IP Library Granted Patent US 10,281,650
Granted Patent B2
US 10,281,650 · App. 15/303,524 · Granted May 7, 2019

Optical comb filter having first, second and third GT resonant cavities

Inventors: Shuliang Huang (Guangdong, CN); Yimin Hua (Guangdong, CN); Liancheng Li (Guangdong, CN)
Assignee: O-NET COMMUNICATIONS (SHENZHEN) LIMITED
G02B6/29358G02B5/288G02B6/293G02B6/421G02B6/4215H04J14/02G01B9/02008G02B1/11G02B5/284G02B6/29349G02B6/29361G02B26/001G02B26/004G02F2203/54G02F2203/56
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Quick Facts
Patent No.
US 10,281,650
App. No.
15/303,524
Granted
May 7, 2019
Kind
B2
Abstract

An optical comb filter, comprising an input/output collimator ( 50 ), an output collimator ( 60 ), a spectroscope ( 10 ), and first, second and third GT resonant cavities ( 20, 30, 40 ), wherein each GT resonant cavity comprises a transparent solid block coated with a membrane layer and a spacing part, a through hole is provided on the transparent solid block, and the transparent solid block and the spacing part form a hollow cavity; and rectangular orientation of an insertion loss curve is realized, and the bandwidth utilization rate is high.

Claims (20)

1. An optical comb filter comprising:

an input/output collimator ( 50 ),

an output collimator ( 60 ),

a beam splitter ( 10 ),

a first GT resonant cavity ( 20 ),

a second GT resonant cavity ( 30 ), and

a third GT resonant cavity ( 40 ),

wherein the GT resonant cavity ( 20 ) comprises transparent solid blocks ( 201 , 202 ) coated with a first reflective membrane layer ( 201 f ) and a second reflective membrane layer ( 202 f ) and spacing parts ( 211 , 212 ), wherein the transparent solid block ( 202 ) has a through-hole ( 202 a ), the transparent solid blocks ( 201 , 202 ) and the spacing parts ( 211 , 212 ) form a hollow cavity ( 221 ), and the through-hole ( 202 a ) included in the first GT resonant cavity ( 20 ) connects with the hollow cavity ( 221 ) included in the first GT resonant cavity ( 20 ); the second GT resonant cavity ( 30 ) comprises a membrane layer transparent solid block ( 301 ) coated with a membrane layer ( 3010 f ), an antireflection membrane layer ( 100 f ) and spacing parts ( 311 , 312 ) coated on a surface of the beam splitter ( 10 ), wherein a through-hole ( 301 a ) is set on the transparent solid block ( 301 ), the transparent solid block ( 301 ), the beam splitter ( 10 ) and the spacing parts ( 311 , 312 ) form a hollow cavity ( 321 ), and the through-hole ( 301 a ) included in the second GT resonant cavity ( 30 ) connects with the hollow cavity ( 321 ) included in the second GT resonant cavity ( 30 ); the third GT resonant cavity ( 40 ) comprises a transparent solid block ( 402 ) coated with a reflective membrane layer ( 402 f ), reflective membrane layer ( 401 f ) coated on another surface of the transparent solid block ( 301 ) and spacing parts ( 411 , 412 ), wherein a through-hole ( 402 a ) is set on the transparent solid block ( 402 ), and the transparent solid blocks ( 301 , 402 ) and the spacing parts ( 411 , 412 ) form a hollow cavity ( 421 ), and the through-hole ( 402 a ) included in the third GT resonant cavity ( 40 ) connects with the hollow cavity ( 421 ) included in the third GT resonant cavity ( 40 );

wherein the transparent solid block ( 201 ) included in the first GT cavity ( 20 ) and the transparent solid block ( 301 ) included in the second GT resonant cavity ( 30 ) are of a same material and a same thickness in their respective optical path directions to realize temperature compensation;

gases are supplied and released to or from the hollow cavity ( 221 ) included in the first GT resonant cavity ( 20 ), the hollow cavity ( 321 ) included in the second GT resonant cavity ( 30 ) and the hollow cavity ( 421 ) included in the third GT resonant cavity ( 40 ) via the through-hole ( 202 a ) included in the first GT resonant cavity ( 20 ), the through-hole ( 301 a ) included in the second GT resonant cavity ( 30 ), and the through-hole ( 402 a ) included in the third GT resonant cavity ( 40 ) to adjust pressure in the first GT resonant cavity ( 20 ), the second GT resonant cavity ( 30 ) and the third GT resonant cavity ( 40 );

the second GT resonant cavity ( 30 ) and the third resonant cavity ( 40 ) form a composite GT cavity structure to realize appearance of an insertion loss curve as a rectangle.

2. The optical comb filter as claimed in claim 1 , wherein the second reflective membrane layer ( 202 f ) of the first GT cavity ( 20 ) is a highly reflective membrane layer, and the first reflective membrane layer ( 201 f ) is a partially reflective membrane layer.

3. The optical comb filter as claimed in claim 2 , wherein the antireflection membrane layer ( 100 f ) and the membrane layer ( 301 f ) of the second GT cavity ( 30 ) are both antireflection membrane layer.

4. The optical comb filter as claimed in claim 3 , wherein the reflective membrane layer ( 402 f ) of the third GT cavity ( 40 ) is a highly reflective membrane layer, and the reflective membrane layer ( 401 f ) of the third GT cavity ( 40 ) is a partially reflective membrane layer.

5. The optical comb filter as claimed in claim 1 , wherein the beam splitter is coated with a membrane layer with a splitting ratio of 50:50.

6. The optical comb filter as claimed in claim 1 , wherein the input/output collimator is a fiber collimator.

7. The optical comb filter as claimed in claim 6 , wherein the output collimator is a fiber collimator.

8. The optical comb filter as claimed in claim 1 , wherein a length of an optical path of the hollow cavity ( 421 ) included in the third GT cavity ( 40 ) and a length of an optical path of the hollow cavity ( 221 ) included in the first GT cavity ( 20 ) are equal, and both of the lengths of the optical paths are twice of a length of an optical path of the hollow cavity ( 312 ) included in the second GT cavity ( 30 ).

9. The optical comb filter as claimed in claim 8 , wherein when a channel spacing is selected as 100 GHz, the length of the optical path of the hollow cavity ( 421 ) included in the third GT cavity ( 40 ) and the length of the optical path of the hollow cavity ( 221 ) included in the first GT cavity ( 20 ) are both 3 mm, and the length of the optical path of the hollow cavity ( 312 ) of the second GT cavity ( 30 ) is 1.5 mm.

10. The optical comb filter as claimed in claim 1 , wherein the through-hole ( 202 a ) included in the first GT resonant cavity ( 20 ) is perpendicular to the hollow cavity ( 221 ) included in the first GT resonant cavity ( 20 ); a first portion of the through-hole ( 301 a ) included in the second GT resonant cavity ( 30 ) is perpendicular to the hollow cavity ( 321 ) included in the second GT resonant cavity ( 30 ); a second portion of the through-hole ( 301 a ) included in the second GT resonant cavity ( 30 ) is perpendicular to the first portion of the through-hole ( 301 a ) included in the second GT resonant cavity ( 30 ); and the through-hole ( 402 a ) included in the third GT resonant cavity ( 40 ) is perpendicular to the hollow cavity ( 421 ) included in the third GT resonant cavity ( 40 ).

Assignments (2)
CHANGE OF NAME Recorded Feb 23, 2023
From: O-NET COMMUNICATIONS (SHENZHEN) LIMITED
To: O-NET TECHNOLOGIES (SHENZHEN) GROUP CO., LTD
Reel/Frame 062836/0439 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 12, 2016
From: HUANG, SHULIANG; HUA, YIMIN; LI, LIANCHENG
To: O-NET COMMUNICATIONS (SHENZHEN) LIMITED
Reel/Frame 039990/0065 →
Priority Claims (1)
CN 2014 1 0828912 · Dec 26, 2014 · national
Continuity (1)
Related Publication 20170038535A1 · Feb 9, 2017