Jun. 27, 2013 @ Baryons2013, Glasgow Motoi Tachibana (Saga Univ.) Dark matter capture in neutron stars with exotic phases.

Slides:



Advertisements
Similar presentations
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 18 – Mass-radius relation for black dwarfs Chandrasekhar limiting mass Comparison.
Advertisements

Xavier Barcons Instituto de Física de Cantabria (CSIC-UC) On behalf of The Athena+ Co-ordination Group, the Athena+ Working Groups and Supporters A theme.
Questions and Probems. Matter inside protoneutron stars Hydrostatic equilibrium in the protoneutron star: Rough estimate of the central pressure is: Note.
White Dwarf Stars Low mass stars are unable to reach high enough temperatures to ignite elements heavier than carbon in their core become white dwarfs.
Ch.C. Moustakidis Department of Theoretical Physics Aristotle University of Thessaloniki Greece Equation of state for dense supernova matter 28o International.
Neutron Stars. Gradual compression of a stellar iron core  trans. [g cm -3 ] CompositionDegen. pressure Remarks Iron nuclei; nonrel. free e - nonrel.
Lecture 26: The Bizarre Stellar Graveyard: White Dwarfs and Neutron Stars.
Star Formation and the Interstellar Medium
End States Read Your Textbook: Foundations of Astronomy
Accretion Processes in GRBs Andrew King Theoretical Astrophysics Group, University of Leicester, UK Venice 2006.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Motoi Tachibana (Saga Univ.) Dark matter capture in compact stars -stellar constraints on dark matter- Oct. 20, 2014 @ QCS2014, KIAA, Beijin Dark matter.
Dark matter and stars Malcolm Fairbairn. Hertzsprung-Russell (luminosity-temperature) Diagram.
Neutron Stars and Black Holes
The role of neutrinos in the evolution and dynamics of neutron stars José A. Pons University of Alicante (SPAIN)  Transparent and opaque regimes.  NS.
Neutron Stars Chapter Twenty-Three.
The neutron radius of 208 Pb and neutron star structure. guitar nebula, neutron star bow wave.
Constraining Dark Matter Hai-Bo Yu University of Michigan, Ann Arbor USTC, 06/17/2011.
Neutron Star Formation and the Supernova Engine Bounce Masses Mass at Explosion Fallback.
Chandra Science Workshops Paul J Green  CXC-sponsored annual summer workshops focus on X-ray- related science topics.  Workshop size (80-120) and length.
P460 - Quan. Stats. III1 Nuclei Protons and neutrons in nuclei separately fill their energy levels: 1s, 1p, 1d, 2s, 2p, 2d, 3s…………… (we’ll see in 461 their.
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 17 – AGB evolution: … MS mass > 8 solar masses … explosive nucleosynthesis … MS.
The latest experimental evidence suggests that the universe is made up of just 4% ordinary matter, 23% cold dark matter and 73% dark energy. These values.
Primordial BHs. 2 Main reviews and articles astro-ph/ Primordial Black Holes - Recent Developments astro-ph/ Gamma Rays from Primordial.
1 Announcements There will be a star map on the exam. I will not tell you in advance what month. Grades are not yet posted, sorry. They will be posted.
Compact Objects Astronomy 315 Professor Lee Carkner Lecture 15 “How will we see when the sun goes dark?” “We will be forced to grope and feel our way.”
Lecture 4. Big bang, nucleosynthesis, the lives and deaths of stars. reading: Chapter 1.
New States of Matter and RHIC Outstanding questions about strongly interacting matter: How does matter behave at very high temperature and/or density?
Lecture 3 - Formation of Galaxies What processes lead from the tiny fluctuations which we see on the surface of last scattering, to the diverse galaxies.
Exotic Stars By Jason Fiola.
Dense Stellar Matter Strange Quark Matter driven by Kaon Condensation Hyun Kyu Lee Hanyang University Kyungmin Kim HKL and Mannque Rho arXiv:
Black Hole (BH)  Introduction to BH  Motivation to study BH  Formation of BH  Cool slides  Size of BH  Properties of BH  Evidence for BH.
Gravitational Waves from Massive Black-Hole Binaries Stuart Wyithe (U. Melb) NGC 6420.
JP ©1 2 3 Stars are born, grow up, mature, and die. A star’s mass determines its lifepath. Let M S = mass of the Sun = ONE SOLAR MASS Stellar Evolution.
AS2001 / 2101 Chemical Evolution of the Universe Keith Horne Room 315A
Motoi Tachibana (Saga Univ.) Dark matter capture in neutron stars -stellar constraints on dark matter- Oct. 25, 2013 @ NS matter symposium, Kyoto Dark.
AS2001 Chemical Evolution of the Universe Keith Horne 315a
Crystal Ball Collaboration Meeting, Mainz, October 2007 Claire Tarbert, Univeristy of Edinburgh Coherent  0 Photoproduction on Nuclei Claire Tarbert,
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
High Energy Nuclear Physics and the Nature of Matter Outstanding questions about strongly interacting matter: How does matter behave at very high temperature.
Neutron Star Binaries and Related Astrophysical Issues Chang-Hwan 1.
Black Holes Chapter 14. Review What is the life cycle of a low mass star (
Astronomy 1143 – Spring 2014 Lecture 30: Dark Matter Revisted…..
Classification The difference between a small star and a brown dwarf is fairly clear. If hydrogen fusion is taking place then the object is a dwarf star.
Introduction to CERN Activities
Neutron Star. Gravitational Crush The balance point to maintain degenerate matter is 1.4 M . When the mass of the core is greater than 1.4 M , electrons.
Death of Stars II Physics 113 Goderya Chapter(s): 14
Termination of Stars. Some Quantum Concepts Pauli Exclusion Principle: Effectively limits the amount of certain kinds of stuff that can be crammed into.
Nuclear Isovector Equation-of-State (EOS) and Astrophysics Hermann Wolter Dep. f. Physik, LMU Topics: 1.Phase diagram of strongly interacting matter and.
Death of sun-like Massive star death Elemental my dear Watson Novas Neutron Stars Black holes $ 200 $ 200$200 $ 200 $ 200 $400 $ 400$400 $ 400$400.
Semi-analytical model of galaxy formation Xi Kang Purple Mountain Observatory, CAS.
The cosmic connection There is a very close connection between particle physics and astrophysics. I’m going to show two examples: Type II supernovas Dark.
The Big Bang. Big Bang Theory A well tested Scientific Theory Widely accepted by the Scientific Community It explains the development of the Universe.
Stellar Evolution From Protostars to Black Holes.
Soichiro Isoyama Collaborators : Norichika Sago, Ryuichi Fujita, and Takahiro Tanaka The gravitational wave from an EMRI binary Influence of the beyond.
When a star dies…. Introduction What are compact objects? –White dwarf, neutron stars & black holes Why study? –Because it’s fun! –Test of physics in.
Supernova explosions. The lives of stars Type I supernovae –Destruction of white dwarfs Type II supernovae –Core collapse of massive stars What’s left.
Waseda univ. Yamada lab. D1 Chinami Kato
Announcements Quiz 7 due tonight, practice problems in Problem Sets 7A, 7B Approximate schedule for this week: Today: Finish Chapter 12, Chapter 13 Remainder.
EOS discussion.
Announcements Quiz 7 due tonight, practice problems in Problem Sets 7A, 7B Approximate schedule for this week: Today: Finish Chapter 12, Chapter 13 Remainder.
MERGING REVEALS Neutron Star INNARDS
Big World of Small Neutrinos
Primordial BHs.
Take out 2 sheets of paper for notes
Stars, Galaxies, and the Universe
High Energy Astrophysics: problems and expectations
Early Universe.
Black Holes Chapter 14.
Presentation transcript:

Jun. 27, 2013 @ Baryons2013, Glasgow Motoi Tachibana (Saga Univ.) Dark matter capture in neutron stars with exotic phases

A modern physics perspective “UROBOROS” = unity of matters & universe Galaxy Stars Sun Earth Mountain Human Atom Nuclei Particles Universe DNA astro physics cosmology nuclear particle physics chemistry biology

Interesting connection between matters and universe Dark Matter and Neutron Stars Harmony of particle, astro-, and condensed matter physics

What/Why dark matter (DM)? Undoubtedly exists, but properties unknown Just weakly-interacting with other particles Proposed by Zwicky as missing mass (1934)

arXiv: What/Why neutron star (NS)? Landau’s gigantic nucleus Good market selling ultimate environments Proposed by Baade and Zwicky as a remnant after supernova explosion (1934)

Why their connections? Possibly constraining WIMP-DM properties via NS For a typical neutron star, Way below the CDMS limit! NS may constrain the DM properties CDMSII,

Constraining the dark matter mass and its scattering cross section through the impacts on neutron stars Mass-radius relation with the DM EOS Cooling in the presence of dark matter : cf) This is not so a new idea. People have considered the DM capture by Sun and the Earth since 80’s. [W. Press and D. Spergel (1984) etc] (Asymmetric) dark matter capture in NS and black hole formation to collapse neutron stars

DM capture in NS *based on paper by McDermott-Yu-Zurek (2012) *

(1)Accretion of DM (1)Thermalization of DM (energy loss) (2)BH formation and destruction of host NS

(1) DM capture rate The accretion rate (A. Gould, 1987) neutron-DM elastic cross section

Capture efficiency factor ξ (i) If momentum transfer δp is less than p, only neutrons with momentum larger than p -δp can participate in (ii) If not, all neutrons can join F F In NS, neutrons are highly degenerated

(2) Thermalization of DM Thermalization time scale: If δp is less than p, then After the capture, DMs lose energy via scattering with neutrons and get thermalized with the star F

(3) Self–gravitation & BH formation If the DM density gets larger than the baryon density within thermal radius, DM particles be self-gravitating. This is the on-set of the gravitational collapse and black-hole formation (the Chandrasekhar limit) To avoid destruction of NS,

Observational constraints For the case of the pulsar B :

So far people have been mainly studying the issue from particle physics side. However, as I told you, hadrons in NS are in EXTREME, and exotic phases could appear. An idea (e.g.) neutron superfluidity Bose condensation of mesons superconductivity of quarks What if those effects are incorporated?

Possible effects ① Modification of capture efficiency via energy gap ② Modification of low-energy effective theory We are on the way of the calculations (e.g.) neutron superfluidity dominant d.o.f. is a superfluid phonon. Cirigliano, Reddy, Sharma (2011) (e.g.) color-flavor-locked(CFL) quark matter larger suppression On-going project w/ M. Ruggieri

Summary Constraining dark matter properties via neutron star --dark matter capture in neutron stars— Accretion, thermalization and on-set of BH formation Models for DM, but not considering NS seriously Proposal of medium effects for hadrons in NS --modified vacuum structures and collective modes--

Thank you