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Plasma Physics and Pulsars
Plasma Physics and Pulsars On the evolution of compact o bjects and plasma physics in weak and strong gravitational and electromagnetic fields by Anouk Ehreiser supervised by Axel Jessner, Maria Massi and Li Kejia as part of an internship at the Max Planck Institute for Radioastronomy, Bonn March 2010 2 This composition was written as part of two internships at the Max Planck Institute for Radioastronomy in April 2009 at the Radiotelescope in Effelsberg and in February/March 2010 at the Institute in Bonn. I am very grateful for the support, expertise and patience of Axel Jessner, Maria Massi and Li Kejia, who supervised my internship and introduced me to the basic concepts and the current research in the field. Contents I. Life-cycle of stars 1. Formation and inner structure 2. Gravitational collapse and supernova 3. Star remnants II. Properties of Compact Objects 1. White Dwarfs 2. Neutron Stars 3. Black Holes 4. Hypothetical Quark Stars 5. Relativistic Effects III. Plasma Physics 1. Essentials 2. Single Particle Motion in a magnetic field 3. Interaction of plasma flows with magnetic fields – the aurora as an example IV. Pulsars 1. The Discovery of Pulsars 2. Basic Features of Pulsar Signals 3. Theoretical models for the Pulsar Magnetosphere and Emission Mechanism 4. Towards a Dynamical Model of Pulsar Electrodynamics References 3 Plasma Physics and Pulsars I. The life-cycle of stars 1. Formation and inner structure Stars are formed in molecular clouds in the interstellar medium, which consist mostly of molecular hydrogen (primordial elements made a few minutes after the beginning of the universe) and dust. -
Surface Structure of Quark Stars with Magnetic Fields
PRAMANA °c Indian Academy of Sciences Vol. 67, No. 5 | journal of November 2006 physics pp. 937{949 Surface structure of quark stars with magnetic ¯elds PRASHANTH JAIKUMAR Department of Physics and Astronomy, Ohio University, Athens, OH 45701, USA E-mail: [email protected] Abstract. We investigate the impact of magnetic ¯elds on the electron distribution of the electrosphere of quark stars. For moderately strong magnetic ¯elds of B » 1013 G, quantization e®ects are generally weak due to the large number density of electrons at surface, but can nevertheless a®ect the photon emission properties of quark stars. We outline the main observational characteristics of quark stars as determined by their surface emission, and briefly discuss their formation in explosive events termed as quark-novae, which may be connected to the r-process. Keywords. Quark stars; magnetic ¯elds; nucleosynthesis. PACS Nos 26.60.+c; 24.85.+p; 97.60.Jd 1. Introduction There is a renewed interest in the theory and observation of strange quark stars, which are believed to contain, or be entirely composed of, decon¯ned quark mat- ter [1]. An observational con¯rmation of their existence would be conclusive ev- idence of quark decon¯nement at large baryon densities, an expected feature of quantum chromodynamics (QCD). Furthermore, discovery of a stable bare quark star a±rms the Bodmer{Terazawa{Witten conjecture [2], that at high enough den- sity, strange quark matter, composed of up, down and strange quarks, is absolutely stable with respect to nuclear matter. This intriguing hypothesis is over three decades old, and bare quark stars are but one possible realization put forward in the intervening years. -
MG0414+0534 by John D
High Resolution Observations and Modeling of MG0414+0534 by John D. Ellithorpe B.S. Physics, University of California, Irvine (1990) Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 1995 () Massachusetts Institute of Technology 1995. All rights reserved. Author -- Department of Physics May 18, 1995 Certified by. I- v I Jacqueline N. Hewitt d Class of 1948 Associate Professor of Physics Thesis Supervisor Accepted by George F. Koster nOFTCI 4t4L0GY LTEuChairman, Graduate Committee JUN 2 61995 LIBRARIES High Resolution Observations and Modeling of MG0414+0534 by John D. Ellithorpe Submitted to the Department of Physics on May 18, 1995, in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics Abstract Gravitational lenses provide unique opportunities to probe distant galaxies and to examine models of the universe. We focus our attention on the gravitational lens MG 0414+0534. The bright four-image geometry and source variability make this system an excellent candidate for study. The first step in addressing astrophysical applications is the accurate determination of the lens matter distribution. In this thesis, we focused on improving the lens inversion algorithms and obtaining high- resolution observations of MG 0414+0534 to yield a reliable reconstruction of the lens. We then use this information to measure astrophysical properties of the lens and universe. Multiple imaging by the lens provides strong constraints in the observed images allowingreconstruction of both the total matter distribution in the lens and the light distribution in the source. -
Collapsing Supra-Massive Magnetars: Frbs, the Repeating FRB121102 and Grbs
J. Astrophys. Astr. (2018) 39:14 © Indian Academy of Sciences https://doi.org/10.1007/s12036-017-9499-9 Review Collapsing supra-massive magnetars: FRBs, the repeating FRB121102 and GRBs PATRICK DAS GUPTA∗ and NIDHI SAINI Department of Physics and Astrophysics, University of Delhi, Delhi 110007, India. ∗Corresponding author. E-mail: [email protected], [email protected] MS received 30 August 2017; accepted 3 October 2017; published online 10 February 2018 Abstract. Fast Radio Bursts (FRBs) last for ∼ few milli-seconds and, hence, are likely to arise from the gravitational collapse of supra-massive, spinning neutron stars after they lose the centrifugal support (Falcke & Rezzolla 2014). In this paper, we provide arguments to show that the repeating burst, FRB 121102, can also be modeled in the collapse framework provided the supra-massive object implodes either into a Kerr black hole surrounded by highly magnetized plasma or into a strange quark star. Since the estimated rates of FRBs and SN Ib/c are comparable, we put forward a common progenitor scenario for FRBs and long GRBs in which only those compact remnants entail prompt γ -emission whose kick velocities are almost aligned or anti-aligned with the stellar spin axes. In such a scenario, emission of detectable gravitational radiation and, possibly, of neutrinos are expected to occur during the SN Ib/c explosion as well as, later, at the time of magnetar implosion. Keywords. FRBs—FRB 121102—Kerr black holes—Blandford–Znajek process—strange stars—GRBs— pre-natal kicks. 1. Introduction 43% linear polarization and 3% circular polarization (Petroff et al. -
When Neutron Stars Melt, What’S Left Behind Is Spectacular Explosion
Space oddity implodes. The outer layers are cast off in a When neutron stars melt, what’s left behind is spectacular explosion. What’s left behind is truly strange. Anil Ananthaswamy reports a rapidly spinning neutron star, which as the name implies is made mainly of neutrons, with a crust of iron. Whirling up to 1000 times per second, a neutron star is constantly shedding magnetic fields. Over time, this loss of energy causes the star to spin slower and slower. As it spins down, the centrifugal forces that kept gravity at bay start weakening, allowing gravity to squish the star still further. In what is a blink of an eye in cosmic time, the neutrons can be converted to strange N 22 September last year, the website of fundamental building blocks of matter in quark matter, which is a soup of up, down and The Astronomer’s Telegram alerted ways that even machines like the Large strange quarks. In theory, this unusual change Oresearchers to a supernova explosion in Hadron Collider cannot. happens when the density inside the neutron a spiral galaxy about 84 million light years Astrophysicists can thank string theorist star starts increasing. New particles called away. There was just one problem. The same Edward Witten for quark stars. In 1984, he hyperons begin forming that contain at least object, SN 2009ip, had blown up in a similarly hypothesised that protons and neutrons one strange quark bound to others. spectacular fashion just weeks earlier. Such may not be the most stable forms of matter. However, the appearance of hyperons stars shouldn’t go supernova twice, let alone Both are made of two types of smaller marks the beginning of the end of the neutron in quick succession. -
Experiencing Hubble
PRESCOTT ASTRONOMY CLUB PRESENTS EXPERIENCING HUBBLE John Carter August 7, 2019 GET OUT LOOK UP • When Galaxies Collide https://www.youtube.com/watch?v=HP3x7TgvgR8 • How Hubble Images Get Color https://www.youtube.com/watch? time_continue=3&v=WSG0MnmUsEY Experiencing Hubble Sagittarius Star Cloud 1. 12,000 stars 2. ½ percent of full Moon area. 3. Not one star in the image can be seen by the naked eye. 4. Color of star reflects its surface temperature. Eagle Nebula. M 16 1. Messier 16 is a conspicuous region of active star formation, appearing in the constellation Serpens Cauda. This giant cloud of interstellar gas and dust is commonly known as the Eagle Nebula, and has already created a cluster of young stars. The nebula is also referred to the Star Queen Nebula and as IC 4703; the cluster is NGC 6611. With an overall visual magnitude of 6.4, and an apparent diameter of 7', the Eagle Nebula's star cluster is best seen with low power telescopes. The brightest star in the cluster has an apparent magnitude of +8.24, easily visible with good binoculars. A 4" scope reveals about 20 stars in an uneven background of fainter stars and nebulosity; three nebulous concentrations can be glimpsed under good conditions. Under very good conditions, suggestions of dark obscuring matter can be seen to the north of the cluster. In an 8" telescope at low power, M 16 is an impressive object. The nebula extends much farther out, to a diameter of over 30'. It is filled with dark regions and globules, including a peculiar dark column and a luminous rim around the cluster. -
Star Formation Relations and CO Sleds Across the J-Ladder and Redshift 3 on the ESA Herschel Space Observatory20 (Pilbratt Et Al
Draft version July 17, 2014 Preprint typeset using LATEX style emulateapj v. 5/2/11 STAR FORMATION RELATIONS AND CO SPECTRAL LINE ENERGY DISTRIBUTIONS ACROSS THE J-LADDER AND REDSHIFT T. R. Greve1, I. Leonidaki2, E. M. Xilouris2, A. Weiß3, Z.-Y. Zhang4,5, P. van der Werf6, S. Aalto7, L. Armus8, T. D´ıaz-Santos8, A.S. Evans9,10, J. Fischer11, Y. Gao12, E. Gonzalez-Alfonso´ 13, A. Harris14, C. Henkel3, R. Meijerink6,15, D. A. Naylor16 H. A. Smith17 M. Spaans15 G. J. Stacey18 S. Veilleux14 F. Walter19 Draft version July 17, 2014 ABSTRACT 0 We present FIR[50 − 300 µm]−CO luminosity relations (i.e., log LFIR = α log LCO + β) for the full CO rotational ladder from J = 1 − 0 up to J = 13 − 12 for a sample of 62 local (z ≤ 0:1) (Ultra) 11 Luminous Infrared Galaxies (LIRGs; LIR[8−1000 µm] > 10 L ) using data from Herschel SPIRE-FTS and ground-based telescopes. We extend our sample to high redshifts (z > 1) by including 35 (sub)- millimeter selected dusty star forming galaxies from the literature with robust CO observations, and sufficiently well-sampled FIR/sub-millimeter spectral energy distributions (SEDs) so that accurate FIR luminosities can be deduced. The addition of luminous starbursts at high redshifts enlarge the range of the FIR−CO luminosity relations towards the high-IR-luminosity end while also significantly increasing the small amount of mid-J/high-J CO line data (J = 5 − 4 and higher) that was available prior to Herschel. This new data-set (both in terms of IR luminosity and J-ladder) reveals linear FIR−CO luminosity relations (i.e., α ' 1) for J = 1 − 0 up to J = 5 − 4, with a nearly constant normalization (β ∼ 2). -
Arxiv:2102.09424V2 [Astro-Ph.EP] 20 Feb 2021 the first Exoplanet
Draft version February 23, 2021 Typeset using LATEX twocolumn style in AASTeX63 Planets Across Space and Time (PAST). I. Characterizing the Memberships of Galactic Components and Stellar Ages: Revisiting the Kinematic Methods and Applying to Planet Host Stars Di-Chang Chen,1, 2 Ji-Wei Xie,1, 2 Ji-Lin Zhou,1, 2 Su-Bo Dong,3 Chao Liu,4, 5 Hai-Feng Wang,6 Mao-Sheng Xiang,7, 8 Yang Huang,9 Ali Luo,7 and Zheng Zheng10 1School of Astronomy and Space Science, Nanjing University, Nanjing 210023, China 2Key Laboratory of Modern Astronomy and Astrophysics, Ministry of Education, Nanjing 210023, China 3Kavli Institute for Astronomy and Astrophysics, Peking University, Beijing 100871, China 4Key Lab of Space Astronomy and Technology, National Astronomical Observatories, CAS, 100101, China 5University of Chinese Academy of Sciences, Beijing, 100049, China. 6South-Western Institute for Astronomy Research, Yunnan University, Kunming, 650500, China; LAMOST Fellow 7National Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, China 8Max-Planck Institute for Astronomy, K¨onigstuhl17, D-69117 Heidelberg, Germany 9South-Western Institute for Astronomy Research, Yunnan University, Kunming, 650500, China 10Department of Physics and Astronomy, University of Utah, Salt Lake City, UT 84112 ABSTRACT Over 4,000 exoplanets have been identified and thousands of candidates are to be confirmed. The relations between the characteristics of these planetary systems and the kinematics, Galactic compo- nents, and ages of their host stars have yet to be well explored. Aiming to addressing these questions, we conduct a research project, dubbed as PAST (Planets Across Space and Time). To do this, one of the key steps is to accurately characterize the planet host stars. -
The Evolution of Cluster E and S0 Galaxies Measured from The
A Mon. Not. R. Astron. So c. 000, 000{000 (0000) Printed 12 May1999 (MN L T Xstyle le v1.4) E The evolution of cluster E and S0 galaxies measured from ? the Fundamental Plane 1;2 yzx 3;4;5 zx 6;7;8 x 3;5 x Inger Jrgensen Marijn Franx , Jens Hjorth , Pieter G. van Dokkum 1 McDonald Observatory, The University of Texas at Austin, RLM 15.308, Austin, TX 78712, USA 2 Gemini Observatory, 670 N. A`ohoku Pl., Hilo, HI 96720, USA (Postal address for IJ) 3 Kapteyn Institute, P.O.Box 800, 9700 AVGroningen, The Netherlands 4 Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA 5 Leiden Observatory, P.O.Box 9513, 2300 RA Leiden, The Netherlands (Postal address for MF and PvD) 6 Institute of Astronomy, Madingley Road, Cambridge CB3 0HA, UK 7 NORDITA, Blegdamsvej 17, DK-2100 Copenhagen , Denmark 8 Astronomical Observatory, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen , Denmark (Postal address for JH) May 5, 1999, accepted for publication in Mon. Not. Royal Astron. Sco., Gemini Preprint #43 ABSTRACT Photometry has b een obtained for magnitude limited samples of galaxies in the two rich clusters Ab ell 665 (37 galaxies) and Ab ell 2218 (61 galaxies). Both clusters have m a redshift of 0.18. The limiting magnitude of the samples is 19 in the I-band. Sp ec- troscopy has b een obtained for seven galaxies in A665 and nine galaxies in A2218, all of whichalsohaveavailable photometry. Sp ectroscopy has b een obtained for two additional galaxies in A2218, one of whichisabackground galaxy. -
Arxiv:2103.02709V1
Draft version September 19, 2021 Typeset using LATEX default style in AASTeX63 A Gaussian Process Regression Reveals No Evidence for Planets Orbiting Kapteyn's Star Anna Bortle,1 Hallie Fausey,1 Jinbiao Ji,1 Sarah Dodson-Robinson,1 Victor Ramirez Delgado,1 and John Gizis1 1University of Delaware Department of Physics and Astronomy 217 Sharp Lab Newark, DE 19716 USA ABSTRACT Radial-velocity (RV) planet searches are often polluted by signals caused by gas motion at the star's surface. Stellar activity can mimic or mask changes in the RVs caused by orbiting planets, resulting in false positives or missed detections. Here we use Gaussian Process (GP) regression to disentangle the contradictory reports of planets vs. rotation artifacts in Kapteyn's star (Anglada-Escud´eet al. 2014; Robertson et al. 2015a; Anglada-Escud´eet al. 2016). To model rotation, we use joint quasi-periodic kernels for the RV and Hα signals, requiring that their periods and correlation timescales be the same. We find that the rotation period of Kapteyn's star is 125 days, while the characteristic active-region lifetime is 694 days. Adding a planet to the RV model produces a best-fit orbital period of 100 years, or 10 times the observing time baseline, indicating that the observed RVs are best explained by star rotation only. We also find no significant periodic signals in residual RV data sets constructed by subtracting off realizations of the best-fit rotation model and conclude that both previously reported \planets" are artifacts of the star's rotation and activity. Our results highlight the pitfalls of using sinusoids to model quasi-periodic rotation signals. -
Meeting Program
A A S MEETING PROGRAM 211TH MEETING OF THE AMERICAN ASTRONOMICAL SOCIETY WITH THE HIGH ENERGY ASTROPHYSICS DIVISION (HEAD) AND THE HISTORICAL ASTRONOMY DIVISION (HAD) 7-11 JANUARY 2008 AUSTIN, TX All scientific session will be held at the: Austin Convention Center COUNCIL .......................... 2 500 East Cesar Chavez St. Austin, TX 78701 EXHIBITS ........................... 4 FURTHER IN GRATITUDE INFORMATION ............... 6 AAS Paper Sorters SCHEDULE ....................... 7 Rachel Akeson, David Bartlett, Elizabeth Barton, SUNDAY ........................17 Joan Centrella, Jun Cui, Susana Deustua, Tapasi Ghosh, Jennifer Grier, Joe Hahn, Hugh Harris, MONDAY .......................21 Chryssa Kouveliotou, John Martin, Kevin Marvel, Kristen Menou, Brian Patten, Robert Quimby, Chris Springob, Joe Tenn, Dirk Terrell, Dave TUESDAY .......................25 Thompson, Liese van Zee, and Amy Winebarger WEDNESDAY ................77 We would like to thank the THURSDAY ................. 143 following sponsors: FRIDAY ......................... 203 Elsevier Northrop Grumman SATURDAY .................. 241 Lockheed Martin The TABASGO Foundation AUTHOR INDEX ........ 242 AAS COUNCIL J. Craig Wheeler Univ. of Texas President (6/2006-6/2008) John P. Huchra Harvard-Smithsonian, President-Elect CfA (6/2007-6/2008) Paul Vanden Bout NRAO Vice-President (6/2005-6/2008) Robert W. O’Connell Univ. of Virginia Vice-President (6/2006-6/2009) Lee W. Hartman Univ. of Michigan Vice-President (6/2007-6/2010) John Graham CIW Secretary (6/2004-6/2010) OFFICERS Hervey (Peter) STScI Treasurer Stockman (6/2005-6/2008) Timothy F. Slater Univ. of Arizona Education Officer (6/2006-6/2009) Mike A’Hearn Univ. of Maryland Pub. Board Chair (6/2005-6/2008) Kevin Marvel AAS Executive Officer (6/2006-Present) Gary J. Ferland Univ. of Kentucky (6/2007-6/2008) Suzanne Hawley Univ. -
(NASA/Chandra X-Ray Image) Type Ia Supernova Remnant – Thermonuclear Explosion of a White Dwarf
Stellar Evolution Card Set Description and Links 1. Tycho’s SNR (NASA/Chandra X-ray image) Type Ia supernova remnant – thermonuclear explosion of a white dwarf http://chandra.harvard.edu/photo/2011/tycho2/ 2. Protostar formation (NASA/JPL/Caltech/Spitzer/R. Hurt illustration) A young star/protostar forming within a cloud of gas and dust http://www.spitzer.caltech.edu/images/1852-ssc2007-14d-Planet-Forming-Disk- Around-a-Baby-Star 3. The Crab Nebula (NASA/Chandra X-ray/Hubble optical/Spitzer IR composite image) A type II supernova remnant with a millisecond pulsar stellar core http://chandra.harvard.edu/photo/2009/crab/ 4. Cygnus X-1 (NASA/Chandra/M Weiss illustration) A stellar mass black hole in an X-ray binary system with a main sequence companion star http://chandra.harvard.edu/photo/2011/cygx1/ 5. White dwarf with red giant companion star (ESO/M. Kornmesser illustration/video) A white dwarf accreting material from a red giant companion could result in a Type Ia supernova http://www.eso.org/public/videos/eso0943b/ 6. Eight Burst Nebula (NASA/Hubble optical image) A planetary nebula with a white dwarf and companion star binary system in its center http://apod.nasa.gov/apod/ap150607.html 7. The Carina Nebula star-formation complex (NASA/Hubble optical image) A massive and active star formation region with newly forming protostars and stars http://www.spacetelescope.org/images/heic0707b/ 8. NGC 6826 (Chandra X-ray/Hubble optical composite image) A planetary nebula with a white dwarf stellar core in its center http://chandra.harvard.edu/photo/2012/pne/ 9.