Laser radar system

Claim 2

A laser radar method for detecting stationary and movable objects and for measuring velocity, the method comprising the steps of: illuminating the object with a laser transmitted beam generated by a laser defining a laser resonator thereby causing laser light to be backscattered from the object; generating a laser beam with a laser defining a laser resonator containing a medium with the resonator having a first natural frequency corresponding to a transversal mode thereof and a second natural frequency corresponding to a longitudinal mode thereof; passing the laser beam through a λ/4-phase shifter and illuminating the object with the laser beam thereby causing light to be backscattered from the object; passing the backscattered light through a frequency shifter for imparting a frequency offset to the backscattered light; selecting the frequency shifter to have a predetermined doubled modulation frequency which corresponds to one of said first and second natural frequencies; coupling the backscattered laser light into the laser resonator; and, passing the backscattered light from the laser resonator to an optical element for defining the polarization direction of the backscattered light and a polarizer whereafter the backscattered light is passed to and detected by an optical heterodyne receiver.

Claim 3

The laser radar method of claim 1, the method comprising the further step of collinearly passing the laser transmitted beam and the reflected light through a scanner to determine the spatial coordinates of the object.

Claim 4

The laser radar method of claim 1, wherein the frequency shifter is a Bragg cell.

Claim 5

A laser radar apparatus for detecting stationary and movable objects and for measuring velocity, the apparatus comprising: a laser for generating a laser transmitted beam; a telescope for directing the laser transmitted beam toward the object thereby producing a reflected laser light; an optical heterodyne receiver; said laser defining a beam axis and being disposed between said heterodyne receiver and said telescope; a λ/4-phase shifter arranged on said beam downstream of said laser viewed in the direction of said laser transmitted beam; said laser including a resonator for receiving and passing the reflected laser light to said heterodyne receiver; and, a laser active medium for interacting with the reflected laser light to produce an amplification effect thereby providing an improved signal-to-noise ratio; said resonator further including a first out-coupling element arranged on said beam axis so as to be disposed between said laser active medium and said telescope and a second out-coupling element arranged between said laser active medium and said heterodyne receiver; a polarizer disposed between said second out-coupling element and said heterogyne receiver; said second out-coupling element being an optical element for defining the polarization direction of the laser reflected light passed to said heterodyne receiver; said heterodyne receiver being disposed directly rearward of said second out-coupling element; a frequency shifter mounted on said beam axis between said laser and said telescope for imparting a frequency offset to said reflected laser light; and, said frequency shifter having a predetermined doubled modulation frequency and said resonator having a first natural frequency corresponding to a transversal mode thereof and a second natural frequency corresponding to a longitudinal mode thereof, and said doubled modulation frequency being selected so as to correspond to one of said first and second natural frequencies.

Claim 6

A laser radar apparatus for detecting stationary and movable objects and for measuring velocity, the apparatus comprising: a laser for generating a laser transmitted beam; a telescope for directing the laser transmitted beam toward the object thereby producing a reflected laser light; an optical heterodyne receiver; said laser defining a beam axis and being disposed between said heterodyne receiver and said telescope; a λ/4-phase shifter arranged on said beam downstream of said laser viewed in the direction of said laser transmitted beam; said laser including a resonator for receiving and passing the reflected laser light to said heterodyne receiver; and, a laser active medium for interacting with the reflected laser light to produce an amplification effect thereby providing an improved signal-to-noise ratio; said resonator further including a first out-coupling element arranged on said beam axis so as to be disposed between said laser active medium and said telescope and a second out-coupling element arranged between said laser active medium and said heterodyne receiver; a polarizer disposed between said second out-coupling element and said heterogyne receiver; said second out-coupling element being an optical element for defining the polarization direction of the laser reflected light passed to said heterodyne receiver; said heterodyne receiver being disposed directly rearward of said second out-coupling element; a frequency shifter mounted on said beam axis between said laser and said telescope for imparting a frequency offset to said reflected laser light; and, said frequency shifter having a predetermined doubled modulation frequency and said resonator having a first natural frequency corresponding to a transversal mode thereof and a second natural frequency corresponding to a longitudinal mode thereof, and said doubled modulation frequency being selected so as to correspond to one of said first and second natural frequencies.

Claim 7

The laser radar apparatus of claim 4, said second out-coupling element being a polarization selective out-coupling element having different reflectivities and transmissions for different polarization directions of the reflected laser light.

Claim 8

The laser radar apparatus of claim 5, one of said out-coupling elements being a reflection grating in a Littrow arrangement.

Claim 9

The laser radar apparatus of claim 4, said second out-coupling element being a polarization selective out-coupling element having different reflectivities and transmissions for different polarization directions of the reflected laser light.

Claim 10

The laser radar apparatus of claim 7, said resonator being dimensioned so as to cause only low intercavity losses except for the mirror transmission.

Claim 11

The laser radar apparatus of claim 8, wherein the transmission of said resonator at the end thereof facing toward said heterodyne receiver is selected so as to cause said heterodyne receiver to operate at the quantum noise limit and below saturation.

Claim 12

The laser radar apparatus of claim 9, wherein the transmission of said resonator at the end thereof facing toward the object is selected so as to cause the laser to operate so close to the threshold that a reproducible operation is just still possible.

Claim 13

The laser radar apparatus of claim 10, said laser being a CO 2 -laser.

Claim 14

The laser radar apparatus of claim 4, wherein said frequency shifter is a Bragg cell.

Claim 15

A laser radar method for detecting stationary and movable objects and for measuring velocity, the method comprising the steps of: illuminating the object with a laser transmitted beam generated by a laser defining a laser resonator containing a medium thereby causing laser light to be backscattered from the object; generating a laser beam with a laser defining a laser resonator containing a medium with the resonator having a first natural frequency corresponding to a transversal mode thereof and a second natural frequency corresponding to a longitudinal mode thereof; passing the laser beam through a λ/4-phase shifter and illuminating the object with the laser beam thereby causing light to be backscattered from the object; passing the backscattered light through a frequency shifter for imparting a frequency offset to the backscattered light; selecting the frequency shifter to have a predetermined doubled modulation frequency which corresponds to one of said first and second natural frequencies; coupling the backscattered laser light into the laser resonator for interacting with the laser medium to produce an amplification effect thereby providing an improved signal-to-noise ratio; and, passing the backscattered light from the laser resonator to an optical element for defining the polarization direction of the backscattered light and a polarizer whereafter the backscattered light is passed to and detected by an optical heterodyne receiver.

Claim 16

A laser radar method for detecting stationary and movable objects and for measuring velocity, the method comprising the steps of: illuminating the object with a laser transmitted beam generated by a laser defining a laser resonator containing a medium thereby causing laser light to be backscattered from the object; generating a laser beam with a laser defining a laser resonator containing a medium with the resonator having a first natural frequency corresponding to a transversal mode thereof and a second natural frequency corresponding to a longitudinal mode thereof; passing the laser beam through a λ/4-phase shifter and illuminating the object with the laser beam thereby causing light to be backscattered from the object; passing the backscattered light through a frequency shifter for imparting a frequency offset to the backscattered light; selecting the frequency shifter to have a predetermined doubled modulation frequency which corresponds to one of said first and second natural frequencies; coupling the backscattered laser light into the laser resonator for interacting with the laser medium to produce an amplification effect thereby providing an improved signal-to-noise ratio; and, passing the backscattered light from the laser resonator to an optical element for defining the polarization direction of the backscattered light and a polarizer whereafter the backscattered light is passed to and detected by an optical heterodyne receiver.

Claim 17

The laser radar apparatus of claim 13, wherein said frequency shifter is a Bragg cell.