Optical inspection device and method

Claim 2

A closed loop optical gauge comprising: laser means for producing a first beam; means for directing at least a portion of said first beam toward a target from which a beam is reflected; means for providing a reference beam having the frequency of said first beam; frequency shift means receiving said reference beam and receiving a modulation input signal, for providing a shifted reference beam whose frequency is shifted from that of the reference beam in accordance with the modulation input signal; means for producing interference of said shifted reference beam and said reflected beam to produce a beat frequency signal; negative feedback means for utilizing said beat frequency signal to control the frequency of said modulation input signal; whereby the frequency of said shifted reference beam tracks the reference of said reflected beam and has a known relationship to the radial component of velocity of said target.

Claim 3

A closed loop optical gauge as defined in claim 1 and wherein said means for producing interference of said beams comprises: detection means for detecting the envelope of a light beam incident thereon and producing an electrical signal corresponding to the envelope; and means for combining said shifted reference beam and said reflected beam to be incident upon said detection means.

Claim 4

A closed loop optical gauge as defined in claim 1 and wherein said negative feedback means for utilizing said beat frequency signal to control said modulation input signal comprises FM discriminator means receiving said beat frequency signal from said interference means, for controlling a voltage controlled oscillator to track the frequency of said beat frequency signal, the output of said voltage controlled oscillator being arranged to provide said modulation input signal.

Claim 5

A closed loop optical gauge as defined in claim 1 and wherein said means for providing a reference beam having the frequency of said first beam comprises: beam splitter means in said first beam for redirecting a portion of said first beam to said frequency shift means.

Claim 6

A closed loop optical gauge as defined in claim 1 and wherein said frequency shift means comprises acoustooptical modulator means for shifting the frequency of said reference beam by an amount dependent upon the modulation input signal.

Claim 7

A closed loop optical gauge as defined in claim 5 and wherein said acoustooptical modulator means comprises a Raman-Nath acoustooptical modulator.

Claim 8

Apparatus for measuring the distance to an object by optical time of flight measurement, comprising: light source means for providing an envelope modulated light beam directed to impinge upon said reflect from the object, whose envelope has a fundamental first harmonic component and at least one higher harmonic component; first detector means receiving a reference sample of the direct beam, for providing a first detected signal representing the envelope of said reference sample; phase locked loop means receiving said first signal, for locking the phase locked loop to said reference envelope; said loop comprising a controllable oscillator of predetermined output frequency, communicating with a frequency divider having a correspondingly predetermined divisor so that the divider's output frequency is equal to reference envelopes' fundamental frequency; second detector means receiving the beam reflected from the object, for providing a second detected signal representing the envelope of said reflected beam; main phase comparison means receiving (a) the output signal of said controllable oscillator and (b) at least the corresponding harmonic frequency of said second signal, for providing a third signal indicative of the phase difference between them.

Claim 9

Apparatus for measuring the distance to an object by optical time of flight measurement, comprising: light source means for providing an envelope modulated light beam directed to impinge upon said reflect from the object, whose envelope has a fundamental first harmonic component and at least one higher harmonic component; first detector means receiving a reference sample of the direct beam, for providing a first detected signal representing the envelope of said reference sample; phase locked loop means receiving said first signal, for locking the phase locked loop to said reference envelope; said loop comprising a controllable oscillator of predetermined output frequency, communicating with a frequency divider having a correspondingly predetermined divisor so that the divider's output frequency is equal to reference envelopes' fundamental frequency; second detector means receiving the beam reflected from the object, for providing a second detected signal representing the envelope of said reflected beam; main phase comparison means receiving (a) the output signal of said controllable oscillator and (b) at least the corresponding harmonic frequency of said second signal, for providing a third signal indicative of the phase difference between them.

Claim 10

Apparatus as defined in claim 7 and wherein said phase locked loop comprises means for selecting said predetermined oscillator frequency and said corresponding predetermined divisor from among more than one harmonic frequency.

Claim 11

Apparatus as defined in claim 7 and wherein said light source means for providing an envelope modulated beam comprises means for providing a substantially rectangular pulse modulated beam.

Claim 12

Apparatus as defined in claim 7 and wherein said light source means comprises laser means.

Claim 13

Apparatus as defined in claim 7 and wherein said phase locked loop means comprises, in addition to said controllable oscillator; phase lock phase comparison means receiving said first signal and the output signal of said divider, for producing a phase error signal; and frequency selective filter means receiving said phase error signal, for transmitting a predetermined range of frequency components of said phase error signal, and connected to provide a filtered phase error signal to said controllable oscillator.

Claim 14

Apparatus as defined in claim 7 and wherein said main phase comparison means comprises a second frequency selective filter means receiving the phase comparison of said signals (a) and (b), adapted for transmitting a predetermined range of frequency components thereof to constitute said third signal.

Claim 15

Apparatus for measuring the distance to an object by optical time of flight measurement, comprising: pulse laser means for providing a periodic train of pulse envelopes of linearly polarized light in a directed beam, said train of envelopes comprising a fundamental first harmonic component and at least one higher harmonic component; first polarized beam splitter means receiving said directed beam for directly transmitting a portion of it toward the object and redirecting a portion of it to serve as a reference beam; first photodetector means receiving said reference beam from said first polarized beam splitter means, for providing a detected reference signal, in accordance with the envelope of pulses of said reference beam; controllable oscillator means for producing a local signal having the frequency of one of said first and higher harmonic components of said detected reference signal; frequency divider means communicating with the output of said controllable oscillator means, for dividing the frequency thereof by an integer that is the harmonic number of the frequency of the controllable oscillator means relative to the envelope of said pulse train; phase comparison means receiving said detected reference signal and the output signal of said divider, for producing a phase lock error signal in accordance with the phase difference between them; frequency selective filter means receiving said phase lock error signal, for transmitting a predetermined range of frequency components of said phase lock error signal, and having an output connected control the frequency of said controllable oscillator; quarter wave plate means for circularly polarizing said direct portion of beam transmitted toward said object, and linearly polarizing the return beam reflected from said object; polarized second beam splitter means receiving said reflected beam through said quarter wave plate means and redirecting at least a portion to represent said reflected beam; second photodetector means receiving said redirected portion from said second beam splitter means, for providing a second detected signal in accordance with the envelope of pulses of said portion of said reflected beam; phase comparison means receiving (a) the output signal of said controllable oscillator and (b) said second detected signal, for providing a third signal indicative of the phase difference between the output signal of the controllable oscillator and said selected harmonic frequency component of said second detected signal; filter means receiving said third signal, for providing an output signal responsive to the difference in the time of flight of the two signals received by said phase comparison means.

Claim 16

Apparatus for measuring the distance to an object by optical time of flight measurement, comprising: pulse laser means for providing a periodic train of pulse envelopes of linearly polarized light in a directed beam, said train of envelopes comprising a fundamental first harmonic component and at least one higher harmonic component; first polarized beam splitter means receiving said directed beam for directly transmitting a portion of it toward the object and redirecting a portion of it to serve as a reference beam; first photodetector means receiving said reference beam from said first polarized beam splitter means, for providing a detected reference signal, in accordance with the envelope of pulses of said reference beam; controllable oscillator means for producing a local signal having the frequency of one of said first and higher harmonic components of said detected reference signal; frequency divider means communicating with the output of said controllable oscillator means, for dividing the frequency thereof by an integer that is the harmonic number of the frequency of the controllable oscillator means relative to the envelope of said pulse train; phase comparison means receiving said detected reference signal and the output signal of said divider, for producing a phase lock error signal in accordance with the phase difference between them; frequency selective filter means receiving said phase lock error signal, for transmitting a predetermined range of frequency components of said phase lock error signal, and having an output connected control the frequency of said controllable oscillator; quarter wave plate means for circularly polarizing said direct portion of beam transmitted toward said object, and linearly polarizing the return beam reflected from said object; polarized second beam splitter means receiving said reflected beam through said quarter wave plate means and redirecting at least a portion to represent said reflected beam; second photodetector means receiving said redirected portion from said second beam splitter means, for providing a second detected signal in accordance with the envelope of pulses of said portion of said reflected beam; phase comparison means receiving (a) the output signal of said controllable oscillator and (b) said second detected signal, for providing a third signal indicative of the phase difference between the output signal of the controllable oscillator and said selected harmonic frequency component of said second detected signal; filter means receiving said third signal, for providing an output signal responsive to the difference in the time of flight of the two signals received by said phase comparison means.

Claim 19

A method of closed loop optical gauging as defined in claim 14 and wherein said step of interfering said shifted reference beam and said reflected beam comprises: combining said shifted reference beam and said reflected beam to produce a light beam incident upon a detector; and, detecting the envelope of said light beam incident upon the detector and producing an electrical signal corresponding to the envelope.

Claim 20

A method of closed loop optical gauging as defined in claim 14 and wherein the step of utilizing said beat frequency signal to control said modulation input signal comprises; communicating said beat frequency signal to an FM discriminator for controlling the voltage controlled oscillator; and arranging the output of said voltage controlled oscillator to provide said modulation input signal.

Claim 21

A method for closed loop optical gauging as defined in claim 14 and wherein said step of providing a reference beam having the frequency of said first beam comprises: redirecting a portion of said first beam to said modulator with a beam splitter positioned in said first beam.

Claim 22

A method for closed loop optical gauging as defined in claim 14 and wherein said step of modulating said reference beam comprises modulating it in a Raman-Nath acoustooptical modulator.