MICROSCOPE
Transcription
MICROSCOPE
MICROSCOPE and the Equivalence Principle / MICROSCOPE et le principe d’équivalence Joel Bergé (ONERA) For the Microscope team 1 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 MICROSCOPE Micro-satellite à traînée compensée pour l’Observation du Principe d’Equivalence Drag-free microsatellite for the observation of the Equivalence Principle CNES mission to test Equivalence Principle with 10-15 precision / Mission du CNES pour mesurer le Principe d’Equivalence avec une précision de 10-15 PI: Pierre Touboul (ONERA) Co-PI: Gilles Métris (Observatoire de la Côte d’Azur) Partners: ESA, ZARM, PTB, DLR 2 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 Weak Equivalence Principle: the universality of free fall Galileo observed that all bodies fall at the same rate: the traveled distance is proportional to the time of fall => x ~ t2 This means that their acceleration is constant and the same for all bodies: a = g (g = 10 m/s2 on Earth) All test bodies follow the same universal trajectory in a gravitational field, independently of their mass, detailed internal structure and composition. Newton’s laws: F = mi a, Fg = mg g F = Fg => mi = mg mi = inertial mass: “opposes” changes in motion (universal) mg = gravitational mass: feels gravity (specific to the gravitational force) mg/mi = “gravitational charge” For all test bodies, the inertial mass and the gravitational mass are equal: mi = mg Precision measured in terms of the Eötvös ratio 3 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 Equivalence Principle and General Relativity Universality of gravitation: locally, an observer cannot tell if he/she is at rest in a gravity field or in an accelerated frame far from any gravitational field source; gravity is inescapable Weak Equivalence Principle The motion of freely-falling particles are the same in a gravitational field and a uniformly accelerated frame, in small enough regions of spacetime. As mass is a form of energy (E=mc2), Einstein generalized the WEP to a principle encompassing other interactions: Einstein Equivalence Principle “In small enough regions of spacetime, the (nongravitational) laws of physics reduce to those of special relativity; it is impossible to detect the existence of a gravitational field by means of local experiments.” 4 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 Equivalence Principle and General Relativity Direct consequence of the EEP: we cannot define the acceleration due to gravity, but instead define “unaccelerated” as “freely falling” In other words: gravity is not a force; “zero acceleration” = “moving freely in the presence of whatever gravitational field happens to be around” Very profound implication: it is not possible to define inertial frames, but only locally inertial frames Gravity = Curvature Other direct implications (with no need of full GR): gravitational redshift and time dilation + Implications of GR: perihelion precession of Mercury, gravitational lensing, gravitational waves 5 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 The Equivalence Principle Weak Equivalence Principle The motion of freely-falling particles are the same in a gravitational field and a uniformly accelerated frame, in small enough regions of spacetime. Einstein Equivalence Principle In small enough regions of spacetime, the (nongravitational) laws of physics reduce to those of special relativity; it is impossible to detect the existence of a gravitational field by means of local experiments. Strong Equivalence Principle In small enough regions of spacetime, all laws of physics reduce to those of special relativity; it is impossible to detect the existence of a gravitational field by means of local experiments. 6 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 Should we doubt the Equivalence Principle? • Towards a “Theory of Everything” General Relativity: gravity, large scale, low energy Quantum Physics: electroweak / nuclear forces, small scale, high energy => how to unify them? • Dark energy / Cosmological constant The expansion of the Universe is accelerating => concordance problem • Solutions to those problem string theory, quantum gravity, modified gravity => all predict a weak violation of the WEP • Underlying question: is General Relativity the right theory of gravitation on all scales? 7 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 WEP tests up to now Will 2006 Wagner+ 2012 Eötvös, Eöt-Wash Torsion balance Lunar Laser Range Williams+ 1996 Probes fall of Earth and Moon towards the Sun 8 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 The near future, what to expect? Will 2006 Wagner+ 2012 Eötvös, Eöt-Wash Torsion balance Lunar Laser Range Williams+ 1996 Probes fall of Earth and Moon towards the Sun Expected violations (string theory, new scalar fields...) Microscope 10-15 20 9 16 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 MICROSCOPE measurement principle Aim: test mi = mg at the 10-15 level 10-15: difference of weight of a 500,000 ton-tanker with or without a 0.5 mg drosophilia on board Differential electrostatic accelerometer: 2 coaxial cylindrical inertial sensors Sensors forced to follow the same orbit (permanent pico-meter control) => we measure the electrostatic forces needed to keep the sensors centered. Signal measured along an ultra-sensitive axis. Drag-free control on 6 degrees-of-freedom to achieve highest possible stability 10 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 MICROSCOPE measurement principle Signal: gravity field modulated by satellite’s motion around the Earth => sine of known frequency fEP fEP can be varied by either: - Keeping the satellite in inertial motion - Or spinning it How to extract the signal? Easy! We must look for a noise-dominated sine in measured time series. . . . Time domain Frequency domain Equivalence Principle Violation (3x10-15) Baghi+ in prep 11 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 MICROSCOPE instrument: T-SAGE (Twin Space Accelerometer for Gravitation Experiment) 2 differential accelerometers • SUREF: reference, test masses of the same material (Pt/Rh) • SUEP: used for Equivalence Principal test, test masses of different materials (Pt/Rh, Ti) 12 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 Integration in the satellite © CNES/Emmanuel GRIMAULT, 2015 13 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 MICROSCOPE satellite © CNES/Emmanuel GRIMAULT, 2015 14 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 MICROSCOPE: Ready for the launch and the space experiment • • • • • Shipped next week to Kourou Launch scheduled April 22, 2016 from the Kourou spaceport, on a Soyuz rocket Commissioning phase until August 2016 First science measurements in September 2016 Mission will last 2 years • Main goal - Perform the most precise test of the Weak Equivalence Principle ever (10-15), and the first one in space • Additional goals - 15 Specific search for new physics Geodesy Very high atmosphere physics Demonstrate that the 6 degree-of-freedom drag-free technology is ready (complement to LISA Pathfinder) Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16 To know more about MICROSCOPE On the web • http://microscope.onera.fr • https://microscope.cnes.fr 16 Joel Bergé, Gravitational Waves Fiesta, March 1st, 2016 Tuesday, March 8, 16