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Comparison of atom and photon interferometers using 5D optics Comparison of atom and photon interferometers using 5D optics Christian J. Bordé Académie des Sciences FLORENCE 2009
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π/2 Pulses Atoms a b space time cτcτ Total phase=Action integral+End splitting+Beam splitters Laser beams
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Total phase=Action integral+End splitting+Beam splitters Atoms BORDÉ-CHU INTERFEROMETER π/2 π
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BORDÉ-RAMSEY INTERFEROMETERS
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Multiple wave interferometer
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FROM 3 TO 4 SPATIAL DIMENSIONS
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E(p) p // a b Mac2Mac2 Mbc2Mbc2
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p Mc E
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x S =c t
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OPTICAL PATH & FERMAT’S PRINCIPLE IN (4+1)D
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E(p) p BASICS OF ATOM /PHOTON OPTICS Parabolic approximation of slowly varying phase and amplitude
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Schroedinger-like equation for the atom /photon field: BASICS OF ATOM /PHOTON OPTICS
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ABCD LAW OF ATOM/PHOTON OPTICS
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Ehrenfest theorem + Hamilton equations
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GENERAL FORMULA FOR THE PHASE SHIFT OF AN ATOM/PHOTON INTERFEROMETER
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Exact phase shift for the atom gravimeter which can be written to first-order in with T=T’ Reference: Ch. J. B., Theoretical tools for atom optics and interferometry, C.R. Acad. Sci. Paris, 2, Série IV, p. 509-530, 2001
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ARBITRARY 3D TIME-DEPENDENT GRAVITO-INERTIAL FIELDS Example: Phase shift induced by a gravitational wave
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Atomic phase shift induced by a gravitational wave Ch.J. Bordé, Gen. Rel. Grav. 36 (March 2004) Ch.J. Bordé, J. Sharma, Ph. Tourrenc and Th. Damour, Theoretical approaches to laser spectroscopy in the presence of gravitational fields, J. Physique Lettres 44 (1983) L983-990
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Bordé-Ramsey interferometers Laser beams Atom beam
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