University, China [email protected]. edu.cn 02 Nils Andersson University of Southampton, UK N.A.Andersson@sot on.ac.uk Contribution Title: Using gravitational waves to constrain matter at extreme densities Abstract: The spectacular GW170817 neutron star merger event provided interesting constraint on neutron star physics (in terms of the tidal deformability). Future detections are expected improve on this. In this talk I will discuss if we can expect to also make progress on issues relating to the composition and state of matter. 03 Zhan Bai 摆展 Peking University, China [email protected] n Contribution Title: Constraining Hadron-Quark Phase Transition Chemical Potential via Astronomical observation 04 Shishao Bao 鲍世绍 Shanxi Normal University, China [email protected] du.cn 05 Andreas Bauswein GSI Darmstadt, Germany Andreas.Bauswein @h-its.org Contribution Title: Neutron star mergers and the high-density equation of state 06 Subrata kumar Biswal Institute of Theoretical Physics, [email protected] Chinese Academy of Sciences, China Contribution Title: Effects of the φ-meson on the hyperon production in the hyperon star Abstract: Using relativistic mean field formalism, we have studied the effects of the strange vector φ-meson on the equation of state and consequently on the maximum mass and radius of the hyperon star. Effects of the hyperon coupling constants on the strangeness content of the hyperon star are discussed with a number of the relativistic parameter set. The canonical mass-radius relationship also discussed with various relativistic parameter set. -
The Single Degenerate Progenitor Scenario for Type Ia Supernovae and the Convective Urca Process
The Single Degenerate Progenitor Scenario for Type Ia Supernovae and the Convective Urca Process ADissertationpresented by Donald Eugene Willcox to The Graduate School in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy in Physics Stony Brook University August 2018 Stony Brook University The Graduate School Donald Eugene Willcox We, the dissertation committe for the above candidate for the Doctor of Philosophy degree, hereby recommend acceptance of this dissertation Alan Calder – Dissertation Advisor Associate Professor, Physics and Astronomy Michael Zingale – Chairperson of Defense Associate Professor, Physics and Astronomy Joanna Kiryluk – Committee Member Associate Professor, Physics and Astronomy Matthew Reuter – External Committee Member Assistant Professor, Applied Mathematics and Statistics This dissertation is accepted by the Graduate School Charles Taber Dean of the Graduate School ii Abstract of the Dissertation The Single Degenerate Progenitor Scenario for Type Ia Supernovae and the Convective Urca Process by Donald Eugene Willcox Doctor of Philosophy in Physics Stony Brook University 2018 This dissertation explores the e↵ects of properties of the progenitor massive white dwarf (WD) on thermonuclear (Type Ia) supernovae. It includes a study of explosions from “hy- brid” C/O/Ne progenitors and focuses primarily on the convective Urca process occurring in C/O progenitors shortly before their explosion. Pre-supernova WDs approaching the Chan- drasekhar mass can possess sufficiently high central densities that 23Na synthesized via 12C fusion undergoes electron capture to 23Ne. Convection sweeps 23Ne to regions of lower den- sity where it reverts via beta decay to 23Na, and vice versa. Cyclic weak nuclear processes of this type constitute the convective Urca process in WDs. -
Acknowledgments
Acknowledgments J. Arons: I have benefitted from many discussions with A. Spitkovsky, P. Chang, N. Bucciantini, E. Amato, R. Blandford, F. Coroniti, D. Backer and E. Quataert. My research efforts on these topics have been supported by NSF grant AST-0507813 and NASA grant NNG06G108G, both to the University of California, Berkeley; by the Department of Energy contract to the Stanford Linear Accelerator Center no. DE-AC3-76SF00515; and by the taxpayers of California. W. Becker: I’m grateful to the Heraeus-Foundation for financing the 363rd Heraeus-Seminar on Neutron Stars and Pulsars which took place in May 2006 at the Physikzentrum in Bad Honnef. A selection of papers presented at this meet- ing and at the IAU Joined Discussion JD02 in Prague in August 2006 became the groundwork to produce this book. I’m further thankful to Joachim Trumper¨ and Harald Lesch for their help and support in organizing the Heraeus-Seminar and to Gunther¨ Hasinger as well as the MPE for additional financial support. Without the great organizational talent and help of Christa Ingram the meetings would not have been what they were. Thanks also for her help in producing this book. Christian Saedtler has spend many days in producing the index of this book. Sincere thanks to him for taking the time. All articles in this book were refereed. I am much obliged to all colleagues who helped in this process. Special thanks goes to Dr. Jaroslaw Dyks, Dr. Ulrich Geppert, Prof. Dr. Yashwant Gupta, Dr. John Kirk, Dr. Maura McLaughlin, Prof. Dr. Andreas Reisenegger and Prof. -
Pos(Confinement8)151
Cooling of isolated neutron stars as a probe of PoS(Confinement8)151 superdense matter physics Alexander Kaminker∗, Alexander Potekhin and Dmitry Yakovlev Ioffe Physical Technical Institute - Politekhnicheskaya 26, 194021 Saint-Petersburg, Russia E-mail: [email protected], [email protected], [email protected] We review a current state of cooling theory of isolated neutron stars. The main regulators of neutron star cooling are discussed. We outline the sensitivity of cooling models to equation of state of matter in the neutron star core; the presence or absence of enhanced neutrino emission; superfluidity of baryonic component of matter. A comparison of the cooling theory with observa- tions of thermal emission of isolated neutron stars gives a potentially powerful method to study fundamental properties of superdense matter in neutron star interiors. The prospects of studying neutron star parameters and internal structure are outlined. 8th Conference Quark Confinement and the Hadron Spectrum September 1-6, 2008 Mainz. Germany ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it/ Cooling of isolated neutron stars as a probe of superdense matter physics Alexander Kaminker 1. Introduction Microscopic theories of superdense matter in neutron star cores are model dependent and give a vast scatter of possible equation of states (EOSs) (e.g., [1, 2]) with different composition of neu- tron star cores (nucleons, hyperons, pion or kaon condensates, quarks), and different superfluid properties of baryons. The fundamental properties of supranuclear matter cannot be determined on purely theoretical basis, but viable theoretical models can be selected by comparing their predic- tions with observations of neutron stars. -
Implication for the Core-Collapse Supernova Rate from 21 Years of Data of the Large Volume Detector
IMPLICATION FOR THE CORE-COLLAPSE SUPERNOVA RATE FROM 21 YEARS OF DATA OF THE LARGE VOLUME DETECTOR The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Agafonova, N. Y., M. Aglietta, P. Antonioli, V. V. Ashikhmin, G. Badino, G. Bari, R. Bertoni, et al. “IMPLICATION FOR THE CORE-COLLAPSE SUPERNOVA RATE FROM 21 YEARS OF DATA OF THE LARGE VOLUME DETECTOR.” The Astrophysical Journal 802, no. 1 (March 20, 2015): 47. © 2015 The American Astronomical Society As Published http://dx.doi.org/10.1088/0004-637x/802/1/47 Publisher IOP Publishing Version Final published version Citable link http://hdl.handle.net/1721.1/97081 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. The Astrophysical Journal, 802:47 (9pp), 2015 March 20 doi:10.1088/0004-637X/802/1/47 © 2015. The American Astronomical Society. All rights reserved. IMPLICATION FOR THE CORE-COLLAPSE SUPERNOVA RATE FROM 21 YEARS OF DATA OF THE LARGE VOLUME DETECTOR N. Y. Agafonova1, M. Aglietta2, P. Antonioli3, V. V. Ashikhmin1, G. Badino2,7, G. Bari3, R. Bertoni2, E. Bressan4,5, G. Bruno6, V. L. Dadykin1, E. A. Dobrynina1, R. I. Enikeev1, W. Fulgione2,6, P. Galeotti2,7, M. Garbini3, P. L. Ghia8, P. Giusti3, F. Gomez2, E. Kemp9, A. S. Malgin1, A. Molinario2,6, R. Persiani3, I. A. Pless10, A. Porta2, V. G. Ryasny1, O. G. Ryazhskaya1, O. Saavedra2,7, G. -
Thermal Spectrum and Neutrino Cooling Rate of the Vela Pulsar
Article Thermal Spectrum and Neutrino Cooling Rate of the Vela Pulsar Dmitry D. Ofengeim and Dmitry A. Zyuzin Ioffe Institute, 26 Politekhnicheskaya str., St. Petersburg 194021, Russia; [email protected] * Correspondence: [email protected]; Tel.: +7-812-292-7180 Received: 22 June 2018; Accepted: 24 July 2018; Published: 30 July 2018 Abstract: We reanalyse the X-ray spectrum of the PSR B0833–45 (the Vela pulsar) using the data of the Chandra space observatory. In contrast to previous works, we consider a wide range of possible masses ¥ +0.04 and radii of the pulsar. The derived surface temperature of the star Ts = 0.66−0.01 MK (1s level over the entire mass and radius range of our study) is consistent with earlier results. However, the preferable values of Vela’s mass and radius given by the spectral analysis are different from those used previously; they are consistent with modern equation of state models of neutron star matter. In addition, we evaluate the Vela’s surface temperature as a function of assumed values of its mass and radius. This allows us to analyse the neutrino cooling rates consistent with the evaluated surface temperatures and explore the additional restrictions that could be set on the Vela’s mass and radius using different versions of the neutron star cooling theory. Keywords: the Vela pulsar; X-ray spectrum; neutrino cooling rate 1. Introduction In this presentation, we reanalyze the observations of the X-ray surface emission of the Vela pulsar ¥ (PSR B0833-45) and evaluate its effective surface temperature Ts (redshifted for a distant observer), mass M, radius R and the internal neutrino cooling rate using the cooling theory of neutron stars (NSs) [1]. -
Dependence of Failed Supernova on Progenitor Models
Dependence of failed supernova on progenitor models Kazuki Onogi,Hideyuki Suzuki Tokyo University of Science,Noda Chiba 278-8510,Japan Failed supernova We study the ejection of mass during stellar core-collapse when the stalled shock does not revive and a black hole forms. Phenomenon Neutrino emission during the protoneutron star phase reduces the gravitational mass of the core, resulting in an outward going sound pulse that steepens into a shock as it travels out through the star. Purpose Identify the dependence on neutrino emission and progenitor model Method and models We use 1D stellar evolution code MESA and 1D time-dependent hydrodynamic simulation which can treat neutrino mass loss parametrically. We use exponential neutrino cooling model which is same as Fernandez(2017) MG: gravitational mass of protoneutron star MB:the baryonic mass of protoneutron star BEC: the binding energy of a cold neutron star , M* ��# = 0.084 M⊙ τc: neutrino cooling time(~3s) M⊙ This model emit most of the energy as neutrino Stop the neutrino emission once in �4. the black hole form � = 0.1�, � = 2.0� 4 9:; ⨀ Results Fig 1 is a velocity profile of the star. It shows the shock propagate toward the surface of the star. The protoneutron star is also extremely hot and thus behaves in different manner from cold neutron stars. change the paremeter neutrino cooling time �? ,maximum Fig 1:shock propagation mass of neutron star systematically (0.1s ≤ �? ≤ 5.0s, 2.2M⊙ ≤ �9:; ≤ 2.8M⊙) �9:; = 2.6�⨀ Fig2 shows the velocity profile with different τc after shock breakout. the case, �? = 5.0s shows lower energy because the time reaching to the maximum mass of netron star is around 5s.