Modulated laser for atom interferometers

Abstract

The present invention is directed to a modulated which includes a semiconductor laser being driven by direct current for frequency tuning, and an AC current with two radio frequencies that can generate repump and Raman frequencies, such that only one laser is needed to produce all the frequencies required to operate an atom interferometer. The present invention is also directed to a method of double modulating a laser to produce all required frequencies for an atom interferometer.

Claims

1. A modulated laser for atom interferometers, the laser comprising: a semiconductor laser being driven by direct current for frequency tuning, and an AC current with two radio frequencies that can generate repump and Raman frequencies, such that only one laser is needed to produce all the frequencies required to operate an atom interferometer.

2. The method of double modulating a laser to produce all required frequencies for an atom interferometer using laser cooled atoms, the interferometer having an interferometry region, the method comprising: tuning laser current such that laser frequency coincides with required cooling frequency; modulating laser current to generate a frequency of light at a required repump frequency; modulating the laser current to generate two more frequencies of light that form laser frequency Raman #1 and laser frequency Raman #2; and, selecting an appropriate radio frequency modulation power such that optical power at each frequency is sufficient for interferometer operation, filtering the repump frequency and the cooling frequency using an atomic filter such the repump frequency and the cooling frequency do not reach the atoms in interferometry region.

3. The method of claim 2 wherein an atomic filter filters out unwanted frequencies (cooling and repump) from the atom interferometer region.

Description

DRAWINGS

(1) These and other features, aspects and advantages of the present invention will become better understood with reference to the following description and appended claims, and accompanying drawings wherein:

(2) FIG. 1 is a depiction of the first portion of the invention wherein two radio frequency sources of appropriate power are connected to a semiconductor laser via a bias-tee; and,

(3) FIG. 2 is a depiction of the entire invention including a possible implementation in atomic sensors wherein two radio frequency sources of appropriate power are connected to a semiconductor laser via a bias-tee. Light emanating from the laser consists of four frequencies labeled .sub.1, .sub.2, .sub.3, .sub.4. Some of the light is split and sent to the laser cooled atom source with all four frequencies present. The remaining light passes through the atomic filter. Emerging from the filter are the frequencies .sub.3, .sub.4. These are sent to the atom interferometer.

DESCRIPTION

(4) The preferred embodiments of the present invention are illustrated by way of example below and in FIGS. 1-2. As shown in FIG. 1, a modulated laser for atom interferometers 10 includes a semiconductor laser 100 being driven by direct current 170 for frequency tuning, and an AC current 175 with two radio frequencies that can generate repump 200 and Raman frequencies 300, such that only one laser 100 is needed to produce all the frequencies required to operate an atom interferometer 10.

(5) A method of double modulating a laser to produce all required frequencies for an atom interferometer using laser cooled atoms is also presented. The interferometer has an interferometry region. The method comprises of tuning laser current such that laser frequency coincides with required cooling frequency, modulating laser current to generate a frequency of light at a required repump frequency, modulating the laser current to generate two more frequencies of light that form laser frequency Raman #1 and laser frequency Raman #2, and filtering the repump frequency and the cooling frequency using an atomic filter such the repump frequency and the cooling frequency do not reach the atoms in the interferometry region. In both the method and apparatus an atomic filter 400 may be used to filter out unwanted frequencies (cooling and repump) from the atom interferometer region.

(6) In the description of the present invention, the invention will be discussed in a laboratory environment; however, this invention can be utilized for any type of application that requires use of atom interferometers.

(7) As shown in FIG. 1, the invention comprises of a semiconductor laser 100, whose frequency is set by a direct current source 170. Two radio frequency sources 200, 300 are connected to the semiconductor laser 100 directly via a bias-tee 250. The power of the radio frequency sources 200, 300 is set such that the majority of the optical power is at the desired frequencies, at the expense of the fundamental frequency. The frequencies of the radio frequency sources are chosen such that they can be used as a repump frequency 200 and as the Raman frequencies 300.

(8) As shown in FIG. 2, light 150 emanating from the laser 100 will now include four frequencies; a cooling frequency .sub.1, a repump frequency .sub.2, and the two Raman frequencies .sub.3, .sub.4. To utilize this invention for atomic sensors 600, the laser light 150 can be divided into two portions. The first portion 151 can be directed with all four frequencies .sub.1, .sub.2, .sub.3, .sub.4 towards a cell or laser cooled atom source 500 to produce laser cooled atoms. The second portion 152 of the light 150 passes through an atomic filter 400, which is a hot cell filled with the same atoms to be used in the atomic sensor 600. The atomic filter 400 has the effect of filtering out the cooling frequencies .sub.1 and the repump frequencies .sub.2, but not the Raman frequencies .sub.3, .sub.4, because they are off-resonant. The light emerging from the atomic filter 400 then can be used in the interferometer region.

(9) When introducing elements of the present invention or the preferred embodiment(s) thereof, the articles a, an, the, and said are intended to mean there are one or more of the elements. The terms comprising, including, and having are intended to be inclusive and mean that there may be additional elements other than the listed elements.

(10) Although the present invention has been described in considerable detail with reference to certain preferred embodiments thereof, other embodiments are possible. Therefore, the spirit and scope of the appended claims should not be limited to the description of the preferred embodiment(s) contained herein.