Atomic interferometric accelerometer with enhanced vibrational stability

US2017307652A1 · US · A1

Patent metadata
FieldValue
Publication numberUS-2017307652-A1
Application numberUS-201615138035-A
CountryUS
Kind codeA1
Filing dateApr 25, 2016
Priority dateApr 25, 2016
Publication dateOct 26, 2017
Grant date

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  5. First independent claim

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Abstract

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An atomic interferometric accelerometer comprises a laser that emits a pulsed beam at a first frequency, an electro-optic modulator that receives the beam, and a vacuum cell in communication with the electro-optic modulator. The electro-optic modulator outputs a first optical signal corresponding to the beam at the first frequency and a second optical signal having a second frequency different from the first frequency. The vacuum cell has a chamber for laser cooled atoms. The vacuum cell receives the optical signals such that they propagate in a direction that passes through the atoms. A piezo mirror retro-reflects the optical signals back through the vacuum cell in a counter-propagating direction. The piezo mirror is driven with substantially constant velocity during a beam pulse, thereby imparting a Doppler shift to the retro-reflected optical signals to create two non-symmetric counter-propagating lightwave pairs. One of the lightwave pairs supports interferometry while the other is non-resonant.

First claim

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What is claimed is: 1 . An atomic interferometric accelerometer, comprising: a laser device configured to emit a pulsed laser beam at a first frequency; an electro-optic modulator in optical communication with the laser device and configured to receive the pulsed laser beam at the first frequency, the electro-optic modulator configured to output a first optical signal corresponding to the pulsed laser beam at the first frequency and a second optical signal having a second frequency different from the first frequency; a vacuum cell in optical communication with the electro-optic modulator, the vacuum cell comprising a plurality of optically transparent sides that enclose a vacuum chamber in which laser cooled atoms reside, the vacuum cell configured to receive the first and second optical signals such that the first and second optical signals propagate in a direction that passes through the laser cooled atoms; and a piezo mirror structure in optical communication with the vacuum cell and configured to retro-reflect the first and second optical signals back through the laser cooled atoms in a counter-propagating direction; wherein the piezo mirror structure is driven with substantially constant velocity during each individual laser beam pulse, thereby imparting a Doppler shift to the retro-reflected first and second optical signals to create two non-symmetric counter-propagating lightwave pairs, wherein one of the lightwave pairs supports interferometry while the other of the lightwave pairs is non-resonant. 2 . The atomic interferometric accelerometer of claim 1 , wherein the laser device comprises a laser diode. 3 . The atomic interferometric accelerometer of claim 1 , further comprising a first collimator located in a first optical path between the laser device and the electro-optic modulator, wherein the pulsed laser beam is passed through the first collimator prior to being received by the electro-optic modulator. 4 . The atomic interferometric accelerometer of claim 3 , further comprising a second collimator located in a second optical path between the electro-optic modulator and the vacuum cell, wherein the first and second optical signals pass through the second collimator prior to being received by the vacuum cell. 5 . The atomic interferometric accelerometer of claim 4 , wherein the first and second collimators each comprise a single lens collimator or a multi-lens collimator. 6 . The atomic interferometric accelerometer of claim 1 , wherein the laser cooled atoms comprise alkali atoms selected from the group consisting of rubidium, and cesium. 7 . The atomic interferometric accelerometer of claim 1 , wherein the piezo mirror structure is located outside of the vacuum cell on an opposite side from the second collimator. 8 . The atomic interferometric accelerometer of claim 1 , wherein the piezo mirror structure comprises: a piezoelectric element; a mirror element coupled to the piezoelectric element; and a quarter-waveplate coupled to the mirror element. 9 . The atomic interferometric accelerometer of claim 8 , further comprising a piezo controller operatively coupled to the piezoelectric element, the piezo controller imparting a sawtooth displacement at a first velocity to the piezoelectric element. 10 . The atomic interferometric accelerometer of claim 9 , further comprising a photodetector configured to receive a portion of the retro-reflected first and second optical signals and detect a beat note. 11 . The atomic interferometric accelerometer of claim 10 , wherein a retro-reflected frequency is beat with an incident frequency so that the beat note encodes information about the velocity of the piezoelectric element. 12 . The atomic interferometric accelerometer of claim 11 , wherein the beat note detected by the photodetector is used to track the velocity of the piezoelectric element. 13 . The atomic interferometric accelerometer of claim 10 , wherein the beat note produces an error signal that is sent in a feedback loop from the photodetector to the piezo controller to stabilize the velocity of the piezoelectric element. 14 . The atomic interferometric accelerometer of claim 10 , wherein the beat note is combined with a reference RF signal to produce an error signal that is sent in a feedback loop from the photodetector to the piezo controller to stabilize the velocity of the piezoelectric element. 15 . The atomic interferometric accelerometer of claim 10 , further comprising a set of beam splitters or Faraday isolators, which direct the emitted pulsed laser beam and the retro-reflected first and second optical signals to the photodetector. 16 . An atomic interferometric accelerometer, comprising: a laser device configured to emit a pulsed laser beam at a first frequency; an electro-optic modulator in optical communication with the laser device and configured to receive the pulsed laser beam at the first frequency, the electro-optic modulator configured to output a first optical signal corresponding to the pulsed laser beam at the first frequency and a second optical signal have a second frequency different from the first frequency; a vacuum cell in optical communication with the electro-optic modulator, the vacuum cell comprising a plurality of optically transparent sides that enclose a vacuum chamber in which laser cooled atoms reside, the vacuum cell configured to receive the first and second optical signals such that the first and second optical signals propagate in a direction that passes through the laser cooled atoms; a piezo mirror structure in optical communication with the vacuum cell and configured to retro-reflect the first and second optical signals back through the laser cooled atoms in a counter-propagating direction; a piezo controller operatively coupled to the piezo mirror structure, the piezo controller imparting a periodic displacement at a first velocity to the piezo mirror structure; and a photodetector configured to receive a portion of the retro-reflected first and second optical signals and detect a beat note; wherein the beat note produces an error signal that is sent in a feedback loop from the photodetector to the piezo controller to stabilize the velocity of the piezo mirror structure; wherein the piezo mirror structure is driven with substantially constant velocity during each individual laser beam pulse, thereby imparting a Doppler shift to the retro-reflected first and second optical signals to create two non-symmetric counter-propagating lightwave pairs, wherein one of the lightwave pairs supports interferometry while the other of the lightwave pairs is non-resonant. 17 . The atomic interferometric accelerometer of claim 16 , wherein the laser device comprises a distributed Bragg reflector laser. 18 . The atomic interferometric accelerometer of claim 16 , wherein the piezo mirror structure comprises: a piezoelectric element; a mirror element coupled to the piezoelectric element; and a quarter-waveplate coupled to the mirror element. 19 . The atomic interferometric accelerometer of claim 18 , wherein the piezo mirror structure is located outside of the vacuum cell on an opposite side from the electro-optic modulator. 20 . The atomic interferometric accelerometer of claim 18 , further comprising a set of beam splitters or Faraday isolators, which direct the emitted pulsed laser beam and the retro-reflected first and second optical signals to the photodetector.

Assignees

Inventors

Classifications

  • G01P15/093Primary

    by photoelectric pick-up · CPC title

  • Details · CPC title

  • G01V7/00Primary

    Measuring gravitational fields or waves; Gravimetric prospecting or detecting · CPC title

  • Details · CPC title

  • Fluorescence; Phosphorescence · CPC title

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What does patent US2017307652A1 cover?
An atomic interferometric accelerometer comprises a laser that emits a pulsed beam at a first frequency, an electro-optic modulator that receives the beam, and a vacuum cell in communication with the electro-optic modulator. The electro-optic modulator outputs a first optical signal corresponding to the beam at the first frequency and a second optical signal having a second frequency different …
Who is the assignee on this patent?
Honeywell Int Inc
What technology area does this patent fall under?
Primary CPC classification G01P15/093. Mapped technology areas include Physics.
When was this patent published?
Publication date Thu Oct 26 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 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).