# US 5,347,392 A · Electric-optic resonant phase modulator > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 5,347,392 A - Document ID: US5347392A - Status: Granted - Kind: A - Application number: 07/842,300 - Filed: 1992-02-26 - Granted: 1994-09-13 - Earliest claimed: 1992-02-26 - Assignees: The United States of America as represented by the Administrator of the National Aeronautics and Space Administration - Inventors: Chien-Chung Chen; Deborah L. Robinson; Hamid Hemmati - Web page: https://patentgrep.com/patent/US5347392A ## CPC - H04B 10/50: Transmitters - G02F 1/21: by interference - H04B: TRANSMISSION - 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 electro-optic resonant cavity is used to achieve phase modulation with lower driving voltages. Laser damage thresholds are inherently higher than with previously used integrated optics due to the utilization of bulk optics. Phase modulation is achieved at higher speeds with lower driving voltages than previously obtained with non-resonant electro-optic phase modulators. The instant scheme uses a data locking dither approach as opposed to the conventional sinusoidal locking schemes. In accordance with a disclosed embodiment, a resonant cavity modulator has been designed to operate at a data rate in excess of 100 Mbps. By carefully choosing the cavity finesse and its dimension, it is possible to control the pulse switching time to within 4 ns and to limit the required switching voltage to within 10 V. Experimentally, the resonant cavity can be maintained on resonance with respect to the input laser signal by monitoring the fluctuation of output intensity as the cavity is switched. This cavity locking scheme can be applied by using only the random data sequence, and without the need of additional dithering of the cavity. Compared to waveguide modulators, the resonant cavity has a comparable modulating voltage requirement. Because of its bulk geometry, resonant cavity modulator has the potential of accommodating higher throughput power. Furthermore, mode matching into a bulk device is easier and typically can be achieved with higher efficiency. On the other hand, unlike waveguide modulators which are essentially traveling wave devices, the resonant cavity modulator requires that the cavity be maintained in resonance with respect to the incoming laser signal. An additional control loop is incorporated into the modulator to maintain the cavity on resonance. ## Claims ### Claim 1 A resonant cavity electro-optic phase modulator for coherent optical communications, the modulator comprising: an elongated electro-optic crystal for receiving a beam of coherent light, said crystal having an input end and an output end; a mirror positioned near the output end of said crystal for reflecting coherent light traveling through said crystal; means at said input end of said crystal for coupling said coherent light into said crystal; means for applying a voltage across said crystal for modulating the index of refraction of said crystal and thus the phase of said coherent light; and means for applying a bias voltage to said crystal for maintaining said cavity on resonance with said beam of coherent light. ### Claim 2 (depends on 1) The phase modulator recited in claim 1 wherein said coupling means comprises a reflective coating on said input end of said crystal. ### Claim 3 (depends on 1) The phase modulator recited in claim 1 wherein said mirror and said crystal are spaced apart by an air gap. ### Claim 4 (depends on 1) The phase modulator recited in claim 1 wherein said voltage applying means generates pulses at a frequency of at least 100 Mbps, ### Claim 5 (depends on 1) The phase modulator recited in claim 1 further comprising a mode-matching lens positioned in front of the input end of said crystal, ### Claim 6 (depends on 1) The phase modulator recited in claim 1 further comprising a Faraday isolator positioned in front of the input end of said crystal. ### Claim 7 (depends on 1) The phase modulator recited in claim 1 wherein said bias voltage applying means comprises electrical feedback means for correlating optical intensity fluctuation at said output end of said crystal with said modulating voltage. ### Claim 8 (depends on 1) The phase modulator recited in claim 1 wherein said voltage applying means modulates said crystal with a pseudo-random data sequence. ### Claim 9 (depends on 8) The phase modulator recited in claim 8 wherein said data sequence includes pulses at a frequency of at least 100 Mbps. ### Claim 10 An external phase modulator for use with a laser; the modulator comprising: a crystal responsive to applied voltage for varying refractive index at the frequency of said laser; means for coupling a portion of the output of said laser into said crystal; means for reflecting said portion of said laser output after said portion travels through said crystal; a pulse generator for applying said voltage to said crystal for phase modulating said portion of said laser output; and means for locking said modulator on resonance with said laser. ### Claim 11 (depends on 10) The phase modulator recited in claim 10 wherein said coupling means comprises a reflective coating on the input end of said crystal. ### Claim 12 (depends on 10) The phase modulator recited in claim 10 wherein said pulse generator generates pulses at a frequency of at least 100 Mbps. ### Claim 13 (depends on 10) The phase modulator recited in claim 10 wherein said crystal is biased at resonance with said laser by feedback means for correlating the output light intensity fluctuations of said crystal with the output of said pulse generator. ### Claim 14 (depends on 13) The phase modulator recited in claim 13 wherein said reflecting means passes a small fraction of said laser output portion; said feedback means comprising a detector positioned for detecting said small fractions, an RF mixer for comparing said detected small fraction with a delayed version of said pulse generator output, and means for generating a biasing voltage dependent upon the output of said RF mixer. ### Claim 15 (depends on 10) The phase modulator recited in claim 10 wherein said crystal comprises an input end and an output end, wherein said coupling means comprises a partially reflective coating on said input end and wherein said reflecting means comprises a reflector positioned in alignment with and external to the output end of said crystal. ### Claim 16 (depends on 10) The phase modulator recited in claim 10 wherein said pulse generator produces a pseudo-random data sequence.