IP Library Granted Patent US 11,366,017
Granted Patent B2
US 11,366,017 · App. 17/252,978 · Granted Jun 21, 2022

Method for measuring complex degree of coherence of random optical field by using mutual intensity-intensity correlation

Inventors: Yahong Chen (Suzhou, CN); Zhaofeng Huang (Suzhou, CN); Fei Wang (Suzhou, CN); Yangjian Cai (Suzhou, CN)
Assignee: SOOCHOW UNIVERSITY
G01J9/0215G01B9/02011G01B9/02072G01J1/4257G01B2290/70G01J2009/0211
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Quick Facts
Patent No.
US 11,366,017
App. No.
17/252,978
Granted
Jun 21, 2022
Kind
B2
Abstract

The invention discloses a method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation, including the steps of: building a test optical path; rotating a quarter-wave plate to enable the fast axis of the quarter-wave plate to be consistent with a polarization direction of reference light, to obtain light intensity distribution information of a first combined light; rotating the quarter-wave plate to enable the slow axis of the quarter-wave plate to be consistent with the polarization direction of the reference light, to obtain light intensity distribution information of a second combined light; blocking the reference light to obtain light intensity distribution information of to-be-tested light; blocking the to-be-tested light to obtain light intensity distribution information of the reference light; and calculating the amplitude and phase of a complex degree of coherence of the to-be-tested light.

Claims (362)

1. A method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation, comprising steps of:

building a test optical path comprising a quarter-wave plate, a beam splitter, a condensing element, and a light detector, using a laser as reference light, wherein the reference light is modulated by the quarter-wave plate and then enters the beam splitter, and to-be-tested light enters the beam splitter at the same time, the beam splitter combines the modulated reference light and the to-be-tested light to obtain combined light, and the combined light passes through the condensing element to be imaged on the light detector;

rotating the quarter-wave plate to enable the fast axis of the quarter-wave plate to be consistent with a polarization direction of the reference light to obtain first combined light, and photographing and recording light intensity distribution information I S (1) (r) of the first combined light by using the light detector;

rotating the quarter-wave plate to enable the slow axis of the quarter-wave plate to be consistent with the polarization direction of the reference light to obtain second combined light, and photographing and recording light intensity distribution information I S (2) (r) of the second combined light by using the light detector;

blocking the reference light, and photographing and recording light intensity distribution information I(r) of the to-be-tested light by using the light detector;

blocking the to-be-tested light, and photographing and recording light intensity distribution information S r (r) of the reference light by using the light detector; and

calculating the amplitude and phase of a complex degree of coherence of the to-be-tested light.

2. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 1 , wherein calculating the amplitude and phase of a complex degree of coherence of the to-be-tested light comprises the following steps:

S61: calculating a mutual correlation G S (1,2) (r 1 ,r 2 ) between the light intensity distribution information I S (1) (r) of the first combined light and the light intensity distribution information I S (2) (r) of the second combined light;

S62: calculating a mutual correlation G B (1,2) (r 1 ,r 2 ) obtained by adding the reference light and the to-be-tested light;

S63: calculating a difference value ΔG (1,2) (r 1 ,r 2 ,Δϕ) between the two mutual correlations G S (1,2) (r 1 ,r 2 ) and G B (1,2) (r 1 ,r 2 ); and

S64: analyzing the difference value ΔG (1,2) (r 1 ,r 2 ,Δϕ) between the two mutual correlations, to obtain the amplitude and phase of the complex degree of coherence of the to-be-tested light.

3. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 1 , wherein S61 comprises:

according to a second-order coherence matrix in the space-frequency domain, representing, by using a cross-spectral density function, a second-order statistical feature of the to-be-tested light as:

W ( r 1 ,r 2 )= E *( r 1 ) E ( r 2 )   (1),

wherein E(r) represents a random electrical field at a point r in a space, a superscript asterisk represents a complex conjugate, an angle bracket represents ensemble averaging, and in this case, a complex spatial degree of coherence between two points r 1 and r 2 in the space may be defined as:

μ

(

r

1

,

r

2

)

=

W

(

r

1

,

r

2

)

S

(

r

1

)

S

(

r

2

)

,

(

2

)

wherein S(r)=W(r,r)= I(r) represents average light intensity of a random optical field at the point r in the space;

in the step of rotating the quarter-wave plate to enable the fast axis of the quarter-wave plate to be consistent with a polarization direction of the reference light, an electrical field of the reference light obtained through modulation by using the quarter-wave plate is denoted as E r (1) (r), in the step of “rotating the quarter-wave plate to enable the slow axis of the quarter-wave plate to be consistent with the polarization direction of the reference light”, an electrical field of the reference light obtained through modulation by using the quarter-wave plate is denoted as E r (2) (r), and an electrical field of the to-be-tested light is denoted as E(r);

there is a phase difference of

π

2

between the electrical fields E r (1) (r) and E r (2) (r), that is:

Δϕ

=

Arg

[

E

r

(

1

)

(

r

)

]

-

Arg

[

E

r

(

2

)

(

r

)

]

=

π

2

,

(

3

)

wherein Arg represents calculating the phase of a complex function;

an electrical field E S (1) (r) of the first combined light and an electrical field E S (2) (r) of the second combined light are represented as follows:

E S (1) ( r )= E ( r )+ E r (1) ( r )  (4),

E S (2) ( r )= E ( r )+ E r (2) ( r )  (5),

the mutual correlation between the light intensity distribution information I S (1) (r) of the first combined light and the light intensity distribution information I S (2) (r) of the second combined light is:

G S (1,2) ( r 1 ,r 2 )= I S (1) ( r 1 ) I S (2) ( r 2 )   (6), and

according to theorem of Gaussian statistics, Formula (1) to Formula (5) are substituted into Formula (6), to obtain:

G S (1,2) ( r 1 ,r 2 )= G S (1,2) ( r 1 ,r 2 ,Δϕ)= S S (1) ( r 1 ) S S (2) ( r 2 )+| W ( r 1 ,r 2 )| 2 +2√{square root over ( S r (1) ( r 1 ) S r (2) ( r 2 ))} Re [ e iΔϕ W ( r 1 ,r 2 )]  (7).

4. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 3 , wherein S62 comprises:

G

B

(

1

,

2

)

(

r

1

,

r

2

)

=

[

S

r

(

1

)

(

r

1

)

+

I

(

r

1

)

]

[

S

r

(

2

)

(

r

2

)

+

I

(

r

2

)

]

=

S

S

(

1

)

(

r

1

)

S

S

(

2

)

(

r

2

)

+

|

W

(

r

1

,

r

2

)

|

2

.

(

8

)

5. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 4 , wherein S63 comprises:

Δ G S (1,2) ( r 1 ,r 2 ,Δϕ)= G S (1,2) ( r 1 ,r 2 ,Δϕ)− G B (1,2) ( r 1 ,r 2 )=√{square root over ( S r (1) ( r 1 ) S r (2) ( r 2 ))} Re [ e iΔϕ W ( r 1 ,r 2 )]  (9).

6. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 5 , wherein S64 comprises:

for ΔG (1,2) (r 1 ,r 2 ,Δϕ), taking a distribution Δϕ to be 0 and

π

2

,

and obtaining the real part and the imaginary part of the complex degree of coherence according to Formula (2):

Re

[

μ

(

r

1

,

r

2

)

]

=

Δ

G

(

1

,

2

)

(

r

1

,

r

2

,

Δϕ

=

0

)

2

S

r

(

1

)

(

r

1

)

S

r

(

2

)

(

r

2

)

S

(

r

1

)

S

(

r

2

)

,

(

10

)

Im

[

μ

(

r

1

,

r

2

)

]

=

Δ

G

(

1

,

2

)

(

r

1

,

r

2

,

Δϕ

=

π

2

)

2

S

r

(

1

)

(

r

1

)

S

r

(

2

)

(

r

2

)

S

(

r

1

)

S

(

r

2

)

,

(

11

)

in the foregoing formulas, Im represents calculating the imaginary part of the complex function, and obtaining the amplitude and phase of the complex degree of coherence of the to-be-tested light by using Formula (10) and Formula (11).

7. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 1 , wherein the light detector is a charge-coupled device (CCD) or a complementary metal-oxide-semiconductor (CMOS).

8. The method for measuring a complex degree of coherence of a random optical field by using a mutual intensity-intensity correlation according to claim 1 , wherein the reference light is emitted by a helium-neon laser.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 16, 2020
From: CHEN, YAHONG; HUANG, ZHAOFENG; WANG, FEI; CAI, YANGJIAN
To: SOOCHOW UNIVERSITY
Reel/Frame 054670/0595 →
Priority Claims (1)
CN 201910791478.3 · Aug 26, 2019 · national
Continuity (1)
Related Publication 20210278283A1 · Sep 9, 2021