Cold Atom Interferometry

US2017372808A1 · US · A1

Patent metadata
FieldValue
Publication numberUS-2017372808-A1
Application numberUS-201715685330-A
CountryUS
Kind codeA1
Filing dateAug 24, 2017
Priority dateJun 22, 2016
Publication dateDec 28, 2017
Grant date

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Abstract

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Improvements to atom interferometers. An improved atom interferometer has a single polarization-preserving fiber, coupled for propagation of beams of two Raman frequencies, and a parallel displacement beamsplitter for separating the laser beams into respective free-space-propagating parallel beams traversing at least one ensemble of atoms. A reflector generates one or more beams counterpropagating through the ensemble of atoms. Other improvements include interposing a beam-splitting surface common to a plurality of parallel pairs of beams counterpropagating through the ensemble of atoms, generating interference fringes between reflections of the beams to generate a detector signal; and processing the detector signal to derive at least one of relative phase and relative alignment between respective pairs of the counterpropagating beams.

First claim

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We claim: 1 . An improvement to measurement methods that have steps of trapping an ensemble of atoms and measuring interference fringes between populations of internal states of a quantum system based on interaction of the ensemble of atoms with a plurality of counterpropagating optical beam pairs, the improvement comprising: a. coupling the plurality of counterpropagating beam pairs such that each pair of beams traverses the ensemble of atoms in parallel counterpropagating beam paths; b. interposing a beam-splitting surface common to the plurality of counterpropagating beam pairs; c. generating interference fringes between reflections of the plurality of parallel pairs of counterpropagating beams to generate a detector signal; and d. processing the detector signal to derive at least one of relative phase and relative alignment between respective pairs of the counterpropagating beams. 2 . An improvement in accordance with claim 1 , wherein processing the detector signal includes inferring relative alignment of the parallel pairs of counterpropagating beams from a depth of the interference fringes. 3 . An improvement in accordance with claim 1 , wherein processing the detector signal includes measuring phase shear across the plurality of parallel pairs of counterpropagating beams. 4 . An improvement in accordance with claim 1 , wherein detecting the interference fringes includes spatially resolving the interference fringes using a detector array. 5 . An improvement in accordance with claim 1 , further comprising feeding back the at least one of relative phase and relative alignment between respective pairs of the counterpropagating beams to an optical element for stabilizing the at least one of relative phase and relative alignment between respective pairs of the counterpropagating beams. 6 . An atom interferometer comprising: a. an ensemble of atoms successively launched between a pair of magneto-optical traps; b. a plurality of pairs of counterpropagating laser beams traversing the ensemble of atoms for probing quantum states characterizing the atoms; and c. a beam-splitting surface common to the plurality of counterpropagating beam pairs, configured to reflect a portion of each of plurality of counterpropagating beam pair; d. a reflector for redirecting one of each pair of counterpropagating laser beams to form an interference pattern with the other of each pair of counterpropagating laser beams; and e. a detector configured to detect the interference pattern and generate a detector signal; and f. a processor for receiving the detector signal and deriving a measure of at least of relative phase and relative spatial alignment of each pair of counterpropagating laser beams. 7 . An improvement to an atom interferometer having at least one distinct ensemble of atoms, the improvement comprising: a. a single polarization-preserving fiber coupled for propagation of a first laser beam characterized by a first Raman frequency and a second laser beam characterized by a second Raman frequency distinct from the first Raman frequency, from at least one source of the first and second laser beams; and b. a first parallel displacement beamsplitter for separating the first laser beam and the second laser beam coupled out of the polarization-preserving fiber into respective free-space-propagating parallel beams each respective free-space-propagating parallel beam traversing the at least one distinct ensemble of atoms. 8 . The improvement in accordance with claim 8 , further comprising a reflector for turning the second laser beam into a direction antiparallel to the first laser beam. 9 . The improvement in accordance with claim 8 , further comprising a second parallel displacement beamsplitter for creating a plurality of counterpropagating laser beam pairs. 10 . The improvement in accordance with claim 8 , wherein the reflector is a corner cube reflector. 11 . An atom interferometer comprising: a. an ensemble of atoms successively launched between a pair of magneto-optical traps; b. a first plurality of laser beams, all characterized by a first Raman frequency, traversing the ensemble of atoms in a first set of parallel directions for probing quantum states characterizing the ensemble of atoms; c. a second plurality of laser beams, all characterized by a second Raman frequency, traversing the ensemble of atoms in a second set of parallel directions substantially counterpropagating with respect to the first set of parallel directions; d. a first fiber collimator for coupling the first laser beam from optical fiber to free-space propagation substantially parallel to a baseplate; e. a first parallel displacement beam splitter for splitting the first laser beam into a plurality of parallel beam paths; f. a second fiber collimator for coupling the second laser beam from optical fiber to free-space propagation substantially parallel to the baseplate; g. a beam-turning optic for steering the second laser beam in a path substantially parallel to the baseplate and substantially parallel to the plurality of parallel beam paths traversed by the first laser beam; h. a reflector for turning the second laser beam into a direction substantially antiparallel to the plurality of parallel beam paths traversed by the first laser beam; and i. a second parallel displacement beam splitter for splitting the second laser beam into a plurality of parallel beam paths each counterpropagating on the plurality of parallel beam paths traversed by the first laser beam. 13 . An atomic interferometer in accordance with claim 12 , wherein the reflector is a corner cube reflector. 14 . An improvement to an atom interferometer having a first and a second magneto-optical trap (MOT) displaced with respect to each other by an inter-trap distance bisected by a center displaced from either MOT by a “center-to-trap distance,” with substantially orthogonal blue-detuned cooling beams traversing a first MOT in directions substantially opposing directions in which another pair of substantially orthogonal blue-detuned cooling beams traverse a second MOT, and substantially orthogonal red-detuned cooling beams traversing the first MOT in directions substantially opposing directions in which another pair of substantially orthogonal red-detuned cooling beams traverse the second MOT, wherein the improvement comprises: a. a first fiber collimator for coupling a first laser beam from optical fiber to free-space propagation in a first laser direction substantially parallel to a baseplate and displaced from the center by the center-to-trap distance; b. a second fiber collimator for coupling a second laser beam from optical fiber to free-space propagation substantially parallel to the baseplate, substantially orthogonal to the first laser direction, and also displaced from the center by the center-to-trap distance; c. a first pentaprism, disposed entirely within a sphere of radius no greater than three times the inter-trap distance about the center, for splitting the first laser beam into two orthogonal cooling beams; and d. a second pentaprism, disposed entirely within the sphere of radius no greater than three times the inter-trap distance about the center, for splitting the second laser beam into two orthogonal cooling beams. 15 . An atom interferometer in accordance with claim 14 , in which the improvement further comprises: e. a third pentaprism, disposed entirely within the sphere of radius no greater than three times the inter-trap distance about the center, for further splitting the first laser beam into two orthogonal cooling beams; and

Assignees

Inventors

Classifications

  • G21K1/30Primary

    for confining neutral particles or handling confined neutral particles, e.g. atom traps · CPC title

  • characterised by the beam path configuration · CPC title

  • using surface reflection, e.g. grazing incidence mirrors, gratings (multilayer mirrors G21K1/062) · CPC title

  • using multiple collimators, e.g. Bucky screens; other devices for eliminating undesired or dispersed radiation · CPC title

  • G21K1/006Primary

    Physics · mapped topic

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What does patent US2017372808A1 cover?
Improvements to atom interferometers. An improved atom interferometer has a single polarization-preserving fiber, coupled for propagation of beams of two Raman frequencies, and a parallel displacement beamsplitter for separating the laser beams into respective free-space-propagating parallel beams traversing at least one ensemble of atoms. A reflector generates one or more beams counterpropagat…
Who is the assignee on this patent?
Charles Stark Draper Laboratory Inc
What technology area does this patent fall under?
Primary CPC classification G21K1/30. Mapped technology areas include Physics.
When was this patent published?
Publication date Thu Dec 28 2017 00:00:00 GMT+0000 (Coordinated Universal Time) (A1). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 3 related publications on this page (citations in our corpus or others sharing the same primary CPC).