Dicke's Superradiance in Astrophysics
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Cyclotron Maser Emission in Solar and Stellar Flares 1
32nd URSI GASS, Montreal, 19–26 August 2017 CYCLOTRON MASER EMISSION IN SOLAR AND STELLAR FLARES Donald B. Melrose SIfA, School of Physics, University of Sydney, NSW 2006, Australia, http://www.physics.usyd.edu.au/ melrose 1 Introduction The problem discussed in this paper is whether the now accepted form of electron cyclotron maser emission (ECME) for the Earth’s auroral kilometric radiation (AKR) also applies to other suggested applications of ECME, which would have radical implications for solar and stellar applications, or whether AKR is an exception and a different form of ECME applies to other sources. Since circa 1980, ECME has been the accepted emission mechanism for AKR, for Jupiter’s decametric radiation (DAM), for solar spike bursts and for bright radio emission from flare stars. Originally, a loss-cone driven form of ECME [1] was widely accepted for all these application, but this changed for AKR in the 1990s when it was recognized that the driving electrons have a horseshoe distribution, and a horseshoe-driven form of ECME [2, 3] became the favored mechanism [13]. This form of ECME requires an extremely low electron density in the source region, in order for the radio emission to escape. This extreme condition appears to be satisfied in the “auroral cavity” that develops in association with the precipitating electrons [4]. The question discussed in this paper is whether the horseshoe-driven form of ECME, known to apply to AKR, applies to other sources of ECME, specifically to DAM, solar spike bursts and bright emission from flare stars. 2 Forms of ECME ECME corresponds to negative gyromagnetic absorption. -
Schwarzschild Black Hole Can Also Produce Super-Radiation Phenomena
Schwarzschild black hole can also produce super-radiation phenomena Wen-Xiang Chen∗ Department of Astronomy, School of Physics and Materials Science, GuangZhou University According to traditional theory, the Schwarzschild black hole does not produce super radiation. If the boundary conditions are set in advance, the possibility is combined with the wave function of the coupling of the boson in the Schwarzschild black hole, and the mass of the incident boson acts as a mirror, so even if the Schwarzschild black hole can also produce super-radiation phenomena. Keywords: Schwarzschild black hole, superradiance, Wronskian determinant I. INTRODUCTION In a closely related study in 1962, Roger Penrose proposed a theory that by using point particles, it is possible to extract rotational energy from black holes. The Penrose process describes the fact that the Kerr black hole energy layer region may have negative energy relative to the observer outside the horizon. When a particle falls into the energy layer region, such a process may occur: the particle from the black hole To escape, its energy is greater than the initial state. It can also show that in Reissner-Nordstrom (charged, static) and rotating black holes, a generalized ergoregion and similar energy extraction process is possible. The Penrose process is a process inferred by Roger Penrose that can extract energy from a rotating black hole. Because the rotating energy is at the position of the black hole, not in the event horizon, but in the area called the energy layer in Kerr space-time, where the particles must be like a propelling locomotive, rotating with space-time, so it is possible to extract energy . -
Review of Zeeman Effect Observations of Regions of Star Formation
Review of Zeeman Effect Observations of Regions of Star Formation Richard M. Crutcher 1,∗ and Athol J. Kemball 1 1Department of Astronomy, University of Illinois, Urbana, IL, USA Correspondence*: 1002 W. Green St., Urbana, IL 61801 USA [email protected] ABSTRACT The Zeeman effect is the only observational technique available to measure directly the strength of magnetic fields in regions of star formation. This chapter reviews the physics of the Zeeman effect and its practical use in both extended gas and in masers. We discuss observational results for the five species for which the Zeeman effect has been detected in the interstellar medium – H I, OH, and CN in extended gas and OH, CH3OH, and H2O in masers. These species cover a wide range in density, from ∼ 10 cm−3 to ∼ 1010 cm −3, which allows magnetic fields to be measured over the full range of cloud densities. However, there are significant limitations, including that only the line-of-sight component of the magnetic field strength can usually be measured and that there are often significant uncertainties about the physical conditions being sampled, particularly for masers. We discuss statistical methods to partially overcome these limitations. The results of Zeeman observations are that the mass to magnetic flux ratio, which measures the relative importance of gravity to magnetic support, is subcritical (gravity dominates 22 −2 magnetic support) at lower densities but supercritical for NH & 10 cm . Above nH ∼ 300 cm−3, which is roughly the density at which clouds typically become self-gravitating, the strength of magnetic fields increases approximately as B ∝ n2/3, which suggest that magnetic fields do not provide significant support at high densities. -
Radio Emission Toward Regions of Massive Star Formation in the Large Magellanic Cloud
Brigham Young University BYU ScholarsArchive Theses and Dissertations 2015-03-01 Radio Emission Toward Regions of Massive Star Formation in the Large Magellanic Cloud Adam Johanson Brigham Young University - Provo Follow this and additional works at: https://scholarsarchive.byu.edu/etd Part of the Astrophysics and Astronomy Commons, and the Physics Commons BYU ScholarsArchive Citation Johanson, Adam, "Radio Emission Toward Regions of Massive Star Formation in the Large Magellanic Cloud" (2015). Theses and Dissertations. 4419. https://scholarsarchive.byu.edu/etd/4419 This Dissertation is brought to you for free and open access by BYU ScholarsArchive. It has been accepted for inclusion in Theses and Dissertations by an authorized administrator of BYU ScholarsArchive. For more information, please contact [email protected], [email protected]. Radio Emission Toward Regions of Massive Star Formation in the Large Magellanic Cloud Adam K. Johanson A dissertation submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the degree of Doctor of Philosophy Victor Migenes, Chair Clark G. Christensen Timothy W. Leishman J. Ward Moody Denise Stephens Department of Physics and Astronomy Brigham Young University March 2015 Copyright © 2015 Adam K. Johanson All Rights Reserved ABSTRACT Radio Emission Toward Regions of Massive Star Formation in the Large Magellanic Cloud Adam K. Johanson Department of Physics and Astronomy, BYU Doctor of Philosophy Four regions of massive star formation in the Large Magellanic Cloud (LMC) were observed for water and methanol maser emission and radio continuum emission. A total of 42 radio detec- tions were made including 27 new radio sources, four water masers, and eight compact H II regions. -
Coherently Amplifying Photon Production from Vacuum with a Dense Cloud of Accelerating Photodetectors ✉ Hui Wang 1 & Miles Blencowe 1
ARTICLE https://doi.org/10.1038/s42005-021-00622-3 OPEN Coherently amplifying photon production from vacuum with a dense cloud of accelerating photodetectors ✉ Hui Wang 1 & Miles Blencowe 1 An accelerating photodetector is predicted to see photons in the electromagnetic vacuum. However, the extreme accelerations required have prevented the direct experimental ver- ification of this quantum vacuum effect. In this work, we consider many accelerating pho- todetectors that are contained within an electromagnetic cavity. We show that the resulting photon production from the cavity vacuum can be collectively enhanced such as to be 1234567890():,; measurable. The combined cavity-photodetectors system maps onto a parametrically driven Dicke-type model; when the detector number exceeds a certain critical value, the vacuum photon production undergoes a phase transition from a normal phase to an enhanced superradiant-like, inverted lasing phase. Such a model may be realized as a mechanical membrane with a dense concentration of optically active defects undergoing gigahertz flexural motion within a superconducting microwave cavity. We provide estimates suggesting that recent related experimental devices are close to demonstrating this inverted, vacuum photon lasing phase. ✉ 1 Department of Physics and Astronomy, Dartmouth College, Hanover, NH, USA. email: [email protected] COMMUNICATIONS PHYSICS | (2021) 4:128 | https://doi.org/10.1038/s42005-021-00622-3 | www.nature.com/commsphys 1 ARTICLE COMMUNICATIONS PHYSICS | https://doi.org/10.1038/s42005-021-00622-3 ne of the most striking consequences of the interplay Cavity wall Obetween relativity and the uncertainty principle is the predicted detection of real photons from the quantum fi TLS defects electromagnetic eld vacuum by non-inertial, accelerating pho- Cavity mode todetectors. -
Dicke Superradiance in Solids [Invited]
C80 Vol. 33, No. 7 / July 2016 / Journal of the Optical Society of America B Review Dicke superradiance in solids [Invited] 1 1 2 1 2 KANKAN CONG, QI ZHANG, YONGRUI WANG, G. TIMOTHY NOE II, ALEXEY BELYANIN, AND 1,3,4, JUNICHIRO KONO * 1Department of Electrical and Computer Engineering, Rice University, Houston, Texas 77005, USA 2Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843, USA 3Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA 4Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA *Corresponding author: [email protected] Received 18 February 2016; revised 7 April 2016; accepted 7 April 2016; posted 8 April 2016 (Doc. ID 259437); published 13 May 2016 Recent advances in optical studies of condensed matter systems have led to the emergence of a variety of phenomena that have conventionally been studied in the realm of quantum optics. These studies have not only deepened our understanding of light–matter interactions but have also introduced aspects of many-body corre- lations inherent in optical processes in condensed matter systems. This paper is concerned with the phenomenon of superradiance (SR), a profound quantum optical process originally predicted by Dicke in 1954. The basic concept of SR applies to a general N body system, where constituent oscillating dipoles couple together through interaction with a common light field and accelerate the radiative decay of the whole system. Hence, the term SR ubiquitously appears in order to describe radiative coupling of an arbitrary number of oscillators in many situations in modern science of both classical and quantum description. -
The Black Hole Bomb and Superradiant Instabilities
The black hole bomb and superradiant instabilities Vitor Cardoso∗ Centro de F´ısica Computacional, Universidade de Coimbra, P-3004-516 Coimbra, Portugal Oscar´ J. C. Dias† Centro Multidisciplinar de Astrof´ısica - CENTRA, Departamento de F´ısica, F.C.T., Universidade do Algarve, Campus de Gambelas, 8005-139 Faro, Portugal Jos´e P. S. Lemos‡ Centro Multidisciplinar de Astrof´ısica - CENTRA, Departamento de F´ısica, Instituto Superior T´ecnico, Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal Shijun Yoshida§ Centro Multidisciplinar de Astrof´ısica - CENTRA, Departamento de F´ısica, Instituto Superior T´ecnico, Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal ¶ (Dated: February 1, 2008) A wave impinging on a Kerr black hole can be amplified as it scatters off the hole if certain conditions are satisfied giving rise to superradiant scattering. By placing a mirror around the black hole one can make the system unstable. This is the black hole bomb of Press and Teukolsky. We investigate in detail this process and compute the growing timescales and oscillation frequencies as a function of the mirror’s location. It is found that in order for the system black hole plus mirror to become unstable there is a minimum distance at which the mirror must be located. We also give an explicit example showing that such a bomb can be built. In addition, our arguments enable us to justify why large Kerr-AdS black holes are stable and small Kerr-AdS black holes should be unstable. PACS numbers: 04.70.-s I. INTRODUCTION one can extract as much rotational energy as one likes from the black hole. -
A Modern Approach to Superradiance
A Modern Approach to Superradiance Solomon Endlicha and Riccardo Pencob,c a Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA 94306, USA b Physics Department, Center for Theoretical Physics & Institute for Strings, Cosmology, and Astroparticle Physics, Columbia University, New York, NY 10027, USA c Center for Particle Cosmology, Department of Physics and Astronomy, University of Pennsylvania, Philadelphia, Pennsylvania 19104, USA Abstract In this paper, we provide a simple and modern discussion of rotational superradiance based on quantum field theory. We work with an effective theory valid at scales much larger than the size of the spinning object responsible for superradiance. Within this framework, the probability of absorption by an object at rest completely determines the superradiant amplification rate when that same object is spinning. We first discuss in detail superradiant scattering of spin 0 particles with orbital angular momentum ℓ = 1, and then extend our analysis to higher values of orbital angular momentum and spin. Along the way, we provide a simple derivation of vacuum friction—a “quantum torque” acting on spinning objects in empty space. Our results apply not only to black holes but to arbitrary spinning objects. We also discuss superradiant instability due to formation of bound states and, as an illustration, we calculate the instability rate Γ for bound states with massive spin 1 particles. For a black hole with mass M and angular velocity Ω, we find Γ (GMµ)7Ω when the particle’s Compton wavelength 1/µ is ∼ much greater than the size GM of the spinning object. This rate is parametrically much larger than the instability rate for spin 0 particles, which scales like (GMµ)9Ω. -
Super- and Subradiance by Entangled Free Particles
Super- and subradiance by entangled free particles Aviv Karnieli1,*, Nicholas Rivera2, Ady Arie3 and Ido Kaminer4 1Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Ramat Aviv 69978, Tel Aviv, Israel 2Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA 3School of Electrical Engineering, Fleischman Faculty of Engineering, Tel Aviv University, Tel Aviv 69978, Israel 4Department of Electrical Engineering, Technion–Israel Institute of Technology, Haifa 32000, Israel *corresponding authors: [email protected]; [email protected] When multiple quantum emitters radiate, their emission rate may be enhanced or suppressed due to collective interference in a process known as super- or subradiance. Such processes are well-known to occur also in light emission by free charged particles. To date, all experimental and theoretical studies of super- and subradiance in these systems involved the classical correlations between the emitters. However, dependence on quantum correlations, such as entanglement between different emitting particles, has not been studied. Recent advances in coherent-shaping of free-electron wavefunctions motivate the investigation of such quantum regimes of super- and subradiance. In this Letter, we show how a pair of coincident path-entangled electrons can demonstrate either super- or subradiant light emission, depending on the two-particle wavefunction. By choosing different free-electron Bell-states, the spectrum and emission pattern of the light can be reshaped, in a manner that cannot be accounted for by a classical mixed state. We show these results for light emission in any optical medium, and discuss their generalization to many-body quantum states. Our findings suggest that light emission can be sensitive to the explicit quantum state of the emitting matter wave, and possibly serve as a non-destructive measurement scheme for measuring the quantum state of many-body systems. -
Coherent Emission Mechanisms in Astrophysical Plasmas
Reviews of Modern Plasma Physics manuscript No. (will be inserted by the editor) Coherent Emission Mechanisms in Astrophysical Plasmas D. B. Melrose Received: date / Accepted: date Abstract Three known examples of coherent emission in radio astronomical sources are reviewed: plasma emission, electron cyclotron maser emission (ECME) and pulsar radio emission. Plasma emission is a multi-stage mechanism with the first stage being gener- ation of Langmuir waves through a streaming instability, and subsequent stages involving partial conversion of the Langmuir turbulence into escaping radiation at the fundamental (F) and second harmonic (H) of the plasma frequency. The early development and subsequent refinements of the theory, motivated by application to solar radio bursts, are reviewed. The driver of the instability is faster electrons outpacing slower electrons, resulting in a positive gradient (df(vk)/dvk > 0) at the front of the beam. Despite many successes of the theory, there is no widely accepted explanation for type I bursts and various radio continua. The earliest models for ECME were purely theoretical, and the theory was later adapted and applied to Jupiter (DAM), the Earth (AKR), solar spike bursts and flare stars. ECME strongly favors the x mode, whereas plasma emission favors the o mode. Two drivers for ECME are a ring feature (implying df(v)/dv > 0) and a loss-cone feature. Loss-cone driven ECME was initially favored for all applications. The now favored driver for AKR is the ring-feature in a horseshoe distribution, which results from acceleration by a parallel electric on converging magnetic field lines. The driver in DAM and solar and stellar applications is uncertain. -
How to Construct a 3D Model of the Planetary Nebula NGC 6781 with SHAPE
How to construct a 3D model of the planetary nebula NGC 6781 with SHAPE Josefine Bergstedt, 850506-1484 June 30, 2015 Uppsala University, Department of Physics and Astronomy Bachelor of Science Degree in Physics, VT -15 Supervisor: Sofia Ramstedt Referee: Kjell Eriksson Sammanfattning Målet med det här arbetet är att i dataprogrammet SHAPE konstruera en 3D-modell av den planetariska nebulosan NGC 6781. En planetarisk nebulosa bildas när en viss typ av stjärnor, med en ur- sprunglig massa mellan 0.8-8 M (där M står för solmassan) har nått slut- fasen i sin utveckling och är på väg att avsluta sina liv. I denna slutfas uppkommer pulsationer hos stjärnan samt en stark vind som tillsammans blåser bort de yttre, sfäriska lagren av stjärnan tills endast den innersta kär- nan återstår. Kärnan kommer att svalna av och blir till slut en så kallad vit dvärg vilken omges av ett skal bestående av den utkastade gasen och stoftet från stjärnans yttre lager. Detta expanderande skal bestående av lysande, joniserad gas är vad som kallas för planetarisk nebulosa. Ordet "nebulosa" är latin och betyder moln eller dimma, namnen plane- tarisk nebulosa uppkom på 1780-talet då man först observerade dessa objekt och tyckte de liknade stora gasplaneter. Planetariska nebulosor förekommer i flera olika former, allt från bipolär till väldigt komplexa strukturer. Den snabba vinden tillsammans med den starka strålning som kommer från stjär- nan antas vara orsaken till att planetariska nebulosor uppkommer. Exakt hur dessa processer fungerar samt vilka mekanismer som påverkar att stjär- nans yttre sfäriska lager kan anta de spektakulära former som planetariska nebulosor har är något som man i dagsläget inte vet med säkerhet. -
Masers: Precision Probes of Molecular Gas
Available online at www.sciencedirect.com ScienceDirect Advances in Space Research 65 (2020) 780–789 www.elsevier.com/locate/asr Masers: Precision probes of molecular gas A.M.S. Richards a,⇑, A. Sobolev b, A. Baudry c, F. Herpin c, L. Decin d, M.D. Gray a S. Etoka a, E.M.L. Humphreys e, W. Vlemmings f a JBCA, School of Physics and Astronomy, University of Manchester, M13 9PL, UK b Astronomical Observatory, Ural Federal University, Ekaterinburg 620083, Russia c Laboratoire d’astrophysique de Bordeaux, Universite´ de Bordeaux, 33615 Pessac, France d Instituut voor Sterrenkunde, Katholieke Universiteit Leuven, 3001 Leuven, Belgium e ESO, Karl-Schwarzschild-Str. 2, 85748 Garching bei Munchen, Germany f Chalmers University of Technology, Onsala Space Observatory, 439 92 Onsala, Sweden Received 18 December 2018; received in revised form 7 May 2019; accepted 15 May 2019 Available online 11 June 2019 Abstract Maser emission from water, methanol, silicon monoxide and other molecules can reach brightness temperatures 1010 K. Such observations can achieve sub-pc precision for discs around black holes or sub-au scale interactions in protostellar discs and the regions where evolved star winds reach escape velocity. Ultra-high resolution maser observations also provide photon statistics, for fundamental physics experiments. RadioAstron has shown the success – and limitations – of cm-wave maser observations on scales 1 mas with sparse baseline coverage. ALMA, APEX and earlier single dish searches have found a wealth of mm and sub-mm masers, some of which probably also attain high brightness temperatures. Masers are ideal for high-resolution observations throughout the radio regime and we need to consider the current lessons for the best observational strategies to meet specific science cases.