Accrete, accrete, accrete Bang! (and repeat): The remarkable recurrent novae
|
|
- Mavis Mason
- 5 years ago
- Views:
Transcription
1 Accrete, accrete, accrete Bang! (and repeat): The remarkable recurrent novae Ma= Darnley Liverpool John Moores University Co-conspirators: Mike Bode (LJMU), MarGn Henze (CSIC-IEEC), Rebekah Hounsell (Urbana-Champaign), Mariko Kato (Keio), Tim O Brien (Manchester), Valerio Ribeiro (Radboud), Allen ShaRer (SDSU), Mike Shara (AMNH), and Steve Williams (Lancaster)
2 Novae: Vital StaGsGcs Primary: White Dwarf 0.5 ~1.4 Solar Masses (Chandrasekhar mass) CO or ONe(Mg) Plus He and H layers Secondary: `Late Type MS star Typically Solar-ish composigon Orbital period hrs Roche lobe filling Mass AccreGon: Solar material Hydrogen rich AccreGon rate: 10-9 Solar masses / year Luminosity: Quiescence: ~ Solar Luminosity ErupGon: ~10 4 Solar Eddington luminosity Ejected Mass: Solar Masses ComposiGon: depleted H, enhanced He/N Possible Ne enhancement is ONe WD Recurrence Period: 1,000 1,000,000 years 1,000s of erupgons per system Recurrent Novae: >1 observed erupgon Secondary: Evolved Orbital period: >1 day High accregon rate (up to 10-7 M sun / yr High mass WD (>1.2 M sun )
3 Nova mechanism
4 Classical vs Recurrent Novae Classical Novae Only one observed erupgon Recurrence Gmescales few thousand million years (predicted) Secondaries main sequence stars Low mass transfer/accregon rates Range of WD masses Range of evolugon speeds Range of ejecgon velociges Mix of Fe II and He/N spectra 400 GalacGc systems (1000 M31) WD mass decreasing Recurrent Novae >1 observed erupgon Recurrence Gmescales years Secondaries sub-giants (U Sco) or red giants (RS Oph) High mass transfer/accregon rates High WD Masses Rapid erupgon evolugon High ejecgon velociges He/N spectra 10 GalacGc systems (16 M31, 3 LMC) WD mass increasing è SN Ia (?)
5 Classical vs Recurrent Novae Classical Novae Only one observed erupgon Recurrence Gmescales few thousand million years (predicted) The problema6c systems Secondaries main sequence stars Low mass transfer/accregon rates Range of WD masses Recurrent Novae >1 observed erupgon Recurrence Gmescales years Secondaries sub-giants (U Sco) or red giants (RS Oph) GK Per classical nova hosgng a sub-giant secondary T Pyx recurrent nova with a main High sequence mass transfer/accregon secondary, rates low mass WD, slowly evolving erupgons, High WD Fe Masses II spectrum Range of evolugon Plus speeds others! Rapid erupgon evolugon Range of ejecgon velociges High ejecgon velociges Mix of Fe II and He/N spectra He/N spectra 400 GalacGc systems (1000 M31) 10 GalacGc systems (16 M31, 3 LMC) WD mass decreasing WD mass increasing è SN Ia (?)
6 The Liverpool Telescope The World s Largest Fully Robo)c Telescope
7 M31N b Bode & Darnley et al The first extragalacgc nova to be observed in opgcal, UV and X-rays, and spectroscopically confirmed IniGally thought to be recurrent due to posigonal coincidence with a X-ray observagons and opgcal spectra consistent with recurrent nova HST archival data revealed progenitor system red giant secondary First recovery of a nova progenitor beyond the Milky Way
8 M31N b Bode & Darnley et al The first extragalacgc nova to be observed in opgcal, UV and X-rays, and spectroscopically confirmed IniGally thought to be recurrent due to posigonal coincidence with a X-ray observagons and opgcal spectra consistent with recurrent nova HST archival data revealed progenitor system red giant secondary First recovery of a nova progenitor beyond the Milky Way
9 GalacGc Progenitors Darnley The problem with GalacGc nova studies is the distance... the problem with extragalacgc studies is the distance(!) Can we carry out a stagcally significant survey of extragalacgc progenitors AssumpGon: the colour & magnitude of a quiescent nova can be used to determine secondary type Colour-mag posigon is determined by the secondary accregon disk shirs emission blue-wards and luminosity upwards Blue MS-novae (CNe); Green SGnovae; Red RG-novae
10 GalacGc Progenitors Darnley The problem with GalacGc nova studies is the distance... the problem with extragalacgc studies is the distance(!) Can we carry out a stagcally significant survey of extragalacgc progenitors AssumpGon: the colour & magnitude of a quiescent nova can be used to determine secondary type Colour-mag posigon is determined by the secondary accregon disk shirs emission blue-wards and luminosity upwards Blue MS-novae (CNe); Green SGnovae; Red RG-novae
11 ExtragalacGc novae
12 ExtragalacGc Progenitors Darnley+ 2013
13 M31 Nova Survey ShaRer & Darnley et al. (2011), Williams & Darnley et al. (2014, 2016) Extensive follow-up survey of M31 novae: August 2006?? (Sala in prep) Lead faciliges: Liverpool Telescope (phot +spec), HET (spec), HST (archive) Photometric, spectroscopic, astrometric follow-up survey of almost 100 novae (3x the spectroscopically confirmed sample) As with M31N b, uglising the HST archive for quiescent detecgon
14 M31 Quiescent Nova Survey Williams & Darnley et al. (2014)
15 M31 Quiescent Nova Survey Williams & Darnley et al. (2016) Progenitor Survey Highlights 30±12 % of M31 nova erupgons occur in RGnova systems The tradigonal GalacGc proporgon is ~3 % Order of magnitude increase in the RG-nova populagon size same affect to their SN Ia contribugon(?) RG-novae are associated with the disk (young) stellar populagon of M31 Result is consistent with all the RG-novae being disk novae No nova SN Ia contribugon from novae in early-type galaxies(?)
16 RNe / RG-novae è SNe Ia (?) Many models now show RN WD mass is growing with Gme He-flashes on high mass WDs may not cause significant mass loss High mass WD and high accregon rate drive shorter recurrence Gmes Short recurrence Gmes drive WD mass growth rates PredicGons limit recurrence periods to 50 days as approach Chandrasekhar limit Minor quesgon about the WD composigon CO vs. ONe GalacGcally RG-nova: RS Oph 20 yrs SG-nova: U Sco 10 yrs LMC LMCN a 6 years (as of 2016) M31 M31N c 5 years But wouldn't it be nice to find something more extreme?! A system much closer to the 50 day limit? But we need to find the extreme system(s)
17 M31N a 2008 M31 transient discovered 2009 ErupGon announced (PTF; Tang+ 2014) 2010 ErupGon recovered (Henze+ 2015) 2011 Erupted again 2012 Spectroscopically confirmed 2013 iptf discover erupgon 2014 LT detects predicted erupgon (Darnley+ 2015) Transient X-ray detecgons: 1992, 1993, and 2001 At least one opgcal erupgon in 1960s
18 M31N a: The missing 2010 erupgon Henze & Darnley et al
19 M31N a: The recurrence period Henze & Darnley et al The OpGcal ErupGons 26 Dec Dec Nov Oct Oct Nov Oct 2014 Extrapolated from X-ray detecgons 5 Feb 1992 (ROSAT) 11 Jan 1993 (ROSAT) 8 Sep 2001 (XMM)
20 M31N a: Recurrence period opgcal erupgons Henze & Darnley et al t rec = 351 ± 13 days
21 M31N a: The recurrence period Henze & Darnley et al The OpGcal ErupGons 26 Dec Dec Nov Oct Oct Nov Oct 2014 Extrapolated from X-ray detecgons 5 Feb 1992 (ROSAT) 11 Jan 1993 (ROSAT) 8 Sep 2001 (XMM)
22 M31N a: Recurrence period vs. X-ray detecgons Henze & Darnley et al. 2015
23 M31N a: Recurrence period vs. X-ray detecgons Henze & Darnley et al. 2015
24 M31N a: A recurrence period of 6 months? Henze & Darnley et al t rec = 175 ± 11 days
25 M31N a: Where are the missing erupgons? Henze & Darnley et al. 2015
26 M31N a: The recurrence period Darnley+ in prep The OpGcal ErupGons 26 Dec Dec Nov Oct Oct Nov Oct Aug 2015 Extrapolated from X-ray detecgons 5 Feb 1992 (ROSAT) 11 Jan 1993 (ROSAT) 8 Sep 2001 (XMM)
27 M31N a: 2015 erupgon r -band Darnley+ in prep
28 M31N a: erupgon r -band Darnley+ in prep
29 M31N a: Always the same? Darnley+ in prep
30 M31N a: 2015 erupgon opgcal spectra Darnley+ in prep
31 M31N a: 2014 vs 2015 Hα Development Darnley+ in prep
32 M31N a: 2014 vs 2015 Hα Development Darnley+ in prep
33 M31N a: SupersoR X-ray source light curve Darnley+ in prep No detecgon of SSS following 2012 erupgon First X-ray detecgon followed 2013 erupgon Turn-on detected by SwiR 5.9 ± 0.5 days post erupgon BB fit to X-ray spectra gives kt = 120 ± 5 ev (~1.4 million K) Count rate declined at day 16: turn-off 18.4 ± 0.5 days
34 M31N a: Hubble Space Telescope Campaign
35 M31N a: Hubble Space Telescope Campaign Darnley+ in prep Cycle 23 Proposal Successful (yay) Rapid STIS NUV and FUV (low res spectroscopy; Angstroms) DToO STIS FUV-MAMA 4 orbits, 1 visit DToO STIS NUV-MAMA 4 orbits, split over 2 visits 4 WFC3/UVIS visits (F225W, F275W, F336W, F475W, F814W) Visit 1 3 orbits - ~day 14 Visit 2 3 orbits - ~day 21 Visit 3 3 orbits - ~day 28 Visit 4 3 orbits - ~day 35 (~quiescence)
36 M31N a: HST photometry (F336W U-band) Darnley+ in prep
37 M31N a: HST photometry Darnley+ in prep
38 Quiescent photometry Darnley+ 2014
39 M31N a: HST PHAT photometry Darnley+ in prep
40 M31N a: The remnant?!?!(?!) Darnley+ 2015
41 M31N a: The remnant s spectrum! Darnley+ 2015
42 Models of M31N a WD mass 1.35M, dm/dt > M /yr (Kato+ 2014; based on 2013 data) ErupGons consistent with models of systems with >1.377M & 1.358M WDs (Henze+/Kato+ 2015; 2013/14 data) AccreGon rate > 10-7 M / year Mass accumulagon efficiency 0.64 (Kato+ 2015) Timescale to reach Chandrasekhar mass < 0.6 Myr (Tang+ 2014)
43 Conclusions / ImplicaGons / QuesGons A recurrent nova with an unprecedented 1 year (six months?) inter-erupgon Gme M31N a is the prime SN Ia SD-channel pre-explosion progenitor candidate Are such systems rare or common? Secondary type (RG vs. SG) sgll relagvely uncertain accregon mechanism? White dwarf composigon (CO vs. ONe) unknown can we ever know this? 1 sigma confidence periods for 2016 erupgons: 26 th Feb 19 th Apr & 21 st Aug 13 th Oct DetecGon and follow-up campaigns for the 2016 erupgon(s) coming together including LT, LCOGT, XMM (all confirmed), plus HST, Swi., GTC, Gemini, Keck, LBT + more ground-based
The 2006 Outburst of RS Oph: What are the questions that need to be discussed --and answered?
The 2006 Outburst of RS Oph: What are the questions that need to be discussed --and answered? Sumner Starrfield School of Earth and Space Exploration Arizona State University WHY DO WE CARE? RS Oph may
More informationV2487 Oph 1998: a puzzling recurrent nova observed with XMM-Newton
V2487 Oph 1998: a puzzling recurrent nova observed with XMM-Newton Margarita Hernanz Institute of Space Sciences (CSIC-IEEC) - Barcelona (Spain) Gloria Sala (UPC-IEEC), Nataly Ospina (CSIC-IEEC) V2487
More informationX-rays from nova explosions
X-rays from nova explosions Margarita Hernanz Institute of Space Sciences, ICE (CSIC-IEEC) Bellaterra (Barcelona) Spanish X-ray Astronomy Santander 3-5 June 2015 M. Hernanz 1 Scenario of nova explosions:
More informationX-ray emission from optical novae in M 31. Wolfgang Pietsch (MPE)
X-ray emission from optical novae in M 31 Wolfgang Pietsch (MPE) Outline Introduction to SSS emission from novae in M 31 First XMM-Newton survey of M 31 Optical novae: the major class of SSS in M31 The
More informationBinary Evolution Novae, Supernovae, and X-ray Sources
Binary Evolution Novae, Supernovae, and X-ray Sources The Algol Mystery Algol is a double-lined eclipsing binary system with a period of about 3 days (very short). The two stars are: Star A: B8, 3.4M o
More informationBinary Evolution Novae, Supernovae, and X-ray Sources
Binary Evolution Novae, Supernovae, and X-ray Sources http://apod.nasa.gov/apod/ http://www.space.com/32150-farthest-galaxy-smashes-cosmic-distance-record.html The Algol Mystery Algol is a double-lined
More informationBasics, types Evolution. Novae. Spectra (days after eruption) Nova shells (months to years after eruption) Abundances
Basics, types Evolution Novae Spectra (days after eruption) Nova shells (months to years after eruption) Abundances 1 Cataclysmic Variables (CVs) M.S. dwarf or subgiant overflows Roche lobe and transfers
More informationThe Algol Mystery. Binary Evolution Novae, Supernovae, and X-ray Sources. Algol. Mass Transfer in Binaries
The Algol Mystery Binary Evolution Novae, Supernovae, and X-ray Sources http://apod.nasa.gov/apod/ Algol is a double-lined eclipsing binary system with a period of about 3 days (very short). The two stars
More informationThe multifrequency behaviour of the recurrent nova RS Ophiuchi
Mem. S.A.It. Vol. 83, 762 c SAIt 2012 Memorie della The multifrequency behaviour of the recurrent nova RS Ophiuchi Valério A. R. M. Ribeiro Astrophysics, Cosmology and Gravity Centre, Department of Astronomy,
More informationLJMU Research Online
LJMU Research Online Williams, SC, Darnley, MJ, Bode, MF and Shafter, AW On the Progenitors of Local Group Novae. II. The Red Giant Nova Rate of M31 http://researchonline.ljmu.ac.uk/2476/ Article Citation
More informationAstronomy in the news? Government shut down. No astronomy picture of the day
Wednesday, October 2, 2013 Exam 2 Friday. Review sheet posted. Review session Tomorrow, 5 6 PM, WRW 102 Reading: Sections 6.1 (Type Ib/c), 6.4, 6.5 (but not detail on polarization), 6.6, Betelgeuse, Section
More informationThermonuclear shell flashes II: on WDs (or: classical novae)
: on WDs (or: classical novae) Observations Thermonuclear flash model Nova/X-ray burst comparison Effects of super-eddington fluxes To grow or not to grow = to go supernova Ia or not.. 1 Nova Cygni 1975
More informationThe structure and evolution of stars. Learning Outcomes
The structure and evolution of stars Lecture14: Type Ia Supernovae The Extravagant Universe By R. Kirshner 1 Learning Outcomes In these final two lectures the student will learn about the following issues:
More informationDistant Type Ia supernova Refsdal gravitationally lensed, appears multiple places and times.
Friday, March 6, 2015 Reading for Exam 3: Chapter 6, end of Section 6 (binary evolution), Section 6.7 (radioactive decay), Chapter 7 (SN 1987A) Background in Chapters 3, 4, 5. Background: Sections 3.1,
More informationFORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS
FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS Main Categories of Compact Systems Formation of Compact Objects Mass and Angular Momentum Loss Evolutionary Links to Classes of Binary Systems Future Work
More informationV5116 Sgr (Nova Sgr 2005b): an eclipsing supersoft postoutburst nova?
V5116 Sgr (Nova Sgr 2005b): an eclipsing supersoft postoutburst nova? (UPC-IEEC, Barcelona) Margarita Hernanz, Carlo Ferri (CSIC-IEEC, Barcelona) Jochen Greiner (MPE, Garching) X-ray emission from Classical
More informationBrian P. Schmidt Wolfgang Kerzendorf, Anna Frebel, Martin Asplund, Ken Nomoto, Philipp Podsiadlowski
Brian P. Schmidt Wolfgang Kerzendorf, Anna Frebel, Martin Asplund, Ken Nomoto, Philipp Podsiadlowski The Research School of Astronomy & Astrophysics Mount Stromlo and Siding Spring Observatories 1 2 SkyMapper
More informationThe dynamical sky Two frontiers Joel Johansson, Uppsala university
The dynamical sky Two frontiers Joel Johansson, Uppsala university Time Wavelength Optical surveys faster! HSC, 1.7 deg 2 DES, 2.5 deg 2 PS1, 7 deg 2 PTF/iPTF, 7.3 deg 2 ZTF, 47 deg 2 LSST, 9.6 deg 2 Survey
More informationEvolution and Final Fates of Accreting White Dwarfs. Ken Nomoto (Kavli IPMU / U. Tokyo)
Evolution and Final Fates of Accreting White Dwarfs Ken Nomoto (Kavli IPMU / U. Tokyo) AD 1572 Korean & Chinese Record Guest Star as bright as Venus (Sonjo Sujong Sillok: Korea) AD 1572 Tycho Brahe s Supernova
More informationOptical studies of an ultraluminous X-ray source: NGC1313 X-2
Optical studies of an ultraluminous X-ray source: NGC1313 X-2 Jifeng Liu Harvard-Smithsonian Center for Astrophysics in collaboration with Joel Bregman, Jon Miller, Philip Kaaret outline background: ultraluminous
More informationSupplementary Information for SNLS-03D3bb a super- Chandrasekhar mass Type Ia supernova
1 Supplementary Information for SNLS-03D3bb a super- Chandrasekhar mass Type Ia supernova SN Location SNLS-03D3bb is located at RA: 14:16:18.920 Dec: +52:14:53.66 (J2000) in the D3 (extended Groth Strip)
More informationX-ray Studies of Classical Novae & Super Soft Sources (SSS) Jan-Uwe Ness Chandra Fellow at
X-ray Studies of Classical Novae & Super Soft Sources (SSS) Jan-Uwe Ness Chandra Fellow at outburst Nuclear burning ignites WD Accreted material: H-rich! Radiatively driven expansion Nuclear burning Pseudo
More informationSupernova Explosions. Novae
Supernova Explosions Novae Novae occur in close binary-star systems in which one member is a white dwarf. First, mass is transferred from the normal star to the surface of its white dwarf companion. 1
More informationEmission lines spectra and novae. OHP Spectro Party August 15 Ivan De Gennaro Aquino
Emission lines spectra and novae OHP Spectro Party 2012 - August 15 Ivan De Gennaro Aquino Some cheap atomic physics - 1 The black body spectrum (Planck sp.) Some cheap atomic physics - 2 Niels Bohr atomic
More informationStellar Explosions (ch. 21)
Stellar Explosions (ch. 21) First, a review of low-mass stellar evolution by means of an illustration I showed in class. You should be able to talk your way through this diagram and it should take at least
More informationOld Novae: When New Becomes Old
: When New Becomes Old Instituto de Astrofisica de Canarias C. Tappert (UV), L. Schmidtobreick (ESO), N. Vogt (UV) Evolution of Compact Binaries (Viña del Mar, Chile) 9th March 2009 1 of 14 : An Introduction
More informationThe Deaths of Stars. The Southern Crab Nebula (He2-104), a planetary nebula (left), and the Crab Nebula (M1; right), a supernova remnant.
The Deaths of Stars The Southern Crab Nebula (He2-104), a planetary nebula (left), and the Crab Nebula (M1; right), a supernova remnant. Once the giant phase of a mediummass star ends, it exhales its outer
More informationSymbiotic stars: challenges to binary evolution theory. Joanna Mikołajewska Copernicus Astronomical Center, Warsaw
Symbiotic stars: challenges to binary evolution theory Joanna Mikołajewska Copernicus Astronomical Center, Warsaw Symbiotic stars S(stellar) normal giant 80% M g ~10-7 M sun /yr P orb ~ 1-15 yr Accreting
More informationAnnouncement: Quiz Friday, Oct 31
Announcement: Quiz Friday, Oct 31 What is the difference between the giant, horizontal, and asymptotic-giant branches? What is the Helium flash? Why can t high-mass stars support themselves in hydrostatic
More informationThis 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 informationLecture 8: Stellar evolution II: Massive stars
Lecture 8: Stellar evolution II: Massive stars Senior Astrophysics 2018-03-27 Senior Astrophysics Lecture 8: Stellar evolution II: Massive stars 2018-03-27 1 / 29 Outline 1 Stellar models 2 Convection
More informationSupernova Explosions. Novae
Supernova Explosions Novae Novae occur in close binary-star systems in which one member is a white dwarf. First, mass is transferred from the normal star to the surface of its white dwarf companion. 1
More informationSpectroscopic follow-up of novae
Mem. S.A.It. Vol. 83, 753 c SAIt 2012 Memorie della Spectroscopic follow-up of novae R. Poggiani 1,2 1 Dipartimento di Fisica, Università di Pisa, Largo Pontecorvo, 3, I-56127 Pisa, Italy e-mail: rosa.poggiani@df.unipi.it
More informationSearching for the Progenitors of Subluminous Type Ia Supernovae with SN 2013bc
Hubble Space Telescope Cycle 11 General Observer Proposal Searching for the Progenitors of Subluminous Type Ia Supernovae with SN 2013bc Principal Investigator: Institution: Electronic mail: Maximilian
More informationThe Evolution of Binary-Star Systems
The Evolution of Binary-Star Systems If the stars in a binary-star system are relatively widely separated, their evolution proceeds much as it would have if they were not companions... If they are closer,
More informationThe Evolution of Close Binaries
The Evolution of Close Binaries Philipp Podsiadlowski (Oxford) The case of RS Ophiuchi as a test of binary stellar evolution as a potential Type Ia supernova (SN Ia) progenitor I. Testing Binary Evolution:
More informationNational Science Olympiad Astronomy C Division Event 19 May 2012 University of Central Florida Orlando, FL
National Science Olympiad Astronomy C Division Event 19 May 2012 University of Central Florida Orlando, FL Artist Illustration of Red Giant, White Dwarf and Accretion Disk (Wikimedia) TEAM NUMBER: TEAM
More informationUnconventional observations of classical and recurrent novae
Mem. S.A.It. Vol. 83, 77 c SAIt 01 Memorie della Unconventional observations of classical and recurrent novae E. Mason Space Telescope Science Institute 3700 S. Martin Drive, Baltimore, MD 118 e-mail:
More informationWhite dwarf populations. Gijs Nelemans Radboud University Nijmegen
White dwarf populations Gijs Nelemans Radboud University Nijmegen Outline Introduction: Population synthesis Basic ingredients Observational inputs White dwarf populations Different types and mergers WD
More informationHR Diagram, Star Clusters, and Stellar Evolution
Ay 1 Lecture 9 M7 ESO HR Diagram, Star Clusters, and Stellar Evolution 9.1 The HR Diagram Stellar Spectral Types Temperature L T Y The Hertzsprung-Russel (HR) Diagram It is a plot of stellar luminosity
More informationiptf16fnl - a faint and fast TDE in an E+A galaxy
iptf16fnl - a faint and fast TDE in an E+A galaxy Nadia (Nadejda) Blagorodnova with Suvi Gezari, Tiara Hung, Shri Kulkarni, Brad Cenko, Lin Yan Unveiling the Physics Behind Extreme AGN Variability 12th
More informationDead & Variable Stars
Dead & Variable Stars Supernovae Death of massive Stars As the core collapses, it overshoots and bounces A shock wave travels through the star and blows off the outer layers, including the heavy elements
More informationEndpoints of Stellar Evolution. Dicy Saylor ASTR 8000 Nov 19, 2014
Endpoints of Stellar Evolution Dicy Saylor ASTR 8000 Nov 19, 2014 Overview White Dwarfs PNNe, White Dwarfs, and PG1159, oh my! Novae Classical Novae and Cataclysmic Variables Supernovae Type I and Type
More informationWednesday, September 7, 2011 First exam Friday. First Sky Watch due. Review sheet posted. Reading posted under announcements on web page, Section
Wednesday, September 7, 2011 First exam Friday. First Sky Watch due. Review sheet posted. Reading posted under announcements on web page, Section 5.1, Sections 6.1 6.3, other background. Exam will draw
More informationThe first two transient supersoft X-ray sources in M 31 globular clusters and the connection to classical novae
The first two transient supersoft X-ray sources in M 31 globular clusters and the connection to classical novae Max Planck Institute for extraterrestrial physics Wolfgang Pietsch, Frank Haberl, Gloria
More informationarxiv:astro-ph/ v1 23 Oct 2002
Evolution of the symbiotic nova RX Puppis J. Mikołajewska, E. Brandi, L. Garcia, O. Ferrer, C. Quiroga and G.C. Anupama arxiv:astro-ph/0210505v1 23 Oct 2002 N. Copernicus Astronomical Center, Bartycka
More informationProgenitor signatures in Supernova Remnant Morphology. Jacco Vink Utrecht University
Progenitor signatures in Supernova Remnant Morphology Jacco Vink Utrecht University The evolution of SNRs Heating by two shocks: 1. forward shocks heating ISM/CSM 2. reverse shock heating ejecta radius
More informationHigh Redshift Universe
High Redshift Universe Finding high z galaxies Lyman break galaxies (LBGs) Photometric redshifts Deep fields Starburst galaxies Extremely red objects (EROs) Sub-mm galaxies Lyman α systems Finding high
More informationarxiv: v1 [astro-ph.sr] 1 Oct 2014
STELLA NOVAE: PAST AND FUTURE DECADES ASP Conference Series, Vol. 490 P. A. Woudt and V. A. R. M. Ribeiro, eds c 2014 Astronomical Society of the Pacific On the Evolution of the Late-time Hubble Space
More informationExcavation or Accretion from Classical Novae (or related objects) Sumner Starrfield
Excavation or Accretion from Classical Novae (or related objects) Sumner Starrfield School of Earth and Space Exploration Arizona State University KITP March 20, 2007 Collaborators: Peter Hauschildt: Hamburg
More informationStellar Evolution. Stars are chemical factories The Earth and all life on the Earth are made of elements forged in stars
Lecture 11 Stellar Evolution Stars are chemical factories The Earth and all life on the Earth are made of elements forged in stars A Spiral Galaxy (Milky Way Type) 120,000 ly A few hundred billion stars
More informationOutline. Stellar Explosions. Novae. Death of a High-Mass Star. Binding Energy per nucleon. Nova V838Mon with Hubble, May Dec 2002
Outline Novae (detonations on the surface of a star) Supernovae (detonations of a star) The Mystery of Gamma Ray Bursts (GRBs) Sifting through afterglows for clues! Stellar Explosions Novae Nova V838Mon
More informationDASCH To explore the ~1wk ~100y )mescale and extreme variability of stellar and non stellar objects
The ul'mate Wide Field TDA Survey: DASCH To explore the ~1wk ~100y )mescale and extreme variability of stellar and non stellar objects Josh Grindlay (and Sumin Tang & DASCH Team) Wide Field Surveys lunch,
More informationThe electrons then interact with the surrounding medium, heat it up, and power the light curve. 56 Ni 56 Co + e (1.72 MeV) half life 6.
Supernovae The spectra of supernovae fall into many categories (see below), but beginning in about 1985, astronomers recognized that there were physically, only two basic types of supernovae: Type Ia and
More informationClassification of nova spectra
International Workshop on Stellar Spectral Libraries ASI Conference Series, 2012, Vol. 6, pp 143 149 Edited by Ph. Prugniel & H. P. Singh Classification of nova spectra G. C. Anupama Indian Institute of
More informationClassical Novae as supersoft X-ray sources in the Andromeda galaxy (M 31)
Classical Novae as supersoft X-ray sources in the Andromeda galaxy (M 31) Martin Henze for the M 31 nova monitoring collaboration The monitoring collaboration The Team (past and present) Wolfgang Pietsch
More informationDistribution of X-ray binary stars in the Galaxy (RXTE) High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars
High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars Distribution of X-ray binary stars in the Galaxy (RXTE) Robert Laing Primary Compact accreting binary systems Compact star WD NS BH
More informationHLX-1: unsolved puzzles
HLX-1: unsolved puzzles Roberto Soria Many thanks to: Sean Farrell Francesca Annibali Jeanette Gladstone Pasi Hakala George Hau Paul Kuin Michela Mapelli Manfred Pakull Luca Zampieri Brindisi 2013 Outline
More informationSTELLAR HEAVY ELEMENT ABUNDANCES AND THE NATURE OF THE R-PROCESSR. JOHN COWAN University of Oklahoma
STELLAR HEAVY ELEMENT ABUNDANCES AND THE NATURE OF THE R-PROCESSR JOHN COWAN University of Oklahoma First Stars & Evolution of the Early Universe (INT) - June 19, 2006 Top 11 Greatest Unanswered Questions
More information7. BINARY STARS (ZG: 12; CO: 7, 17)
7. BINARY STARS (ZG: 12; CO: 7, 17) most stars are members of binary systems or multiple systems (triples, quadruples, quintuplets,...) orbital period distribution: P orb = 11 min to 10 6 yr the majority
More informationAstronomy Ch. 21 Stellar Explosions. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Name: Period: Date: Astronomy Ch. 21 Stellar Explosions MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A surface explosion on a white dwarf, caused
More informationObserving the Formation of Dense Stellar Nuclei at Low and High Redshift (?) Roderik Overzier Max-Planck-Institute for Astrophysics
Observing the Formation of Dense Stellar Nuclei at Low and High Redshift (?) Roderik Overzier Max-Planck-Institute for Astrophysics with: Tim Heckman (JHU) GALEX Science Team (PI: Chris Martin), Lee Armus,
More informationThe fundamental INTEGRAL contributions to advance the millisecond X-ray pulsars research field
The fundamental INTEGRAL contributions to advance the millisecond X-ray pulsars research field M A U R I Z I O F A L A N G A Collaborators: L. Kuipers, W. Hermsen, J. Poutanen, A. Goldwurm, L. Stella June
More informationThe Death of Stars. Today s Lecture: Post main-sequence (Chapter 13, pages ) How stars explode: supernovae! White dwarfs Neutron stars
The Death of Stars Today s Lecture: Post main-sequence (Chapter 13, pages 296-323) How stars explode: supernovae! White dwarfs Neutron stars White dwarfs Roughly the size of the Earth with the mass of
More informationRaman Spectroscopy in Symbiotic Stars. Jeong-Eun Heo Sejong University, Korea Gemini Observatory, Chile
Raman Spectroscopy in Symbiotic Stars Jeong-Eun Heo Sejong University, Korea Gemini Observatory, Chile Jeong-Eun, Heo Ph.D Student Dept. of Astronomy, Sejong University, Seoul, Korea The astrophysical
More informationA search for supernova type Ia progenitors in the Magellanic Clouds. Kelly Lepo
A search for supernova type Ia progenitors in the Magellanic Clouds by Kelly Lepo A thesis submitted in conformity with the requirements for the degree of Doctor of Philosophy Graduate Department of Astronomy
More informationLow state transitions in the nova-like cataclysmic variable HS Jeremy Shears. Abstract
Low state transitions in the nova-like cataclysmic variable HS 0506+7725 Jeremy Shears Abstract The twelve-year light curve of the nova-like cataclysmic variable HS 0506+7725 between 2006 April and 2018
More informationLecture 13: Binary evolution
Lecture 13: Binary evolution Senior Astrophysics 2017-04-12 Senior Astrophysics Lecture 13: Binary evolution 2017-04-12 1 / 37 Outline 1 Conservative mass transfer 2 Non-conservative mass transfer 3 Cataclysmic
More informationThe Progenitors of Type Ia Supernovae
The Progenitors of Type Ia Supernovae Philipp Podsiadlowski, Richard Booth, Mark Sullivan (Oxford), Shazrene Mohamed (Bonn), Paolo Mazzali (MPA/Padova), Zhanwen Han (Kunming), Stephen Justham (Beijing),
More informationRupali Chandar University of Toledo
Star Formation in Clusters Rupali Chandar University of Toledo Star Clusters: Near and Far. Very Near: ONC (400 pc) ~103 Msun Near: NGC 3603 (7 kpc) ~104 Msun Star Clusters: Near and Far. Kinda Near: R136
More informationStars and their properties: (Chapters 11 and 12)
Stars and their properties: (Chapters 11 and 12) To classify stars we determine the following properties for stars: 1. Distance : Needed to determine how much energy stars produce and radiate away by using
More informationASTR Midterm 2 Phil Armitage, Bruce Ferguson
ASTR 1120-001 Midterm 2 Phil Armitage, Bruce Ferguson SECOND MID-TERM EXAM MARCH 21 st 2006: Closed books and notes, 1 hour. Please PRINT your name and student ID on the places provided on the scan sheet.
More informationPENNSYLVANIA SCIENCE OLYMPIAD STATE FINALS 2012 ASTRONOMY C DIVISION EXAM APRIL 27, 2012
PENNSYLVANIA SCIENCE OLYMPIAD STATE FINALS 2012 ASTRONOMY C DIVISION EXAM APRIL 27, 2012 TEAM NUMBER SCHOOL NAME INSTRUCTIONS: 1. Turn in all exam materials at the end of this event. Missing exam materials
More informationAstronomy 110: SURVEY OF ASTRONOMY. 11. Dead Stars. 1. White Dwarfs and Supernovae. 2. Neutron Stars & Black Holes
Astronomy 110: SURVEY OF ASTRONOMY 11. Dead Stars 1. White Dwarfs and Supernovae 2. Neutron Stars & Black Holes Low-mass stars fight gravity to a standstill by becoming white dwarfs degenerate spheres
More informationAstronomy. 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 informationA new method to search for Supernova Progenitors in the PTF Archive. Frank Masci & the PTF Collaboration
A new method to search for Supernova Progenitors in the PTF Archive Frank Masci & the PTF Collaboration 1 The Palomar Transient Factory (PTF) Fully automated wide-field time-domain survey in optical Carried
More informationGaia Revue des Exigences préliminaires 1
Gaia Revue des Exigences préliminaires 1 Global top questions 1. Which stars form and have been formed where? - Star formation history of the inner disk - Location and number of spiral arms - Extent of
More informationAstronomy Ch. 22 Neutron Stars and Black Holes. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Name: Period: Date: Astronomy Ch. 22 Neutron Stars and Black Holes MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) In a neutron star, the core
More informationDr. Reed L. Riddle. Close binaries, stellar interactions and novae. Guest lecture Astronomy 20 November 2, 2004
Dr. Reed L. Riddle Close binaries, stellar interactions and novae Guest lecture Astronomy 20 November 2, 2004 Gravitational Tides Look at the forces acting on one body orbiting another - more pull on closer
More informationExplosive Events in the Universe and H-Burning
Explosive Events in the Universe and H-Burning Jordi José Dept. Física i Enginyeria Nuclear, Univ. Politècnica de Catalunya (UPC), & Institut d Estudis Espacials de Catalunya (IEEC), Barcelona Nuclear
More informationThe 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 informationMonday, January 30, 2012 First exam Friday. First Sky Watch due. Review sheet posted. Reading posted under announcements on web page, Chapter 6 -
Monday, January 30, 2012 First exam Friday. First Sky Watch due. Review sheet posted. Reading posted under announcements on web page, Chapter 6 - Sections 6.1, 6.2, 6.3 (also sections 1.2.4, 2.1-2.5, and
More informationThe SWARMS Survey: Unveiling the Galactic population of Compact White Dwarf Binaries
The SWARMS Survey: Unveiling the Galactic population of Compact White Dwarf Binaries Weizmann Institute of Science / Tel-Aviv University Type Ia SN Progenitors Workshop Leiden, September 22 2010 Steve
More informationPhysics HW Set 3 Spring 2015
1) If the Sun were replaced by a one solar mass black hole 1) A) life here would be unchanged. B) we would still orbit it in a period of one year. C) all terrestrial planets would fall in immediately.
More informationSix Years of Astrophysics with the Far Ultraviolet Spectroscopic Explorer
Six Years of Astrophysics with the Far Ultraviolet Spectroscopic Explorer George Sonneborn FUSE Project Scientist NASA s Goddard Space Flight Center 207th AAS Meeting Washington, DC 12 Jan. 2006 FUSE Mission
More informationPlanets around evolved stellar systems. Tom Marsh, Department of Physics, University of Warwick
Planets around evolved stellar systems Tom Marsh Department of Physics, University of Warwick Tom Marsh, Department of Physics, University of Warwick Slide 1 / 35 Tom Marsh, Department of Physics, University
More informationObservational summary
Observational summary Andy Howell Las Cumbres Observatory Global Telescope Network University of California Santa Barbara Entertainment value Scientific quality Rene Magritte: The Treachery of Images
More informationLecture 24. Reprise: Evolution Timescale
Lecture 24 Life as a Low Mass Giant Dating the Stars Shell vs Core Fusion Helium Fusion Planetary Nebulae Mar 22, 2006 Astro 100 Lecture 24 1 Reprise: Evolution Timescale To estimate the duration of any
More informationNames: Team: Team Number:
Astronomy C Michigan Region 8 March 11, 2017 Names: Team: Team Number: Directions 1. There is a separate answer sheet. Answers written elsewhere (e.g. on the test) will not be considered. 2. You may take
More informationBinary stars, their role as determining the specific properties of stars, cluster history and in novae creation
Binary stars, their role as determining the specific properties of stars, cluster history and in novae creation By Emilio GARCIA 13/03/2007 Uppsala University Course:1FA223 - Report code:63061 I Introduction
More informationCompton Lecture #4: Massive Stars and. Supernovae. Welcome! On the back table:
Compton Lecture #4: Massive Stars and Welcome! On the back table: Supernovae Lecture notes for today s s lecture Extra copies of last week s s are on the back table Sign-up sheets please fill one out only
More informationStudies of peculiar transients with TNG Past results and future perspectives
Studies of peculiar transients with TNG Past results and future perspectives ANDREA PASTORELLO (INAF-OAPd) Padova, 2017 March 1-3 TNG Workshop New types of stellar transients The transient sky (past decade)
More informationChapter 6: Stellar Evolution (part 2): Stellar end-products
Chapter 6: Stellar Evolution (part 2): Stellar end-products Final evolution stages of high-mass stars Stellar end-products White dwarfs Neutron stars and black holes Supernovae Core-collapsed SNe Pair-Instability
More informationSubstructure in the Stellar Halo of the Andromeda Spiral Galaxy
Substructure in the Stellar Halo of the Andromeda Spiral Galaxy Raja Guhathakurta University of California Observatories (Lick, Keck, TMT) University of California at Santa Cruz M31 s extended stellar
More informationStars IV Stellar Evolution
Stars IV Stellar Evolution Attendance Quiz Are you here today? Here! (a) yes (b) no (c) my views are evolving on the subject Today s Topics Stellar Evolution An alien visits Earth for a day A star s mass
More informationLecture 24: Testing Stellar Evolution Readings: 20-6, 21-3, 21-4
Lecture 24: Testing Stellar Evolution Readings: 20-6, 21-3, 21-4 Key Ideas HR Diagrams of Star Clusters Ages from the Main Sequence Turn-off Open Clusters Young clusters of ~1000 stars Blue Main-Sequence
More informationSupernova events and neutron stars
Supernova events and neutron stars So far, we have followed stellar evolution up to the formation of a C-rich core. For massive stars ( M initial > 8 M Sun ), the contracting He core proceeds smoothly
More informationTwo projects without apparent connection?
Two projects without apparent connection? SW Sextantis stars SW Sextantis stars The golden age of surveys, Gänsicke 2005, Strassbourg SW Sextantis stars an introduction Original definition (Thorstensen
More informationChapter 0 Introduction X-RAY BINARIES
X-RAY BINARIES 1 Structure of this course 0. Introduction 1. Compact stars: formation and observational appearance. Mass transfer in binaries 3. Observational properties of XRBs 4. Formation and evolution
More informationFusion in first few minutes after Big Bang form lightest elements
Fusion in first few minutes after Big Bang form lightest elements Stars build the rest of the elements up to Iron (Fe) through fusion The rest of the elements beyond Iron (Fe) are produced in the dying
More information