Compact laser source with frequency modulators generating multiple lines

Patent metadata

Field	Value
Publication number	US-11545815-B1
Application number	US-202016831350-A
Country	US
Kind code	B1
Filing date	Mar 26, 2020
Priority date	May 23, 2019
Publication date	Jan 3, 2023
Grant date	Jan 3, 2023

Abstract

A compact laser source and a single sideband modulator used therein is disclosed. The compact laser source includes a seed laser and one or more channels, with each channel generating one or more output laser beams having corresponding different wavelengths. The compact laser source can be formed in whole or in part on a single optical motherboard to thereby minimize space and power requirements. By employing the disclosed single sideband modulator, harmonics in the generated output laser beams can be minimized. The compact laser source finds application in an atom interferometer (AI) system, which may be used to measure gravity, acceleration, or rotation of the AI system.

First claim

The invention claimed is:

1. A laser source comprising:
a seed laser adapted to generate a laser beam;
a beam splitter adapted to receive the laser beam and to split the laser beam into a plurality of sub-beams; and
at least one channel, each channel including:
a frequency shifter adapted to receive a respective one of the plurality of sub-beams and to shift a frequency of the respective one of the plurality of sub-beams;
a non-linear optical element adapted to receive the frequency shifted respective one of the plurality of sub-beams, to increase a frequency of the frequency shifted respective one of the plurality of sub-beams, and to output the increased frequency and frequency shifted respective one of the plurality of sub-beams as a respective output laser beam; and

a feedback loop, the feedback loop adapted to receive a first of the plurality of sub-beams and to control a frequency of the laser beam based upon the received first of the plurality of sub-beams, the feedback loop including:
a feedback optical amplifier adapted to receive the first of the plurality of sub-beams and to amplify the first of the plurality of sub-beams;
a feedback non-linear optical element adapted to receive the amplified first of the plurality of sub-beams and to increase a frequency of the amplified first of the plurality of sub-beams; and
a lock circuit adapted to receive the increased frequency, amplified first of the plurality of sub-beams and to generate a control signal to control the frequency of the laser beam.

2. The laser source of claim 1 , wherein each channel further includes an optical filter adapted to receive the frequency shifted respective one of the plurality of sub-beams, to filter out unwanted sub-bands in the frequency shifted respective one of the plurality of sub-beams, and to output the filtered and frequency shifted respective one of the plurality of sub-beams to the non-linear optical element.

3. The laser source of claim 2 , wherein the optical filter of each channel includes one or more respective micro-ring resonators.

4. The laser source of claim 1 , wherein each channel further includes a variable optical attenuator adapted to receive the frequency shifted respective one of the plurality of sub-beams, to variably attenuate the frequency shifted respective one of the plurality of sub-beams, and to output the variably attenuated and frequency shifted respective one of the plurality of sub-beams to the non-linear optical element.

5. The laser source of claim 4 , wherein the variable optical attenuator of each channel includes a respective high contrast Mach-Zehnder interferometer, each high contrast Mach-Zehnder interferometer including:
a first stage beam splitter adapted to receive the frequency shifted respective one of the plurality of sub-beams and to split the frequency shifted respective one of the plurality of sub-beams into first and second sub-sub-beams;
a first first stage phase shifter adapted to receive the first sub-sub-beam and to impose a predetermined phase shift ψ on the first sub-sub-beam;
a second first stage phase shifter adapted to receive the second sub-sub-beam and to impose a predetermined phase shift −ψ on the second sub-sub-beam;
a second stage coupler adapted to receive the ψ shifted first sub-sub-beam and the −ψ shifted second sub-sub-beam, to combine the ψ shifted first sub-sub-beam and the −ψ shifted second sub-sub-beam to form a third sub-sub-beam, and to split the third sub-sub-beam into fourth and fifth sub-sub-beams;
a first second stage phase shifter adapted to receive the fourth sub-sub-beam and to impose a predetermined phase shift φ on the fourth sub-sub-beam;
a second second stage phase shifter adapted to receive the fifth sub-sub-beam and to impose a predetermined phase shift −φ on the fifth sub-sub-beam; and
a third stage coupler adapted to receive the φ shifted fourth sub-sub-beam and the −φ shifted fifth sub-sub-beam and to combine the φ shifted fourth sub-sub-beam and the −φ shifted fifth sub-sub-beam to form an attenuated, frequency shifted respective one of the plurality of sub-beams.

6. The laser source of claim 1 , wherein each channel further includes an optical amplifier adapted to receive the frequency shifted respective one of the plurality of sub-beams, to amplify the frequency shifted respective one of the plurality of sub-beams, and to output the amplified and frequency shifted respective one of the plurality of sub-beams to the non-linear optical element.

7. The laser source of claim 6 , wherein the optical amplifier of each channel includes one or more respective multiple quantum well gain stages.

8. The laser source of claim 1 , wherein each channel further includes:
an optical filter adapted to receive the frequency shifted respective one of the plurality of sub-beams and to filter out unwanted sub-bands in the frequency shifted respective one of the plurality of sub-beams;
a variable optical attenuator adapted to receive the frequency shifted respective one of the plurality of sub-beams and to variably attenuate the frequency shifted respective one of the plurality of sub-beams; and
an optical amplifier adapted to receive the variably attenuated, filtered, and frequency shifted respective one of the plurality of sub-beams and to amplify the variably attenuated, filtered, and frequency shifted respective one of the plurality of sub-beams, and to output the amplified, variably attenuated, filtered, and frequency shifted respective one of the plurality of sub-beams to the non-linear optical element.

9. The laser source of claim 8 , wherein at least the beam splitter, the frequency shifter of each channel, the optical filter of each channel, the variable optical attenuator of each channel, the optical amplifier of each channel, and the non-linear optical element of each channel are formed on a single optical motherboard.

10. The laser source of claim 9 , wherein the single optical motherboard includes a biased low loss waveguide.

11. The laser source of claim 1 , wherein a wavelength of the laser beam is based upon a transition wavelength of an atom or a molecule.

12. The laser source of claim 1 , wherein the frequency shifter of each channel is a respective single sideband frequency modulator, each single sideband modulator including:
a first stage beam splitter adapted to receive the respective one of the plurality of sub-beams and to split the respective one of the plurality of sub-beams into first and second sub-sub-beams;
a first stage π/2 phase shifter adapted to receive the second sub-sub-beam and to impose a π/2 phase shift on the second sub-sub-beam;
a first second stage beam splitter adapted to receive the first sub-sub-beam and to split the first sub-sub-beam into third and fourth sub-sub-beams;
a second second stage beam splitter adapted to receive the π/2 phase shifted second sub-sub-beam and to split the π/2 phase shifted second sub-sub-beam into fifth and sixth sub-sub-beams;
a first second stage π phase shifter adapted to receive the fourth sub-sub-beam and to impose a π phase shift on the fourth sub-sub-beam;
a second second stage π phase shifter adapted to receive the sixth sub-sub-beam and to impose a π phase shift on the sixth sub-sub-beam;
a first frequency modulator adapted to receive the third sub-sub-beam and to impose a predetermined frequency detuning on the third sub-sub-beam;
a second frequency modulator adapted to receive the π phase shifted fourth sub-sub-beam and to impose the predetermined frequency detuning on the π phase shifted fourth sub-sub-beam;
a third frequency modulator adapted to receive the fifth sub-sub-beam and to impose the predetermined

Assignees

• Nat Tech & Eng Solutions Sandia Llc

Inventors

• Lentine Anthony L
• Biedermann Grant
• Gehl Michael
• Derose Christopher
• Lee Jongmin
• Fortier Kevin Michael

Classifications

• H01S5/041

  Optical pumping · CPC title

• G02B27/106

  for splitting or combining a plurality of identical beams or images, e.g. image replication · CPC title

• G02F2203/48

  Variable attenuator · CPC title

• H01S3/0092

  Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title

• H01S5/5045 Primary

  the arrangement having a frequency filtering function · CPC title