Accession Number:

ADA522902

Title:

Phase-locked Optical Signal Recovery

Descriptive Note:

Final rept. 1 May 2005-26 Aug 2009

Corporate Author:

UNIVERSITY COLL LONDON (UNITED KINGDOM)

Personal Author(s):

Report Date:

2009-01-01

Pagination or Media Count:

53.0

Abstract:

Phase-locked receivers have long been used for the recovery of signals in low signal to noise ratio SNR environments, such as space applications. A loop for use with semiconductor laser generated signals would require a bandwidth of 500 MHz for low phase error variance 0.01 rad2 tracking, constraining the propagation delay to 0.3 ns. Since this requires an equivalent path length of 100 mm, conventional realizations in optical fiber technology are not possible, requiring special micro-optical solutions. An alternative technique is to use optical injection locking. This avoids loop propagation limitations, but stable locking ranges are typically 1 GHz, requiring precision 10 mK control of the receiver laser and continuous adjustment to track drift in the incoming signal. At University College London UCL, we have developed a technique that overcomes the limitations described above-the Optical Injection Phase Lock Loop OIPLL in which a narrow bandwidth optical phase lock loop OPLL is used to control the free-running frequency of an optically injection locked laser to compensate for thermal drift, drift in the incoming signal and low-frequency noise. If successful this would enable low SNR optical signals to be recovered without the need for constant skilled adjustment of the receiver system. For the feasibility study we propose to investigate two possible detection schemes. The first is an homodyne OIPLL. Although this appears simple in principle there are significant challenges in implementation. The second scheme is based on heterodyne detection, with the heterodyne frequency chosen to be remote from data modulation interference. In this approach, the incoming signal passes through a modulator, where it is sinusoidally intensity modulated at microwave frequency by the offset source. The slave laser is injection locked to one of these side frequencies through an optical circulator.

Subject Categories:

  • Electrical and Electronic Equipment
  • Active and Passive Radar Detection and Equipment
  • Radiofrequency Wave Propagation

Distribution Statement:

APPROVED FOR PUBLIC RELEASE