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1988, Applied Optics
Regular free-space interconnects such as the perfect shuffle and banyan provided by beam splitters, lenses, and mirrors connect optical logic gates arranged in 2-D arrays. An algorithmic design technique transforms arbitrary logic equations into a near-optimal depth circuit. Analysis shows that an arbitrary interconnect makes little or no improvement in circuit depth and can even reduce throughput. Gate count is normally higher with a regular interconnect, and we show cost bounds. We conclude that regularly interconnected circuits will have a higher gate count compared with arbitrarily interconnected circuits using the design techniques presented here and that regular free-space interconnects are comparable with arbitrary interconnects in terms of circuit depth and are preferred to arbitrary interconnects for maximizing throughput. 1. Introduction All-optical digital computers have the potential for high speed, cheap communications, and massive parallelism. Logic gates based on nonlinear dielectric constants were investigated theoretically in the early 1960s by von Neumann. 1 In the last few years optical bistable devices, 2 ' 3 nonlinear Fabry-Perots, 4 ' 5 and hybrid electrooptic devices 6 have been studied experimentally. These results encourage development of architectures suitable for optics. Historically, two architectural approaches have dominated the field. One approach uses integrated optics to interconnect optical logic devices. A system designed with this approach is architecturally similar to a conventional computer, with logic gates connected in arbitrary configurations. This similarity means that an optical computer designed with this approach is worth building only if it can be made more cheaply or more powerful. An alternative approach makes use of 2-D arrays of devices interconnected in free space. This approach uses space-variant interconnects (provided by holograms) or space-invariant regular interconnects (provided by beam splitters). We prefer the space-invariant regular interconnect approach for simplicity, extensibility, and high throughput. To take advan
Applied Optics, 1993
We propose the use of a computer-generated hologram that combines a fanout and focusing element that can be used to perform an optical perfect-shuffle interconnection. The hologram is designed by calculation of the interference fringes between diverging waves from four point sources and a reference plane wave. With this element we show experimentally the resulting perfect-shuffle pattern. The use of the computer-generated hologram makes it easy to implement a planar optical perfect-shuffle interconnect, which is compact, has low aberration, and is easy to align. The planar optics configuration for a perfect-shuffle interconnection network is also discussed.
Proceedings of the IEEE, 1994
Within the past 15 years there has been significant progress in the development of two-dimensional arrays of optical and optoelectronic devices. This progress has, in turn, led to the construction of several free-space digital optical system demonstrators. The first was an optical master-slave jlip-jlop using Hughes liquid-crystal light valves as optical logic gates and computer-generated holograms as the gate-to-gate interconnects. This was demonstrated at USC in 1984. Since then there have been numerous demonstrations of free-space digital optical systems including a simple optical computing system (1990) and five switching fabrics designated System, (I988), System, (19891, System, (1990). System, (1991) and System, (1993.
Optics Communications, 1992
The various possibilities of optically interconnecting 16 × 16-data arrays by shuffle patterns are presented and analysed. The pattern analysis is based on evaluating the skew of each particular path of the shuffle interconnections. Geometric quantities of interest (deflection angle, path length of spatial and frequency pattern) are derived. The switch preserving transformation of 2D shuffle interstage patterns into their equivalent 1D shuffles and vice versa, the way a 1D shuffle overlaps into a 2D shuffle in the 3D physical space, is presented. The costs of these different interconnection schemes are evaluated and the results are compared. (The applied cost measure is the total length of the interconnections.) For example, the interconnection of 256 data has the least costs if the arrays are interconnected by a 4D shuffle.
Optics Communications, 1991
We present a three-dimensional optical interconnection architecture that can potentially approach the least possible system size of any architecture within a numerical factor of the order of _ IO. This architecture can provide an arbitrary pattern of connections among a three-dimensional array of points.
Applied Optics, 1992
Heat removal, rather than finite interconnect density, is the major mechanism that limits how densely we can pack three-dimensional computing systems of increasing numbers of elements. Thus highly interconnected approaches can be employed without a further increase in system size. The use of optical interconnections for implementing the longer connections of such systems is advantageous. In fact, if the optical communication energy is sufficiently low and large-bit repetition rates are employed, conductors are useful for only the shortest connections and can be dispensed with altogether with little disadvantage. This justifies consideration of an optical digital computer. This paper is an initial attempt to understand whether and when an all-optical digital computer may prove useful. Several researchers have addressed this issue in the past, often with negative conclusions. We believe that an increasing understanding regarding the importance of communication in computing and the realization that the architectural-logical construction of a computing system can no longer be divorced from its physical construction justifies a reevaluation of previous arguments and a search for hitherto unexplored perspectives.
Applied Optics, 1994
We present a general-purpose three-dimensional interconnection network that models various parallel operations between two data planes. This volume interconnection system exhibits reconfigurable capabilities because of parallel and externally weighted interconnection modules, called nodes. We propose a generic optical implementation based on the cascading of two planar hologram arrays, coupled with a bistable optically addressed spatial light modulator. The role of this component is discussed in terms of energy regeneration and spatial cross-talk limitation. As an example, a binary matrix-matrix multiplier is implemented that uses a ferroelectric liquid-crystal light valve.
Applied Optics, 1994
Methods that a designer can use to optimize the placement of nodes in a large switching network to decrease the requirements on holographic interconnections are investigated. Localized interconnections between subdivided switches are combined with simpler global interconnections. The interconnections between subdivided switches can be implemented by use of metallic traces on smart-pixel arrays. The global interconnections would be provided by optical free-space techniques. Several advantages arise from this procedure: (1) The regular interconnection pattern is decomposed into several pipes (collection of light beams that form a complete pattern) without loss of functionality. (2) The interconnection pattern may be optimized by variation of the placement of the switches in a switching network (e.g., to obtain a minimum deflection angle). (3) The interconnection pattern may be adjusted to the need of an algorithm by an additional parameter (the dimension). The application to photonic switching networks and signal processing is discussed.
Applied Optics, 1994
Several different shuffle-equivalent interconnection topologies that can be used within the optical link stages of photonic-switching networks are studied. These schemes include the two shuffle, the two banyan, and the segmented two shuffle, which can be used to interconnect two-input, two-output switching nodes. The schemes also include the four shuffle and the four banyan, which can be used to interconnect four-input, four-output switching nodes. (Note: The segmented two shuffle and the four banyan are novel interconnection topologies that were developed to satisfy some of the constraints of free-space digital optics). It is shown that each of these interconnection topologies can be implemented by the use of relatively simple imaging optics that contain space-invariant computer-generated binaryphase gratings. The effects of node type and interconnection topology on the laser power requirements and the optical component complexity within the resulting systems are also studied. The general class of networks known as extended generalized shuffle networks is used as a baseline for the analysis. It is shown that (2, 1, 1) nodes and (2, 2, 2) nodes connected by two-banyan interconnections can produce power-efficient and cost-effective systems. The results should help identify the architectural trade-offs that exist when a node type and an interconnection topology are selected for implementation within a switching system based on free-space digital optics.
2000 Proceedings. 50th Electronic Components and Technology Conference (Cat. No.00CH37070)
The central issue of optically interconnected integrated circuits (OIIC) concerns the area optical interconnect approach to the interconnect bottleneck encountered in advanced VLSI-CMOS designs. The envisaged route to solving this problem offers throughput data interconnects on inter-chip and MCM level, facilitating implementation of new digital architectures and systems. The OIIC project is aimed towards the realisation of three demonstrators: a
Applied Optics, 1992
A neural-network architecture of multifaceted planar interconnection holograms and optoelectronic neurons is analyzed. Various computer-generated hologram techniques are analyzed and tested for their ability to produce an interconnection hologram with high-accuracy interconnects and high diffraction efficiency. A new technique is developed by using the Gerchberg-Saxton algorithm, followed by a random-search error minimization that produces the highest interconnect accuracy and the highest diffraction efficiency of the techniques tested. Analysis of the system shows that the hologram has the capacity to connect 5000 neuron outputs to 5000 neuron inputs with bipolar synapses and that the encoded synaptic weights have an accuracy of 5 bits. A simple feedback system is constructed and demonstrated.
Optics Communications, 2000
High-density parallel optical beam arrays are useful for free space optical interconnects. To achieve high-density interconnection the optical beam sizes must be small while the propagation divergence within the specified interconnect range must also be small. This contradictory requirement in free space for a conventional Gaussian beam is however possible to be satisfied with a pseudo-non-diffracting beam. We present herein high-density pseudo-non-diffracting beam arrays achieved by using holographic technique. The demonstrated pseudo-non-diffracting beams can keep their central spot size of about 95 mm within the propagation distance of 40 cm. The center-to-center beam separation is 250 mm, which is much smaller than those achieved by collimated Gaussian beams with the same interconnect range. The small central lobe sizes can further avoid the use of collectionrfocusing lenses at the high-speed photodetector receivers. q 0030-4018r00r$ -see front matter q 2000 Elsevier Science B.V. All rights reserved.
Proceedings of SPIE - The International Society for Optical Engineering
Providing the required interconnections between the processors of a parallel computer is a di cult problem: latency, switching control, cost, and crosstalk e ects have to be taken into account. It is widely believed that the design might be simpli ed if optical technology is used. However, even optical interconnections cannot cater for an unlimited number of processors. For systems with up to about 10 5 ? 10 6 processors, it seems that the arrangement of the processors in space so that each can \see" the others is the limiting factor; A large part of the volume involved must stay empty for the information-bearing light beams. above that, di raction e ects and power requirements place a limit on the number of processors.
Optics Communications, 1991
We compare system sizes for some optical interconnection architectures and introduce the folded multi-facet architecture which can potentially approach the smallest possible system size of any two-dimensional optical architecture. 0030-4018/91/$03.50 © 1991 -Elsevier Science Publishers B.V. (North-Holland)
Applied Optics, 1989
Fundamental and practical limitations to be encountered in the implementation of massive free space optical interconnects are discussed in detail, and some improved architectures are proposed. The long term optimum design uses currently unavailable large arrays of laser diodes. An interim solution, using available spatial light modulators, is shown to be capable of storing -101 bits of information and performing -10" interconnections/s.
Optics Letters, 1992
A three-dimensional optoelectronic multistage permutation network is proposed. Shuffle-exchange stages are implemented by using a folded free-space optical system to connect a two-dimensional array of processing elements to itself. The proposed processing elements contain optoelectronic input and output devices coupled to electronic switches. The analysis shows that pipelined operation for large processing element arrays (>1024) can be achieved with a single optical system by interleaving the source-detector pairs of different stages to exploit the large optical space-bandwidth product. Perfect shuffle (PS) networks' based on free-space optics have been proposed to overcome the skew, cross talk, and area limitations of two-dimensional (2-D) technologies. 24 A pipelined shuffle-exchange network was recently proposed that is based on the folded perfect shuffle' (FPS) and uses a single optical system that spatially interleaves the optoelectronic input-output ports (I/O) of the multiple stages. 6 The parallel use of a single optical system was made possible because each stage of a shufflebased interconnection network is physically identical. This pipelining concept thus applies to all shuffle-based multistage interconnection networks (MIN's) that use cascaded shuffle-exchange stages that are identical and operate on 2-D processingelement (PE) arrays. The anticipated performance benefits of the pipelined optical network are ana
Applied Optics, 1988
Applied Optics, 1988
Proceedings of the IEEE, 2000
Applied Optics - APPL OPT, 2002
An assembly technique is presented to realize pluggable or fully integrated optoelectronic systems based on image relays. A method to visually align and assemble optoelectronic chips or fiber bundles to half of a relay is explained. To validate this technique, two-dimensional arrays of vertical-cavity surface-emitting lasers and photodetectors and a fiber image guide have been integrated to gradient index lenses with simple optomechanical parts. Although the connection of these modules was realized with +/-0.5 mm lateral tolerances, parallel optical interconnects were successfully achieved at 10 MHz. The lateral misalignment between chips was on average 20 mum and at worst 60 mum.
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