Jürgen Ehlers
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Pulsar Physics Without Magnetars
Chin. J. Astron. Astrophys. Vol.8 (2008), Supplement, 213–218 Chinese Journal of (http://www.chjaa.org) Astronomy and Astrophysics Pulsar Physics without Magnetars Wolfgang Kundt Argelander-Institut f¨ur Astronomie der Universit¨at, Auf dem H¨ugel 71, D-53121 Bonn, Germany Abstract Magnetars, as defined some 15 yr ago, are inconsistent both with fundamental physics, and with the (by now) two observed upward jumps of the period derivatives (of two of them). Instead, the class of peculiar X-ray sources commonly interpreted as magnetars can be understood as the class of throttled pulsars, i.e. of pulsars strongly interacting with their CSM. This class is even expected to harbour the sources of the Cosmic Rays, and of all the (extraterrestrial) Gamma-Ray Bursts. Key words: magnetars — throttled pulsars — dying pulsars — cavity — low-mass disk 1 DEFINITION AND PROPERTIES OF THE MAGNETARS Magnetars have been defined by Duncan and Thompson some 15 years ago, as spinning, compact X-ray sources - probably neutron stars - which are powered by the slow decay of their strong magnetic field, of strength 1015 G near the surface, cf. (Duncan & Thompson 1992; Thompson & Duncan 1996). They are now thought to comprise the anomalous X-ray pulsars (AXPs), soft gamma-ray repeaters (SGRs), recurrent radio transients (RRATs), or ‘stammerers’, or ‘burpers’, and the ‘dim isolated neutron stars’ (DINSs), i.e. a large, fairly well defined subclass of all neutron stars, which has the following properties (Mereghetti et al. 2002): 1) They are isolated neutron stars, with spin periods P between 5 s and 12 s, and similar glitch behaviour to other neutron-star sources, which correlates with their X-ray bursting. -
Einstein and Einstein-Maxwell Fields of Weyl's Type Einsteinova A
Einstein and Einstein-Maxwell fields of Weyl’s type Einsteinova a Einsteinova-Maxwellova pole Weylova typu Lukáš Richterek Faculty of Natural Sciences Palacký University Olomouc and Faculty of Natural Sciences Masaryk University Brno PhD thesis May 2000 Submitted theses were completed within the framework of the external postgraduate study at the Department of General Physics, Faculty of Natural Sciences, Masaryk Uni- versity Brno. Candidate: Lukáš Richterek Department of Theoretical Physics Faculty of Natural Sciences Palacký University Svobody 26, Olomouc, CZ-771 46 [email protected] Supervisor: Prof. RNDr. Jan Novotný, CSc. Department of General Physics Faculty of Natural Sciences Masaryk University Kotlářská 2, Brno, CZ-611 37 [email protected] Advisor: Prof. RNDr. Jan Horský, DrSc. Department of Theoretical Physics and Astrophysics Faculty of Natural Sciences Masaryk University Kotlářská 2, Brno, CZ-611 37 [email protected] Examining comission: Abstract The problems solved in this thesis can be divided into two spheres. The first one represents the generation of new Einstein-Maxwell fields, the second one their physical interpretation. The solution of non-linear, self-consistent Einstein-Maxwell equations is an enormously complicated task and was explicitly carried out only in the simplest cases. On the other hand, many exact solutions were discovered by means of special generation techniques that enable us to construct new Einstein-Maxwell fields from those already known or even from the vacuum spacetimes which do not contain any electromagnetic field. A brief review of those techniques together with a summary of necessary mathematical apparatus is given in chapter 1. It is to stress that such techniques are enormously useful, because the more exact solutions will be known and explored, the better we will be able to understand the mathematical and physical background of the theory. -
Axisymmetric Metrics in Arbitrary Dimensions
Preprint typeset in JHEP style. - HYPER VERSION gr-qc/0306069 LPT-ORSAY/0341 DCPT-03/68 IPPP-03/34 Axisymmetric metrics in arbitrary dimensions Christos Charmousis LPT∗, Universit´ede Paris-Sud, Bˆat 210, 91405 Orsay CEDEX, France Ruth Gregory Centre for Particle Theory, University of Durham South Road, Durham, DH1 3LE, U.K. Abstract: We consider axially symmetric static metrics in arbitrary dimension, both with and without a cosmological constant. The most obvious such solutions have an SO(n) group of Killing vectors representing the axial symmetry, although one can also consider abelian groups which represent a flat ‘internal space’. We relate such metrics to lower dimensional dilatonic cosmological metrics with a Liouville potential. We also develop a duality relation between vacuum solutions with internal curvature and those with zero internal curvature but a cosmological constant. This duality relation gives a solution generating technique permitting the mapping of different arXiv:gr-qc/0306069v3 10 Jul 2004 spacetimes. We give a large class of solutions to the vacuum or cosmological constant spacetimes. We comment on the extension of the C-metric to higher dimensions and provide a novel solution for a braneworld black hole. Keywords: p-branes, gravitation, braneworlds, black hole physics. ∗Unit´eMixte de Recherche du CNRS (UMR 8627). Contents 1. Overview 1 2. Four dimensional Weyl metrics: A review 5 2.1 Black hole spacetimes 6 2.2 The Rindler and C-metrics 7 3. General set-up in arbitrary dimensions and the equivalence 8 4. Vacuum spacetimes with a flat transverse space 11 5. Weyl metrics with subspaces of constant curvature 14 5.1 Class I solutions 14 5.2 Class II solutions 16 5.3 Class III solutions 19 6. -
Relativistic Emission Lines from Accreting Black Holes
A&A 413, 861–878 (2004) Astronomy DOI: 10.1051/0004-6361:20031522 & c ESO 2004 Astrophysics Relativistic emission lines from accreting black holes The effect of disk truncation on line profiles A. M¨uller and M. Camenzind Landessternwarte Koenigstuhl, 69117 Heidelberg, Germany Received 30 July 2003 / Accepted 22 September 2003 Abstract. Relativistic emission lines generated by thin accretion disks around rotating black holes are an important diagnostic tool for testing gravity near the horizon. The iron K–line is of special importance for the interpretation of the X–ray emission of Seyfert galaxies, quasars and galactic X–ray binary systems. A generalized kinematic model is presented which includes radial drifts and non–Keplerian rotations for the line emitters. The resulting line profiles are obtained with an object–oriented ray tracer operating in the curved Kerr background metric. The general form of the Doppler factor is presented which includes all kinds of poloidal and toroidal motions near the horizon. The parameters of the model include the spin parameter, the inclination, the truncation and outer radius of the disk, velocity profiles for rotation and radial drift, the emissivity profile and a multi–species line–system. The red wing flux is generally reduced when radial drift is included as compared to the pure Keplerian velocity field. All resulting emission line profiles can be classified as triangular, double–horned, double–peaked, bumpy and shoulder–like. Of particular interest are emission line profiles generated by truncated standard accretion disks (TSD). It is also shown that the emissivity law has a great influence on the profiles. -
Arxiv:Astro-Ph/9601106V2 3 Feb 1997
Line Emission from an Accretion Disk around a Rotating Black Hole: Toward a Measurement of Frame Dragging Benjamin C. Bromley1,2, Kaiyou Chen1,3 and Warner A. Miller1 1Theoretical Astrophysics, MS B288, Los Alamos National Laboratory, Los Alamos, NM 87545 2Theoretical Astrophysics, MS-51, Harvard-Smithsonian Center for Astrophysics 60 Garden Street, Cambridge, MA 02138 3Columbia Astrophysics Laboratory, Columbia University, 538 West 120th Street, New York, NY 10027 ABSTRACT Line emission from an accretion disk and a corotating hot spot about a rotating black hole are considered for possible signatures of the frame-dragging effect. We explicitly compare integrated line profiles from a geometrically thin disk about a Schwarzschild and an extreme Kerr black hole, and show that the line profile differences are small if the inner radius of the disk is near or above the Schwarzschild stable-orbit limit of radius 6GM/c2. However, if the inner disk radius extends below this limit, as is pos- sible in the extreme Kerr spacetime, then differences can become significant, especially if the disk emissivity is stronger near the inner regions. We demonstrate that the first three moments of a line profile define a three-dimensional space in which the presence of material at small radii becomes quantitatively evident in broad classes of disk mod- els. In the context of the simple, thin disk paradigm, this moment-mapping scheme suggests formally that the iron line detected by the Advanced Satellite for Cosmology and Astrophysics mission from MCG-6-30-15 (Tanaka et al. 1995) is 3 times more likely to originate from a disk about a rotating black hole than from a Schwarzschild system. -
Weyl Metrics and Wormholes
Prepared for submission to JCAP Weyl metrics and wormholes Gary W. Gibbons,a;b Mikhail S. Volkovb;c aDAMTP, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, UK bLaboratoire de Math´ematiqueset Physique Th´eorique,LMPT CNRS { UMR 7350, Universit´ede Tours, Parc de Grandmont, 37200 Tours, France cDepartment of General Relativity and Gravitation, Institute of Physics, Kazan Federal University, Kremlevskaya street 18, 420008 Kazan, Russia E-mail: [email protected], [email protected] Abstract. We study solutions obtained via applying dualities and complexifications to the vacuum Weyl metrics generated by massive rods and by point masses. Rescal- ing them and extending to complex parameter values yields axially symmetric vacuum solutions containing singularities along circles that can be viewed as singular mat- ter sources. These solutions have wormhole topology with several asymptotic regions interconnected by throats and their sources can be viewed as thin rings of negative tension encircling the throats. For a particular value of the ring tension the geometry becomes exactly flat although the topology remains non-trivial, so that the rings liter- ally produce holes in flat space. To create a single ring wormhole of one metre radius one needs a negative energy equivalent to the mass of Jupiter. Further duality trans- formations dress the rings with the scalar field, either conventional or phantom. This gives rise to large classes of static, axially symmetric solutions, presumably including all previously known solutions for a gravity-coupled massless scalar field, as for exam- ple the spherically symmetric Bronnikov-Ellis wormholes with phantom scalar. The multi-wormholes contain infinite struts everywhere at the symmetry axes, apart from arXiv:1701.05533v3 [hep-th] 25 May 2017 solutions with locally flat geometry. -
A Brief Observational History of the Black-Hole Spacetimes Wolfgang Kundt Argelander Institute of Bonn University
A brief Observational History of the Black-Hole Spacetimes Wolfgang Kundt Argelander Institute of Bonn University Abstract. In this year (2015), Black Holes (BHs) celebrate their 100th birthday, if their birth is taken to be triggered by a handwrit- ten letter from Martin Schwarzschild to Albert Einstein, in connec- tion with his newly found spherically symmetric vacuum solution. 1.1 Introduction Black Holes are brainchildren of Einstein-Hilbert's General Relativity Theory (GRT). They arose naturally as the non-singular solutions describing the axi- ally symmetric vacuum far fields of the gravitational collapse of a sufficiently massive (rotating) burnt-out star under its own weight, and were subsequently likewise taken seriously on superstellar mass scales { at the centers of galaxies { as well as on distinctly substellar mass scales, as evaporating mountain-sized objects (in mass) formed during earlier cosmic epochs. The (more) general pos- sibility of a (slightly) non-symmetrical gravitational collapse, without a regular event horizon { known under the name of `naked singularity' { was eliminated from consideration by Roger Penrose's postulate of `cosmic censorship' (CC, [1972]), with the plausible expectation that collapsing bodies would always re- move their non-fitting higher multipole moments via gravitational radiation { strongly suggested by the heroic work of Richard Price [1972] { an expectation which has meanwhile been proven unjustified [Joshi, 2009, Joshi & Malafarina, 2013]: BH spacetimes form a subset of measure zero within the class of all collapse scenarios. Should we worry? I do not think so. Observations have shown that we live inside a comparatively young (part of the) Universe, with a significant fraction of its primordial hydrogen yet unburnt (towards chemical elements of higher nuclear binding energy). -
The Astrophysical Jets Wolfgang Kundt Argelander Institute of Bonn University, Auf Dem H¨Ugel71, D-53121 Bonn, Germany Email: [email protected]
Jets at All Scales Proceedings IAU Symposium No. 275, 2010 c 2010 International Astronomical Union G. Romero, eds. DOI: 00.0000/X000000000000000X The Astrophysical Jets Wolfgang Kundt Argelander Institute of Bonn University, Auf dem H¨ugel71, D-53121 Bonn, Germany email: [email protected] Abstract. In this published note I attempt to sketch my understanding of the universal working scheme of all the astrophysical jet sources, or ‘bipolar flows’, on both stellar and galactic scales, also called ‘microquasars’, and ‘quasars’. A crucial building block will be their medium: ex- tremely relativistic e±-pair plasma performing quasi loss-free E x B-drifts through self-rammed channels, whose guiding equi-partition E- and B-fields convect the electric potential necessary for eventual single-step post-acceleration, at their terminating ‘knots’, or ‘hotspots’. The in- dispensible pair plasma is generated in magnetospheric reconnections of the central rotator. Already for this reason, black holes cannot serve as jet engines. Keywords. Jets, black holes, pair plasma, E x B-drift 1. How to make jets? Astrophysical jet sources involve powerful engines of the Universe: The engines can eject charges at very-high energies (VHE), continually at almost luminal speeds to astro- 7 nomical distances of order .Mpc, for &10 yr, in two antipodal directions, in a beamed manner, aimed within an angle of ≈1%, whereby particles arrive with .PeV energies at their termination sites. Militaries would appreciate availing of such guns. How does non-animated matter achieve such a difficult goal, time and again, on various size and mass scales? After years of intense deliberation, it is my distinct understanding that all the jet engines follow a uniform working pattern. -
Pos(FRAPWS2016)012 Assumptions
Astrophysical Fashions - A Warning PoS(FRAPWS2016)012 Wolfgang Kundt∗ Argelander Institut of Bonn University, Germany E-mail: [email protected] Some 14 more or less tacit, but crucial assumptions will be highlighted which have been fre- quently made in standard literature on geophysical, astrophysical, and (even) biophysical prob- lems – between 1978 and 2016 – and proposed to be replaced by alternative assumptions. Frontier Research in Astrophysics - II 23-28 May 2016 Mondello (Palermo), Italy ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License (CC BY-NC-ND 4.0). http://pos.sissa.it/ Astrophysical Fashions - A Warning Wolfgang Kundt 1. Astrophysical Alternatives (1) Distances: A fundamental and nontrivial problem in astrophysics is to measure the distances of observed objects, in particular when they are far from us; whereby ”far” begins already near 108cm for certain terrestrial problems, e.g. in deserts, or on oceans, and gets increasingly more difficult to determine when the edge of the observable Universe is approached, at distances of 28 .10 cm. On those largest scales, distances tend to be measured in units of cosmic recession velocities at trans-luminal (expansion) speeds, whereby spectral redshift z and Lorentz factor g are related by the well-known special-relativistic law: PoS(FRAPWS2016)012 z + 1 = g(1 + b) and take the values {z, g}= {9,5} in extreme cases for the well-known gamma-ray bursts (GRBs) p (of which 3 on average strike our planet per day); z := d H / c , H := R˙=R , g := 1/ 1 − b 2. -
Dynamics of Self-Gravitating Disks
University of Cambridge May, 1994 Dynamics of self-gravitating disks Christophe Pichon Clare College and Institute of Astronomy A dissertation submitted to the University of Cambridge in accordance with the regulations for admission to the degree of Doctor of Philosophy ii Summary A fair fraction of observed galactic disks present a bar corresponding to elongated isophotes beyond the central core. Numerical simulations also suggest that bar instabilities are quite common. Why should some galaxies have bars and others not? This question is addressed here by investigating the stability of a self gravitating disk with respect to instabilities induced by the adiabatic re-alignment of resonant orbits. It is shown that the dynamical equations can be recast in terms of the interaction of resonant flows. Concentrating on the stars belonging to the inner Lindblad resonance, it is argued that this interaction yields an instability of Jeans’ type. The Jeans instability traps stars moving in phase with respect to a growing potential; here the azimuthal instability corresponds to a rotating growing potential that captures the lobe of orbital streams of resonant stars. The precession rate of this growing potential is identified with the pattern speed of the bar. The instability criterion puts constraints on the relative dispersion in angular frequency of the underlying distribution function. The outcome of orbital instability is investigated while constructing distribution functions induced by the adiabatic re-alignment of inner Lindblad orbits. These distribution functions maximise entropy while preserving the underlying axisymmetric component of the galaxy and the constraints of angular momentum, total energy, and detailed circulations conservation. -
The Astrophysical Jets – After 30 Years of Deliberation
THE ASTROPHYSICAL JETS { AFTER 30 YEARS OF DELIBERATION Wolfgang Kundt Argelander Institute of Bonn University Auf dem Hugel¨ 71, D-53121 Bonn, Germany Abstract An update is presented of my 2004 semi-analytical model with Gopal Krishna for E x B-drifting jets, which may well describe sat- isfactorily all the astrophysical jet sources, or bipolar flows, both on galactic and on stellar scales. 1 Introduction Jet sources have been discovered in the sky, and mapped since more than 30 years, beginning at radio frequencies, closely followed by optical frequencies, then X-rays and γ-rays up to GeV energies, and recently even up to TeV energies, or even . PeV energies! Whilst more and more morphological and temporal details have been elaborated, the modes of their generation, propagation, termination, and evolution have found deploringly diverging treatments in the extended literature. This decades-long stagnation of in- sight, it appears to me, is predominantly due to the black-hole dictatorship in present-day astrophysics: Black Holes (BHs) lack persistent, time-varying magnetic fields (for pair formation, and for their post-acceleration via an outgoing strong wave), and lack quasi-static (high-density) deLaval nozzles for the formation of a pair of supersonic antipodal jets { as opposed to fast- rotating magnetized stars inside shearing accretion disks, or differentially rotating magnetized coronas of central galactic disks which have been the preferred jet sources in Kundt & Gopal-Krishna [1980, 2004] as well as in 1 Blome & Kundt [1988], and in Kundt [1979, 1989, 1996, 2001a,b, 2002, 2005, 2009a,b], to be revisited in section 4. -
New Approaches to Space-Time Singularities
\b'to'ql NE\M APPROACHES TO .¡vA. SPACE.TIME SINGULARITIES by Susan M. Scott Bachelor of Science (Honours) Department of Physics and Mathematical Physics The University of Adelaide Thesis submitted in accordance with the requirements for the degree of DOCTOR OF PHILOSOPHY May 1991 Contents Contents I Abstract ul Statement lv Acknowledgements v Preface vl 1 An Historical Perspective on the Curzon Solution L 1.1 Introduction . I I.2 The Curzon metric 2 1.3 Past analyses of the Curzon singularity . 4 t.4 The szekeres and Morgan extension of the curzon metric . 8 1.5 Comments on past analyses of the Curzon singularity L4 1.6 Israel's theorem 18 2 The Spacelike Hypersurfaces of the Curzon Solution 24 24 2.t Introduction . 2.2 Spacelike geodesics approaching R : 0 26 2.3 Analysis of curves approaching R : 0 . 30 2.4 New coordinates for the r-z Plane 34 2.5 Conclusions 40 3 The Global Structure of the Curzon Solution 44 44 3.1 Introduction . 3.2 Behaviour of geodesics approaching R : 0 45 3.3 New coordinates for the Curzon metric 49 3.4 Features of the new coordinates 52 3.5 Discussion and conclusions 56 'WeYl 4 A Survey of the Metrics 63 63 4.1 Introduction . 4.2 The Weyl metrics 65 4.3 The Schwarzschild solution 66 4.4 The Zipoy-Voorhees metrics 68 4.5 Possible sources for the Zipoy-Voorhees metrics 7t 4.6 Possible extensions of the Zipoy-Voorhees metrics 74 4.7 Some general properties of the Weyl metrics 75 4.8 The two-particle Curzon solution 77 4.9 Recent mathematical developments 79 4.10 Ring singularities 80 5 The Abstract BoundarY 84 I Introduction 84 2 Parametrized curves on a manifold 86 3 Enveloped manifolds and boundary sets 89 4 Limit points and C-completeness 92 Ð Abstract boundaries .