黎卓 HB Perets, JC Lombardi Jr, SR Milcarek Jr JUNO会议,南京,2016/4/17-18

Slides:



Advertisements
Similar presentations
The Physics of Supernovae
Advertisements

Who are the usual suspects? Type I Supernovae No fusion in white dwarf, star is supported only by electron degeneracy pressure. This sets max mass for.
Accretion Processes in GRBs Andrew King Theoretical Astrophysics Group, University of Leicester, UK Venice 2006.
Gamma-Ray bursts from binary neutron star mergers Roland Oechslin MPA Garching, SFB/TR 7 SFB/TR7 Albert Einstein‘s Century, Paris,
Stars and the HR Diagram Dr. Matt Penn National Solar Observatory
Jets from stellar tidal disruptions by supermassive black holes Dimitrios Giannios Princeton University HEPRO3, Barcelona, June 30.
Black holes: Introduction. 2 Main general surveys astro-ph/ Neven Bilic BH phenomenology astro-ph/ Thomas W. Baumgarte BHs: from speculations.
Understanding LMXBs in Elliptical Galaxies Vicky Kalogera.
Kick of neutron stars as a possible mechanism for gamma-ray bursts Yong-Feng Huang Department of Astronomy, Nanjing University.
Gamma Ray Bursts and LIGO Emelie Harstad University of Oregon HEP Group Meeting Aug 6, 2007.
X-ray Binaries in Nearby Galaxies Vicky Kalogera Northwestern University Super Star Clusters Starburst galaxies Ultra-Luminous X-Ray Sources Elliptical.
High-energy emission from the tidal disruption of stars by massive black holes Xiang-Yu Wang Nanjing University, China Collaborators: K. S. Cheng(HKU),
Stellar Disruptions of Super Massive Black Holes Ron Caplan March 7, 2003.
Black holes: do they exist?
He star evolutionary channel to intermediate-mass binary pulsars with a short-orbital-period Chen Wen-Cong School of Physics, Peking University Department.
Star Clusters and their stars Open clusters and globular clusters General characteristics of globular clusters Globular cluster stars in the H-R diagram.
Quasars, black holes and galaxy evolution Clive Tadhunter University of Sheffield 3C273.
Black Hole Chaos The Environments of the most super- massive black holes in the Universe Belinda Wilkes, Chandra X-ray Center, CfA Francesca Civano, CfA.
Double NS: Detection Rate and Stochastic Background Tania Regimbau VIRGO/NICE.
Collapsar Accretion and the Gamma-Ray Burst X-Ray Light Curve Chris Lindner Milos Milosavljevic, Sean M. Couch, Pawan Kumar.
Dec. 6, Review: >8Msun stars become Type II SNe As nuclear burning proceeds to, finally, burning Silicon (Si) into iron (Fe), catastrophe looms.
Population of dynamically formed triples in dense stellar systems Natalia Ivanova Fred Rasio, Vicky Kalogera, John Fregeau, Laura Blecha, Ryan O'Leary.
A Tidal Disruption model for gamma-ray burst of GRB YE LU National Astronomical Observatories, Chinese Academy of Sciences June 22-27, 2008 Nanjing.
Dec. 11, Review Neutron Stars(NSs) and SNR (Crab Nebula…) and then on to BHs… SN-II produce a NS for massive stars in approx. range 8-15Msun; and.
Supercritical Accretion in the Evolution of Neutron Star Binaries and Its Implications Chang-Hwan 1 Nuclear Physics A 928 (2014)
Progenitor stars of supernovae Poonam Chandra Royal Military College of Canada.
Tidal Disruption Events
Gamma-Ray Bursts Please press “1” to test your transmitter.
Gravitational wave sources
Waseda univ. Yamada lab. D1 Chinami Kato
Astrophysics: 2016 highlights and the way forward
Neutron Stars and Black Holes
The Fate of High-Mass Stars
Long GRB rate in the binary merger model
On recent detection of a gravitational wave from double neutron stars
Virgo cluster survey with MXT
Rebecca Surman Union College
Short-Duration Gamma-Ray Burst Central Engines
Supernovae and Gamma-Ray Bursts
Supernovae.
Chapter 21 Galaxy Evolution
The “Milky Way”.
Neutron Stars and Black Holes
No BH at the GC and Supernova Explosion Driven by Magnetic Molopoles
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.
Double NS: Detection Rate and Stochastic Background
Short Gamma Ray Bursts Curtis DeWitt.
Neutrinos as probes of ultra-high energy astrophysical phenomena
Paola Rodriguez Hidalgo High Energy Astrophysics
M. Benacquista Montana State University-Billings
Galaxies.
Stellar Explosions Novae White dwarf in close binary system
GRB-Supernova observations: State of the art
Star Clusters and their stars
Delay time distribution of type Ia supernovae
The Deaths of Stars.
Star-planet coalescence
Dongyue Li 2018/4/27 Ref: Saxton et al Esquej et al. 2008, 2012
Galaxies.
Black holes: observations Lecture 1: Introduction
Galaxies With Active Nuclei
Gamma-Ray Bursts Ehud Nakar Caltech APCTP 2007 Feb. 22.
Super Massive Black Holes
Galaxies With Active Nuclei
Black holes: observations Lecture 1: Introduction
Galaxies.
Clusters Clusters and Age Stars are born from molecular clouds
Evolutionary Link between X-ray Pulsars and Millisecond Radio Pulsars
Transient emission associated with the birth of neutron stars
Gamma-Ray Bursts: Death of a Star and the Birth of a Black Hole
Presentation transcript:

黎卓 HB Perets, JC Lombardi Jr, SR Milcarek Jr JUNO会议,南京,2016/4/17-18 微型潮汐瓦解事件 (Micro-TDE) 黎卓 HB Perets, JC Lombardi Jr, SR Milcarek Jr JUNO会议,南京,2016/4/17-18 Perets et al. 2016 ApJ, arXiv:1602.07698

Tidal disruption events

Observed TDEs ROSAT Swift: jetted TDE

What about TDEs by stellar mass compact objects? Stellar mass COs smaller by >> 106  micro-TDE Radiation properties? Timescale, energy, luminosity, event rate…

Fall-back time . Low mass-ratio TDE: planet High mass-ratio partial TDE: star Remnant object affects the dynamic of marginally bound debris StarSmasher code: SPH . CO

BH: 10 Msun Star: 1 Msun, ~ 1 Rsun BH: 10 Msun Planet: 10-3 Msun, ~ 0.1 Rsun Decay faster: -7/3 Earlier: few ks -5/3 Sub Ms

Partial disruption

Accretion time circularization of bound debris disk/torus forms at rc=2Rp accretion time thick disk h~1 tmin~ a few 103 s

Light curve and energy Light curve could be more relevant to mass accretion rate tmin>>tacc: planet accretion rate = fall-back rate tmin<<tacc: star accretion rate << fall-back rate Released energy

CO+star/planet encounters may happen in dense stellar cluster: randomly binary/planetary system: natal kick of CO wide binary: multiple-scattering with field stars  highly eccentric orbits Quasi-stable triple system: secular evolution  close encounter

Dense cluster TDE happens once the closest distance is smaller than Rt The TD rate for one CO typically The TD rate for a stellar cluster For ~150 globular clusters in Milky Way BH: 10 Msun NS: 1.4Msun

Natal kick of CO Supernova kick; CO-merger kick TD probability after kick Core-collapse SN rate ~3/100yr per galaxy; TDE rate is 1.4E-6/yr for BHs (10Msun) per galaxy 3.4E-7/yr for NSs (1.4Msun) per galaxy (Neglect poorly known compact binary case, a<10AU)

Micro-TDE radiation Duration ~1E4s (True) energy ~ 1E52erg Super-Eddington: >1010Ledd; jetted Non-thermal Rate ~ a fewE-6 per yr per galaxy 10’s/yr Gpc3 (tens times GRB rate) X/gamma sky monitors may observe many micro-TDEs.

Ultra-long GRBs Liso ~1E49 erg/s T~1E4 s

Application: Ultra-long GRB 111209A SN 2011kl Short SN-GRB delay: <day compact binary; post common-envelope phase Greiner et al. 2015

Application: Short GRB 050709 x-ray flare 16 d after GRB NS-NS + planet: BH kick at birth  planet disruption Fox et al. 2005

Neutrino from micro-TDE accretion disc High mass accretion rate  hot disc  ignite neutrino production JUNO detection rate Neutrino energy/spectrum comparable to SN JUNO can detect 1 nu for SN at <~1Mpc 1 Micro-TDE per <108yr much rare  diffuse neutrino from micro-TDE Stacking search for EM-detected micro-TDE? X/gamma monitor – JUNO Nearby micro-TDE (lucky?)

Observations help to narrow down the large uncertainties.