# US 10,483,720 B2 · Laser device with a beam carrying controlled orbital angular momentum

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- Number: US 10,483,720 B2
- Document ID: US10483720B2
- Status: Granted
- Kind: B2
- Application number: 15/535,528
- Filed: 2015-12-15
- Published: 2017-11-30
- Granted: 2019-11-19
- Earliest claimed: 2014-12-15
- Assignees: Universite De Montpellier; Centre National De La Recherche Scientifique
- Applicants: Universite De Montpellier; Centre National De La Recherche Scientifique
- Inventors: Arnaud Garnache-Creuillot; Mikhael Myara; Isabelle Sagnes; Luc Le Gratiet; Mohammed Sellahi; Mohammed Seghilani; Philippe Lalanne
- Web page: https://patentgrep.com/patent/US10483720B2

## CPC

- H01S 5/18319: {comprising a periodical structure in lateral directions}
- H01S 5/14: External cavity lasers (H01S5/18 takes precedence; mode locking H01S5/065)
- H01S 5/11: Comprising a photonic bandgap structure
- H01S 2301/20: Lasers with a special output beam profile or cross-section, e.g. non-Gaussian
- H01S 2301/203: with at least one hole in the intensity distribution, e.g. annular or doughnut mode
- H01S: DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL

## Abstract

A laser device is provided for generating a helical-shaped optical wave and includes: (i) a gain region located between one first end defined by a first mirror and a second end defined by an exit region, (ii) a second mirror arranged so as to form with the first mirror an optical cavity including the gain region and a gap between the exit region and the second mirror, (iii) apparatus for pumping the gain region so as to generate the optical wave, wherein the laser device further includes at least one apparatus for shaping the light intensity and/or phase profiles of the optical wave and arranged for selecting at least one rotary-symmetrical transverse mode of the optical wave, the rotary-symmetrical transverse mode being chosen between those with a radial index equal to zero and with an azimuthal index being an integer with a module higher or equal to 1.

## Claims

### Claim 1

A laser device for generating a helical-shaped phase optical wave, the laser device comprising:
a gain region located between one first end defined by a first mirror and a second end defined by an exit region;
a second mirror configured to form, with the first mirror, an optical cavity including the gain region and a gap between the exit region and the second mirror;
means for pumping the gain region so as to generate the optical wave;
at least one means for transverse filtering the optical wave configured for selecting at least one rotary-symmetrical transverse mode of the optical wave, said rotary-symmetrical transverse mode being chosen among those with a radial index equal to zero and with an azimuthal index being an integer with a module higher or equal to 1; and
the at least one means for transverse filtering the optical wave comprises the following functionalized areas:
a center-discoidal area providing high losses between a minimum phase shift value and a maximum phase shift value, and
a first annular area, located around the center-longitudinal axis and a second annular area located around the first annular area, wherein said first annular area and said second annular area each provide modal azimuthal graded phase shift; and
a functionalized absorbing area or pumping area, located on a peripheral region, which is outside of the first annular area.

### Claim 2 (depends on 1)

The device according to claim 1, wherein the at least one means for transverse filtering the optical wave is centered on a longitudinal axis.

### Claim 3 (depends on 1)

The device according to claim 1, wherein the center-discoidal area is divided onto two sub-areas, the first sub-area providing the minimum phase shift value, and the second sub-area providing the maximum phase shift value, said center-discoidal area providing modal losses.

### Claim 4 (depends on 1)

The device according to claim 1, wherein the said first annular area provides at least one graduated perturbative spiral phase shift between the minimum phase shift value and the maximum phase shift value for at most one turn and for one roundtrip of the optical wave in the optical cavity, said first annular area providing a modal phase shift comprised between 2π*1·10−5 and 2π/5.

### Claim 5 (depends on 1)

The device according to claim 1, wherein the at least one means for transverse filtering consists in one single mask located at or close to one of the following locations:
an antinode of the optical wave,
onto the gain region, and
onto the second mirror surface.

### Claim 6 (depends on 1)

The device according to claim 1, wherein the at least one means for transverse filtering consists in a plurality of masks patterned with at least one functionalized area and at least one of the plurality of masks is located at or close to an antinode of the optical wave.

### Claim 7 (depends on 1)

The device according to claim 1, wherein the at least one means for transverse filtering the optical wave is a flat photonic element fabricated using III-V semiconductor technology.

### Claim 8 (depends on 1)

The device according to claim 1, wherein the phase shifts of the center-discoidal area and said first annular area are provided by refractive index variations of the at least one means for transverse filtering.

### Claim 9 (depends on 1)

The device according to claim 1, wherein the phase shift values of said center-discoidal area and said first annular area are provided by controlling the 2D grating dimensional characteristics of the at least one means for transverse filtering.

### Claim 10 (depends on 1)

The device according to claim 1, wherein the means for pumping the gain region comprise:
a pump laser emitting a pumping laser beam;
means arranged for spatially shaping the pumping laser beam intensity; and
the at least one means for shaping the light intensity and phase profiles of the optical wave comprise the means for spatially shaping the pumping laser beam intensity and are configured to project a pumping beam intensity pattern onto the exit region corresponding with the at least one selected rotary-symmetrical transverse mode of the optical wave.

### Claim 11 (depends on 1)

The device according to claim 1, wherein the means for pumping the gain region consists in an electrical pumping of the gain region.

### Claim 12 (depends on 1)

The device according to claim 1, wherein the laser device comprises a Vertical External Cavity Surface Emitting Laser.

### Claim 13 (depends on 1)

The device according to claim 1, wherein the second mirror is a flat end mirror.

### Claim 14

A method for generating a helical-shaped phase optical wave comprising the following steps:
generating an optical wave inside a gain region, said optical wave oscillating inside an optical cavity;
pumping the optical wave with means for pumping; and
shaping the light intensity and phase profiles of the optical wave for selecting at least one rotary-symmetrical transverse mode of the optical wave between those with a radial index equal to zero and with an azimuthal index being an integer with a module higher or equal to 1, by at least one means for transverse filtering the optical wave, which comprises:
providing high losses between a minimum phase shift value and a maximum phase shift value using a center-discoidal area, and
providing modal azimuthal graded phase shift using a first annular area, located around the center-longitudinal axis, and a second annular area, located around the first annular area; and
absorbing or pumping with a functionalized absorbing area or pumping area, located on a peripheral region, which is outside of the first annular area.