Quantum collimation method for atomic beam, quantum collimator for atomic beam, atomic interferometer, and atomic gyroscope

Patent metadata

Field	Value
Publication number	US-2025027770-A1
Application number	US-202418743697-A
Country	US
Kind code	A1
Filing date	Jun 14, 2024
Priority date	Jul 19, 2023
Publication date	Jan 23, 2025
Grant date	—

Abstract

An atomic beam is quantum-mechanically collimated. The atomic beam is irradiated with a pumping laser beam and a filtering laser beam in this order. The pumping laser beam has a wavelength corresponding to a transition between a ground state and an excited state of atoms in the atomic beam. Irradiation with the pumping laser beam causes atoms to make transition from the ground state to the excited state and further relax from the excited state to a metastable state. The filtering laser beam has a wavelength corresponding to a transition between the ground state and the metastable state. By irradiating the filtering laser beam, atoms in the metastable state having velocity components equal to or smaller than a predetermined velocity component Δv in a traveling direction of the filtering laser beam are caused to make transition to the ground state.

First claim

What is claimed is:

1 . A method for quantum-mechanically collimating an atomic beam comprising:
irradiating the atomic beam with a pumping laser beam having a wavelength corresponding to a transition between a ground state and an excited state of atoms in the atomic beam, thereby causing the atoms to make transition from the ground state to the excited state and further relax from the excited state to a metastable state of the atoms; and irradiating, after the irradiating of the atomic beam with the pumping laser beam, the atomic beam with a filtering laser beam having a wavelength corresponding to a transition between the ground state and the metastable state, whereby the atoms in the metastable state having velocity components equal to or smaller than a predetermined velocity component Δv in a traveling direction of the filtering laser beam are caused to make transition to the ground state.

2 . A collimator for quantum-mechanically collimating an atomic beam comprising an irradiation device configured to irradiate the atomic beam with a pumping laser beam and a filtering laser beam in this order, wherein
the pumping laser beam is a laser beam having a wavelength corresponding to a transition between a ground state and an excited state of atoms in the atomic beam, and the filtering laser beam is a laser beam having a wavelength corresponding to a transition between the ground state and a metastable state to which atoms in the excited state make transition in a relaxation process.

3 . The collimator according to claim 2 , wherein
the filtering laser beam is a Gaussian beam, and Δv=α×Δv/k is satisfied, where Δv represents a predetermined maximum value of velocity components, in a traveling direction of the filtering laser beam, of the atoms that make transition from the metastable state to the ground state due to passage of the atomic beam through the filtering laser beam, Δv represents transit-time broadening of atoms that cross the filtering laser beam and have no velocity component in the traveling direction of the filtering laser beam, α represents a correction coefficient smaller than 1 indicating that a linewidth of a spectral line of atoms that cross the filtering laser beam and have velocity components in the traveling direction of the filtering laser beam is reduced to be narrower than Δv, and k represents a wave number of the filtering laser beam.

4 . The collimator according to claim 3 , wherein α≅0.95 is satisfied.

5 . The collimator according to claim 2 , wherein a power density of the pumping laser beam is greater than a saturation intensity of the transition between the ground state and the excited state, and W>v×E×N is satisfied, where W represents a width of the pumping laser beam through which the atomic beam passes, v represents velocity components of the atoms in a traveling direction of the atomic beam, N represents a number of times of excitation and relaxation cycles required for each of the atoms to relax to the metastable state with a predetermined probability in the relaxation process, and E represents an expected value of a time required for each of the atoms in the excited state to relax only once.

6 . The collimator according to claim 2 , wherein a traveling direction of the pumping laser beam is unparallel to the traveling direction of the filtering laser beam.

7 . An atomic interferometer comprising:
an atomic beam generation device configured to continuously generate an atomic beam; a moving standing light wave generation device configured to generate three or more moving standing light waves; and an interference device configured to obtain an atomic beam resulting from an interaction between the atomic beam and the three or more moving standing light waves, wherein the atomic beam generation device comprises an atomic beam source, and a collimator, the collimator comprises an irradiation device configured to irradiate the atomic beam with a pumping laser beam and a filtering laser beam in this order, the pumping laser beam is a laser beam having a wavelength corresponding to a transition between a ground state and an excited state of atoms in the atomic beam, and the filtering laser beam is a laser beam having a wavelength corresponding to a transition between the ground state and a metastable state to which atoms in the excited state make transition in a relaxation process.

8 . An atomic gyroscope comprising:
an atomic beam generation device configured to continuously generate an atomic beam; a moving standing light wave generation device configured to generate three or more moving standing light waves; an interference device configured to obtain an atomic beam resulting from an interaction between the atomic beam and the three or more moving standing light waves; and an observation device configured to detect an angular velocity or acceleration by observing the atomic beam from the interference device, wherein the atomic beam generation device comprises an atomic beam source, and a collimator, the collimator comprises an irradiation device configured to irradiate the atomic beam with a pumping laser beam and a filtering laser beam in this order, the pumping laser beam is a laser beam having a wavelength corresponding to a transition between a ground state and an excited state of atoms in the atomic beam, and the filtering laser beam is a laser beam having a wavelength corresponding to a transition between the ground state and a metastable state to which atoms in the excited state make transition in a relaxation process.

Assignees

• Japan Aviation Electronics Ind Ltd
• Tokyo Inst Tech

Inventors

• Kozuma Mikio
• Inoue Ryotaro
• Sato Tomoya
• Tanaka Atsushi
• Hosoya Toshiyuki

Classifications

• G21K1/30 Primary

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

• G01C19/66 Primary

  Ring laser gyrometers · CPC title

• G21K1/02

  using diaphragms, collimators · CPC title

• H05H3/00

  Production or acceleration of neutral particle beams, e.g. molecular or atomic beams · CPC title