Star-planet coalescence

Slides:



Advertisements
Similar presentations
Proto-Planetary Disk and Planetary Formation
Advertisements

AGN Eddington Ratio Distributions
Felipe Garrido and Jorge Cuadra PUC, Chile XI SOCHIAS Annual Meeting January 2014.
Felipe Garrido (PUC), Jorge Cuadra (PUC), Alberto Sesana (AEI) and Takamitsu Tanaka (MPA) IAU Symposium 312: “Black Holes and Clusters across cosmic time”
Tidal Disruption from Supermassive Black Hole Binaries in Merging Galaxies: Before & After the Coalescence Shuo Li NAOC Collaborated with Rainer Spurzem,
Transits and Starspots Jeremy Tregloan-Reed Ph.D. Research Student Supervisor: John Southworth.
Magnetars origin and progenitors with enhanced rotation S.B. Popov, M.E. Prokhorov (Sternberg Astronomical Institute) (astro-ph/ )
Black holes: Introduction. 2 Main general surveys astro-ph/ Neven Bilic BH phenomenology astro-ph/ Thomas W. Baumgarte BHs: from speculations.
Dark Matter and Galaxy Formation Section 4: Semi-Analytic Models of Galaxy Formation Joel R. Primack 2009, eprint arXiv: Presented by: Michael.
Fabio Antonini Joshua Faber Alessia Gualandris and David Merritt Rochester Institute of Technology.
A Unified, Merger-Driven Model of the Origin of Starbursts, Quasars, the Cosmic X-Ray Background, Supermassive Black Holes, and Galaxy Spheroids Hopkins,
Two stories from the life of binaries: getting bigger and making magnetars Sergei Popov, Mikhail Prokhorov (SAI MSU) This week SAI celebrates its 175 anniversary.
Dark Matter and Galaxy Formation (Section 3: Galaxy Data vs. Simulations) Joel R. Primack 2009, eprint arXiv: Presented by: Michael Solway.
“ Testing the predictive power of semi-analytic models using the Sloan Digital Sky Survey” Juan Esteban González Birmingham, 24/06/08 Collaborators: Cedric.
Ch. 8 – Characterizing Stars part 3: The Hertzsprung-Russell Diagram Luminosity Classes Spectral Types.
Advanced Methods for Studying Astronomical Populations: Inferring Distributions and Evolution of Derived (not Measured!) Quantities Brandon C. Kelly (CfA,
Black holes: do they exist?
Chaotic Case Studies: Sensitive dependence on initial conditions in star/planet formation Fred C. Adams Physics Department University of Michigan With:
I N T R O D U C T I O N The mechanism of galaxy formation involves the cooling and condensation of baryons inside the gravitational potential well provided.
Extinction. Frequency vs Size for impacts – 1 “killer” impact every one hundred million years  is this the random mechanisms to populate the galaxy?
Quasars, black holes and galaxy evolution Clive Tadhunter University of Sheffield 3C273.
Double NS: Detection Rate and Stochastic Background Tania Regimbau VIRGO/NICE.
The Dark Side of the Universe Sukanya Chakrabarti (FAU)
Black holes: observations Lecture 4: BH coalescence Sergei Popov (SAI MSU)
AIMS OF G ALACTIC C HEMICAL E VOLUTION STUDIES To check / constrain our understanding of stellar nucleosynthesis (i.e. stellar yields), either statistically.
Expected Coalescence Rate of NS/NS Binaries for Ground Based Interferometers Tania Regimbau OCA/ARTEMIS on the behalf of J.A. de Freitas Pacheco, T. Regimbau,
Test #3 Same types of questions Bring a calculator Study the other exam reviews.
Globular Clusters. A globular cluster is an almost spherical conglomeration of 100,000 to 1,000,000 stars of different masses that have practically.
Intermediate-mass Black Holes in Star Clusters Holger Baumgardt Astrophysical Computing Laboratory, RIKEN, Tokyo new address:
Disk Disruption in Young Embedded Clusters Eva-Marie Proszkow University of Michigan 18 May 2006 Fred Adams (University of Michigan) Phil Myers (Harvard.
The Inter-Galactic Populations and Unbound Dark Matter Ing-Guey Jiang and Yu-Ting Wu National Tsing-Hua University Taiwan.
Blue stragglers in dwarf spheroidal galaxies L.Rizzi Osservatorio Astronomico di Padova In collaboration with: Enrico V. Held, Giampaolo Bertelli, Ivo.
Evolution of massive binary black holes Qingjuan Yu Princeton University July 21, 2002.
Stars and the HR Diagram Dr. Matt Penn National Solar Observatory.
Figure 4. Same as Fig. 3 but for x = 5.5.
Capture of Irregular Satellites during Planetary Encounters
Simulated black hole picture
Figure 2. A comparison between the modern PMS spectral type-to-effective temperature conversion scales of Pecaut & Mamajek (2013, solid red line, labelled.
Compare the planets in our Solar System!
The interaction-driven model for the starburst galaxies and AGNs
From: Discovery of carbon-rich Miras in the Galactic bulge
黎卓 HB Perets, JC Lombardi Jr, SR Milcarek Jr JUNO会议,南京,2016/4/17-18
Luciano del Valle & Andrés Escala Universidad de Chile
Young planetary systems
Fig. 2. Semi-major axis vs. eccentricity (left) and semi-major axis vs
Isolated BHs.
Solar system Sergei popov.
Fermi Bubble Z.G.,Xiong.
Lecture 10: Black Holes and How They Shine
HUBBLE DEEP FIELD:.
Previous Classes: This Class interacting galaxies cosmology
Chapter 14 Spiral Galaxy.
BH coalescence.
Evolution with decaying magnetic field
BH binaries.
Star Clusters and their stars
Center for Gravitational Wave Physics Penn State University
Lecture 11: Age and Metalicity from Observations
Population synthesis of exoplanets
Surface Brightness Profile - NGC 3379 (giant elliptical)
Black holes: observations Lecture 1: Introduction
Planets in binaries Sergei popov.
Direct imaging discovery of a Jovian exoplanet within a triple-star system by Kevin Wagner, Dániel Apai, Markus Kasper, Kaitlin Kratter, Melissa McClure,
Black holes: Introduction
Population synthesis of exoplanets
by W. R. Binns, M. H. Israel, E. R. Christian, A. C. Cummings, G. A
Black holes: observations Lecture 1: Introduction
Galactic Astronomy 銀河物理学特論 I Lecture 3-3: Stellar mass function of galaxies Seminar: Perez-Gonzalez et al. 2008, ApJ, 675, 234 Lecture: 2012/01/16.
by W. R. Binns, M. H. Israel, E. R. Christian, A. C. Cummings, G. A
Top: probability distribution of the mass-to-light ratios observed when nebular emission is included in the fitting, stacked across all of the MC samples.
Presentation transcript:

Star-planet coalescence Sergei Popov, aleksandr popkov

Tidal interaction

Types of mergers Stable accretion ρpl<ρ* Tidal disruptin 1<ρpl/ρ*<5 Direct impact ρpl>5ρ* Metzger et al. 2012

Direct impact dinamics Metzger et al. 2012

Direct impact luminosity

Estimates by Metzger et al. (2012) Numbers can reach 0.1-1 mergers per year!

M-a distribution Initial distribution in a-M plane is taken from population synthesis.

Planetary parameters

Other perameters Disc lifetime Stellar IMF Galactic star formation rate

Tidal evolution

Results-1 Probability of a merger of a planet with a main sequence host star vs. system's age, p(t). Line style marks the type of merger: solid curve | direct impact, dotted curve | tidal disruption.

Distribution of stellar masses for mergers Distribution of mergers with main sequence stars. Curves show fraction of merging planets depending on the host mass (given in solar units). Only coalescences which happened at ages less than the age of the Galaxy are taken into account. Solid line - direct impacts, dotted line - tidal disruptions, dashedline - stable accretion events.

Which planets merge? Mass and initial orbital radius of planets which merge with their host stars during the main sequence phase in simultaneously formed population of planetary systems. Symbol style marks the type of mergers: dots - direct impacts, circles – tidal disruptions, triangles - stable accretion events. Only mergers happening at ages less than the age of the Galaxy are included. Total number of planets in the population is 105, the number of planets on this diagram is 269.

Luminosity distribution of mergers Distribution in luminosity of planet-star mergers in a Milky Way-like galaxy. Type of merger is marked by hatching. The quantity on the ordinate is the rate of mergers per year per galaxy in a luminosity bin.

Dependences Illustration of the dependence of coalescence statistics on initial distribution in the a-M plane. Symbols encode host star masses: Circles: 0.09-1 Msolar; triangles: 1-1.5 Msolar; crosses: 1.5-4 Msolar; dots: 4-7 Msolar; stars: 7-14 Msolar. Inclined lines mark the boundary of the “fall region" for stars of different masses (labeled in the legend in units of the Solar mass). The solid line on the top corresponds to 1 Msolar. Maximum radii of stars of 7 and 14 Msolar at the end of their evolution on the main sequence are plotted by vertical dashed lines and marked by the value of mass.