A proposed electro-optical apparatus would shift the frequency of a laser beam by a controllable amount within the range of about ±10 GHz. It would be a wide-band alternative to an acousto-optical tunable filter, which is limited to a frequency shift of about 100 kHz. The power efficiency of the proposed apparatus would be nearly 100 percent; the main insertion loss would be only about 2 dB and would be associated with fiber-optic input and output.

The apparatus would produce a constant frequency shift by exploiting the phase shift of the laser beam in an electro-optical medium. The effect, upon frequency, of a steadily increasing or decreasing phase shift is equivalent to the Doppler frequency shift produced by a steadily advancing or retreating mirror. Of course, there is no practical way to realize, in a compact apparatus, a steadily advancing or retreating mirror. Similarly, there is no practical way to realize its functional equivalent in a phase modulator in which the phase shift could be made to increase or decrease steadily without limit.

The Switch Would Direct the Laser Beam alternately through one phase modulator, then the other. The rectangular switching waveform would be synchronized so that at any given instant of time, the laser beam would be exposed to the rising edge (only) of the sawtooth modulating waveform.

However, it is possible to drive two electro-optical modulators with identical sawtooth waveforms that differ in phase by about 180°. It is also possible to switch a laser beam electro-optically so that it repeatedly passes through one modulator and then the other. If this switching were done in proper synchronization with the sawtooth modulation waveform, then laser beam could be made to undergo either an increasing or a decreasing phase shift at all times. The proposed apparatus is based on this concept.

The apparatus (see figure) would be made from standard lithium niobate integrated optics. A Mach-Zehnder switch driven by a rectangular waveform synchronized with the sawtooth modulating waveform would direct the laser beam alternately along optical paths to two phase modulators. The amplitude of the sawtooth waveform would typically be chosen to obtain a peak-to-peak phase modulation of 4π radians. The shift in frequency of the laser beam would equal the phase-modulation rate, which would be proportional to the amplitude and repetition frequency of the sawtooth waveform; for example, at a typical repetition frequency of 1 GHz, the frequency shift would be about 2 GHz.

The amplitude and phase relationships between the two sawtooth modulating waveforms would be chosen so that during the brief switching intervals in which parts of the laser power were passing partly through both phase modulators, the difference between the phase shifts produced by the two modulators would be 2π radians. This choice would ensure coherent addition of the outputs of the two modulators and prevent the introduction of a spurious phase modulation associated with the switching.

This work was done by Roman C. Gutierrez of Caltech for NASA's Jet Propulsion Laboratory.

In accordance with Public Law 96-517, the contractor has elected to retain title to this invention. Inquiries concerning rights for its commercial use should be addressed to

Technology Reporting Office
JPL
Mail Stop 122-116
4800 Oak Grove Drive
Pasadena, CA 91109
(818) 354-2240

Refer to NPO-20531



This Brief includes a Technical Support Package (TSP).
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An Electro-Optical Frquency Shifter

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Photonics Tech Briefs Magazine

This article first appeared in the September, 2000 issue of Photonics Tech Briefs Magazine (Vol. 24 No. 9).

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Overview

The document presents a technical support package from NASA detailing a novel electro-optical frequency shifter developed by inventor Roman C. Gutierrez. This innovative apparatus is designed to shift the frequency of a laser beam by a controllable amount within a range of ±10 GHz, significantly surpassing the capabilities of existing technologies, such as the acousto-optical tunable filter (AOTF), which is limited to about 100 kHz.

The proposed frequency shifter operates using two phase modulators driven by triangular saw-tooth waveforms that are 180 degrees out of phase. This configuration allows for the generation of a frequency shift anywhere between 0 Hz and 10 GHz, achieving nearly 100% power efficiency with an insertion loss of only about 2 dB, primarily due to fiber-optic input and output. The device exploits the principle of phase modulation, akin to the Doppler effect produced by a moving mirror, but in a more compact and practical form.

The document outlines the limitations of traditional methods, such as the AOTF, which relies on the acousto-optic effect in Lithium Niobate and requires a surface acoustic wave transducer. In contrast, the proposed device utilizes integrated optics and a Mach-Zender intensity modulator to switch the optical signal between the two phase modulators in synchronization with the saw-tooth waveform. This mechanism ensures a constant frequency shift, effectively mimicking the behavior of a continuously moving mirror without the practical challenges associated with such a setup.

Applications for this frequency shifter include its potential use in optical fiber communications, particularly in tunable add-drop multiplexers, and as a frequency modulator for heterodyne interferometry. The document also suggests that the technology could be implemented using bulk optics or micromachining techniques, further enhancing its versatility.

Overall, this technical disclosure highlights a significant advancement in optical frequency shifting technology, offering a high-efficiency, low-loss solution that could revolutionize various optical applications. The work was conducted at the Jet Propulsion Laboratory under NASA's contract, emphasizing its relevance to ongoing research and development in the field of optics.