Claims Analysis
Total Claims: 16
Claim 1
Independent Claim
163 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and first and second optical gratings situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the gratings, said gratings being plane, one-dimensional, binary phase gratings each having a rectangular groove profile and each having a duty factor of substantially 1:1; characterized in that: the optical path difference, H=(N-1)h, of the first grating is substantially given by H=0.32λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . ; the optical path difference of the second grating is substantially 0.32λ+mλ , where m=0, 1, 2 . . . ; and the two gratings are rotated relative to each other.
Claim 2
Dependent Claim
163 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and first and second optical gratings situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the gratings, said gratings being plane, one-dimensional, binary phase gratings each having a rectangular groove profile and each having a duty factor of substantially 1:1; characterized in that: the optical path difference, H=(N-1)h, of the first grating is substantially given by H=0.32λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . ; the optical path difference of the second grating is substantially 0.32λ+mλ , where m=0, 1, 2 . . . ; and the two gratings are rotated relative to each other.
Claim 3
Dependent Claim
162 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and first and second optical gratings situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the gratings, and gratings being plane, one-dimensional, binary phase gratings each having a rectangular groove profile and each having a duty factor of substantially 1:1; characterized in that: the optical path difference, H=(N-1)h, of the first grating is substantially given by H=0.32λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . ; the optical path difference of the second grating is substantially 0.5λ+mλ, where m=0, 1, 2 . . . ; and the two gratings are rotated relative to each other.
Claim 4
Dependent Claim
162 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and first and second optical gratings situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the gratings, and gratings being plane, one-dimensional, binary phase gratings each having a rectangular groove profile and each having a duty factor of substantially 1:1; characterized in that: the optical path difference, H=(N-1)h, of the first grating is substantially given by H=0.32λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . ; the optical path difference of the second grating is substantially 0.5λ+mλ, where m=0, 1, 2 . . . ; and the two gratings are rotated relative to each other.
Claim 5
Dependent Claim
162 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and first and second optical gratings situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the gratings, said gratings being plane, one-dimensional, binary phase gratings each having a rectangular groove profile and each having a duty factor of substantially 1:1; characterized in that: the optical path difference, H=(N-1)h, of the first grating is substantially given by H=0.5λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . ; the optical path difference of the second grating is substantially 0.5λ+mλ, where m=0, 1, 2 . . . ; and the two gratings are rotated relative to each other.
Claim 6
Dependent Claim
162 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and first and second optical gratings situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the gratings, said gratings being plane, one-dimensional, binary phase gratings each having a rectangular groove profile and each having a duty factor of substantially 1:1; characterized in that: the optical path difference, H=(N-1)h, of the first grating is substantially given by H=0.5λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . ; the optical path difference of the second grating is substantially 0.5λ+mλ, where m=0, 1, 2 . . . ; and the two gratings are rotated relative to each other.
Claim 7
Dependent Claim
36 words
An optical power divider as claimed in claim 1, 2, or 3, characterized in that the imaging devices are Selfoc lenses having a common optical axis, and the phase gratings are perpendicular to the optical axis.
Claim 8
Dependent Claim
27 words
An optical power divider as claimed in claim 4, characterized in that the angle at which the gratings are rotated relative to each other is substantially 60°.
Claim 9
Dependent Claim
27 words
An optical power divider as claimed in claim 5, characterized in that at least one grating is formed on an end of one of the Selfoc lenses.
Claim 10
Dependent Claim
22 words
An optical power divider as claimed in claim 6, characterized in that both gratings are formed in ends of the Selfoc lenses.
Claim 11
Dependent Claim
31 words
An optical power divider as claimed in claim 6, characterized in that both gratings are formed in an end of one of the Selfoc lenses to produce a two-dimensional checkerboard-like grating.
Claim 12
Dependent Claim
20 words
An optical power divider as claimed in claim 8, characterized in that the phase gratings are formed by reactive sputtering.
Claim 13
Dependent Claim
127 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and an optical grating situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the grating; characterized in that: the grating is a plane, one-dimensional, binary phase grating having a rectangular groove profile and having a duty factor of substantially 1:1; and the optical path difference, H=(N-1)h, is substantially given by H=0.32λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . .
Claim 14
Dependent Claim
127 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and an optical grating situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the grating; characterized in that: the grating is a plane, one-dimensional, binary phase grating having a rectangular groove profile and having a duty factor of substantially 1:1; and the optical path difference, H=(N-1)h, is substantially given by H=0.32λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . .
Claim 15
Dependent Claim
127 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and an optical grating situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the grating; characterized in that: the grating is a plane, one-dimensional, binary phase grating having a rectangular groove profile and having a duty factor of substantially 1:1; and the optical path difference, H=(N-1)h, is substantially given by H=0.5λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . .
Claim 16
Dependent Claim
127 words
An optical power divider comprising: first and second imaging devices, each of which can convert a point light source into parallel rays and can convert parallel rays into a point light source; and an optical grating situated between the imaging devices such that parallel rays, produced by the imaging devices from point light sources, will pass through the grating; characterized in that: the grating is a plane, one-dimensional, binary phase grating having a rectangular groove profile and having a duty factor of substantially 1:1; and the optical path difference, H=(N-1)h, is substantially given by H=0.5λ+nλ, where N is the refractive index of the grating material, h is the grating height, λ is the wavelength of the light being divided, and n=0, 1, 2 . . . .