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MIGA : Mater-wave laser Interferometry Gravita7on Antenna

MIGA : Mater-wave laser Interferometry Gravita7on Antenna

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BOUYER - PQE 2011 - 01/03/11<br />

!"#$%&%!'()*+,'-)%.'/)*%<br />

"01)*2)*34)1*5%#*'-61'730%$01)00'%<br />

P. Bouyer<br />

Laboratoire Photonique, Numérique et Nanoscience, Bordeaux, France<br />

on the behalf of the <strong>MIGA</strong> Study team


Design study proposal : France – Germany – Italy – UK – USA<br />

Underground Infrastructure for<br />

geophysics and fundamental<br />

studies<br />

An array of atom interferometers<br />

allowing for correlated gravity<br />

measurements at different<br />

positions :<br />

- Geophysics studies – resolutions<br />

better than 10 -11 g, drifts below<br />

10 -10 g/yr.<br />

- Fundamental physics – strain<br />

measurements below 10 -15 at low<br />

frequency.<br />

BOUYER - PQE 2011 - 01/03/11<br />

15 ins'tutes<br />

External scien'fic comitee<br />

Hans BACHOR Australia<br />

Christian BORDÉ France<br />

John CLOSE Australia<br />

Eugenio COCCIA University of Rome "Tor Vergata"<br />

Michel DIAMENT IPG Paris<br />

Federico FERRINI EGO<br />

Malcolm JOHNSTON USGS, USA<br />

William H LEE USGS, USA<br />

Harald LUECK Hannover<br />

Vuk MANDIC University of minesota, USA.<br />

Marie-Christine ANGONIN<br />

Andrea BERTOLDI<br />

Kai BONGS<br />

Frédérick BOUDIN<br />

Philippe BOUYER<br />

Daniel BOYER<br />

Alain BRILLET<br />

Alain CAVAILLOU<br />

Walid CHAIBI<br />

Cédric CHAMPOLLION<br />

Jean CHERY<br />

Pacôme DELVA<br />

Wolfgang ERTMER<br />

Marco FATTORI<br />

Christian FREIER<br />

Stéphane GAFFET<br />

Gianluca GUIDI<br />

Matthias HAUTH<br />

Mark KASEVICH<br />

Brahim LAMINE<br />

Arnaud LANDRAGIN<br />

Nary MAN<br />

Jörg NEUMANN<br />

Franck PEREIRA DOS SANTOS<br />

Achim PETERS<br />

Nicola POLI<br />

Ernst M. RASEL<br />

Serge REYNAUD<br />

Giorgio SANTARELLI<br />

Wolfgang P. SCHEICH<br />

Fiodor SORRENTINO<br />

Guglielmo M. TINO<br />

Flavio VETRANO<br />

Andrea VICERE<br />

Peter WEßELS<br />

Andreas WICHT


Interference fringes : Nat~cos(2πaT 2 ∕λ+Φ)<br />

BOUYER - PQE 2011 - 01/03/11<br />

Long term stability<br />

< 4 10 -10 g<br />

Landragin et al.<br />

Observatoire Paris<br />

arXiv:1008.2884v2<br />

Peters et al.<br />

Berlin gravimeter


BOUYER - PQE 2011 - 01/03/11


Mirror<br />

BOUYER - PQE 2011 - 01/03/11


Mirror<br />

BOUYER - PQE 2011 - 01/03/11


Mirror<br />

BOUYER - PQE 2011 - 01/03/11


BOUYER - PQE 2011 - 01/03/11


BOUYER - PQE 2011 - 01/03/11<br />

Geiger et al., I.C.E.<br />

project, in preparation<br />

Correlated measurements allows to<br />

extend accuracy to low frequency<br />

thanks to atoms


<strong>MIGA</strong> : can we use atoms to extend GW detector sensiEvity to low frequency<br />

BOUYER - PQE 2011 - 01/03/11


<strong>MIGA</strong> : can we use atoms to extend GW detector sensiEvity to low frequency<br />

BOUYER - PQE 2011 - 01/03/11


<strong>MIGA</strong> : can we use atoms to extend GW detector sensiEvity to low frequency<br />

BOUYER - PQE 2011 - 01/03/11<br />

L = 1+h.sin(Ω t)<br />

Cavity length detection : x ~ h.sin(Ω t)


<strong>MIGA</strong> : can we use atoms to extend GW detector sensiEvity to low frequency<br />

BOUYER - PQE 2011 - 01/03/11<br />

L = 1+h.sin(Ω t)<br />

Cavity length detection : x ~ h.sin(Ω t)<br />

<strong>MIGA</strong>-study: current state-of development technology for<br />

compact sensors<br />

.3 second interrogation time, L = 100 m, 4 recoil light<br />

pulse splitter, atomic shot noise limited phase shift<br />

sensitivity of 100 μrad<br />

<strong>MIGA</strong>: shortterm enhanced design performances<br />

.5 second interrogation time, L=1 km, 100 recoil.<br />

<strong>MIGA</strong>-GW: ambitious design performance<br />

3 second interrogation time, L=10 km, 1000 recoil, 1<br />

μrad atomic phase shift sensitivity<br />

S. Dimopoulos, et al. Phys. Rev. D 78, 122002 (2008)<br />

Atom acceleration detection : a ~ h.L.Ω 2 sin(Ω t)


Free falling atom sensors<br />

B. Canuel, et al. Phys. Rev.<br />

Lett. 97, 010402, (2006). Paris<br />

T. Muller et al., EPJD 53, 273<br />

(2009). hannover<br />

BOUYER - PQE 2011 - 01/03/11<br />

For .5 seconds, launch veloci'es of 3 m/s and single<br />

atom interferometer beam size of 50 cm diameter.<br />

Need full analysis of influence of op'cal aberra'ons<br />

J. Fils et al., “Influence of optical aberrations in an atomic<br />

gyroscope”, Euro. phys. J. D. 36, 257 (2005)<br />

J. Hogan et al, arxiv :1009.2702


Free falling atom sensors<br />

B. Canuel, et al. Phys. Rev.<br />

Lett. 97, 010402, (2006). Paris<br />

T. Muller et al., EPJD 53, 273<br />

(2009). hannover<br />

BOUYER - PQE 2011 - 01/03/11<br />

For .5 seconds, launch veloci'es of 3 m/s and single<br />

atom interferometer beam size of 50 cm diameter.<br />

Need full analysis of influence of op'cal aberra'ons<br />

J. Fils et al., “Influence of optical aberrations in an atomic<br />

gyroscope”, Euro. phys. J. D. 36, 257 (2005)<br />

J. Hogan et al, arxiv :1009.2702<br />

Possibility to use levita'on techniques in the future<br />

Bloch oscillation (Tino et al.)<br />

Trampoline techniques (F. Impens, et al.,<br />

Applied Physics B, 84, 603-615, (2006)


ImplementaEon of <strong>MIGA</strong> in the underground laboratory in Rustrel, France<br />

BOUYER - PQE 2011 - 01/03/11<br />

Two horizontal galleries with 1<br />

km!"#$%&%!'()*+,'-)%.'/)*% length, (almost)<br />

orthogonal<br />

"01)*2)*34)1*5%#*'-61'730%$01)00'%<br />

Possibility of third ver'cal<br />

gallery<br />

<strong>MIGA</strong> arms could be<br />

«connected» via ultra-­‐high<br />

stability <strong>laser</strong> link


BOUYER - PQE 2011 - 01/03/11<br />

Two horizontal galleries with 1<br />

km!"#$%&%!'()*+,'-)%.'/)*% length, (almost)<br />

orthogonal<br />

"01)*2)*34)1*5%#*'-61'730%$01)00'%<br />

Possibility of third ver'cal<br />

gallery<br />

<strong>MIGA</strong> arms could be<br />

«connected» via ultra-­‐high<br />

stability <strong>laser</strong> link


BOUYER - PQE 2011 - 01/03/11<br />

Possibility of «mul'-­‐sensor» antenna to monitor, gradients,<br />

curvature ...<br />

Geophysics applica'ons, monitoring ...<br />

Two horizontal galleries with 1<br />

km!"#$%&%!'()*+,'-)%.'/)*% length, (almost)<br />

orthogonal<br />

"01)*2)*34)1*5%#*'-61'730%$01)00'%<br />

Possibility of third ver'cal<br />

gallery<br />

<strong>MIGA</strong> arms could be<br />

«connected» via ultra-­‐high<br />

stability <strong>laser</strong> link


!"#$%&%!'()*+,'-)%.'/)*%<br />

"01)*2)*34)1*5%#*'-61'730%$01)00'%<br />

FP7-Infrastructure design study proposal to build a new type of antenna.<br />

There is hope that <strong>MIGA</strong> can close one of the sensitivity windows in regard to<br />

gravitational spectrum and by offering a new technique also address the riddle<br />

of gravitational <strong>wave</strong>s. If <strong>MIGA</strong> succeed, it will complement already existing<br />

antennas.<br />

Beyond the study of gravitational <strong>wave</strong>s, there is promise to advance<br />

significantly the understanding of the Earth seismology, due in essence to<br />

availibility of greatly improved sensitivity to seismic <strong>wave</strong>s, this may lead to<br />

advance warning about timing of great earth quakes by detecting and<br />

learning more about probable weak precursors.<br />

BOUYER - PQE 2011 - 01/03/11

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