COMPACT LASER SOURCE WITH REDUCED SPECTRAL WIDTH

• US 20110038389A1
• Filed: 04/24/2008
• Published: 02/17/2011
• Est. Priority Date: 04/27/2007
• Status: Active Grant

• Current Assignee: Centre National D'Etudes Spatiales, Observatoire De Paris, Thales SA
• Original Assignee: Thales SA
• Inventors: Esnault, Francois-Xavier, Perrin, Stephanie, Dimarcq, Noel, Holleville, David
• Granted Patent: US 8,385,376 B2
• Time in Patent Office: Days
• US Class Current: 372/19
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence

Abstract

The invention relates to a laser source with an external cavity generating a useful laser beam (Fu), that comprises at least one laser diode DL (10) mounted in an extended optical cavity (30, 82) defined between two reflecting surfaces (92, 48) forming an optical path for a laser beam Fd generated by the laser diode DL, a mode selection filter (44, 86) in the optical path of the cavity for selecting a resonance mode from a range of resonance modes of the laser beam in the cavity. The extended cavity (2) includes in the optical path thereof an optical device (94) including a polariser (100) that is 100% permissive to a rectilinear polarisation of the beam Fd generated by the laser diode, the reference polarisation angle θ₀ being of 0 degrees, a polarisation rotator (102) of the beam at the output of the polariser (Fc1) by a predetermined rotation angle θ₋₁, a polarisation separator (04) of the beam (Frt) at the output of the polarisation rotator, the polarisation separator being inclined in the cavity so that its transmission axis (tt′) is oriented at an angle (−θ₋₁) having an opposite sign to and the same value as the polarisation angle of the beam (Frt) at the output of the rotator (102), wherein the optical device prevents any feedback of a reflection beam (Fretum) of the useful beam (Fu) towards said laser diode DL. The invention can be used in a laser for cooling atoms, in interferometry experiments, inertial sensors and atomic clocks.

Claims

1. An external-cavity laser source generating a useful laser beam (Fu) comprising at least one laser diode LD (10) mounted in an extended optical cavity (30, 82) bounded between two reflecting surfaces (92, 48), providing an optical path for a laser beam Fd generated by the laser diode LD, and a mode selection filter (44, 86) in the optical path of the cavity in order to select a resonance mode from a number of resonance modes of the laser beam in the cavity,

wherein the extended cavity (82) includes, in its optical path, an optical device (94) comprising a polarizer (100) that lets through 100% of a linear polarization of the beam Fd generated by the laser diode, having a reference polarization angle θ

₀ of 0°

, a polarization rotator (102) that rotates the polarization of the beam (Fc1) leaving the polarizer through a predetermined rotation angle θ

₁, a polarization splitter (104) for splitting the beam (Frt) leaving the polarization rotator, the polarization splitter being inclined in the cavity so that its transmission axis (tt′

) is oriented at an angle (−

θ

₁) of opposite sign to and of the same value as the polarization angle of the beam (Frt) leaving the rotator (102), the optical device preventing a reflection beam (Fretum), namely the reflection of the useful beam (Fu), from returning to the laser diode LD.

2. The external-cavity laser source as claimed in claim 1, wherein the polarization splitter (104) splits the beam (Frt) leaving the polarization rotator (102) into a reflected beam along its reflection axis (rr′

) forming the useful laser beam (Fu) and into a transmitted beam (Ftr) along a transmission axis (tt′

) perpendicular to the reflection axis (rr′

), intended to be reflected by one of the two reflecting surfaces (92) of the extended cavity back onto the laser diode LD.

3. The external-cavity laser source as claimed in claim 1 or 2, wherein the optical device (94) is configured in such a way that, on the one hand, the beam reflected by one of the two reflecting surfaces (92) of the cavity back toward the laser diode LD through the optical device (94) has the same 0°

polarization as that of the beam (Fd) leaving the laser diode LD in order to create resonance in the extended cavity and, on the other hand, the reflected beam (Fretum), namely the reflection of the useful beam (Fu), coming back via the exit SI of the source through the polarization splitter (104) and the polarization rotator (102) has a polarization perpendicular to the polarization of the beam (Fc1) leaving the polarizer (100), the polarizer (100) preventing the reflected beam (Fretum) from returning to the laser diode LD.

4. The external-cavity laser source as claimed in either of claims 1 to 3, wherein it comprises, along the main axis XX′

of propagation of the laser beam in the cavity;

a laser diode LD (80) mounted in an extended cavity (82), providing an optical path for a linearly polarized laser beam (Fd), having a reference polarization angle θ

₀ of 0°

, generates by the laser diode, the extended cavity (82) being bounded between two reflecting surfaces, a mirror (92), placed at one end of the cavity, forming a first reflecting surface of the cavity and a reflecting plate (48) of the resonator of the laser diode LD, at the other end of the extended cavity (82), forming a second reflecting surface;

an input collimation lens (84) for the laser beam (Fd) in the cavity;

an etalon (86) for selecting a resonance mode in the extended cavity;

an output cat'"'"'s eye lens (90) focusing the laser beam onto the mirror (92) of the cavity; and

the optical device (94) between the input collimation lens (84) and the etalon (86) (mode selection filter).

5. The external-cavity laser source as claimed in claim 1, wherein the rotation angle (θ

₁) of the polarization of the beam (Frt) leaving the rotator (102) and the angle of the transmission axis (−

θ

₁) of the polarization splitter (104) are determined according to the desired intensities of the transmitted beam It and reflected beam Ir that are transmitted and reflected by the polarization splitter (104), these intensities being defined by;

It=cos²(2θ

₁)

Ir=sin²(2θ

₁).

8. The external-cavity laser source as claimed in claim 1, wherein the mode selection filter (86) is an interference filter.

9. The external-cavity laser source as claimed in claim 4, wherein it includes a piezoelectric block (120) for modulating the position of the mirror (92) in the extended cavity produced from a solid cube or cylinder having a reflecting face.

10. The external-cavity laser source as claimed in claim 9, wherein the reflecting face acting as mirror (92) is produced by metallizing that one of the faces of the piezoelectric block which is intended for reflecting the laser beam in the cavity.

11. The external-cavity laser source as claimed in claim 2, wherein the rotation angle (θ

₁) of the polarization of the beam (Frt) leaving the rotator (102) and the angle of the transmission axis (−

θ

₁) of the polarization splitter (104) are determined according to the desired intensities of the transmitted beam It and reflected beam Ir that are transmitted and reflected by the polarization splitter (104), these intensities being defined by;

It=cos²(2θ

₁)

Ir=sin²(2θ

₁).

12. The external-cavity laser source as claimed in claim 3, wherein the rotation angle (θ

₁) of the polarization of the beam (Frt) leaving the rotator (102) and the angle of the transmission axis (−

θ

₁) of the polarization splitter (104) are determined according to the desired intensities of the transmitted beam It and reflected beam Ir that are transmitted and reflected by the polarization splitter (104), these intensities being defined by;

It=cos²(2θ

₁)

Ir=sin²(2θ

₁).

6. The external-cavity laser source as claimed in claim, wherein the polarization rotation angle (θ

₁) of the beam (Frt) leaving the polarization rotator (102) is chosen to be +28°

, the transmission axis (tt′

) of the polarization splitter (104) being in this case oriented at −

28° and

the reflection axis (rr′

) oriented at 90−

θ

₁, i.e. +62°

.

7. The external-cavity laser source as claimed in claim, wherein the rotator (102) is a Faraday rotator.