Claims Analysis
Total Claims: 6
Claim 1
Independent Claim
196 words
A method for initially adjusting a phase comparator for a desired initial condition of the phase of a first plane-polarized light beam along a first path with respect to a second plane-polarized light beam of the same frequency along a second path different from said first path comprising the steps of placing said first light beam in a circularly polarized form, directing said circularly polarized beam through a half-wave plate capable of having its optic axis rotated through an angle for shifting the phase of said circularly polarized beam as a function of said angle, and passing said circularly polarized and phase-shifted beam through a first polarizer, detecting the light passed by said first polarizer to produce at a first detector a first electrical signal having a phase that depends on the orientation of said half-wave plate, passing said second beam through a second polarizer to produce at a second detector a second electrical signal having a phase that depends on the phase of said second beam, comparing the phase of the two electrical signals thus produced, and rotating said half-wave plate to bring two electrical signals into the desired initial condition of being in phase.
Claim 2
Independent Claim
196 words
A method for initially adjusting a phase comparator for a desired initial condition of the phase of a first plane-polarized light beam along a first path with respect to a second plane-polarized light beam of the same frequency along a second path different from said first path comprising the steps of placing said first light beam in a circularly polarized form, directing said circularly polarized beam through a half-wave plate capable of having its optic axis rotated through an angle for shifting the phase of said circularly polarized beam as a function of said angle, and passing said circularly polarized and phase-shifted beam through a first polarizer, detecting the light passed by said first polarizer to produce at a first detector a first electrical signal having a phase that depends on the orientation of said half-wave plate, passing said second beam through a second polarizer to produce at a second detector a second electrical signal having a phase that depends on the phase of said second beam, comparing the phase of the two electrical signals thus produced, and rotating said half-wave plate to bring two electrical signals into the desired initial condition of being in phase.
Claim 3
Dependent Claim
81 words
A method as defined in claim 1 wherein said first light beam is comprised of two orthogonal plane-polarized components at two distinct frequencies with a predetermined constant frequency difference, and said second light beam is comprised of two orthogonal plane-polarized components at two distinct frequencies with said predetermined constant frequency difference, and where said first beam is placed in a circularly polarized form by a quarter-wave plate having its optic axis at 45° with respect to the two orthogonally polarized components.
Claim 4
Dependent Claim
205 words
Apparatus for adjusting the phase of a first coherent light beam along a first path with respect to a second coherent light beam of the same frequency along a second path different from said first path, comprising means for placing said first coherent light beam in a circularly polarized form, a half-wave plate in the path of said circularly polarized coherent light beam, said half-wave plate being capable of having its optic axis rotated through an angle for the phase of said circularly coherent beam to be shifted as a function of said angle, a first polarizer in the path of said circularly polarized and phase shifted components, means for detecting the light passed by said first polarizer to produce a first electrical signal having a phase that depends on the orientation of said half-wave plate, a second polarizer in the path of said second coherent light beam, means for detecting light passed through said second polarizer to produce a second electrical signal having a phase that depends on the phase of said second coherent light beam, and means for comparing the phase of the two electrical signals thus produced, whereby said half-wave plate may be rotated to bring said two electrical signals into phase.
Claim 5
Dependent Claim
205 words
Apparatus for adjusting the phase of a first coherent light beam along a first path with respect to a second coherent light beam of the same frequency along a second path different from said first path, comprising means for placing said first coherent light beam in a circularly polarized form, a half-wave plate in the path of said circularly polarized coherent light beam, said half-wave plate being capable of having its optic axis rotated through an angle for the phase of said circularly coherent beam to be shifted as a function of said angle, a first polarizer in the path of said circularly polarized and phase shifted components, means for detecting the light passed by said first polarizer to produce a first electrical signal having a phase that depends on the orientation of said half-wave plate, a second polarizer in the path of said second coherent light beam, means for detecting light passed through said second polarizer to produce a second electrical signal having a phase that depends on the phase of said second coherent light beam, and means for comparing the phase of the two electrical signals thus produced, whereby said half-wave plate may be rotated to bring said two electrical signals into phase.
Claim 6
Dependent Claim
84 words
Apparatus as defined by claim 3 wherein said first light beam is comprised of two orthogonal plane-polarized components at two distinct frequencies with a predetermined constant frequency difference, and said second light beam is comprised of two orthogonal plane-polarized components at two distinct frequencies with said predetermined constant frequency difference, and where said means for placing said first beam in a circularly polarized form is comprised of a quarter-wave plate having its optic axis at 45° with respect to the two orthogonally polarized components.