G. Auger
Paris Diderot University
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Featured researches published by G. Auger.
Classical and Quantum Gravity | 2011
F. Antonucci; M. Armano; H. Audley; G. Auger; M. Benedetti; P. Binetruy; C. Boatella; J. Bogenstahl; D. Bortoluzzi; Paolo Bosetti; M. Caleno; A. Cavalleri; M. Cesa; M. Chmeissani; G. Ciani; A. Conchillo; Giuseppe Congedo; I. Cristofolini; M. Cruise; Karsten Danzmann; F. De Marchi; M. Diaz-Aguilo; I. Diepholz; G. Dixon; R. Dolesi; N. Dunbar; J. Fauste; L. Ferraioli; D. Fertin; Walter Fichter
LISA Pathfinder, the second of the European Space Agencys Small Missions for Advanced Research in Technology (SMART), is a dedicated technology demonstrator for the joint ESA/NASA Laser Interferometer Space Antenna (LISA) mission. The technologies required for LISA are many and extremely challenging. This coupled with the fact that some flight hardware cannot be fully tested on ground due to Earth-induced noise led to the implementation of the LISA Pathfinder mission to test the critical LISA technologies in a flight environment. LISA Pathfinder essentially mimics one arm of the LISA constellation by shrinking the 5 million kilometre armlength down to a few tens of centimetres, giving up the sensitivity to gravitational waves, but keeping the measurement technology: the distance between the two test masses is measured using a laser interferometric technique similar to one aspect of the LISA interferometry system. The scientific objective of the LISA Pathfinder mission consists then of the first in-flight test of low frequency gravitational wave detection metrology. LISA Pathfinder is due to be launched in 2013 on-board a dedicated small launch vehicle (VEGA). After a series of apogee raising manoeuvres using an expendable propulsion module, LISA Pathfinder will enter a transfer orbit towards the first Sun?Earth Lagrange point (L1). After separation from the propulsion module, the LPF spacecraft will be stabilized using the micro-Newton thrusters, entering a 500?000 km by 800?000 km Lissajous orbit around L1. Science results will be available approximately 2 months after launch.
Classical and Quantum Gravity | 2012
F. Antonucci; M. Armano; H. Audley; G. Auger; M. Benedetti; P. Binetruy; J. Bogenstahl; D. Bortoluzzi; Paolo Bosetti; N. Brandt; M. Caleno; Priscilla Canizares; A. Cavalleri; M. Cesa; M. Chmeissani; A. Conchillo; Giuseppe Congedo; I. Cristofolini; M. Cruise; Karsten Danzmann; F. De Marchi; M. Diaz-Aguilo; I. Diepholz; G. Dixon; R. Dolesi; N. Dunbar; J. Fauste; L. Ferraioli; V. Ferrone; Walter Fichter
In this paper, we describe the current status of the LISA Pathfinder mission, a precursor mission aimed at demonstrating key technologies for future space-based gravitational wave detectors, like LISA. Since much of the flight hardware has already been constructed and tested, we will show that performance measurements and analysis of these flight components lead to an expected performance of the LISA Pathfinder which is a significant improvement over the mission requirements, and which actually reaches the LISA requirements over the entire LISA Pathfinder measurement band.
Classical and Quantum Gravity | 2011
F. Antonucci; M. Armano; H. Audley; G. Auger; M. Benedetti; P. Binetruy; C. Boatella; J. Bogenstahl; D. Bortoluzzi; Paolo Bosetti; M. Caleno; A. Cavalleri; M. Cesa; M. Chmeissani; G. Ciani; A. Conchillo; Giuseppe Congedo; I. Cristofolini; M. Cruise; Karsten Danzmann; F. De Marchi; M. Diaz-Aguilo; I. Diepholz; G. Dixon; R. Dolesi; J. Fauste; L. Ferraioli; D. Fertin; Walter Fichter; E. Fitzsimons
As the launch of LISA Pathfinder (LPF) draws near, more and more effort is being put in to the preparation of the data analysis activities that will be carried out during the mission operations. The operations phase of the mission will be composed of a series of experiments that will be carried out on the satellite. These experiments will be directed and analysed by the data analysis team, which is part of the operations team. The operations phase will last about 90 days, during which time the data analysis team aims to fully characterize the LPF, and in particular, its core instrument the LISA Technology Package. By analysing the various couplings present in the system, the different noise sources that will disturb the system, and through the identification of the key physical parameters of the system, a detailed noise budget of the instrument will be constructed that will allow the performance of the different subsystems to be assessed and projected towards LISA. This paper describes the various aspects of the full data analysis chain that are needed to successfully characterize the LPF and build up the noise budget during mission operations.
Physical Review Letters | 2017
M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N. Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Karsten Danzmann; M. de Deus Silva; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; Ewan Fitzsimons; R. Flatscher; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L. Gesa; F. Gibert; Domenico Giardini; R. Giusteri
We report on electrostatic measurements made on board the European Space Agency mission LISA Pathfinder. Detailed measurements of the charge-induced electrostatic forces exerted on free-falling test masses (TMs) inside the capacitive gravitational reference sensor are the first made in a relevant environment for a space-based gravitational wave detector. Employing a combination of charge control and electric-field compensation, we show that the level of charge-induced acceleration noise on a single TM can be maintained at a level close to 1.0u2009u2009fmu2009s^{-2}u2009Hz^{-1/2} across the 0.1-100xa0mHz frequency band that is crucial to an observatory such as the Laser Interferometer Space Antenna (LISA). Using dedicated measurements that detect these effects in the differential acceleration between the two test masses, we resolve the stochastic nature of the TM charge buildup due to interplanetary cosmic rays and the TM charge-to-force coupling through stray electric fields in the sensor. All our measurements are in good agreement with predictions based on a relatively simple electrostatic model of the LISA Pathfinder instrument.
Classical and Quantum Gravity | 2016
M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N. Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Karsten Danzmann; M. de Deus Silva; D. Desiderio; E Piersanti; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; E. Fitzsimons; R. Flatscher; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L. Gesa; F. Gibert
LISA Pathfinder satellite has been launched on 3th December 2015 toward the Sun-Earth first Lagrangian point (L1) where the LISA Technology Package (LTP), which is the main science payload, will be tested. With its cutting-edge technology, the LTP will provide the ability to achieve unprecedented geodesic motion residual acceleration measurements down to the order of
Journal of Physics: Conference Series | 2015
M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N. Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Karsten Danzmann; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; E. Fitzsimons; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L. Gesa; F. Gibert; Domenico Giardini; R. Giusteri; C. Grimani; I. Harrison
3 times 10^{-14},mathrm{m/s^2/{Hz^{1/2}}}
Journal of Physics: Conference Series | 2015
M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N. Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Karsten Danzmann; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; E. Fitzsimons; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L. Gesa; F. Gibert; Domenico Giardini; R. Giusteri; C. Grimani; I. Harrison
within the
arXiv: General Relativity and Quantum Cosmology | 2015
M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Curt Cutler; Karsten Danzmann; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; E. Fitzsimons; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L. Gesa; F. Gibert; Domenico Giardini; R. Giusteri; C. Grimani
1-30,mathrm{mHz}
Journal of Physics: Conference Series | 2015
F. Gibert; M. Nofrarias; M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N. Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Karsten Danzmann; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; E. Fitzsimons; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L Gesa; Domenico Giardini; R. Giusteri; C. Grimani
frequency band. The presence of the spacecraft itself is responsible of the local gravitational field which will interact with the two proof test-masses. Potentially, such a force interaction might prevent to achieve the targeted free-fall level originating a significant source of noise. We balanced this gravitational force with sub
Journal of Physics: Conference Series | 2015
M. Armano; H. Audley; G. Auger; J. Baird; P. Binetruy; M. Born; D. Bortoluzzi; N. Brandt; A. Bursi; M. Caleno; A. Cavalleri; A. Cesarini; M. Cruise; Karsten Danzmann; I. Diepholz; R. Dolesi; N. Dunbar; L. Ferraioli; V. Ferroni; E. Fitzsimons; M. Freschi; J. Gallegos; C. García Marirrodriga; R. Gerndt; L. Gesa; F. Gibert; Domenico Giardini; R. Giusteri; C. Grimani; I. Harrison
mathrm{nm/s^2}