Array illuminator using a binary optics phase plate

Claim 2

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance from said phase plate, said array of illuminated spots having a fill factor in at least one dimension that is less than 1/3; and a spacer assembly installed on the phase plate, said spacer assembly defining an image plane disposed parallel to and at the preselected distance from the phase plate.

Claim 3

The optical element of claim 1 wherein the preselected distance is mZ t +Z t /2N where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 4

The optical element of claim 2 wherein m equals 0.

Claim 5

The optical element of claim 2 wherein the phase plate is constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU4## where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 6

The optical element of claim 1 wherein the preselected distance is mZ t -Z t /2N where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 7

The optical element of claim 5 wherein m equals 0.

Claim 8

The optical element of claim 5 wherein the phase plate is constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU5## where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 9

The optical element of claim 1 wherein the preselected distance is mZ t +Z t /(2N-1), where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 10

The optical element of claim 1 wherein the preselected distance is mZ t -Z t /(2N-1), where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 11

The optical element of claim 1 wherein the phase plate is a one-dimensional array of constant phase zones.

Claim 12

The optical element of claim 1 wherein the phase plate is constructed from an N×1 unit cell comprising N constant phase zones, the phase φ I associated with each constant phase zone in the unit cell being given by ##EQU6## where N is an integer that is greater than 3 and where I is an index identifying the particular constant phase zone in the unit cell, when N is even, I is an integer ranging from -N/2 to (N/2-1) and when N is odd, I is a half integer ranging from -N/2 to (N/2-1).

Claim 13

The optical element of claim 1 wherein said phase plate comprises an array of constant phase zones.

Claim 14

The optical element of claim 1 further comprising an array of light receivers located in said image plane, each light receiver of said array of light receivers being aligned to be illuminated by a different one of the illuminated spots of said array of illuminated spots.

Claim 15

The optical element of claim 1 further comprising a light source for generating said uniform beam of light.

Claim 16

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a substrate having a top surface and a bottom surface parallel to and separated from the top surface by a preselected distance; and a phase plate formed on the top surface, the phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at the preselected distance from said phase plate; the preselected distance being selected so that illuminating the phase plate with uniform coherent illumination of wavelength λ produces the array of illuminated spots on the bottom surface, the spot array having a fill factor in at least one dimension that is less than 1/3.

Claim 17

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a substrate having a top surface and a bottom surface parallel to and separated from the top surface by a preselected distance; and a phase plate formed on the top surface, the phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at the preselected distance from said phase plate; the preselected distance being selected so that illuminating the phase plate with uniform coherent illumination of wavelength λ produces the array of illuminated spots on the bottom surface, the spot array having a fill factor in at least one dimension that is less than 1/3.

Claim 18

The optical element of claim 15 wherein said phase plate comprises an array of constant phase zones.

Claim 19

The optical element of claim 16 wherein the phase plate is a two-dimensional array of constant phase zones and the spot array has a fill factor of less than 1/9.

Claim 20

The optical element of claim 16 wherein the phase plate is a two-dimensional array of constant phase zones and the spot array has a fill factor of less than 1/9.

Claim 21

The optical element of claim 16 wherein the preselected distance is mZ t +Z t /2N where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 22

The optical element of claim 19 wherein m equals 0.

Claim 23

The optical element of claim 19 wherein the phase plate is constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zones in the unit cell being given by ##EQU7## where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 24

The optical element of claim 16 wherein the preselected distance is mZ t -Z t /2N where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 25

The optical element of claim 22 wherein m equals 0.

Claim 26

The optical element of claim 22 wherein the phase plate is constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU8## where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 27

The optical element of claim 16 wherein the preselected distance is mZ t +Z t /(2N-1 ), where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 28

The optical element of claim 16 wherein the preselected distance is mZ t -Z t /(2N-1), where Z t is the Talbot distance for the phase plate, m is an integer or half integer and N is an integer greater than 3.

Claim 29

The optical element of claim 16 wherein the phase plate is a one-dimensional array of constant phase zones.

Claim 30

The optical element of claim 16 wherein the phase plate is constructed from an N×1 unit cell comprising N constant phase zones, the phase φ I associated with each constant phase zone in the unit cell being given by ##EQU9## where N is an integer that is greater than 3 and where I is an index identifying the particular constant phase zone in the unit cell, when N is even, I is an integer ranging from -N/2 to (N/2-1) and when N is odd, I is a half integer ranging from -N/2 to (N/2-1).

Claim 31

The optical element of claim 15 further comprising an array of light receivers located in said image plane, each light receiver of said array of light receivers being aligned to be illuminated by a different one of the illuminated spots of said array of illuminated spots.

Claim 32

The optical element of claim 15 further comprising a light source for generating said uniform beam of light.

Claim 35

The method of claim 31 wherein the substrate comprises silica.

Claim 36

The method of claim 31 wherein the step of forming a phase plate is done by etching the top surface.

Claim 37

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate comprising an array of constant phase zones, the phases associated with said array of constant phase zones including more than two different values if said phase plate is a one-dimensional phase plate and more than four different values if said phase plate is a two-dimensional phase plate, said phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance from said phase plate; and a spacer assembly installed on the phase plate, said spacer assembly defining an image plane disposed parallel to and at the preselected distance from the phase plate.

Claim 38

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate comprising an array of constant phase zones, the phases associated with said array of constant phase zones including more than two different values if said phase plate is a one-dimensional phase plate and more than four different values if said phase plate is a two-dimensional phase plate, said phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance from said phase plate; and a spacer assembly installed on the phase plate, said spacer assembly defining an image plane disposed parallel to and at the preselected distance from the phase plate.

Claim 39

The optical element of claim 34 wherein the phase plate is constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU10## where N is an integer that is greater than 2 and where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 40

The optical element of claim 34 wherein the phase plate is constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU11## where N is an integer that is greater than 2 and where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 41

The optical element of claim 34 wherein the phase plate is constructed from an N×1 unit cell comprising N constant phase zones, the phase φ I associated with each constant phase zone in the unit cell being given by ##EQU12## where N is an integer that is greater than 2 and where I is an index identifying the particular constant phase zone in the unit cell, when N is even, I is an integer ranging from -N/2 to (N/2-1) and when N is odd, I is a half integer ranging from -N/2 to (N/2-1).

Claim 42

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance from said phase plate, said array of illuminated spots having a fill factor in at least one dimension that is less than 1/3; said phase plate constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU13## where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 43

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance from said phase plate, said array of illuminated spots having a fill factor in at least one dimension that is less than 1/3; said phase plate constructed from an N×N unit cell comprising N 2 constant phase zones, the phase φ I ,J associated with each constant phase zone in the unit cell being given by ##EQU13## where I and J are indexes identifying the particular constant phase zone in the unit cell, when N is even, I and J are integers ranging from -N/2 to (N/2-1) and when N is odd, I and J are half integers ranging from -N/2 to (N/2-1).

Claim 44

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance form said phase plate, said array of illuminated spots having a fill factor in at least one dimension that is less than 1/3; said phase plate constructed from an N×1 unit cell comprising N constant phase zones, the phase φ I associated with each constant phase zone in the unit cell being given by ##EQU14## where N is an integer that is greater than 2 and where I is an index identifying the particular constant phase zone in the unit cell, when N is even, I is an integer ranging from -N/2 to (N/2-1) and when N is odd, I is half integer ranging from -N/2 to (N/2-1).

Claim 45

An optical element for converting a uniform beam of light of wavelength λ into an array of illuminated spots, the optical element comprising: a phase plate for receiving said uniform beam of light of wavelength λ and generating an output beam of light therefrom, said output beam of light producing, through a reverse operation of the Talbot self-imaging phenomenon, an array of illuminated spots at a preselected distance form said phase plate, said array of illuminated spots having a fill factor in at least one dimension that is less than 1/3; said phase plate constructed from an N×1 unit cell comprising N constant phase zones, the phase φ I associated with each constant phase zone in the unit cell being given by ##EQU14## where N is an integer that is greater than 2 and where I is an index identifying the particular constant phase zone in the unit cell, when N is even, I is an integer ranging from -N/2 to (N/2-1) and when N is odd, I is half integer ranging from -N/2 to (N/2-1).