SN 2012Au: a GOLDEN LINK BETWEEN SUPERLUMINOUS SUPERNOVAE and THEIR LOWER-LUMINOSITY COUNTERPARTS
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Copyright by Robert Michael Quimby 2006 the Dissertation Committee for Robert Michael Quimby Certifies That This Is the Approved Version of the Following Dissertation
Copyright by Robert Michael Quimby 2006 The Dissertation Committee for Robert Michael Quimby certifies that this is the approved version of the following dissertation: The Texas Supernova Search Committee: J. Craig Wheeler, Supervisor Peter H¨oflich Carl Akerlof Gary Hill Pawan Kumar Edward L. Robinson The Texas Supernova Search by Robert Michael Quimby, A.B., M.A. DISSERTATION Presented to the Faculty of the Graduate School of The University of Texas at Austin in Partial Fulfillment of the Requirements for the Degree of DOCTOR OF PHILOSOPHY THE UNIVERSITY OF TEXAS AT AUSTIN December 2006 Acknowledgments I would like to thank J. Craig Wheeler, Pawan Kumar, Gary Hill, Peter H¨oflich, Rob Robinson and Christopher Gerardy for their support and advice that led to the realization of this project and greatly improved its quality. Carl Akerlof, Don Smith, and Eli Rykoff labored to install and maintain the ROTSE-IIIb telescope with help from David Doss, making this project possi- ble. Finally, I thank Greg Aldering, Saul Perlmutter, Robert Knop, Michael Wood-Vasey, and the Supernova Cosmology Project for lending me their image subtraction code and assisting me with its installation. iv The Texas Supernova Search Publication No. Robert Michael Quimby, Ph.D. The University of Texas at Austin, 2006 Supervisor: J. Craig Wheeler Supernovae (SNe) are popular tools to explore the cosmological expan- sion of the Universe owing to their bright peak magnitudes and reasonably high rates; however, even the relatively homogeneous Type Ia supernovae are not intrinsically perfect standard candles. Their absolute peak brightness must be established by corrections that have been largely empirical. -
R-Process Elements from Magnetorotational Hypernovae
r-Process elements from magnetorotational hypernovae D. Yong1,2*, C. Kobayashi3,2, G. S. Da Costa1,2, M. S. Bessell1, A. Chiti4, A. Frebel4, K. Lind5, A. D. Mackey1,2, T. Nordlander1,2, M. Asplund6, A. R. Casey7,2, A. F. Marino8, S. J. Murphy9,1 & B. P. Schmidt1 1Research School of Astronomy & Astrophysics, Australian National University, Canberra, ACT 2611, Australia 2ARC Centre of Excellence for All Sky Astrophysics in 3 Dimensions (ASTRO 3D), Australia 3Centre for Astrophysics Research, Department of Physics, Astronomy and Mathematics, University of Hertfordshire, Hatfield, AL10 9AB, UK 4Department of Physics and Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 5Department of Astronomy, Stockholm University, AlbaNova University Center, 106 91 Stockholm, Sweden 6Max Planck Institute for Astrophysics, Karl-Schwarzschild-Str. 1, D-85741 Garching, Germany 7School of Physics and Astronomy, Monash University, VIC 3800, Australia 8Istituto NaZionale di Astrofisica - Osservatorio Astronomico di Arcetri, Largo Enrico Fermi, 5, 50125, Firenze, Italy 9School of Science, The University of New South Wales, Canberra, ACT 2600, Australia Neutron-star mergers were recently confirmed as sites of rapid-neutron-capture (r-process) nucleosynthesis1–3. However, in Galactic chemical evolution models, neutron-star mergers alone cannot reproduce the observed element abundance patterns of extremely metal-poor stars, which indicates the existence of other sites of r-process nucleosynthesis4–6. These sites may be investigated by studying the element abundance patterns of chemically primitive stars in the halo of the Milky Way, because these objects retain the nucleosynthetic signatures of the earliest generation of stars7–13. -
Chapter 22 Neutron Stars and Black Holes Units of Chapter 22 22.1 Neutron Stars 22.2 Pulsars 22.3 Xxneutron-Star Binaries: X-Ray Bursters
Chapter 22 Neutron Stars and Black Holes Units of Chapter 22 22.1 Neutron Stars 22.2 Pulsars 22.3 XXNeutron-Star Binaries: X-ray bursters [Look at the slides and the pictures in your book, but I won’t test you on this in detail, and we may skip altogether in class.] 22.4 Gamma-Ray Bursts 22.5 Black Holes 22.6 XXEinstein’s Theories of Relativity Special Relativity 22.7 Space Travel Near Black Holes 22.8 Observational Evidence for Black Holes Tests of General Relativity Gravity Waves: A New Window on the Universe Neutron Stars and Pulsars (sec. 22.1, 2 in textbook) 22.1 Neutron Stars According to models for stellar explosions: After a carbon detonation supernova (white dwarf in binary), little or nothing remains of the original star. After a core collapse supernova, part of the core may survive. It is very dense—as dense as an atomic nucleus—and is called a neutron star. [Recall that during core collapse the iron core (ashes of previous fusion reactions) is disintegrated into protons and neutrons, the protons combine with the surrounding electrons to make more neutrons, so the core becomes pure neutron matter. Because of this, core collapse can be halted if the core’s mass is between 1.4 (the Chandrasekhar limit) and about 3-4 solar masses, by neutron degeneracy.] What do you get if the core mass is less than 1.4 solar masses? Greater than 3-4 solar masses? 22.1 Neutron Stars Neutron stars, although they have 1–3 solar masses, are so dense that they are very small. -
Arxiv:0709.0302V1 [Astro-Ph] 3 Sep 2007 N Ro,M,414 USA 48104, MI, Arbor, Ann USA As(..Mcayne L 01.Sc Aeilcudslow Could Material Such Some 2001)
DRAFT VERSION NOVEMBER 4, 2018 Preprint typeset using LATEX style emulateapj v. 03/07/07 SN 2005AP: A MOST BRILLIANT EXPLOSION ROBERT M. QUIMBY1,GREG ALDERING2,J.CRAIG WHEELER1,PETER HÖFLICH3,CARL W. AKERLOF4,ELI S. RYKOFF4 Draft version November 4, 2018 ABSTRACT We present unfiltered photometric observations with ROTSE-III and optical spectroscopic follow-up with the HET and Keck of the most luminous supernova yet identified, SN 2005ap. The spectra taken about 3 days before and 6 days after maximum light show narrow emission lines (likely originating in the dwarf host) and absorption lines at a redshift of z =0.2832, which puts the peak unfiltered magnitude at −22.7 ± 0.1 absolute. Broad P-Cygni features corresponding to Hα, C III,N III, and O III, are further detected with a photospheric velocity of ∼ 20,000kms−1. Unlike other highly luminous supernovae such as 2006gy and 2006tf that show slow photometric evolution, the light curve of SN 2005ap indicates a 1-3 week rise to peak followed by a relatively rapid decay. The spectra also lack the distinct emission peaks from moderately broadened (FWHM ∼ 2,000kms−1) Balmer lines seen in SN 2006gyand SN 2006tf. We briefly discuss the origin of the extraordinary luminosity from a strong interaction as may be expected from a pair instability eruption or a GRB-like engine encased in a H/He envelope. Subject headings: Supernovae, SN 2005ap 1. INTRODUCTION the ultra-relativistic flow and thus mask the gamma-ray bea- Luminous supernovae (SNe) are most commonly associ- con announcing their creation, unlike their stripped progeni- ated with the Type Ia class, which are thought to involve tor cousins. -
Are Superluminous Supernovae Powered by Collision Or By
Are Superluminous Supernovae Powered By Collision Or By Millisecond Magnetars? Shlomo Dado1 and Arnon Dar1 ABSTRACT Using our previously derived simple analytic expression for the bolometric light curves of supernovae, we demonstrate that the collision of the fast de- bris of ordinary supernova explosions with relatively slow-moving shells from pre-supernova eruptions can produce the observed bolometric light curves of su- perluminous supernovae (SLSNe) of all types. These include both, those which can be explained as powered by spinning-down millisecond magnetars and those which cannot. That and the observed close similarity between the bolometric light-curves of SLSNe and ordinary interacting SNe suggest that SLSNe are pow- ered mainly by collisions with relatively slow moving circumstellar shells from pre-supernova eruptions rather than by the spin-down of millisecond magnetars born in core collapse supernova explosions. Subject headings: supernovae: general 1. Introduction For a long time, it has been widely believed that the observed luminosity of all known types of supernova (SN) explosions is powered by one or more of the following sources: radioactive decay of freshly-synthesized elements, typically 56Ni (Colgate and McKee 1969; Colgate et al. 1980), heat deposited in the envelope of a supergiant star by the explosion arXiv:1312.5273v1 [astro-ph.HE] 18 Dec 2013 shock (Grassberg et al. 1971), and interaction between the SN debris and the circumstellar wind environment (Chevalier 1982). Recently, however, a new type of SNe, superluminous SNe (SLSNe) whose peak luminosity exceeds 1044 ergs per second, much brighter than that of the brightest normal thermonuclear supernovae (type Ia) and core collapse supernova (types Ib/c and II) was discovered by modern supernova surveys. -
Searching for Gravitational Waves
Astronomy group seminar, University of Southampton, Jan 2015 LIGO-DCC G1500072 1. Gravitational wave (GW) background What are gravitational waves? • Gravitational waves are a direct prediction of Einstein’s General Theory of Relativity • Solutions to (weak field) Einstein equations in vacuum are wave equations 휕2 − + 훻2 ℎ휇휈 = −16휋푇휇휈 휕푡 2 Vacuum so stress- energy tensor 2 휕 푇휇휈 = 0 − + 훻2 ℎ휇휈 = 0 휕푡 2 휇휈 휇휈 휇 ℎ = 퐴 exp 푘휇 푥 • “Ripples in space-time” What are GWs? • Einstein first predicted GWs in 1916 paper • This had a major error – the waves carried no energy! Einstein, “Näherungsweise Integration der Feldgleichungen der Gravitation“, Sitzungsberichte der Königlich Preußischen Akademie der Wissenschaften, 1916 What are GWs? • Corrected in 1918 paper which introduced the now famous “quadrupole formula” Einstein, “Über Gravitationswellen“, Sitzungsberichte der Königlich Preußischen Akademie der Wissenschaften, 1918 What are GWs Source: Bulk Motion Oscillating Tidal Field Observer Detects Produces Changing Tidal Field Propagates (Unobstructed) Distortion Strain to Observer 푙 + Δ푙 푙 Δ푙 Strain: ℎ = 푙 2 퐺 mass quadruple Quadrupole ℎ(푡) = 퐼( 푡) formula: 푟 푐4 -45 source distance (1/r - ~ 8x10 small number! amplitude not power!) What are GWs? For two 1.4 M⊙ neutron stars 2 퐺 mass near coalescence at a distance of ℎ(푡) = 퐼( 푡) quadruple 10 Mpc ℎ~1.4 × 10−22 푟 푐4 -45 Displacement measured by 4km long ~ 8x10 detector ~5.6 × 10−19m - about 1/10000th source distance (1/r - amplitude not power!) diameter of a proton, or measuring change in distance to α Centauri to ~1/10th diameter of a human hair! • Detectable gravitational waves (GWs) will only come from the most massive and energetic systems in the universe e.g. -
Central Engines and Environment of Superluminous Supernovae
Central Engines and Environment of Superluminous Supernovae Blinnikov S.I.1;2;3 1 NIC Kurchatov Inst. ITEP, Moscow 2 SAI, MSU, Moscow 3 Kavli IPMU, Kashiwa with E.Sorokina, K.Nomoto, P. Baklanov, A.Tolstov, E.Kozyreva, M.Potashov, et al. Schloss Ringberg, 26 July 2017 First Superluminous Supernova (SLSN) is discovered in 2006 -21 1994I 1997ef 1998bw -21 -20 56 2002ap Co to 2003jd 56 2007bg -19 Fe 2007bi -20 -18 -19 -17 -16 -18 Absolute magnitude -15 -17 -14 -13 -16 0 50 100 150 200 250 300 350 -20 0 20 40 60 Epoch (days) Superluminous SN of type II Superluminous SN of type I SN2006gy used to be the most luminous SN in 2006, but not now. Now many SNe are discovered even more luminous. The number of Superluminous Supernovae (SLSNe) discovered is growing. The models explaining those events with the minimum energy budget involve multiple ejections of mass in presupernova stars. Mass loss and build-up of envelopes around massive stars are generic features of stellar evolution. Normally, those envelopes are rather diluted, and they do not change significantly the light produced in the majority of supernovae. 2 SLSNe are not equal to Hypernovae Hypernovae are not extremely luminous, but they have high kinetic energy of explosion. Afterglow of GRB130702A with bumps interpreted as a hypernova. Alina Volnova, et al. 2017. Multicolour modelling of SN 2013dx associated with GRB130702A. MNRAS 467, 3500. 3 Our models of LC with STELLA E ≈ 35 foe. First year light ∼ 0:03 foe while for SLSNe it is an order of magnitude larger. -
Modeling Hyperenergetic and Superluminous Supernovae
Modeling hyperenergetic and superluminous supernovae Philipp Mösta Einstein fellow @ UC Berkeley [email protected] Roland Haas, Goni Halevi, Christian Ott, Sherwood Richers, Luke Roberts, Erik Schnetter BlueWaters symposium 2017 May 17, 2017 Astrophysics of core-collapse supernovae M82/Chandra/NASA ~ Galaxy evolution/feedback Heavy element nucleosynthesis Birth sites of black holes / neutron stars 2 Neutrinos New era of transient science • Current (PTF, DeCAM, ASAS-SN) and upcoming wide-field time domain astronomy (ZTF, LSST, …) -> wealth of data • adv LIGO / gravitational waves detected • Computational tools at dawn of new exascale era Image: PTF/ZTF/COO Image: LSST 3 New era of transient science • Current (PTF, DeCAM, ASAS-SN) and upcoming wide-field time domain astronomy (ZTF, LSST, …) -> wealth of data • adv LIGO / gravitational waves detected • Computational tools at dawn of new exascale era Transformative years ahead for our understanding of these events Image: PTF/ZTF/COO Image: LSST 4 Hypernovae & GRBs • 11 long GRB – core-collapse supernova associations. • All GRB-SNe are stripped envelope, show outflows v~0.1c • But not all stripped-envelope supernovae come with GRBs • Trace low metallicity and low redshift Neutrino mechanism is inefficient; can’t deliver a hypernova 5 Superluminous supernovae Some events: stripped envelope no interaction 45 Elum ~ 10 erg 52 Erad up to 10 erg Gal-Yam+12 6 Superluminous / hyperenergetic supernovae SLSN Ic lGRBs SN Ic-bl Common engine? 7 Core collapse basics Iron core Protoneutron star r~30km -
Explosive Nucleosynthesis in GRB Jets Accompanied by Hypernovae
SLAC-PUB-12126 astro-ph/0601111 September 2006 Explosive Nucleosynthesis in GRB Jets Accompanied by Hypernovae Shigehiro Nagataki1,2, Akira Mizuta3, Katsuhiko Sato4,5 ABSTRACT Two-dimensional hydrodynamic simulations are performed to investigate ex- plosive nucleosynthesis in a collapsar using the model of MacFadyen and Woosley (1999). It is shown that 56Ni is not produced in the jet of the collapsar suffi- ciently to explain the observed amount of a hypernova when the duration of the explosion is ∼10 sec, which is considered to be the typical timescale of explosion in the collapsar model. Even though a considerable amount of 56Ni is synthesized if all explosion energy is deposited initially, the opening angles of the jets become too wide to realize highly relativistic outflows and gamma-ray bursts in such a case. From these results, it is concluded that the origin of 56Ni in hypernovae associated with GRBs is not the explosive nucleosynthesis in the jet. We consider that the idea that the origin is the explosive nucleosynthesis in the accretion disk is more promising. We also show that the explosion becomes bi-polar naturally due to the effect of the deformed progenitor. This fact suggests that the 56Ni synthesized in the accretion disk and conveyed as outflows are blown along to the rotation axis, which will explain the line features of SN 1998bw and double peaked line features of SN 2003jd. Some fraction of the gamma-ray lines from 56Ni decays in the jet will appear without losing their energies because the jet becomes optically thin before a considerable amount of 56Ni decays as long as the jet is a relativistic flow, which may be observed as relativistically Lorentz boosted line profiles in future. -
Radioactive Decay), Chapter 7 (SN 1987A), Background: Sections 3.1, 3.2, 3.3, 3.4, 3.5, 3.8, 3.10, 4.1, 4.2, 4.3, 4.4, 5.2, 5.4 (Binary Stars and Accretion Disks)
Friday, March 10, 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, 4.1, 4.2, 4.3, 4.4, 5.2, 5.4 (binary stars and accretion disks). Plus superluminous supernovae, not in the book. Astronomy in the news? Potatoes can grow just about anywhere, including Mars, according to researchers who tested the idea put forth in the movie "The Martian." Scientists are growing potatoes in Mars-like soil from a Peruvian desert inside a CubeSat under extreme conditions, and the findings could not only benefit future Mars colonists but also help undernourished populations here on Earth. Goal: To understand the nature and importance of SN 1987A for our understanding of massive star evolution and iron core collapse. Chapter 7 Image of SN 1987A and environs in Large Magellanic Cloud, taken by Hubble Space Telescope, January 2017 One Minute Exam What was the most important thing about SN 1987A in terms of the basic physics of core collapse? It exploded in a blue, not a red supergiant It was surrounded by three rings It produced radioactive nickel and cobalt Neutrinos were detected from it Saw neutrinos! Neutron star must have formed and survived for at least 10 seconds. If a black hole had formed in the first instants, neither light nor neutrinos could have been emitted. No sign of neutron star since, despite looking hard for 30 years. Whatever is in the center of Cas A, most likely a neutron star, is too dim to be seen at the distance of the LMC, so SN 1987A might have made one of those (probably a neutron star, but not bright like the one in the Crab Nebula). -
Observations of Crab Nebula and Pulsar with VERITAS
University of California Los Angeles Observations of Crab Nebula and Pulsar with VERITAS A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Physics by Ozlem¨ C¸elik 2008 c Copyright by Ozlem¨ C¸elik 2008 The dissertation of Ozlem¨ C¸elik is approved. Katsushi Arisaka Ferdinand Coroniti Kevin McKeegan Ren´eOng, Committee Chair University of California, Los Angeles 2008 ii To my parents . for their endless love and support at all times. iii Table of Contents 1 Gamma-Ray Astronomy ........................ 1 1.1 Introduction.............................. 1 1.2 GammaRays ............................. 2 1.3 MotivationsforGamma-RayAstronomy . 4 1.4 Gamma-RayDetectors ........................ 6 1.4.1 Space-BasedDetectors . 6 1.4.2 Ground-basedDetectors . 12 1.4.3 AlternativeDetectors. 16 1.5 Gamma-RaySources ......................... 16 1.5.1 GalacticSources ....................... 17 1.5.2 ExtragalacticSources. 21 1.6 GuidetoThesis............................ 24 2 Pulsars and Their Nebulae ...................... 25 2.1 Birth of the PWNe Complex: Supernovae . 26 2.2 ThePulsarStar............................ 29 2.2.1 ConnectiontoNeutronStars. 29 2.2.2 CharacteristicsofPulsars . 30 2.2.3 Non-Thermal Radiation Mechanisms at Work in PWNe . 33 2.2.4 PulsedEmission. .. .. 38 2.2.5 HE Pulsed Emission Models . 40 iv 2.2.6 Predictions of HE Emission Models . 44 2.2.7 VHE gamma-ray Observations of Pulsed Emission . 50 2.3 PulsarWindNebulae......................... 52 2.3.1 RegionsinaPWN ...................... 52 2.3.2 The Central Pulsar: The Energy Source . 53 2.3.3 Pulsar Winds: Energy Transport between Pulsar and Nebula 55 2.3.4 The Wind Termination Shock . 57 2.3.5 The Nebular Emission . -
ASTRONOMICAL IMAGE SUBTRACTION by CROSS-CONVOLUTION Fang Yuan1 and Carl W
The Astrophysical Journal, 677:808–812, 2008 April 10 # 2008. The American Astronomical Society. All rights reserved. Printed in U.S.A. ASTRONOMICAL IMAGE SUBTRACTION BY CROSS-CONVOLUTION Fang Yuan1 and Carl W. Akerlof1 Received 2007 November 20; accepted 2008 January 1 ABSTRACT In recent years, there has been a proliferation of wide-field sky surveys to search for a variety of transient objects. Using relatively short focal lengths, the optics of these systems produce undersampled stellar images often marred by a variety of aberrations. As participants in such activities, we have developed a new algorithm for image subtraction that no longer requires high-quality reference images for comparison. The computational efficiency is comparable with similar procedures currently in use. The general technique is cross-convolution: two convolution kernels are generated to make a test image and a reference image separately transform to match as closely as possible. In analogy to the optimization technique for generating smoothing splines, the inclusion of an rms width penalty term constrains the diffusion of stellar images. In addition, by evaluating the convolution kernels on uniformly spaced subimages across the total area, these routines can accommodate point-spread functions that vary considerably across the focal plane. Subject headinggs: methods: statistical — techniques: photometric 1. INTRODUCTION and was quite familiar with the SN discovery process. Quimby adapted the SCP image-subtraction code (Perlmutter et al. 1999) The advent of low-noise megapixel electronic image sensors, for use as the basic tool for finding 30 SNe over a period of 2 years cheap fast computers, and terabyte data storage systems has en- abled searches for rare astrophysical phenomena that would from observations with the University of Texas 30% allocation of ROTSE-IIIb time at the McDonald Observatory.