Understanding Magnetars with Conventional Physics. David Eichler

Size: px
Start display at page:

Download "Understanding Magnetars with Conventional Physics. David Eichler"

Transcription

1 Understanding Magnetars with Conventional Physics David Eichler

2 My collaborators Yuri Lyubarsky Chris Thompson Peter Woods Michael Gedalin Andrew Cheng (back in )

3 How can we tell what magnetars are made of?

4 How can we tell what magnetars are made of? Try thermal echos as a diagnostic (Eichler and Cheng 1989).

5 Short-term afterglow (hours): Settling of uplifted matter Medium-term afterglow (weeks): Cooling of outer crust Long-term afterglow (years): Cooling of inner crust

6

7 Energy deposition Heat conductivity increases inward. Most heat goes in, not out. deeper

8 The Storage Problem research Physics Math research Central Administration Etc.

9 The change in the magnetic field geometry of

10 Periodic Emission: trapped pair plasma

11 The medium term afterglow of Flux F F=kt day 40 days Steady emission

12 The predicted medium term afterglow Lyubarsky,, Eichler, and Thompson (2002), especially Lyubarsky Assume central temperature corresponding to steady emission, 7 x 10 8 K, uniform energy deposition corresponding to observed burst energy

13 Conductivity E Fermi =E Landau

14 B= 3 x Gauss

15 B= 3 x Gauss

16 Several percent of burst energy escapes as surface radiation, the rest gets sucked into the star

17 White dwarf cooling after dwarf nova Arras, Bildsten

18 The really long term afterglow of Kouveliotou, Lyubarsky,, Eichler,..(2003) Assume deep heating of crust, but not core

19

20

21

22

23

24

25

26

27

28 (Pairing energy for neutrons) Free, unpaired neutrons Neutrons becoming unpaired, heat capacity rising rapidly with T Neutrons all in superfluid state because T<<T c

29

30

31

32

33

34

35

36

37

38

39 τ M

40 Perhaps the persistent emission from some magnetars is, in fact, long-term afterglow from heating of the inner crust. In this case, we may see their steady x-ray emission decline over a time scale of 5 10 years.

41 The short term afterglow of Thompson, Woods, Eichler and Lyubarsky 2003 Assume outer layer is heated by energy flux from above surface during initial flare, uplifted by pair pressure

42 Short Term Afterglow Hot Spot Pair free zone T=100KeV Pairs

43 Short Term Afterglow (some time later) Pair free zone T=100KeV Pairs Rate of cooling measures magnetic field T T constant, specific enthalpy h constant Flux = T/optical depth= TB/Σ dσ/dt = Flux/h Flux = kbtk -1/2

44 Short Term Afterglow (still later) Pairs have gone away Rate of cooling measures magnetic field Find B= Gauss (Thompson, Woods, Lyubarsky and DE 2003)

45 Ibrahim et al 2001 B= 6 x B=1 x10 14

46 Column density is at least about g in normal material

47 Magnetars as Optical Lasers

48 Dereddened flux > 2 x10-13 erg/cm 2 s D=5 to 10 Kpc Lopt >5 x erg/s

49 Magnetars as Optical Lasers Magnetospheric currents Magnetosphere Say the currents are relativistic pairs. Lorentz factor about Density about charges/cm 3. Plasma frequency as seen in the lab frame hz. Two stream instability (Gedalin( Gedalin, Gruman and Melrose, 2002) makes coherent optical or IR emission.

50 Optical Pulses from 4U0412 (Kern and Martin, Nature May )

51 Tearing Nucleons Apart

52 photo neutron - + V B

53 - + - V B

54 - - B + A ton of force

55 - - B Quark pair materializes

56 - - B + - +? N+Π o 2 γ

57 - - B - + +? + Π + Π + n µ +ν µ e+ν e +ν µ

58 Relativistic Petschek reconnection Current sheet Γ=σ 1/2 σ can be to for a magnetar,, so Γ can exceed 10 5

59 Polarization-induced charged mesons photoneutron p X-ray

60 Other indications of baryons in NS peripheries: GRB X-ray afterglow nearly always present Afterglow from 27 December event: Baryons seem to have been ejected at about 0.6c (Gelfand et al 2005)

61 Conclusions We may actually understand some of the crazy physics of magnetars.

62 Conclusions We may actually understand some of the crazy physics of magnetars. Magnetar crusts are consistent with ordinary matter. No ice nine scenario implied (yet). More research needed.

63 Conclusions We may actually understand some of the crazy physics of magnetars. Magnetar crusts are consistent with ordinary matter. No ice nine scenario implied (yet). Short term afterglow confirms B = 6 x Gauss

64 Conclusions We may actually understand some of the crazy physics of magnetars. Magnetar crusts are consistent with ordinary matter. No ice nine scenario implied (yet). Short term afterglow confirms B = 6 x Gauss Magnetars may be free electron optical lasers. Many predictions (wavefront( coherence, photon statistics, polarization ) ) can be tested.

65 Magnetars offer New quantum electrodynamics new condensed matter physics, new nuclear physics, maybe new laser physics, and lots of new astrophysics.

Infrared-Optical observations of magnetars

Infrared-Optical observations of magnetars Infrared-Optical observations of magnetars Mikio Morii Tokyo Institute of Technology 2012.09.01 @ Rikkyo Univ. Contents Search for Near-Infrared Pulsation of the AXP 4U 0142+61 M. M., N. Kobayashi, N.

More information

Crustal cooling in accretion heated neutron stars

Crustal cooling in accretion heated neutron stars Crustal cooling in accretion heated neutron stars Ed Cackett ecackett@umich.edu University of Michigan Collaborators: Rudy Wijnands, Jon Miller, Jeroen Homan, Walter Lewin, Manuel Linares Outline X-ray

More information

Instability and different burning regimes

Instability and different burning regimes 1 X-ray bursts Last time we talked about one of the major differences between NS and BH: NS have strong magnetic fields. That means that hot spots can be produced near the magnetic poles, leading to pulsations

More information

MAGNETARS AS COOLING NEUTRON STARS

MAGNETARS AS COOLING NEUTRON STARS MAGNETARS AS COOLING NEUTRON STARS D.G. Yakovlev Ioffe Physical Technical Institute, Saint-Petersburg, Russia Main coauthors: A.D. Kaminker, A.Y. Potekhin, D.A. Baiko February 2009, Aspen HISTORY The first

More information

THERMAL EVOLUTION OF ORDINARY NEUTRON STARS AND MAGNETARS

THERMAL EVOLUTION OF ORDINARY NEUTRON STARS AND MAGNETARS THERMAL EVOLUTION OF ORDINARY NEUTRON STARS AND MAGNETARS D.G. Yakovlev Ioffe Physical Technical Institute, Saint-Petersburg, Russia Introduction Thermal evolution of ordinary neutron stars Thermal evolution

More information

Neutron Stars. We now know that SN 1054 was a Type II supernova that ended the life of a massive star and left behind a neutron star.

Neutron Stars. We now know that SN 1054 was a Type II supernova that ended the life of a massive star and left behind a neutron star. Neutron Stars Neutron Stars The emission from the supernova that produced the crab nebula was observed in 1054 AD by Chinese, Japanese, Native Americans, and Persian/Arab astronomers as being bright enough

More information

EXTREME NEUTRON STARS

EXTREME NEUTRON STARS EXTREME NEUTRON STARS Christopher Thompson Canadian Institute for Theoretical Astrophysics University of Toronto SLAC Summer Institute 2005 Extreme Magnetism: B ~ 10 8-9 G (Low-mass X-ray binaries, millisecond

More information

The Secret Life of Neutron Stars. Jeremy Heyl Harvard-Smithsonian CfA

The Secret Life of Neutron Stars. Jeremy Heyl Harvard-Smithsonian CfA The Secret Life of Neutron Stars Jeremy Heyl Harvard-Smithsonian CfA The Life of a 10 M Star PNS 10 5 yr 10 6 yr 10 7 yr 10 8 yr 10 9 yr 10 10 yr PMS MS Radio Pulsars Thermal Accretion-, Nuclear-, GWpowered

More information

Nucleon Superfluidity vs Thermal States of INSs & SXTs in quiescence

Nucleon Superfluidity vs Thermal States of INSs & SXTs in quiescence Nucleon Superfluidity vs Thermal States of INSs & SXTs in quiescence K.P.Levenfish, D.G.Yakovlev, P.Haensel I Ioffe Institute, S.Petersburg Copernicus Astronomical Center, Warsaw Brown, Bildstein, Rutledge`98

More information

This class: Life cycle of high mass stars Supernovae Neutron stars, pulsars, pulsar wind nebulae, magnetars Quark-nova stars Gamma-ray bursts (GRBs)

This class: Life cycle of high mass stars Supernovae Neutron stars, pulsars, pulsar wind nebulae, magnetars Quark-nova stars Gamma-ray bursts (GRBs) This class: Life cycle of high mass stars Supernovae Neutron stars, pulsars, pulsar wind nebulae, magnetars Quark-nova stars Gamma-ray bursts (GRBs)!1 Cas$A$ All$Image$&$video$credits:$Chandra$X7ray$ Observatory$

More information

Pulsar Winds in High Energy Astrophysics

Pulsar Winds in High Energy Astrophysics Pulsar Winds in High Energy Astrophysics Dmitry Khangulyan Institute of Space and Astronautical Science (ISAS/JAXA) The extreme Universe viewed in very high energy gamma-rays, Kashiwa 09/25/2012 OUTLINE

More information

Extreme optical outbursts from a magnetar-like transient source: SWIFT J

Extreme optical outbursts from a magnetar-like transient source: SWIFT J Extreme optical outbursts from a magnetar-like transient source: SWIFT J1955+26 Gottfried Kanbach 1 Alexander Stefanescu 1,2 Agnieszka Słowikowska 3 Jochen Greiner 1 Sheila McBreen 4 Glòria Sala 5 1 Max-Planck-Institut

More information

The Mystery of Fast Radio Bursts and its possible resolution. Pawan Kumar

The Mystery of Fast Radio Bursts and its possible resolution. Pawan Kumar The Mystery of Fast Radio Bursts and its possible resolution Outline Pawan Kumar FRBs: summary of relevant observations Radiation mechanism and polarization FRB cosmology Wenbin Lu Niels Bohr Institute,

More information

Systematic study of magnetar outbursts

Systematic study of magnetar outbursts Systematic study of magnetar outbursts Francesco Coti Zelati Institute for Space Sciences, CSIC-IEEC, Barcelona In collaboration with N. Rea (CSIC-IEEC, U. Amsterdam), J. A. Pons (U. Alicante), S. Campana

More information

(Anomalous) X-Ray Pulsars. Vicky Kaspi. Montreal, Canada. Stanford December 16, 2004

(Anomalous) X-Ray Pulsars. Vicky Kaspi. Montreal, Canada. Stanford December 16, 2004 (Anomalous) X-Ray Pulsars Vicky Kaspi Montreal, Canada Texas @ Stanford December 16, 2004 Summary Introduction to AXPs Evidence that AXPs are magnetars Open Issues and Recent Results: IR emission Transient

More information

Pulsar Winds. John Kirk. Max-Planck-Institut für Kernphysik Heidelberg, Germany. < > p.1/18

Pulsar Winds. John Kirk. Max-Planck-Institut für Kernphysik Heidelberg, Germany. < > p.1/18 Pulsar Winds John Kirk Max-Planck-Institut für Kernphysik Heidelberg, Germany < > p.1/18 About 50 years after... The Crab Nebula Central star is source of particles and magnetic field (Piddington 1957)

More information

Understanding the pulsar magnetosphere through first-principle simulations

Understanding the pulsar magnetosphere through first-principle simulations Understanding the pulsar magnetosphere through first-principle simulations Alexander Y. Chen In collaboration with: Andrei Beloborodov Rui Hu The Many Faces of Neutron Stars August 25, 2015 Pulsars: Rotating

More information

The Stellar Graveyard Neutron Stars & White Dwarfs

The Stellar Graveyard Neutron Stars & White Dwarfs The Stellar Graveyard Neutron Stars & White Dwarfs White Dwarfs White dwarfs are the remaining cores of low-mass (M < 8M sun ) stars Electron degeneracy pressure supports them against gravity Density ~

More information

SGRs Long term variability

SGRs Long term variability SGRs Long term variability Silvia Zane, MSSL, UCL INT-07-2a The Neutron Star Crust and Surface 27 June 2007, Seattle o SGRs (and AXPs): long term spectral variability o A magnetar at work? Interpretation

More information

Chapter 18 Reading Quiz Clickers. The Cosmic Perspective Seventh Edition. The Bizarre Stellar Graveyard Pearson Education, Inc.

Chapter 18 Reading Quiz Clickers. The Cosmic Perspective Seventh Edition. The Bizarre Stellar Graveyard Pearson Education, Inc. Reading Quiz Clickers The Cosmic Perspective Seventh Edition The Bizarre Stellar Graveyard 18.1 White Dwarfs What is a white dwarf? What can happen to a white dwarf in a close binary system? What supports

More information

Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version

Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version Purpose: To determine if two end products of stellar evolution GK Per and Cen X-3 could be white dwarfs or neutron stars by calculating

More information

Phase Oscillation between Superfluid and Normal State of Neutrons in Neutron Stars The Origin of Glitches of Pulsars 1

Phase Oscillation between Superfluid and Normal State of Neutrons in Neutron Stars The Origin of Glitches of Pulsars 1 Phase Oscillation between Superfluid and Normal State of Neutrons in Neutron Stars The Origin of Glitches of Pulsars Qiu-he Peng a,b ( qhpeng@nju.edu.cn ) Zhi quan Luo a,c a School of Physics and electronic

More information

Accretion Disks. Accretion Disks. Flat Stars. 1. Background Perspective

Accretion Disks. Accretion Disks. Flat Stars. 1. Background Perspective Accretion Disks 4 Accretion Disks Flat Stars 1. Background Perspective One of the major developments of mid-twentieth-century stellar astrophysics was the understanding that there is often a third object

More information

Properties of Stars. Characteristics of Stars

Properties of Stars. Characteristics of Stars Properties of Stars Characteristics of Stars A constellation is an apparent group of stars originally named for mythical characters. The sky contains 88 constellations. Star Color and Temperature Color

More information

21. Neutron Stars. The Crab Pulsar: On & Off. Intensity Variations of a Pulsar

21. Neutron Stars. The Crab Pulsar: On & Off. Intensity Variations of a Pulsar 21. Neutron Stars Neutron stars were proposed in the 1930 s Pulsars were discovered in the 1960 s Pulsars are rapidly rotating neutron stars Pulsars slow down as they age Neutron stars are superfluid &

More information

Cooling Neutron Stars. What we actually see.

Cooling Neutron Stars. What we actually see. Cooling Neutron Stars What we actually see. The Equilibrium We discussed the equilibrium in neutron star cores through this reaction (direct Urca). nëp + e à + ö e ö n = ö p + ö e + ö öe Does the reaction

More information

Electrodynamics of Magnetized Rotators Anatoly Spitkovsky,, UC Berkeley

Electrodynamics of Magnetized Rotators Anatoly Spitkovsky,, UC Berkeley Electrodynamics of Magnetized Rotators Anatoly Spitkovsky,, UC Berkeley Magnetized rotators are ubiquitous: pulsars, AGN, GRBs (?) Rotation very efficient at long-term energy storage Extraction of rotational

More information

Chapter 18 The Bizarre Stellar Graveyard

Chapter 18 The Bizarre Stellar Graveyard Chapter 18 The Bizarre Stellar Graveyard 18.1 White Dwarfs Our goals for learning What is a white dwarf? What can happen to a white dwarf in a close binary system? What is a white dwarf? White Dwarfs White

More information

Identifying the Remnants of Neutron Star Mergers. Wen-fai Fong University of Arizona

Identifying the Remnants of Neutron Star Mergers. Wen-fai Fong University of Arizona Identifying the Remnants of Neutron Star Mergers Wen-fai Fong University of Arizona Einstein Fellows Symposium, Harvard-Smithsonian Center for Astrophysics, 10.27.2015 What s left after two neutron stars

More information

Gamma-ray Astrophysics

Gamma-ray Astrophysics Gamma-ray Astrophysics AGN Pulsar SNR GRB Radio Galaxy The very high energy -ray sky NEPPSR 25 Aug. 2004 Many thanks to Rene Ong at UCLA Guy Blaylock U. of Massachusetts Why gamma rays? Extragalactic Background

More information

Diffusive shock acceleration: a first order Fermi process. jan.-fév NPAC, rayons cosmiques E. Parizot (APC)

Diffusive shock acceleration: a first order Fermi process. jan.-fév NPAC, rayons cosmiques E. Parizot (APC) 1 Diffusive shock acceleration: a first order Fermi process 2 Shock waves Discontinuity in physical parameters shock front n 2, p 2, T 2 n 1, p 1, T 1 v 2 v 1 downstream medium (immaterial surface) upstream

More information

Radiation-hydrodynamic Models for ULXs and ULX-pulsars

Radiation-hydrodynamic Models for ULXs and ULX-pulsars Radiation-hydrodynamic Models for ULXs and ULX-pulsars Tomohisa KAWASHIMA Division of Theoretical Astrophysics, NAOJ in collaboration with Ken OHSUGA, Hiroyuki TAKAHASHI (NAOJ) Shin MINESHIGE, Takumi OGAWA

More information

On (shock. shock) acceleration. Martin Lemoine. Institut d Astrophysique d. CNRS, Université Pierre & Marie Curie

On (shock. shock) acceleration. Martin Lemoine. Institut d Astrophysique d. CNRS, Université Pierre & Marie Curie On (shock ( shock) acceleration of ultrahigh energy cosmic rays Martin Lemoine Institut d Astrophysique d de Paris CNRS, Université Pierre & Marie Curie 1 Acceleration Hillas criterion log 10 (B/1 G) 15

More information

Chapter 10 Our Star. X-ray. visible

Chapter 10 Our Star. X-ray. visible Chapter 10 Our Star X-ray visible Radius: 6.9 10 8 m (109 times Earth) Mass: 2 10 30 kg (300,000 Earths) Luminosity: 3.8 10 26 watts (more than our entire world uses in 1 year!) Why does the Sun shine?

More information

Ultra High Energy Cosmic Rays I

Ultra High Energy Cosmic Rays I Ultra High Energy Cosmic Rays I John Linsley (PRL 10 (1963) 146) reports on the detection in Vulcano Ranch of an air shower of energy above 1020 ev. Problem: the microwave background radiation is discovered

More information

SUPERFLUID MAGNETARS AND QPO SPECTRUM

SUPERFLUID MAGNETARS AND QPO SPECTRUM SUPERFLUID MAGNETARS AND QPO SPECTRUM Andrea Passamonti Osservatorio Astronomico di Roma INAF. In collaboration with L. Stella, S. Lander SAIt Bologna 9/5/23 Magnetars Neutron stars with a strong magnetic

More information

Short GRB and kilonova: did observations meet our theoretical predictions?

Short GRB and kilonova: did observations meet our theoretical predictions? Short GRB and kilonova: did observations meet our theoretical predictions? Riccardo Ciolfi INAF - Astronomical Observatory of Padova INFN - Trento Institute for Fundamental Physics and Applications GW170817

More information

A Comparative Study of Quark-Gluon Plasma at the Core of a Neutron Star and in the Very Early Universe. Frikkie de Bruyn

A Comparative Study of Quark-Gluon Plasma at the Core of a Neutron Star and in the Very Early Universe. Frikkie de Bruyn A Comparative Study of Quark-Gluon Plasma at the Core of a Neutron Star and in the Very Early Universe By Frikkie de Bruyn Introduction 1 Study of quark-gluon plasma fluid is of mutual Interest to both

More information

Particle acceleration during the gamma-ray flares of the Crab Nebular

Particle acceleration during the gamma-ray flares of the Crab Nebular Particle acceleration during the gamma-ray flares of the Crab Nebular SLAC Accelerator seminar SLAC 15 June 2011 R. Buehler for the LAT collaboration and A. Tennant, E. Costa, D. Horns, C. Ferrigno, A.

More information

Lecture Outlines. Chapter 22. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

Lecture Outlines. Chapter 22. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc. Lecture Outlines Chapter 22 Astronomy Today 8th Edition Chaisson/McMillan Chapter 22 Neutron Stars and Black Holes Units of Chapter 22 22.1 Neutron Stars 22.2 Pulsars 22.3 Neutron-Star Binaries 22.4 Gamma-Ray

More information

Astronomy. Chapter 15 Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes

Astronomy. Chapter 15 Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes Astronomy Chapter 15 Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes are hot, compact stars whose mass is comparable to the Sun's and size to the Earth's. A. White dwarfs B. Neutron stars

More information

Radiative processes in GRB (prompt) emission. Asaf Pe er (STScI)

Radiative processes in GRB (prompt) emission. Asaf Pe er (STScI) Radiative processes in GRB (prompt) emission Asaf Pe er (STScI) May 2009 Outline Historical approach Synchrotron: pro s and co s Compton scattering in prompt emission (and why it is different than in afterglow)

More information

Chapter 13 2/19/2014. Lecture Outline Neutron Stars. Neutron Stars and Black Holes Neutron Stars. Units of Chapter

Chapter 13 2/19/2014. Lecture Outline Neutron Stars. Neutron Stars and Black Holes Neutron Stars. Units of Chapter 13.1 Neutron Stars Lecture Outline Chapter 13 Neutron Stars and After a Type I supernova, little or nothing remains of the original star. After a Type II supernova, part of the core may survive. It is

More information

Chapter 18 The Bizarre Stellar Graveyard. White Dwarfs. What is a white dwarf? Size of a White Dwarf White Dwarfs

Chapter 18 The Bizarre Stellar Graveyard. White Dwarfs. What is a white dwarf? Size of a White Dwarf White Dwarfs Chapter 18 The Bizarre Stellar Graveyard 18.1 White Dwarfs Our goals for learning What is a white dwarf? What can happen to a white dwarf in a close binary system? What is a white dwarf? White Dwarfs White

More information

Rotating RAdio Transients (RRATs) ApJ, 2006, 646, L139 Nature, 2006, 439, 817 Astro-ph/

Rotating RAdio Transients (RRATs) ApJ, 2006, 646, L139 Nature, 2006, 439, 817 Astro-ph/ Rotating RAdio Transients (RRATs) ApJ, 2006, 646, L139 Nature, 2006, 439, 817 Astro-ph/0608311 Introduction 11 Rotating RAdio Transients (RRATs) (Mclaughlin et al 2006) Repeated, irregular radio bursts

More information

April 13, 2011 Exam 4, Friday. Review sheet posted. Sky Watch 4 due. Review session Thursday, 5 6 PM, Room WEL 3.502, right here! Reading: Chapter 9,

April 13, 2011 Exam 4, Friday. Review sheet posted. Sky Watch 4 due. Review session Thursday, 5 6 PM, Room WEL 3.502, right here! Reading: Chapter 9, April 13, 2011 Exam 4, Friday. Review sheet posted. Sky Watch 4 due. Review session Thursday, 5 6 PM, Room WEL 3.502, right here! Reading: Chapter 9, Sections 9.5.2, 9.6.1, 9.6.2. 9.7, 9.8; Chapter 10,

More information

arxiv:astro-ph/ v1 7 Jul 1999

arxiv:astro-ph/ v1 7 Jul 1999 Gamma-ray Burst Energetics Pawan Kumar Institute for Advanced Study, Princeton, NJ 08540 Abstract arxiv:astro-ph/9907096v1 7 Jul 1999 We estimate the fraction of the total energy in a Gamma-Ray Burst (GRB)

More information

Gamma-ray Bursts. Chapter 4

Gamma-ray Bursts. Chapter 4 Chapter 4 Gamma-ray Bursts At the moment, the most important application of the theory of relativistic shock waves is in explaining the radiation from Gamma-ray Burst sources. I will briefly introduce

More information

Radiative Processes in Astrophysics

Radiative Processes in Astrophysics Radiative Processes in Astrophysics 9. Synchrotron Radiation Eline Tolstoy http://www.astro.rug.nl/~etolstoy/astroa07/ Useful reminders relativistic terms, and simplifications for very high velocities

More information

Explosive reconnection of the double tearing mode in relativistic plasmas

Explosive reconnection of the double tearing mode in relativistic plasmas Explosive reconnection of the double tearing mode in relativistic plasmas Application to the Crab Jérôme Pétri 1 Hubert Baty 1 Makoto Takamoto 2, Seiji Zenitani 3 1 Observatoire astronomique de Strasbourg,

More information

Final States of a Star

Final States of a Star Pulsars Final States of a Star 1. White Dwarf If initial star mass < 8 MSun or so. (and remember: Maximum WD mass is 1.4 MSun, radius is about that of the Earth) 2. Neutron Star If initial mass > 8 MSun

More information

Gamma-Ray Astronomy. Astro 129: Chapter 1a

Gamma-Ray Astronomy. Astro 129: Chapter 1a Gamma-Ray Bursts Gamma-Ray Astronomy Gamma rays are photons with energies > 100 kev and are produced by sub-atomic particle interactions. They are absorbed by our atmosphere making observations from satellites

More information

Editorial comment: research and teaching at UT

Editorial comment: research and teaching at UT Wednesday, March 23, 2017 Reading for Exam 3: Chapter 6, end of Section 6 (binary evolution), Section 6.7 (radioactive decay), Chapter 7 (SN 1987A), Background: Sections 3.1, 3.2, 3.3, 3.4, 3.5, 3.8, 3.10,

More information

Chapter 18 Lecture. The Cosmic Perspective Seventh Edition. The Bizarre Stellar Graveyard Pearson Education, Inc.

Chapter 18 Lecture. The Cosmic Perspective Seventh Edition. The Bizarre Stellar Graveyard Pearson Education, Inc. Chapter 18 Lecture The Cosmic Perspective Seventh Edition The Bizarre Stellar Graveyard The Bizarre Stellar Graveyard 18.1 White Dwarfs Our goals for learning: What is a white dwarf? What can happen to

More information

Bremsstrahlung Radiation

Bremsstrahlung Radiation Bremsstrahlung Radiation Wise (IR) An Example in Everyday Life X-Rays used in medicine (radiographics) are generated via Bremsstrahlung process. In a nutshell: Bremsstrahlung radiation is emitted when

More information

Anomalous X-ray Pulsars

Anomalous X-ray Pulsars Anomalous X-ray Pulsars GRBs: The Brightest Explosions in the Universe Harvard University, May 23, 2002 Vicky Kaspi Montreal, Canada What are Anomalous X-ray Pulsars? exotic class of objects 1st discovered

More information

Chapter 14: The Bizarre Stellar Graveyard

Chapter 14: The Bizarre Stellar Graveyard Lecture Outline Chapter 14: The Bizarre Stellar Graveyard 14.1 White Dwarfs Our goals for learning: What is a white dwarf? What can happen to a white dwarf in a close binary system? What is a white dwarf?

More information

White dwarfs are the remaining cores of dead stars. Electron degeneracy pressure supports them against the crush of gravity. The White Dwarf Limit

White dwarfs are the remaining cores of dead stars. Electron degeneracy pressure supports them against the crush of gravity. The White Dwarf Limit The Bizarre Stellar Graveyard Chapter 18 Lecture The Cosmic Perspective 18.1 White Dwarfs Our goals for learning: What is a white dwarf? What can happen to a white dwarf in a close binary system? Seventh

More information

Chapter 14 Lecture. Chapter 14: Our Star Pearson Education, Inc.

Chapter 14 Lecture. Chapter 14: Our Star Pearson Education, Inc. Chapter 14 Lecture Chapter 14: Our Star 14.1 A Closer Look at the Sun Our goals for learning: Why does the Sun shine? What is the Sun's structure? Why does the Sun shine? Is it on FIRE? Is it on FIRE?

More information

Neutron Star Laboratory

Neutron Star Laboratory The µev-pev Neutron Star Laboratory (With some recent progress at GeV) Roger W. Romani Physics/KIPAC Stanford University RDBfest RWR - 1 Roger B. and Neutron Stars Magdalene 1967-1970 CP 1919+21 Nov 67

More information

What can X-ray observations tell us about: The role of Gravitational Waves in Low Mass X-ray Binaries

What can X-ray observations tell us about: The role of Gravitational Waves in Low Mass X-ray Binaries What can X-ray observations tell us about: The role of Gravitational Waves in Low Mass X-ray Binaries Astronomical Institute Anton Pannekoek Low Mass X-ray Binaries Mass is stripped from the donor Forms

More information

Fermi: Highlights of GeV Gamma-ray Astronomy

Fermi: Highlights of GeV Gamma-ray Astronomy Fermi: Highlights of GeV Gamma-ray Astronomy Dave Thompson NASA GSFC On behalf of the Fermi Gamma-ray Space Telescope Large Area Telescope Collaboration Neutrino Oscillation Workshop Otranto, Lecce, Italy

More information

Astro 1050 Fri. Apr. 10, 2015

Astro 1050 Fri. Apr. 10, 2015 Astro 1050 Fri. Apr. 10, 2015 Today: Continue Ch. 13: Star Stuff Reading in Bennett: For Monday: Finish Chapter 13 Star Stuff Reminders: Ch. 12 HW now on Mastering Astronomy, due Monday. Ch. 13 will be

More information

Nuclear burning on! accreting neutron stars. Andrew Cumming! McGill University

Nuclear burning on! accreting neutron stars. Andrew Cumming! McGill University Nuclear burning on accreting neutron stars Andrew Cumming McGill University An exciting time to study accreting neutron stars Type I X-ray bursts H/He layer heavy element ocean 1 105 1cm outer crust 109

More information

Relativistic Astrophysics Neutron Stars, Black Holes & Grav. W. ... A brief description of the course

Relativistic Astrophysics Neutron Stars, Black Holes & Grav. W. ... A brief description of the course Relativistic Astrophysics Neutron Stars, Black Holes & Grav. Waves... A brief description of the course May 2, 2009 Structure of the Course Introduction to General Theory of Relativity (2-3 weeks) Gravitational

More information

Probing Pulsar Winds with Gamma Rays

Probing Pulsar Winds with Gamma Rays Probing Pulsar Winds with Gamma Rays Dmitry Khangulyan Institute of Space and Astronautical Science (ISAS/JAXA) in coll. with Felix Aharonian&Sergey Bogovalov International School on Neutron Star Matter

More information

arxiv:astro-ph/ v3 27 Jul 2000

arxiv:astro-ph/ v3 27 Jul 2000 Draft version February 1, 2008 Preprint typeset using L A TEX style emulateapj v. 04/03/99 PRECURSORS OF GAMMA-RAY BURSTS: A CLUE TO THE BURSTER S NATURE Maxim Lyutikov Canadian Institute for Theoretical

More information

Shallow Decay of X-ray Afterglows in Short GRBs: Energy Injection from a Millisecond Magnetar?

Shallow Decay of X-ray Afterglows in Short GRBs: Energy Injection from a Millisecond Magnetar? Chin. J. Astron. Astrophys. Vol. 7 2007), No. 5, 669 674 http://www.chjaa.org) Chinese Journal of Astronomy and Astrophysics Shallow Decay of X-ray Afterglows in Short GRBs: Energy Injection from a Millisecond

More information

Neutrinos, nonzero rest mass particles, and production of high energy photons Particle interactions

Neutrinos, nonzero rest mass particles, and production of high energy photons Particle interactions Neutrinos, nonzero rest mass particles, and production of high energy photons Particle interactions Previously we considered interactions from the standpoint of photons: a photon travels along, what happens

More information

GRB history. Discovered 1967 Vela satellites. classified! Published 1973! Ruderman 1974 Texas: More theories than bursts!

GRB history. Discovered 1967 Vela satellites. classified! Published 1973! Ruderman 1974 Texas: More theories than bursts! Discovered 1967 Vela satellites classified! Published 1973! GRB history Ruderman 1974 Texas: More theories than bursts! Burst diversity E peak ~ 300 kev Non-thermal spectrum In some thermal contrib. Short

More information

Extended X- ray emission from PSR B /LS 2883 and other gamma- ray binaries

Extended X- ray emission from PSR B /LS 2883 and other gamma- ray binaries Extended X- ray emission from PSR B1259-63/LS 2883 and other gamma- ray binaries George Pavlov (Pennsylvania State University) Oleg Kargaltsev (George Washington University) Martin Durant (University of

More information

Rosalba Perna. (Stony Brook University)

Rosalba Perna. (Stony Brook University) Rosalba Perna (Stony Brook University) Swift observations opened a new window Pre-Swift Pre-Swift Pre-Swift belief belief. of surprises.with PLATEAUS & FLARES [figure courtesy of R. Mockovitch] PLATEAUS

More information

X-ray Spectra from Magnetar Candidates

X-ray Spectra from Magnetar Candidates X-ray Spectra from Magnetar Candidates A Twist in the Field R Turolla Department of Physics University of Padova, Italy With L Nobili, S Zane, N. Sartore GL Israel, N Rea SGRs and AXPs X-ray Spectra SGR

More information

Astronomy 114. Lecture 22: Neutron Stars. Martin D. Weinberg. UMass/Astronomy Department

Astronomy 114. Lecture 22: Neutron Stars. Martin D. Weinberg. UMass/Astronomy Department Astronomy 114 Lecture 22: Neutron Stars Martin D. Weinberg weinberg@astro.umass.edu UMass/Astronomy Department A114: Lecture 22 02 Apr 2007 Read: Ch. 23,24 Astronomy 114 1/20 Announcements PS#5 due Wednesday

More information

Thermal States of Transiently Accreting Neutron Stars in Quiescence

Thermal States of Transiently Accreting Neutron Stars in Quiescence arxiv:1702.08452 Thermal States of Transiently Accreting Neutron Stars in Quiescence Sophia Han University of Tennessee, Knoxville collaboration with Andrew Steiner, UTK/ORNL ICNT Program at FRIB Wednesday

More information

Type Ia Supernova. White dwarf accumulates mass from (Giant) companion Exceeds Chandrasekar limit Goes supernova Ia simul

Type Ia Supernova. White dwarf accumulates mass from (Giant) companion Exceeds Chandrasekar limit Goes supernova Ia simul Type Ia Supernova White dwarf accumulates mass from (Giant) companion Exceeds Chandrasekar limit Goes supernova Ia simul Last stage of superheavy (>10 M ) stars after completing Main Sequence existence

More information

Particle acceleration at relativistic shock waves and gamma-ray bursts

Particle acceleration at relativistic shock waves and gamma-ray bursts Particle acceleration at relativistic shock waves and gamma-ray bursts Martin Lemoine Institut d Astrophysique de Paris CNRS, Université Pierre & Marie Curie Outline: 1. Particle acceleration and relativistic

More information

Afterglows Theory Re em Sari - Caltech

Afterglows Theory Re em Sari - Caltech Π= Π m /3 Afterglows Theory Re em Sari - Caltech 30s 2h t -2 30m t +1/2 t Rising -1 spectrum ν 1/3 1d t -2.2 100d t -1.5 Gamma-Ray Burst: 4 Stages 1) Compact Source, E>10 51 erg 2) Relativistic Kinetic

More information

Sun s Properties. Overview: The Sun. Composition of the Sun. Sun s Properties. The outer layers. Photosphere: Surface. Nearest.

Sun s Properties. Overview: The Sun. Composition of the Sun. Sun s Properties. The outer layers. Photosphere: Surface. Nearest. Overview: The Sun Properties of the Sun Sun s outer layers Photosphere Chromosphere Corona Solar Activity Sunspots & the sunspot cycle Flares, prominences, CMEs, aurora Sun s Interior The Sun as an energy

More information

Chapter 14 Lecture. The Cosmic Perspective Seventh Edition. Our Star Pearson Education, Inc.

Chapter 14 Lecture. The Cosmic Perspective Seventh Edition. Our Star Pearson Education, Inc. Chapter 14 Lecture The Cosmic Perspective Seventh Edition Our Star 14.1 A Closer Look at the Sun Our goals for learning: Why does the Sun shine? What is the Sun's structure? Why does the Sun shine? Is

More information

Chapter 9 The Sun. Nuclear fusion: Combining of light nuclei into heavier ones Example: In the Sun is conversion of H into He

Chapter 9 The Sun. Nuclear fusion: Combining of light nuclei into heavier ones Example: In the Sun is conversion of H into He Our sole source of light and heat in the solar system A common star: a glowing ball of plasma held together by its own gravity and powered by nuclear fusion at its center. Nuclear fusion: Combining of

More information

Stellar Evolution: Outline

Stellar Evolution: Outline Stellar Evolution: Outline Interstellar Medium (dust) Hydrogen and Helium Small amounts of Carbon Dioxide (makes it easier to detect) Massive amounts of material between 100,000 and 10,000,000 solar masses

More information

Cosmological Fast Radio Bursts from Binary White Dwarf Mergers

Cosmological Fast Radio Bursts from Binary White Dwarf Mergers Cosmological Fast Radio Bursts from Binary White Dwarf Mergers Kunihito Ioka (KEK) Kashiyama, KI & Mészáros 13 ~10 yr ago GRB Cosmology Massive star origin High redshift GRBs Like QSO Like SN Star formation

More information

Nuclear symmetry energy and Neutron star cooling

Nuclear symmetry energy and Neutron star cooling Nuclear symmetry energy and Neutron star cooling Yeunhwan Lim 1 1 Daegu University. July 26, 2013 In Collaboration with J.M. Lattimer (SBU), C.H. Hyun (Daegu), C-H Lee (PNU), and T-S Park (SKKU) NuSYM13

More information

High energy neutrino signals from NS-NS mergers

High energy neutrino signals from NS-NS mergers High energy neutrino signals from NS-NS mergers He Gao 高鹤 University of Nevada Las Vegas Collaborators: Bing Zhang, Xue-Feng Wu & Zi-Gao Dai 2013-05-08 Multi-Messenger Workshop @ KIAA EM signals for a

More information

Recent Advances in our Understanding of GRB emission mechanism. Pawan Kumar. Constraints on radiation mechanisms

Recent Advances in our Understanding of GRB emission mechanism. Pawan Kumar. Constraints on radiation mechanisms Recent Advances in our Understanding of GRB emission mechanism Outline Pawan Kumar Constraints on radiation mechanisms High energy emission from GRBs and our understanding of Fermi data. My goal is to

More information

* What are Jets? * How do Jets Shine? * Why do Jets Form? * When were Jets Made?

* What are Jets? * How do Jets Shine? * Why do Jets Form? * When were Jets Made? * What are Jets? * How do Jets Shine? * Why do Jets Form? * When were Jets Made? 1 * Galaxies contain massive black holes which power AGN * Gas accretes through a magnetized disk * Blazars are relativistically

More information

The Magnificent Seven : Strong Toroidal Fields?

The Magnificent Seven : Strong Toroidal Fields? 1 Basic Neutron Star Cooling Troubles: Surface Effects and Pairing Minimal Cooling The Magnificent Seven : Strong Toroidal Fields? Conclusions 2 Basic Neutron Star Cooling Troubles: Surface Effects and

More information

Theory of the prompt emission of Gamma-Ray Bursts

Theory of the prompt emission of Gamma-Ray Bursts Theory of the prompt emission of Gamma-Ray Bursts Department of Physics, NC State University, Raleigh, NC 27695-8202 E-mail: davide_lazzati@ncsu.edu Since their discovery more than 40 years ago the origin

More information

Radiative Processes in Astrophysics

Radiative Processes in Astrophysics Radiative Processes in Astrophysics 11. Synchrotron Radiation & Compton Scattering Eline Tolstoy http://www.astro.rug.nl/~etolstoy/astroa07/ Synchrotron Self-Absorption synchrotron emission is accompanied

More information

Lecture 3 Pulsars and pulsar wind nebulae

Lecture 3 Pulsars and pulsar wind nebulae Lecture 3 Pulsars and pulsar wind nebulae Pulsars Characteristic parameters Pulsar wind nebulae Properties Evolution Exotic central compact objects - Magnetars The Crab Pulsar http://www.jb.man.ac.uk/~pulsar/education/sounds/sounds.html

More information

Relativistic reconnection at the origin of the Crab gamma-ray flares

Relativistic reconnection at the origin of the Crab gamma-ray flares Relativistic reconnection at the origin of the Crab gamma-ray flares Benoît Cerutti Center for Integrated Plasma Studies University of Colorado, Boulder, USA Collaborators: Gregory Werner (CIPS), Dmitri

More information

Neutron Star Structure

Neutron Star Structure Shapiro and Teukolsky, Chapters 2, 8, 9 Neutron Star Structure We now enter the study of neutron stars. Like black holes, neutron stars are one of the three possible endpoints of stellar evolution (the

More information

Envelopes of neutron stars with strong magnetic fields

Envelopes of neutron stars with strong magnetic fields Envelopes of neutron stars with strong magnetic fields Alexander Y. Potekhin Alexander D. Kaminker Dmitry G. Yakovlev Ioffe Physical-Technical Institute (Saint-Petersburg, Russia) Introduction: neutron

More information

The Bizarre Stellar Graveyard

The Bizarre Stellar Graveyard The Bizarre Stellar Graveyard 18.1 White Dwarfs Our goals for learning: What is a white dwarf? What can happen to a white dwarf in a close binary system? What is a white dwarf? White Dwarfs White dwarfs

More information

Death of Stars Part II Neutron Stars

Death of Stars Part II Neutron Stars Death of Stars Part II Neutron Stars 1 REMEMBER THIS!? 2 Guiding Questions 1. What led scientists to the idea of a neutron star? 2. What are pulsars, and how were they discovered? 3. How did astronomers

More information

Magnetic Fields in Blazar Jets

Magnetic Fields in Blazar Jets Magnetic Fields in Blazar Jets Bidzina Z. Kapanadze Ilia State University, Tbilisi, Georgia MFPO 2010- Cracow, May 17-21 Blazars are defined as a AGN class with following features: featureless spectra;

More information

High-energy emission from Gamma-Ray Bursts. Frédéric Daigne Institut d Astrophysique de Paris, Université Pierre et Marie Curie

High-energy emission from Gamma-Ray Bursts. Frédéric Daigne Institut d Astrophysique de Paris, Université Pierre et Marie Curie High-energy emission from Gamma-Ray Bursts Frédéric Daigne Institut d Astrophysique de Paris, Université Pierre et Marie Curie HEPRO III High Energy Phenomena in Relativistic Outflows Barcelona, June 27

More information

Non-thermal emission from Magnetic White Dwarf binary AR Scorpii

Non-thermal emission from Magnetic White Dwarf binary AR Scorpii Non-thermal emission from Magnetic White Dwarf binary AR Scorpii Jumpei Takata (Huazhong University of Science and Technology, China) On behalf of Y. Hui (HUST), C.-P. Hu, K.S. Cheng (HKU, HK), L.C.C.

More information

Unstable Mass Transfer

Unstable Mass Transfer Unstable Mass Transfer When the mass ratios are large, or when the donor star has a deep convective layer (so R M-1/3), mass loss will occur on a dynamical timescale. The result will be common envelope

More information