# US 12,763,548 B2 · Two-dimensional photonic crystal laser

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- Number: US 12,763,548 B2
- Document ID: US12763548B2
- Status: Granted
- Kind: B2
- Application number: 18/275,963
- Filed: 2022-02-24
- Published: 2024-04-18
- Granted: 2026-10-13
- Earliest claimed: 2021-02-25
- Assignees: Kyoto University
- Applicants: Kyoto University
- Inventors: Susumu Noda; Menaka De Zoysa; Ryoichi Sakata; Kenji Ishizaki; Takuya Inoue; Masahiro Yoshida
- Web page: https://patentgrep.com/patent/US12763548B2

## CPC

- H01S 5/11: Comprising a photonic bandgap structure
- H01S 5/04256: {characterised by the configuration}
- H01S 5/185: having only horizontal cavities, e.g. horizontal cavity surface-emitting lasers [HCSEL] (comprising a photonic bandgap structure H01S5/11)
- 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 two-dimensional photonic crystal laser includes: electrodes; an active layer; and a two-dimensional photonic crystal layer in which modified refractive index regions are disposed to be shifted by different shift amounts from respective lattice points or/and are disposed at the respective lattice points with different areas, the shift amount or/and the area is/are modified with a composite modulation period and expressed by a modulation phase Ψ(r↑) expressed using a vector r↑ indicating a position of each lattice point of the two-dimensional lattice, a vector kn↑ indicating a combination of an inclination angle and an azimuthal angle of each of n laser beams mutually differing in the inclination angle and/or the azimuthal angle, and an amplitude An and a phase exp(iαn) determined for each n and the amplitude An and/or the phase exp(iαn) for each value of n differ(s) from each other in at least two different values of n.

## Claims

### Claim 1

A two-dimensional photonic crystal laser comprising:
a) a pair of electrodes;
b) an active layer provided between the pair of electrodes and configured to generate light of a predetermined wavelength upon being supplied with an electric current from the electrodes; and
c) a two-dimensional photonic crystal layer provided between any one of the pair of electrodes and the active layer and including a plate-shaped base member and a plurality of modified refractive index regions disposed in the base member and having a refractive index different from a refractive index of the base member, wherein
the plurality of modified refractive index regions are disposed to be shifted by different shift amounts from respective lattice points of a two-dimensional lattice which are periodically disposed in the base member with a period corresponding to the predetermined wavelength, or/and are disposed at the respective lattice points with different areas,
the shift amount or/and the area of each of the plurality of modified refractive index regions is/are modified with a composite modulation period in which a plurality of periods different from each other are superposed on each other, and is/are expressed by a modulation phase Ψ′(r↑) expressed using a vector r↑ indicating a position of each of the lattice points of the two-dimensional lattice, a vector kn↑ indicating a combination of an inclination angle and an azimuthal angle of each of n (n is an integer of 2 or more) laser beams differing in the inclination angle and/or the azimuthal angle from each other, and an amplitude An and a phase exp(iαn) determined for each n as
[
Expression
⁢
1
]

Ψ
⁡
(
r
↑
)
=
arg
[
∫
∫
∑
n
A
n
⁢
exp
⁡
(
i
⁢
α
n
)
⁢
δ
⁡
(
k
↑
-
k
n
↑
)
⁢
exp
⁡
(
ik
↑
·
r
↑
)
⁢
dk
↑
]
,
(
1
)
and
the amplitude An and/or the phase exp(iαn) for each value of n differ(s) from each other in at least two different values of n.

### Claim 2 (depends on 1)

The two-dimensional photonic crystal laser according to claim 1, wherein a correction coefficient is added to the modulation phase Ψ(r↑).

### Claim 3 (depends on 1)

The two-dimensional photonic crystal laser according to claim 1, wherein the phase exp (in) is randomly set for each value of n.

### Claim 4 (depends on 3)

The two-dimensional photonic crystal laser according to claim 3, wherein the amplitude An has a different value for each term having a different value of n.

### Claim 5 (depends on 1)

The two-dimensional photonic crystal laser according to claim 1, wherein
the two-dimensional lattice is a square lattice, and
second modified refractive index regions having a refractive index different from the refractive index of the base member is further disposed at second lattice points which are lattice points of a square lattice having a same period length a as a period length of the two-dimensional lattice and shifted from the two-dimensional lattice, or at positions shifted from the second lattice points by different shift amounts each.

### Claim 6 (depends on 5)

The two-dimensional photonic crystal laser according to claim 5, wherein the second lattice points are disposed at a position shifted from the lattice points of the two-dimensional lattice by a distance larger than 0.25 a and smaller than 0.75 a in a same direction as one of basic translation vectors of the two-dimensional lattice.

### Claim 7 (depends on 1)

The two-dimensional photonic crystal laser according to claim 1, wherein
the two-dimensional lattice is a square lattice, and
each of the plurality of modified refractive index regions is disposed at a corresponding one of the lattice points of the two-dimensional lattice so as to be shifted from the lattice point in one predetermined direction or a direction different from the one direction by 180°, the one direction being a direction parallel to the two-dimensional photonic crystal layer and inclined from both two directions in which the lattice points are disposed with the period length.

### Claim 8 (depends on 1)

The two-dimensional photonic crystal laser according to claim 1, wherein the modulation phase Ψ(r↑) of each of the plurality of modified refractive index regions is modulated so as to periodically change with a predetermined modulation period in a direction parallel to the two-dimensional photonic crystal layer, and the modulation period continuously increases or decreases.

### Claim 9 (depends on 1)

The two-dimensional photonic crystal laser according to claim 1, wherein the modulation phase Ψ(r↑) of each of the plurality of modified refractive index regions is adjusted from a basic modulation state, in which the modulation phase Ψ(r↑) is modulated so as to periodically change with a predetermined modulation period in a direction parallel to the two-dimensional photonic crystal layer and the modulation period continuously increases or decreases, such that a radiated electric field distribution indicating a distribution of an electric field radiated from the two-dimensional photonic crystal layer becomes closer to a target radiated electric field distribution obtained by performing an inverse Fourier transform on a predetermined target far electric field distribution to be formed at a position separated from the two-dimensional photonic crystal layer than the radiated electric field distribution in the basic modulation state.

### Claim 10 (depends on 1)

A two-dimensional photonic crystal laser array comprising:
a plurality of the two-dimensional photonic crystal lasers according to claim 1 having the modulations different from each other; and
an electric current supply part configured to simultaneously supply an electric current to the pairs of electrodes individually provided in the plurality of two-dimensional photonic crystal lasers.

### Claim 11 (depends on 10)

The two-dimensional photonic crystal laser array according to claim 10, wherein
the electric current supply part includes a mesh electrode in which a plurality of holes are formed in a plate member having conductivity,
the two-dimensional photonic crystal laser is disposed in each of the plurality of holes, and
in each of the plurality of holes, the plate member around the hole is connected to one of the pair of electrodes, or is one of the pair of electrodes.

### Claim 12

A two-dimensional photonic crystal laser array comprising:
a) a pair of electrode groups including electrode groups of which at least one group includes a plurality of partial electrodes;
b) an active layer provided between the pair of electrode groups and, upon being supplied with an electric current from one of the plurality of partial electrodes, configured to generate light including a predetermined wavelength 2 at a position corresponding to the partial electrode from which the electric current is supplied; and
c) a two-dimensional photonic crystal layer provided between any one of the pair of electrode groups and the active layer and including a plate-shaped base member and a plurality of modified refractive index regions disposed in the base member and having a refractive index different from a refractive index of the base member, wherein
at a corresponding one of lattice points of a square lattice in which the lattice points are periodically disposed with a lattice point period corresponding to the predetermined wavelength 2L, each of the plurality of modified refractive index regions is disposed to be shifted from the lattice point in one predetermined direction or a direction different from the one direction by 180°, the one direction being a direction parallel to the two-dimensional photonic crystal layer and inclined from both two directions in which the lattice points are disposed with the lattice point period, and
in a direction parallel to the two-dimensional photonic crystal layer, a distance from the lattice point or/and an area of a planar shape of each of the plurality of modified refractive index regions is/are modified with a composite modulation period in which a plurality of periods different from each other are superposed on each other, and is/are expressed by a modulation phase Ψ(r↑) expressed using a vector r↑ indicating a position of each of the lattice points of the two-dimensional lattice, a vector kn↑ indicating a combination of an inclination angle and an azimuthal angle of each of n (n is an integer of 2 or more) laser beams differing in the inclination angle and/or the azimuthal angle from each other, and an amplitude An and a phase exp(iαn) determined for each n as
[
Expression
⁢
1
]

Ψ
⁡
(
r
↑
)
=
arg
[
∫
∫
∑
n
A
n
⁢
exp
⁡
(
i
⁢
α
n
)
⁢
δ
⁡
(
k
↑
-
k
n
↑
)
⁢
exp
⁡
(
ik
↑
·
r
↑
)
⁢
dk
↑
]
(
1
)
and
the amplitude An and/or the phase exp(iαn) for each value of n differ(s) from each other in at least two different values of n.