Fiber optic resonator

Claim 2

A fiber optic resonator, comprising: a strand of optical fiber having first and second end portions, and forming a loop portion between said end portions; fiber optic coupling means for optically closing said loop; and the length of said loop portion selected to cooperate with said coupling means to form a resonant cavity for light propagating therethrough.

Claim 3

A fiber optic resonator, defined in claim 1, wherein the total phase delay around said loop for said light propagating therethrough is equal to an integer times 2π.

Claim 4

A fiber optic resonator, defined in claim 2, wherein said coupling means provides π/2 of said total phase delay.

Claim 5

A fiber optic resonator, defined in claim 1, wherein said coupling means has a coupling constant selected in accordance with the following equation: K.sub.r =(1-γ.sub.o) exp (-2α.sub.o L) where: γ o is the insertion loss of said coupling means; α O is the amplitude attenuation coefficient of said fiber; and L is the length of said fiber loop.

Claim 6

A fiber optic resonator, as defined in claim 1, additionally comprising: means for controlling the polarization of light propagating through said fiber loop portion.

Claim 7

A fiber optic resonator, as defined in claim 5, wherein said polarization controlling means comprises a loop formed from a portion of said fiber loop portion.

Claim 8

A fiber optic resonator, as defined in claim 1, additionallly comprising: means for varying the length of said fiber.

Claim 9

A fiber optic resonator, as defined in claim 7, wherein said varying means comprises: a PZT cylinder, about which a portion of said fiber loop portion is wrapped.

Claim 10

A fiber optic resonator, as defined in claim 8, additionally comprising: means for applying a ramp signal to drive said PZT cylinder to linearly stretch said fiber.

Claim 11

A fiber optic resonator, as defined in claim 1, additionally comprising: a light source, for introducing light into said resonant cavity, said light source having a coherence length at least equal to the rise time of said resonant cavity times the free space velocity of light.

Claim 12

A fiber optic resonator, as defined in claim 1, wherein the intensity of said light in said resonant cavity is dependent upon (a) the length of said fiber loop, and (b) the coupling constant of said coupling means, said intensity at a maximum where (i) said loop length L is such that ##EQU9## where q is any integer, and β is the propagation constant of said fiber, and (ii) said coupling constant K r is such that: K r =fiber transmission x coupling means transmission

Claim 13

A fiber optic resonator, comprising: a continuous, uninterrupted length of optical fiber having a first end portion and a second end portion; a light source, for introducing light into said fiber for propagation from said first end portion to said second end portion; fiber optic coupling means for optically coupling said fiber together to form a loop between said first and second end portions, said coupling means coupling a portion of said source light to circulate in said loop, and coupling another portion of said source light to said second end portion, the length of said loop selected to cause said circulating light to destructively interfere with light from said source that is coupled to said second portion and constructively interfere with light from said source that is coupled to said loop, said interference causing the optical power in said loop to increase above that in said first end portion.

Claim 14

A fiber optic resonator, comprising: a continuous, uninterrupted length of optical fiber having a first end portion and a second end portion; a light source, for introducing light into said fiber for propagation from said first end portion to said second end portion; fiber optic coupling means for optically coupling said fiber together to form a loop between said first and second end portions, said coupling means coupling a portion of said source light to circulate in said loop, and coupling another portion of said source light to said second end portion, the length of said loop selected to cause said circulating light to destructively interfere with light from said source that is coupled to said second portion and constructively interfere with light from said source that is coupled to said loop, said interference causing the optical power in said loop to increase above that in said first end portion.

Claim 15

A fiber optic resonator, as defined in claim 12, wherein said coupling means comprises an evanescent field, fiber optic directional coupler.

Claim 16

A fiber optic resonator, as defined in claim 12, wherein the relative amplitudes of said destructively interfering light are dependent upon the coupling constant of said coupling means.

Claim 17

A fiber optic resonator, as defined in claim 14, wherein said coupling constant is selected according to the following equation: K.sub.r =(1-γ.sub.o) exp (-2α.sub.o L) where: γ O is the insertion loss of said coupling means; α O is the amplitude attenuation coefficient of said fiber; and L is the length of said loop portion.

Claim 18

A fiber optic resonator, as defined in claim 12, wherein the length of said optical fiber is selected so that the total phase delay around said loop is equal to an integer times 2π.

Claim 19

A fiber optic resonator, as defined in claim 14, wherein said coupling means provides π/2 of said total phase delay.

Claim 20

A fiber optic resonator, as defined in claim 12, additionally comprising: means for detecting light output from said second fiber portion.

Claim 21

A fiber optic resonator, as defined in claim 12, wherein said coupler and said fiber loop portion cooperate to form a resonant cavity, said light source having a coherence length greater than the cavity rise time of said resonant cavity times the free space velocity of light.

Claim 22

A fiber optic resonator, comprising: a single, uninterrupted strand of optical fiber; a fiber optic directional coupler having four ports, namely ports 1, 2, 3, and 4, said single, uninterrupted strand of fiber extending through all of said ports, said fiber having a loop portion optically connecting ports 2 and 3, a fiber input portion at port 1 and a fiber output portion at port 4; a light source for inputting a continuous lightwave (W i ) into said fiber input portion; said coupler splitting said input lightwave (W i ) into two components, namely a straight through component (W is ), which propagates from port 1 to port 3, and a cross-coupled component (W ic ), which propagates from port 1 to port 4, said straight through component (W is ) providing at least a portion of a circulating wave (W c ) which circulates through said loop portion from port 3 to port 2, said coupler splitting said circulating wave (W c ), after traversing said loop, into two components, namely a straight through component (W cs ) which propagates from port 2 to port 4, and a cross-coupled component (W cc ), which propagates from port 2 to port 3; and said cross-coupled input wave component (W ic ) destructively interfering with said straight through circulating wave component (W cs ), and said cross-coupled circulating wave component (W cc ) constructively interfering with said straight through input wave component (W is ).

Claim 23

A fiber optic resonator, comprising: a single, uninterrupted strand of optical fiber; a fiber optic directional coupler having four ports, namely ports 1, 2, 3, and 4, said single, uninterrupted strand of fiber extending through all of said ports, said fiber having a loop portion optically connecting ports 2 and 3, a fiber input portion at port 1 and a fiber output portion at port 4; a light source for inputting a continuous lightwave (W i ) into said fiber input portion; said coupler splitting said input lightwave (W i ) into two components, namely a straight through component (W is ), which propagates from port 1 to port 3, and a cross-coupled component (W ic ), which propagates from port 1 to port 4, said straight through component (W is ) providing at least a portion of a circulating wave (W c ) which circulates through said loop portion from port 3 to port 2, said coupler splitting said circulating wave (W c ), after traversing said loop, into two components, namely a straight through component (W cs ) which propagates from port 2 to port 4, and a cross-coupled component (W cc ), which propagates from port 2 to port 3; and said cross-coupled input wave component (W ic ) destructively interfering with said straight through circulating wave component (W cs ), and said cross-coupled circulating wave component (W cc ) constructively interfering with said straight through input wave component (W is ).

Claim 24

A fiber optic resonator, as defined in claim 20, additionally comprising: means for equalizing the amplitude of said cross-coupled input wave component (W ic ) and said straight through circulating wave component (W cs ).

Claim 25

A fiber optic resonator, as defined in claim 21, wherein said equalizing means comprises said coupling means.

Claim 26

A fiber optic resonator, as defined in claim 22, wherein the coupling constant of said coupling means is selected to equal the product of fiber transmission and coupler transmission.

Claim 27

A fiber optic resonator, as defined in claim 20, wherein said cross-coupled components (W cc and W ic ) undergo a π/2 phase shift through said coupler.

Claim 28

A fiber optic resonator, as defined in claim 24, wherein the length of said loop portion is selected to provide a phase delay for said circulating wave (W c ) of (q)2π-π/2, where q is any integer.

Claim 31

A method of forming a resonant cavity from an optical fiber, as defined in claim 26, additionally comprising: selecting the length of said loop so that the total phase delay around said loop is equal to an integer times 2π.

Claim 32

A method of forming a resonant cavity from an optical fiber, as defined in claim 27, wherein said fiber optic directional coupler provides π/2 of said total phase delay.

Claim 33

A method of forming a resonant cavity from an optical fiber, as defined in claim 26, additionally comprising: selecting the coupling constant of said coupler to equal the product of fiber transmission and coupler transmission.

Claim 34

A method of forming a resonant cavity from an optical fiber, as defined in claim 26, wherein said fiber comprises a single continuous, uninterrupted strand of single mode fiber optic material.