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International Conference on Photonics in Switching

Optical Beam Routing through Time-Domain Spatial-Spectral Filtering

William Randall Babbitt, THOMAS W. MOSSBERG

Published Jan 1, 1995• 0 citations
Publisher

Abstract

Recent years have seen the development of a variety of techniques for the storage and processing of optical data streams in materials with [1-10] and without [11-12] intrinsic frequency selectivity. These techniques are characterized by very high bandwidth and relatively large time-bandwidth product. It is known, that the optical processes responsible for the storage and/or processing of temporal waveform data frequently also lead to the storage of spatial waveform information [13,14]. It has been demonstrated, for example, that sequences of images can be stored. [5,7,8] An area that is relatively unexplored, however, relates to the possible interactions between stored temporal and spatial information. We explore one example of how the temporal and spatial information stored within a material can interact and lead to a novel functionality, i. e. the passive routing of optical beams along one of many possible temporally encoded directions.

DOI
10.1364/ps.1995.pfb3

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Recent years have seen the development of a variety of techniques for the storage and processing of optical data streams in materials with [1-10] and without [11-12] intrinsic frequency selectivity. These techniques are characterized by very high bandwidth and relatively large time-bandwidth product. It is known, that the optical processes responsible for the storage and/or processing of temporal waveform data frequently also lead to the storage of spatial waveform information [13,14]. It has been demonstrated, for example, that sequences of images can be stored. [5,7,8] An area that is relatively unexplored, however, relates to the possible interactions between stored temporal and spatial information. We explore one example of how the temporal and spatial information stored within a material can interact and lead to a novel functionality, i. e. the passive routing of optical beams along one of many possible temporally encoded directions.
Time-and-space-domain holography [1,2] by stimulated photon echoes [3] provides a means of storing temporal and spatial properties of an ultrafast-varying light signal and recalling its authentic replica at any later moment. The possibility of recording complex time shapes of light pulses, which also means time-domain optical data storage, is based on the ability of frequency-selective absorbers to store with high accuracy the temporal Fourier components of the incident light [1-3]. The time-domain frequency-selective optical storage of binary or analog data is an alternative approach to the concept of frequency-selective high-density data storage that provides a parallel ultrafast data storage and processing in the frequency domain. The shortest detail of the signal to be stored is limited by the reverse inhomogeneous bandwidth of the storing media which reaches 10-100 fs for frequency-selective materials while the duration of the signal is limited by phase relaxation time T2 (usually 10-3-10-6s).
Frequency-selective optical data storage (FSDS) provides for the heavy multiplexing of data at single spatial storage locations. The time-domain approach to FSDS offers in addition the possibility of extremely high data input/output rates. Nevertheless, a variety of technical problems must be resolved before the widespread implementation of FSDS memories becomes feasible. In the case of time-domain FSDS, for example, one must detect signal beams despite the presence of relatively strong memory readout beams in close temporal and spatial proximity. We demonstrate that this difficulty can be turned into an advantage in the case of the newly introduced swept-carrier approach to FSDS.1
Time-and-space-domain holography [1,2] by stimulated photon echoes [3] provides a means of storing temporal and spatial properties of an ultrafast-varying light signal and recalling its authentic replica at any later moment. The possibility of recording complex time shapes of light pulses, which also means time-domain optical data storage, is based on the ability of frequency-selective absorbers to store with high accuracy the temporal Fourier components of the incident light [1-3]. The time-domain frequency-selective optical storage of binary or analog data is an alternative approach to the concept of frequency-selective high-density data storage that provides a parallel ultrafast data storage and processing in the frequency domain. The shortest detail of the signal to be stored is limited by the reverse inhomogeneous bandwidth of the storing media which reaches 10-100 fs for frequency-selective materials while the duration of the signal is limited by phase relaxation time T2 (usually 10−9-10−6s).
A new time-domain approach to frequency-selective optical data storage is described. In this approach, a spatial storage cell is exposed to two cotemporal, spatially angled, frequency-chirped excitation fields whose duration can greatly exceed the homogeneous dephasing time of the storage material employed. The two beams have a fixed frequency offset, and one is temporally encoded with data. The new method averts several of the drawbacks of existing approaches to time- and frequency-domain optical memories.
Storing and delaying optical information is of crucial importance for optical communications, signal processing and in the quantum domain. A plethora of techniques for optical storage have been shown which aim to maintain as much as possible the advantages of optics, such as e.g. the coherence, the bandwidth and capacity. In particular the interaction of optical waves with mechanical motion offers a solution to buffer optical information [1-4]. It was shown that one can use acoustic waves to store and delay optical signals coherently via the effect of stimulated Brillouin scattering (SBS) [3,4]. This allows for simultaneous storage at multiple wavelengths [5], cascaded storage at different spatial positions [6], and nonreciprocal storage with a GHz bandwidth [7]. However, the delay time of this technique is so far limited to the acoustic lifetime of about 10 ns.