Einstein Telescope Design Study: Vision Document
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5 Optical Design
ET-0106A-10 issue :2 ET Design Study date :January27,2011 page :204of315 5 Optical design 5.1 Description Responsible: WP3 coordinator, A. Freise Put here the description of the content of the section . 5.2 Executive Summary Responsible: WP3 coordinator, A. Freise Put here a summary of the main achievement/statements of this section . 5.3 Review on the geometry of the observatory Author(s): Andreas Freise,StefanHild This section briefly reviews the reasoning behind the shape of current gravitational wave detectors and then discusses alternative geometries which can be of interest for third-generation detectors. We will use the ter- minology introduced in the review of a triangular configuration [220] and discriminate between the geometry, topology and configuration of a detector as follows: The geometry describes the position information of one or several interferometers, defined by the number of interferometers, their location and relative orientation. The topology describes the optical system formed by its core elements. The most common examples are the Michelson, Sagnac and Mach–Zehnder topologies. Finally the configuration describes the detail of the optical layout and the set of parameters that can be changed for a given topology, ranging from the specifications of the optical core elements to the control systems, including the operation point of the main interferometer. Please note that the addition of optical components to a given topology is often referred to as a change in configuration. 5.3.1 The L-shape Current gravitational wave detectors represent the most precise instruments for measuring length changes. They are laser interferometers with km-long arms and are operated differently from many precision instruments built for measuring an absolute length. -
Gabriele Veneziano
Strings 2021, June 21 Discussion Session High-Energy Limit of String Theory Gabriele Veneziano Very early days (1967…) • Birth of string theory very much based on the high-energy (Regge) limit: Im A(Regge) ≠ 0! •Duality bootstrap (except for the Pomeron!) => DRM (emphasis shifted on res/res duality, xing) •Need for infinite number of resonances of unlimited mass and spin (linear traj.s => strings?) • Exponential suppression @ high E & fixed θ => colliding objects are extended, soft (=> strings?) •One reason why the NG string lost to QCD. •Q: What’s the Regge limit of (large-N) QCD? 20 years later (1987…) •After 1984, attention in string theory shifted from hadronic physics to Q-gravity. • Thought experiments conceived and efforts made to construct an S-matrix for gravitational scattering @ E >> MP, b < R => “large”-BH formation (RD-3 ~ GE). Questions: • Is quantum information preserved, and how? • What’s the form and role of the short-distance stringy modifications? •N.B. Computations made in flat spacetime: an emergent effective geometry. What about AdS? High-energy vs short-distance Not the same even in QFT ! With gravity it’s even more the case! High-energy, large-distance (b >> R, ls) •Typical grav.al defl. angle is θ ~ R/b = GE/b (D=4) •Scattering at high energy & fixed small θ probes b ~ R/θ > R & growing with energy! •Contradiction w/ exchange of huge Q = θ E? No! • Large classical Q due to exchange of O(Gs/h) soft (q ~ h/b) gravitons: t-channel “fractionation” • Much used in amplitude approach to BH binaries • θ known since ACV90 up to O((R/b)3), universal. -
The Einstein Telescope (ET) Is a Proposed Underground Infrastructure to Host a Third- Generation, Gravitational-Wave Observatory
The Einstein Telescope (ET) is a proposed underground infrastructure to host a third- generation, gravitational-wave observatory. It builds on the success of current, second-generation laser- interferometric detectors Advanced Virgo and Advanced LIGO, whose breakthrough discoveries of merging black holes (BHs) and neutron stars over the past 5 years have ushered scientists into the new era of gravitational-wave astronomy. The Einstein Telescope will achieve a greatly improved sensitivity by increasing the size of the interferometer from the 3km arm length of the Virgo detector to 10km, and by implementing a series of new technologies. These include a cryogenic system to cool some of the main optics to 10 – 20K, new quantum technologies to reduce the fluctuations of the light, and a set of infrastructural and active noise-mitigation measures to reduce environmental perturbations. The Einstein Telescope will make it possible, for the first time, to explore the Universe through gravitational waves along its cosmic history up to the cosmological dark ages, shedding light on open questions of fundamental physics and cosmology. It will probe the physics near black-hole horizons (from tests of general relativity to quantum gravity), help understanding the nature of dark matter (such as primordial BHs, axion clouds, dark matter accreting on compact objects), and the nature of dark energy and possible modifications of general relativity at cosmological scales. Exploiting the ET sensitivity and frequency band, the entire population of stellar and intermediate mass black holes will be accessible over the entire history of the Universe, enabling to understand their origin (stellar versus primordial), evolution, and demography. -
Extreme Gravity and Fundamental Physics
Extreme Gravity and Fundamental Physics Astro2020 Science White Paper EXTREME GRAVITY AND FUNDAMENTAL PHYSICS Thematic Areas: • Cosmology and Fundamental Physics • Multi-Messenger Astronomy and Astrophysics Principal Author: Name: B.S. Sathyaprakash Institution: The Pennsylvania State University Email: [email protected] Phone: +1-814-865-3062 Lead Co-authors: Alessandra Buonanno (Max Planck Institute for Gravitational Physics, Potsdam and University of Maryland), Luis Lehner (Perimeter Institute), Chris Van Den Broeck (NIKHEF) P. Ajith (International Centre for Theoretical Sciences), Archisman Ghosh (NIKHEF), Katerina Chatziioannou (Flatiron Institute), Paolo Pani (Sapienza University of Rome), Michael Pürrer (Max Planck Institute for Gravitational Physics, Potsdam), Thomas Sotiriou (The University of Notting- ham), Salvatore Vitale (MIT), Nicolas Yunes (Montana State University), K.G. Arun (Chennai Mathematical Institute), Enrico Barausse (Institut d’Astrophysique de Paris), Masha Baryakhtar (Perimeter Institute), Richard Brito (Max Planck Institute for Gravitational Physics, Potsdam), Andrea Maselli (Sapienza University of Rome), Tim Dietrich (NIKHEF), William East (Perimeter Institute), Ian Harry (Max Planck Institute for Gravitational Physics, Potsdam and University of Portsmouth), Tanja Hinderer (University of Amsterdam), Geraint Pratten (University of Balearic Islands and University of Birmingham), Lijing Shao (Kavli Institute for Astronomy and Astro- physics, Peking University), Maaretn van de Meent (Max Planck Institute for Gravitational -
Seismic Characterization of the Euregio Meuse-Rhine in View of Einstein Telescope
SEISMIC CHARACTERIZATION OF THE EUREGIO MEUSE-RHINE IN VIEW OF EINSTEIN TELESCOPE 13 September 2019 First results of seismic studies of the Belgian-Dutch-German site for Einstein Telescope Soumen Koley1, Maria Bader1, Alessandro Bertolini1, Jo van den Brand1,2, Henk Jan Bulten1,3, Stefan Hild1,2, Frank Linde1,4, Bas Swinkels1, Bjorn Vink5 1. Nikhef, National Institute for Subatomic Physics, Amsterdam, The Netherlands 2. Maastricht University, Maastricht, The Netherlands 3. VU University Amsterdam, Amsterdam, The Netherlands 4. University of Amsterdam, Amsterdam, The Netherlands 5. Antea Group, Maastricht, The Netherlands CONFIDENTIAL Figure 1: Artist impression of the Einstein Telescope gravitational wave observatory situated at a depth of 200-300 meters in the Euregio Meuse-Rhine landscape. The triangular topology with 10 kilometers long arms allows for the installation of multiple so-called laser interferometers. Each of which can detect ripples in the fabric of space-time – the unique signature of a gravitational wave – as minute relative movements of the mirrors hanging at the bottom of the red and white towers indicated in the illustration at the corners of the triangle. 1 SEISMIC CHARACTERIZATION OF THE EUREGIO MEUSE-RHINE IN VIEW OF EINSTEIN TELESCOPE Figure 2: Drill rig for the 2018-2019 campaign used for the completion of the 260 meters deep borehole near Terziet on the Dutch-Belgian border in South Limburg. Two broadband seismic sensors were installed: one at a depth of 250 meters and one just below the surface. Both sensors are accessible via the KNMI portal: http://rdsa.knmi.nl/dataportal/. 2 SEISMIC CHARACTERIZATION OF THE EUREGIO MEUSE-RHINE IN VIEW OF EINSTEIN TELESCOPE Executive summary The European 2011 Conceptual Design Report for Einstein Telescope identified the Euregio Meuse-Rhine and in particular the South Limburg border region as one of the prospective sites for this next generation gravitational wave observatory. -
String Theory and Particle Physics
Emilian Dudas CPhT-Ecole Polytechnique String Theory and Particle Physics Outline • Fundamental interactions : why gravity is different • String Theory : from strong interactions to gravity • Brane Universes - constraints : strong gravity versus string effects - virtual graviton exchange • Accelerated unification • Superstrings and field theories in strong coupling • Strings and their role in the LHC era october 27, 2008, Bucuresti 1. Fundamental interactions: why gravity is different There are four fundamental interactions in nature : Interaction Description distances Gravitation Rel: gen: Infinity Electromagn: Maxwell Infinity Strong Y ang − Mills (QCD) 10−15m W eak W einberg − Salam 10−17m With the exception of gravity, all the other interactions are described by QFT of the renormalizable type. Physical observables ! perturbation theory. The point-like interactions in Feynman diagrams gen- erate ultraviolet (UV) divergences Renormalizable theory ! the UV divergences reabsorbed in a finite number of parameters ! variation with en- ergy of couplings, confirmed at LEP. Einstein general relativity is a classical theory . Mass (energy) ! spacetime geometry gµν Its quantization 1 gµν = ηµν + hµν MP leads to a non-renormalizable theory. The coupling of the grav. interaction is E (1) MP ! negligeable quantum corrections at low energies. At high energies E ∼ MP (important quantum corrections) or in strong gravitational fields ! theory of quantum gravity is necessary. 2. String Theory : from strong interac- tions to gravity 1964 : M. Gell-Mann propose the quarks as constituents of hadrons. Ex : meson Quarks are confined in hadrons through interactions which increase with the distance ! the mesons are strings "of color" with quarks at their ends. If we try to separate the mesons into quarks, we pro- duce other mesons 1967-1968 : Veneziano, Nambu, Nielsen,Susskind • The properties of the hadronic interactions are well described by string-string interactions. -
Stochastic Gravitational Wave Backgrounds
Stochastic Gravitational Wave Backgrounds Nelson Christensen1;2 z 1ARTEMIS, Universit´eC^oted'Azur, Observatoire C^oted'Azur, CNRS, 06304 Nice, France 2Physics and Astronomy, Carleton College, Northfield, MN 55057, USA Abstract. A stochastic background of gravitational waves can be created by the superposition of a large number of independent sources. The physical processes occurring at the earliest moments of the universe certainly created a stochastic background that exists, at some level, today. This is analogous to the cosmic microwave background, which is an electromagnetic record of the early universe. The recent observations of gravitational waves by the Advanced LIGO and Advanced Virgo detectors imply that there is also a stochastic background that has been created by binary black hole and binary neutron star mergers over the history of the universe. Whether the stochastic background is observed directly, or upper limits placed on it in specific frequency bands, important astrophysical and cosmological statements about it can be made. This review will summarize the current state of research of the stochastic background, from the sources of these gravitational waves, to the current methods used to observe them. Keywords: stochastic gravitational wave background, cosmology, gravitational waves 1. Introduction Gravitational waves are a prediction of Albert Einstein from 1916 [1,2], a consequence of general relativity [3]. Just as an accelerated electric charge will create electromagnetic waves (light), accelerating mass will create gravitational waves. And almost exactly arXiv:1811.08797v1 [gr-qc] 21 Nov 2018 a century after their prediction, gravitational waves were directly observed [4] for the first time by Advanced LIGO [5, 6]. -
A Scenario for Strong Gravity Without Extra Dimensions
A Scenario for Strong Gravity without Extra Dimensions D. G. Coyne (University of California at Santa Cruz) A different reason for the apparent weakness of the gravitational interaction is advanced, and its consequences for Hawking evaporation of a Schwarzschild black hole are investigated. A simple analytical formulation predicts that evaporating black holes will undergo a type of phase transition resulting in variously long-lived objects of reasonable sizes, with normal thermodynamic properties and inherent duality characteristics. Speculations on the implications for particle physics and for some recently-advanced new paradigms are explored. Section I. Motivation In the quest for grand unification of particle physics and gravitational interactions, the vast difference in the scale of the forces, gravity in particular, has long been a puzzle. In recent years, string theory developments [1] have suggested that the “extra” dimensions of that theory are responsible for the weakness of observed gravity, in a scenario where gravitons are unique in not being confined to a brane upon which the remaining force carriers are constrained to lie. While not a complete theory, such a scenario has interesting ramifications and even a prediction of sorts: if the extra dimensions are large enough, the Planck mass M = will be reduced to c G , G P hc GN h b b being a bulk gravitational constant >> GN. Black hole production at the CERN Large Hadron Collider is then predicted [2], together with the inability to probe high-energy particle physics at still higher energies and smaller distances. Experiments searching for consequences of the extra dimensions have not yet shown evidence for their existence, but have set upper limits on their characteristic sizes [3]. -
A Primer on LIGO and Virgo Gravitational Wave Detectors
A primer on LIGO and Virgo gravitational wave detectors Jo van den Brand, Nikhef and VU University Amsterdam, [email protected] Gravitational Wave Open Data Workshop #2, Paris, April 8, 2019 Interferometric gravitational wave detectors Tiny vibrations in space can now be observed by using the kilometer-scale laser-based interferometers of LIGO and Virgo. This enables an entire new field in science Eleven detections…so far First gravitational wave detection with GW150914 and first binary neutron star GW170817 Event GW150914 Chirp-signal from gravitational waves from two Einsteincoalescing black holes were Telescope observed with the LIGO detectors by the LIGO-Virgo Consortium on September 14, 2015 The next gravitational wave observatory Event GW150914 On September 14th 2015 the gravitational waves generated by a binary black hole merger, located about 1.4 Gly from Earth, crossed the two LIGO detectors displacing their test masses by a small fraction of the radius of a proton Displacement Displacement ( 0.005 0.0025 0.000 Proton radii Proton - 0.0025 - 0.005 ) Proton radius=0.87 fm Measuring intervals must be smaller than 0.01 seconds Laser interferometer detectorsEinstein Telescope The next gravitational wave observatory Laser interferometer detectorsEinstein Telescope The next gravitational wave observatory LIGO Hanford VIRGO KAGRA LIGO Livingston GEO600 Effect of a strong gravitational wave on ITF arm 2Δ퐿 h= = 10−22 퐿 Laser interferometer detectors Michelson interferometer If we would use a single photon and only distinguish between bright and dark fringe, then such an ITF would not be sensitive: −6 휆/2 0.5 ×10 m −10 ℎcrude ≈ = ≈ 10 퐿optical 4000 m Need to do 1012 times better. -
Arxiv:2009.09027V2 [Hep-Th] 26 Jul 2021
Echoes in the Kerr/CFT correspondence Ramit Dey1, ∗ and Niayesh Afshordi2, 3, 4, y 1School of Mathematical and Computational Sciences, Indian Association for the Cultivation of Science, Kolkata-700032, India 2Department of Physics and Astronomy, University of Waterloo, 200 University Ave W, N2L 3G1, Waterloo, Canada 3Waterloo Centre for Astrophysics, University of Waterloo, Waterloo, ON, N2L 3G1, Canada 4Perimeter Institute For Theoretical Physics, 31 Caroline St N, Waterloo, Canada The Kerr/CFT correspondence is a possible route to gain insight into the quantum theory of gravity in the near-horizon region of a Kerr black hole via a dual holographic conformal field the- ory (CFT). Predictions of the black hole entropy, scattering cross-section and the quasi normal modes from the dual holographic CFT corroborate this proposed correspondence. More recently, it has been suggested that quantum gravitational effects in the near-horizon region of a black hole may drastically modify the classical general relativistic description, leading to potential observable consequences. In this paper, we study the absorption cross-section and quasi normal modes of a horizonless Kerr-like exotic compact object (ECO) in the dual CFT picture. Our analysis suggests that the near-horizon quantum modifications of the black hole can be understood as finite size and/or finite N effects in the dual CFT. Signature of the near-horizon modification to a black hole geometry manifests itself as delayed echoes in the ringdown (i.e. the postmerger phase) of a binary black hole coalescence. From our dual CFT analysis we show how the length of the circle, on which the dual CFT lives, must be related to the echo time-delay that depends on the position of the near-horizon quantum structure. -
The Virgo Interferometer
The Virgo Interferometer www.virgo-gw.eu THE VIRGO INTERFEROMETER Located near the city of Pisa in Italy, the Virgo interferometer is the most sensitive gravitational wave detector in Europe. The latest version of the interferometer – the Advanced Virgo – was built in 2012, and has been operational since 2017. Virgo is part of a scientific collaboration of more than 100 institutes from 10 European countries. By detecting and analysing gravitational wave signals, which arise from collisions of black holes or neutron stars millions of lightyears away, Virgo’s goal is to advance our understanding of fundamental physics, astronomy and cosmology. In this exclusive interview, we speak with the spokesperson of the Virgo Collaboration, Dr Jo van den Brand, who discusses Virgo’s achievements, plans for the future, and the fascinating field of gravitational wave astronomy. In February 2016, alongside LIGO, the Virgo Collaboration announced the first direct observation of gravitational waves, made using the Advanced LIGO detectors. Please tell us about the excitement amongst members of Collaboration, and what this discovery meant for Virgo. The discovery of gravitational waves from the merger of two black holes was a great achievement and caused excitement to almost all impassioned scientists. The merger was the most powerful event ever detected and could only be observed with gravitational waves. We showed once and for all that spacetime is a dynamical quantity, and we provided the first direct evidence for CREDIT: EGO/Virgo the existence of black holes. Moreover, we detected the collision and How are observable gravitational The curvature fluctuations are tiny and subsequent coalescence of two black waves generated? cause minor relative length differences. -
Hadron Physics in Holographic QCD
5th DAE-BRNS Workshop on Hadron Physics (Hadron 2011) IOP Publishing Journal of Physics: Conference Series 374 (2012) 012004 doi:10.1088/1742-6596/374/1/012004 Hadron physics in holographic QCD A. B. Santraa, U. Lombardob, A. Bonannoc a Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai 400085, India. b INFN-LNS and University of Catania, 44 Via S.-Sofia, I-95125 Catania, Italy. c INAF- Catania Astrophysical Observatory, Via S.Sofia 78, 95123 Catania, Italy. E-mail: [email protected] Abstract. Hadron physics deals with the study of strongly interacting subatomic particles such as neutrons, protons, pions and others, collectively known as baryons and mesons. Physics of strong interaction is difficult. There are several approaches to understand it. However, in the recent years, an approach called, holographic QCD, based on string theory (or gauge-gravity duality) is becoming popular providing an alternative description of strong interaction physics. In this article, we aim to discuss development of strong interaction physics through QCD and string theory, leading to holographic QCD. 1. Introduction The accepted theory of strong nuclear forces, or strong interactions, is Quantum Chromodynamics (QCD) [1], an Yang-Mills gauge theory with SU(3) gauge group. It can be studied at high energies using perturbation theory with enormous success, but, it is very hard, known to be intractable for the analytical analysis at low energies because of the strong coupling problem. The low energy regime of QCD contains the most interesting phenomena related to hadron physics, thus it is of great theoretical interest. Due to unavailability of suitable analytical tools for understanding QCD in the non-perturbative regime, QCD inspired heuristic models and approximation schemes, ranging from the bag models [2, 3] to chiral perturbation theory [4, 5] have been used to get partial information about the dynamics of QCD in the strongly coupled regime.