Method and apparatus for determining the wave number of optical spectrum radiation

Claim 3

A method according to claim 1, wherein the two parts of said beam are provided by spatially dividing said beam into two parallel parts.

Claim 4

A method according to claim 1, wherein the two parts of said beam are provided by two right-angle polarized components of said beam.

Claim 5

A method according to claim 1, wherein the processing of the two electrical sinusoidal waves further comprises dividing said two electrical sinusoidal waves by a signal proportional to the intensity of illumination of said source of radiation and subtracting the constant "1" to obtain first sine and cosine electrical waves in quadrature.

Claim 6

A method according to claim 4, further comprising feeding the first sine and cosine waves to input terminals of an oscilloscope screen to obtain a revolving spot, the position of the spot on its circle of revolution being an indication of σ modulo 1/δ.

Claim 7

A method according to claim 4, for use in obtaining a continuous measurement of the frequency of said source of radiation which is a laser, further comprising the steps of providing second sine and cosine waves having the same phase difference, multiplying the first sine and cosine waves by second sine and cosine waves respectively, adding the products of multiplication of said sine and cosine waves, converting the sum of the products of multiplication into a rectangular waveform, detecting the phase difference of the rectangular waveform with a reference signal to obtain a signal strictly proportional to the phase difference between said first and second waves, using the strictly proportional signal to make the phase difference of said second waves to depend constantly on that of said first waves and to determine the value of the phase difference of said first waves which is proportional to the frequency of said laser, and carrying out the aforesaid steps simultaneously for different values of δ to eliminate uncertainty in the measurement of the frequency of said laser.

Claim 8

A method according to claim 6, providing measurements of the wave number with an optical path length differences δ in geometric progression.

Claim 9

A method according to claim 4, for use in controlling the frequency of said source of radiation which is a laser, further comprising the steps of providing second sine and cosine waves having the same phase difference, multiplying said first sine and cosine waves by said second sine and cosine waves respectively, adding the products of multiplication of said sine and cosine waves, converting the sum of the products of multiplication into a rectangular waveform, detecting the phase difference of the rectangular waveform with a reference signal to obtain a signal strictly proportional to the phase difference between said first and second waves, using said strictly proportional signal for controlling the frequency of said laser while maintaining the phase of the first waves proportional to the frequency of said laser constantly equal to the phase difference of said second waves.

Claim 10

Apparatus for determining the wave number of optical spectrum radiation comprising a source of optical spectrum radiation providing a beam, a double Michelson interferometer including a plane-parallel transparent plate receiving part of said beam and directing two parallel beams to a combined beam splitter and compensator, including a double (plane-parallel) transparent plate, said interferometer having an arm including another plane-parallel transparent plate supporting a thin phase shifting coating disposed along the optical path of one of said two parallel beams and a fixed mirror, and another arm of said interferometer including a compensating plane-parallel transparent plate and a fixed mirror mounted at a distance from the image of the mirror in the first arm of the interferometer of δ/2, the plane parallel plate supporting said phase shifting coating being disposed at an adjustable angle to introduce an additional optical path length difference Δδ equal to λ/4 between said two parallel beams, two detectors arranged along the paths of said two beams, a third detector receiving another part of said beam from said source of radiation, a divider and subtractor circuit connected to output terminals of the two detectors and the third detector, and a display device connected to said divider and subtractor circuit.

Claim 11

Apparatus for determining the wave number of optical spectrum radiation comprising a source of optical spectrum radiation providing a beam, a double Michelson interferometer including a plane-parallel transparent plate receiving part of said beam and directing two parallel beams to a combined beam splitter and compensator, including a double (plane-parallel) transparent plate, said interferometer having an arm including another plane-parallel transparent plate supporting a thin phase shifting coating disposed along the optical path of one of said two parallel beams and a fixed mirror, and another arm of said interferometer including a compensating plane-parallel transparent plate and a fixed mirror mounted at a distance from the image of the mirror in the first arm of the interferometer of δ/2, the plane parallel plate supporting said phase shifting coating being disposed at an adjustable angle to introduce an additional optical path length difference Δδ equal to λ/4 between said two parallel beams, two detectors arranged along the paths of said two beams, a third detector receiving another part of said beam from said source of radiation, a divider and subtractor circuit connected to output terminals of the two detectors and the third detector, and a display device connected to said divider and subtractor circuit.

Claim 12

An apparatus according to claim 9, wherein output terminals of said divider and subtractor circuit are connected to multiplier circuits which are in turn connected to an adder and shaper circuit, the adder and shaper circuit being connected to a phase detection circuit which in turn is connected to a frequency converter, the frequency converter being connected to two dividers which are supplied by pulses from a pulse generator, one of said dividers being connected to the multiplier circuits through a double filter, and a display device being provided for viewing indications from said phase detection circuit.

Claim 13

An apparatus according to claim 9, wherein the outputs of the divider and subtractor circuit are connected to multiplier circuits which are in turn connected to an adder and shaper circuit, the adder and shaper circuit being connected to a phase detection circuit which in turn is connected to a phase shift control circuit connected to two dividers, a pulse generator, supplying pulses to said two dividers, said phase detection circuit being connected to means for controlling the frequency of said source which is a laser, and said phase shift control circuit providing additional phase shift pulses to said two dividers.

Claim 16

An apparatus according to claim 12, wherein output terminals of said divider and subtractor circuit are connected to multiplier circuits which are in turn connected to an adder and shaper circuit, the adder and shaper circuit being connected to a phase detection circuit which in turn is connected to a frequency converter, the frequency converter being connected to two dividers which are supplied by pulses from a pulse generator, one of said dividers being connected to the multiplier circuits through a double filter, and a display device being provided for viewing indications from said phase detection circuit.

Claim 17

An apparatus according to claim 12 wherein the outputs of the divider and subtractor circuit are connected to multiplier circuits which are in turn connected to an adder and shaper circuit, the adder and shaper circuit being connected to a phase detection circuit which in turn is connected to a phase shift control circuit connected to two dividers, a pulse generator, supplying pulses to said two dividers, said phase detection circuit being connected to means for controlling the frequency of said source which is a laser, and said phase shift control circuit providing additional phase shift pulses to said two dividers.