Planar waveguide

Patent metadata

Field	Value
Publication number	US-10422951-B2
Application number	US-201616302032-A
Country	US
Kind code	B2
Filing date	Jun 14, 2016
Priority date	Jun 14, 2016
Publication date	Sep 24, 2019
Grant date	Sep 24, 2019

Abstract

Disclosed is a planar waveguide including: a core (11) which is a flat plate through which light propagates; a cladding (12) which is a flat plate for reflecting the light in a state of being joined to an upper surface of the core (11); and a cladding (13) which is a flat plate for reflecting the light in a state of being joined to a lower surface of the core (11), in which each of the claddings (12) and (13) is a multilayer film in which multiple films made from different materials are layered. As a result, a material having a low index of refraction can be used as the material of the core (11), and the limit on materials usable as the material of the core (11) is relaxed.

First claim

What is claimed is:

1. A planar waveguide comprising:
a core which is a flat plate through which light propagates;
a first cladding which is a flat plate for reflecting the light in a state of being joined to an upper surface of the core; and
a second cladding which is a flat plate for reflecting the light in a state of being joined to a lower surface of the core,
wherein each of the first and second claddings is a multilayer film in which at least one of sets of multiple films made from different materials are layered,
wherein film thicknesses of multiple films belonging to an identical set are determined from a relation between wave numbers in the multiple films, and a light path where the light makes a round trip through the multiple films belonging to the identical set, and
wherein when a number of films belonging to the identical set is two, the film thicknesses of the two films are expressed by d a and d b , respectively, vertical components of the wave numbers in the two films are expressed by k a and k b , respectively, and the light path where the light makes a round trip through the two films is expressed by l×π (l is an integer equal to or larger than 1), the film thicknesses d a and d b of the two films are determined to be ones satisfying a following conditional formula:

(

l
-

1
4

)

×
π

<

(

k
a

×

d
a

)

+

(

k
b

×

d
b

)

<

(

l
+

1
4

)

×

π
.

2. The planar waveguide according to claim 1 , wherein the film thicknesses of the two films are determined to be ones satisfying the conditional formula, as to a zeroth-order propagation angle among propagation angles which are angles at each of which the light is incident upon each of the first and second claddings from the core.

3. The planar waveguide according to claim 1 , wherein the core is a gain generation member for amplifying signal light which is propagating light by absorbing excitation light and forming a population inversion, and wherein the film thicknesses of the two films are determined to be ones satisfying the conditional formula, as to both a wave number determined from a wavelength of the excitation light, and a wave number determined from a wavelength of the signal light.

4. The planar waveguide according to claim 1 , wherein the planar waveguide includes an excitation light source for emitting excitation light, and the excitation light emitted from the excitation light source is guided to the core.

5. The planar waveguide according to claim 1 , wherein in the multilayer film, an amount of phase change of TE polarized light in the light differs from that of TM polarized light in the light.

6. The planar waveguide according to claim 5 , wherein the core is a gain generation member for amplifying signal light which is propagating light by absorbing excitation light and forming a population inversion.

Assignees

• Mitsubishi Electric Corp

Inventors

• Hirosawa Kenichi
• Yanagisawa Takayuki

Classifications

• G02B6/126

  using polarisation effects {(G02B6/1226 takes precedence)} · CPC title

• G02B6/1223

  high refractive index type, i.e. high-contrast waveguides · CPC title

• H01S3/1685

  Ceramics · CPC title

• H01S3/163

  characterised by a crystal matrix · CPC title

• H01S3/162

  transition metal · CPC title