Frequency shifted cavity for electromagnetic radiation

Claim 2

An electromagnetic radiation frequency shifting apparatus comprising: (1) electromagnetic radiation directing means for directing radiation in a predetermined optical cavity configuration; and (2) electromagnetic radiation frequency shifter means positioned in said predetermined optical cavity configuration so that when a diffraction limited beam of electromagnetic radiation is directed to said electromagnetic radiation frequency shifter means, a portion of said radiation from said diffraction limited beam of electromagnetic radiation which emerges from said electromagnetic radiation frequency shifter means, having its frequency shifted, is also directed to said electromagnetic radition frequency shifter means by said electromagnetic radiation directing means along essentially the same predetermined optical cavity configuration and in essentially the same direction as said diffraction limited beam of electromagnetic radiation so as to have essentially the same polarization as said diffraction limited beam of electromagnetic radiation.

Claim 3

The apparatus according to claim 1 wherein said electromagnetic radiation directing means define an optical cavity wherein the geometric configuration of the cavity has a discrete set of modes represented by ##EQU12## wherein, B is the amplitude of the field, T is the time, c is the speed of lighting a vacuum; w is the amount by which the angular frequency of a beam I is shifted by said electromagnetic radiation frequency shifter means; x is the optical path length to the point at which F M (x, T) is being evaluated, wherein x is positive when measured in the direction of propagation of a beam II and negative when measured in the direction opposite thereto; L is the total optical path length as measured along said beam II for one round trip of said predetermined optical cavity configuration; M is the number of discrete cavity modes and is an integer; τ is the amount of time taken for the electromagnetic radiation to make one round trip of the cavity along the path of said beam II, wherein τ equals L/c; ρ is an arbitrary phase term and remains constant for all values of x and T; Ω is a constant which is determined by the phase of an acoustic wave at T=0; and exp is an abbreviation which indicates that the quantity immediately following in brackets is to be considered as the exponent of e.

Claim 4

The apparatus according to claim 1 wherein the electromagnetic radiation directing means is selected from the group consisting of mirrors, folding prisms, optical fibers, or combinations thereof.

Claim 5

The apparatus according to claim 3 wherein said electromagnetic radiation frequency shifter means is an acousto-optic Bragg cell and power supply means to power said acousto-optic Bragg cell.

Claim 6

The apparatus according to claim 4 further comprising means for adjusting the degree of output coupling by said Bragg cell.

Claim 7

The apparatus according to claim 5 wherein said means for adjusting the degree of output coupling by the Bragg cell adjusts the orientation of said Bragg cell.

Claim 8

The apparatus according to claim 5 wherein said means for adjusting the degree of output coupling by the Bragg cell adjusts the intensity of the acoustic wave within the Bragg cell.

Claim 9

The apparatus according to claim 5 further comprising an optical amplifier positioned in the path of the electromagnetic radiation, said optical amplifier selected to have sufficient optical gain to cause oscillation of a cavity mode.

Claim 10

The apparatus according to claim 8 further comprising an etalon placed within the formed optical cavity to suppress the excitation of at least one cavity mode.

Claim 11

The apparatus according to claim 9 further comprising a second acoustic-optic Bragg cell located within the path of electromagnetic radiation and positioned to compensate for the change in the non-zero diffraction order deflection angle resulting from a change in the frequency of the acoustic wave within said acousto-optic Bragg cell.

Claim 12

The apparatus according to claim 10 further comprising an optical diode in the path of electromagnetic radiation.

Claim 15

The apparatus according to claim 13, wherein the electromagnetic radiation is directed along a polygonal geometric path.

Claim 16

The apparatus according to claim 1 further comprising an output coupling means and an optical amplifier so positioned in the path of the electro-magnetic radiation and so selected to have sufficient optical gain within cavity to cause oscillation of a cavity mode.

Claim 17

The apparatus according to claim 1 wherein said electromagnetic radiation frequency shifter means is an acousto-optic Bragg cell and power supply means to power said acousto-optic Bragg cell.

Claim 18

The apparatus according to claim 4, 5, 8, 9, 10, 11, or 16 further comprising beamsteering means for maintaining the diffraction limited beam within the spectral region of Bragg cell.

Claim 21

The apparatus according to claim 18 wherein said electromagnetic radiation directing means comprise at least two mirrors.

Claim 22

The apparatus according to claim 19 further comprising at least one etalon in said configuration to suppress the excitation of at least one cavity mode.

Claim 23

The apparatus according to claim 20 wherein said etalon is tunable to suppress one or more different cavity modes.

Claim 24

The apparatus according to claim 20 further comprising an optical diode in said configuration to suppress the oscillation of cavity modes having radiation traveling in one of the directions within said configuration.

Claim 25

The apparatus according to claim 22, further comprising means for adjusting the degree of the output coupling of said Bragg cell.

Claim 31

The method according to claim 26 wherein a portion of the electromagnetic radiation is shifted by an acousto-optic Bragg cell.

Claim 32

The method according to claim 27 further comprising adjusting the output portion of the electromagnetic radiation from said ring cavity with said Bragg cell.

Claim 33

The method according to claim 28 wherein adjusting the output portion of the Bragg cell adjusts the intensity of the acoustic wave within the Bragg cell.

Claim 34

The method according to claim 29 further comprising suppressing the excitation of at least one cavity mode.

Claim 35

The method according to claim 30 further comprising adjusting for the change in the non-zero diffraction order deflection angle resulting from a change in the frequency of the acoustic wave within the Bragg cell.

Claim 36

The method according to claim 31 further comprising beamsteering the acoustic-wave within said Bragg cell.

Claim 37

The method according to claim 32 further comprising suppressing the cavity modes having radiation traveling in one of the directions within said configuration.

Claim 38

The method according to claim 24 further comprising amplifying the shifted portion of said electromagnetic radiation to cause oscillation of a cavity mode.