# US 10,503,048 B2 · Nonreciprocal light propagation systems and methods > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 10,503,048 B2 - Document ID: US10503048B2 - Status: Granted - Kind: B2 - Application number: 16/312,454 - Filed: 2017-06-23 - Published: 2019-05-02 - Granted: 2019-12-10 - Earliest claimed: 2016-06-24 - Assignees: Npl Management Limited - Applicants: NPL Management Limited - Inventors: Leonardo Del Bino; Sarah Louise Stebbings; Pascal Patrice Del'Haye; Jonathan Michael Silver - Web page: https://patentgrep.com/patent/US10503048B2 ## CPC - G02F 1/3511: {Self-focusing or self-trapping of light; Light-induced birefringence; Induced optical Kerr-effect} - G02F 1/3515: {All-optical modulation, gating, switching, e.g. control of a light beam by another light beam (G02F1/353, G02F1/37, G02F1/39 take precedence)} - G02F 1/3517: {using an interferometer} - G02F 1/355: characterised by the materials used - G02F 2203/15: involving resonance effects, e.g. resonantly enhanced interaction - G02F: OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS ## Abstract An optical resonator system comprises an optical resonator (30) and means (32, 42, 44) for coupling into the resonator counterpropagating waves at total intensities such as to produce a non-linear interaction between the first and second waves whereby to break the symmetry to establish different resonant frequencies between the first and second counterpropagating waves whereby to produce different optical effects in the opposite directions. A common light source, e.g. a laser 32, is employed with an amplifier 40 and a modulator 50, or different light sources can be employed. ## Claims ### Claim 1 An optical signal handling system comprising an optical loop resonator made of material with a non-reciprocal optical non-linearity such that the presence of counterpropagating light induces a stronger resonance frequency change than copropagating light of the same intensity, at least one light source coupled to a first arm for introducing a first optical wave into the resonator and to a second arm for introducing into the resonator a counterpropagating second optical wave having the same frequency as the first wave, said first and second waves having total intensities such as to produce a non-linear interaction between the first and second waves, wherein one of the arms comprises an attenuator or an amplifier whereby to establish different resonant frequencies for the two different directions of light propagation. ### Claim 2 (depends on 1) An optical signal handling system according to claim 1, employing the Kerr effect. ### Claim 3 (depends on 1) An optical signal handling system according to claim 1, wherein the at least one light source is a common light source. ### Claim 4 (depends on 3) An optical signal handling system according to claim 3, comprising one or more further means for introducing the first wave into the resonator and/or one or more further means for introducing the second wave into the resonator. ### Claim 5 (depends on 1) An optical signal handling system according to claim 1, wherein each arm comprises a light separator connected to a respective measurement means. ### Claim 6 (depends on 1) An optical signal handling system according to claim 1, wherein the resonator has a cavity linewidth and wherein the resonant frequencies differ by at least the cavity linewidth. ### Claim 7 (depends on 1) An optical signal handling system according to claim 1, all the components of which are static. ### Claim 8 (depends on 1) An optical signal handling system according to claim 1, wherein at least one of the waves is generated within the resonator itself by means of a nonlinear optical effect or optical gain. ### Claim 9 (depends on 1) An optical signal handling system according to claim 1 used to provide an optical diode or isolator, an optical circulator, an optical flip-flop, an optical power comparator, a proximity sensor, a refractive index sensor, a particle sensor, an oscillator, or a power limiter comprising a resonator system. ### Claim 10 (depends on 1) An optical signal handling system according to claim 1, wherein the resonator is rotatable relative to other components of the system. ### Claim 11 (depends on 10) A Sagnac effect sensor comprising a system according to claim 10. ### Claim 12 A method of producing different optical effects in opposite directions in an optical loop resonator made of material with a non-reciprocal optical non-linearity such that the presence of counterpropagating light induces a stronger resonance frequency change than copropagating light of the same intensity, comprising introducing first and second optical waves via first and second respective arms into the resonator from at least one light source in opposite directions and with the same frequency and at total intensities such as to produce a non-linear interaction between the first and second waves whereby to establish different resonant frequencies for the two different directions of light propagation. ### Claim 13 (depends on 12) A method according to claim 12 for connecting a light source to an output device without reflections wherein the light source introduces light from a first port which is coupled via a first coupler in a direct direction within the resonator, light emerging from the resonator via a second coupler to the output device, and wherein the light reflected from the output device passing back to the second coupler is not coupled back to the resonator. ### Claim 14 A method of adjusting the relative power between waves counterpropagating in a static optical resonator made of material with a non-reciprocal optical non-linearity and comprising first and second arms, the method comprising coupling identical waves into said first and second arms of the resonator in opposite directions and with such a total intensity that a non-linear interaction occurs between the waves, wherein the resonator is subjected to an external effect which has a differing effect on the two waves and the difference is detected. ### Claim 15 (depends on 14) A method according to claim 14, wherein the frequency of one or each wave is tuned to alter the differing effect.