Newtonian Noise Mitigation with Tensor Gravitational Wave Detector

Slides:



Advertisements
Similar presentations
Laser Interferometer Gravitational-wave Detectors: Advancing toward a Global Network Stan Whitcomb LIGO/Caltech ICGC, Goa, 18 December 2011 LIGO-G v1.
Advertisements

Design study for 3rd generation interferometers Work Package 1 Site Identification Jo van den Brand
Louis J. Rubbo, Neil J. Cornish, and Olivier Poujade Support for this project was provided by the NASA EPSCoR program.
Paik-1 Inverse-Square Law Experiment in Space: Search for Extra Dimensions Ho Jung Paik, Violeta Prieto, M. Vol Moody University of Maryland and Donald.
Gravitational-waves: Sources and detection
Paik-1 Exploring Gravity with Proof-Mass Technologies Ho Jung Paik University of Maryland July 6-10, 2008, Warrenton, VA.
Gravity Wave Detectors Riccardo DeSalvo - LIGO Gravity waves GW detectors Strain measurement, sensitivity Newtonian Noise How do we throw away your signal.
Nathan Babcock and Robert R. Stewart Department of Earth and Atmospheric Sciences University of Houston.
Gravitational Wave Detection Overview of Why and How
Brennan Ireland Rochester Institute of Technology Astrophysical Sciences and Technology December 5, 2013 LIGO: Laser Interferometer Gravitational-wave.
RF readout scheme to overcome the SQL Feb. 16 th, 2004 Aspen Meeting Kentaro Somiya LIGO-G Z.
Infrasound detector for Apatity group Asming V.E., Kola Regional Seismological Center, Apatity, Russia.
Paik-1 Search for Gravitational Waves Ho Jung Paik University of Maryland and Seoul National University January 12, 2006 Seoul, Korea KIAS-SNU Physics.
1/25 Current results and future scenarios for gravitational wave’s stochastic background G. Cella – INFN sez. Pisa.
LIGO-G Z Gravity gradient studies Firenze, Pisa, Roma and Urbino Francesco Fidecaro, Pisa.
Ambient ground motion and gravity gradient noise Jo van den Brand, Nikhef, Amsterdam on behalf of the design study team Einstein Telescope site selection.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v1.
New Low-Frequency GW Detector with Superconducting Instrumentation
Authors: Sriram Ganapathy, Samuel Thomas, and Hynek Hermansky Temporal envelope compensation for robust phoneme recognition using modulation spectrum.
Advanced interferometers for astronomical observations Lee Samuel Finn Center for Gravitational Wave Physics, Penn State.
1SBPI 16/06/2009 Heterodyne detection with LISA for gravitational waves parameters estimation Nicolas Douillet.
The Analysis of Binary Inspiral Signals in LIGO Data Jun-Qi Guo Sept.25, 2007 Department of Physics and Astronomy The University of Mississippi LIGO Scientific.
Toward a 3rd generation European Gravitational Wave Observatory Dual R&D: presented by Massimo Cerdonio INFN Section and Department of Physics Padova how.
18/04/2004New Windows on the Universe Jan Kuijpers Part 1: Gravitation & relativityPart 1: Gravitation & relativity J.A. Peacock, Cosmological Physics,
Bridging the Gap between Terrestrial Detectors and LISA Elba 2002 May 24, 2002 Seiji Kawamura National Astronomical Observatory of Japan.
Infrasounds and Background Free Oscillations Naoki Kobayashi [1] T. Kusumi and N. Suda [2] [1] Tokyo Tech [2] Hiroshima Univ.
Testing the slow roll inflation paradigm with the Big Bang Observer
State College May 2004 LIGO- Mining for IMBH Gravitational Waves Fabrizio Barone Enrico Campagna Yanbei Chen Giancarlo Cella Riccardo DeSalvo Seiji Kawamura.
DECIGO – Japanese Space Gravitational Wave Detector International Workshop on GPS Meteorology January 17, Tsukuba Center for Institutes Seiji Kawamura*
GWADW - La Biodola 20061/20 Underground reduction of Gravity Gradient Noise. Giancarlo Cella INFN sez. Pisa/Virgo GWADW – La Biodola 2006.
LIGO-G D Upper Limits on the Stochastic Background of Gravitational Waves from LIGO Vuk Mandic Einstein2005 Conference Paris, July
Parity violating gravitational waves Ben Owen May 21, 2009Tests of Case Western Stephon Alexander (  Haverford) Sam Finn Richard O’Shaughnessy.
Seth Timpano Louis Rubbo Neil Cornish Characterizing the Gravitational Wave Background using LISA.
Deci-hertz Interferometer Gravitational Wave Observatory (DECIGO) 7th Gravitational Wave Data Analysis Workshop December 17, International Institute.
Space Gravitational Wave Antenna DECIGO Project 3rd TAMA Symposium February 7, Institute for Cosmic Ray Research, Japan Seiji Kawamura National.
LOGO Gravitational Waves I.S.Jang Introduction Contents ii. Waves in general relativity iii. Gravitational wave detectors.
G. Cella I.N.F.N. Sezione di Pisa.  The mass density fluctuates..... ..... and the gravitational field will do the same Direct gravitational coupling.
Plans on table-top experiments towards Newtonian noise subtraction Frank Brückner, D. Brown, L. Carbone, P. Fulda, A. Freise University of Birmingham GEO-ISC.
NOTA: Per modificare l'immagine su questa diapositiva, selezionarla ed eliminarla. Fare quindi clic sull'icona delle Immagini nel segnaposto per inserire.
ARENA08 Roma June 2008 Francesco Simeone (Francesco Simeone INFN Roma) Beam-forming and matched filter techniques.
Across the Gravitational Wave Spectrum
Ho Jung Paik University of Maryland GW Astronomy, Korea August, 2016
Activities in the Homestake mine
Current and future ground-based gravitational-wave detectors
GW Policy: The Future: G3 Detectors
Gravity Wave Detectors Riccardo DeSalvo - LIGO
Interferometric speed meter as a low-frequency gravitational-wave detector Helge Müller-Ebhardt Max-Planck-Institut für Gravitationsphysik (AEI) and Leibniz.
Asantha Cooray (Caltech) Based on Seto & Cooray, PRL, astro-ph/
8th January 2008 Taitung workshop Sachie Shiomi
Is there a future for LIGO underground?
Coherent wide parameter space searches for gravitational waves from neutron stars using LIGO S2 data Xavier Siemens, for the LIGO Scientific Collaboration.
Speculations about Newtonian-Noise Filtering
(Superconducting Omni-directional Gravitational Radiation Observatory)
Local gravity gradient noise
Stochastic Background
Ho Jung Paik University of Maryland GW Astronomy, Korea August, 2016
Advanced LIGO Quantum noise everywhere
Instrument Considerations
Gravity gradient studies
Newtonian Noise Mitigation by Using Superconducting Gravity Gradiometers Ho Jung Paik Department of Physics University of Maryland ICGAC-XIII, Seoul.
LIGO, ground-based Gravitational Wave Detectors
Stochastic gravitational wave and its spectral property
Structural analysis of the SOGRO platform
The Laser Interferometer Gravitational-wave Observatory
Shintaro Nakamura (Tokyo University of Science)
K.Somiya Detection of blackhole ringdown signals
Ho Jung Paik University of Maryland E-GRAAL January 10, 2018
WG2 Machine learning for low frequency seismology
Upper limits on gravitational wave bursts
Fig. 1 Comparison of earthquake detection methods in terms of three qualitative metrics: Detection sensitivity, general applicability, and computational.
Presentation transcript:

Newtonian Noise Mitigation with Tensor Gravitational Wave Detector Ho Jung Paik Department of Physics, University of Maryland 8th Japan-Korea Joint Workshop June 27, 2015

Superconducting tensor gravitational wave detector (Superconducting Omni-directional Gravitational Radiation Observatory) SOGRO Rayleigh NN must be mitigated by 102 at 0.1 Hz for SOGRO 1 Infrasound NN must be mitigated by 103 at 0.1 Hz for SOGRO 1. Paik

Newtonian gravity noise Seismic and atmospheric density modulations cause Newtonian gravity gradient noise. At 0.1 Hz, s ~ 35 km >> L.  Gravity gradient noise  L.  Detecting and removing the gravity gradient noise appears to be very challenging. GWs are transverse and cannot have longitudinal components whereas the Newtonian gradient does.  GW could be distinguished from near-field gradients, if all the tensor components are detected. Paik

NN due to Rayleigh waves Metric perturbation tensor in the source frame: Paik

Removal of Rayleigh NN az() is measured by the vertical CM channel. With tensor (SNR 103) + vertical CM (SNR 106) + 7 seism (5 km, SNR 103) With tensor + vertical CM (0 noise) Paik

Removal of infrasound NN Infrasound waves come from half space with an additional unknown: polar angle of incidence  . Microphones are required to measure the air density fluctuations. With tensor + 15 mikes (0, 0.6, 1 km, SNR 104) Harms and Paik, PRD (2015) Satisfies SOGRO 1 requirement Is there any way that we can mitigate NN by using the tensor channels alone? Paik

NN mitigation by correlation? Rayleigh and infrasound waves incident in different angles are uncorrelated with each other and with the GW signal. This allows us to determine autocorrelations of h+() and h() by combining correlations of various tensor outputs. Fourier transform of autocorrelation is power spectral density. Problem: It takes a long time to mitigate the NN by using correlation method. Paik

Could SOGRO help advanced detectors mitigate NN? (HW from R. Weiss) Newtonian noise Worthy mitigation goal Worthy mitigation goal: A factor of ~10 to 10-23 Hz-1/2 at 10 Hz and 10-21 Hz-1/2 at 1 Hz. Paik

KAGRA sensitivity curve The low-frequency noise of KAGRA could benefit from a similar NN rejection. Paik

Sensitivities to GW and NN At 1-10 Hz, cR = 250 m/s (surface), 3.5 km/s (deep underground).  NN is uncorrelated between detector test masses. Paik

Incomplete correlation of NN Mitigation factor S is given by the correlation CSN between the detector and the NN sensor: Beker et al., GRG 43, 623 (2011) It is much more challenging to mitigate the NN of ground detectors. Paik

Mini-SOGRO with 5-m arm length L = 5 m, M = 1 t, T = 0.1 K, Q = 109, n = 2, fD = 1 Hz Mini-SOGRO with L = 5 m, M = 1 ton, T = 0.1 K could mitigate the NN at 1-10 Hz by a factor  5.  NN mitigation appears very challenging but not impossible. Paik