Optical shift register

Abstract: An optoelectronic apparatus where information is communicated to and from the apparatus in the optical domain, but where the apparatus includes a transmission gate (151) interposed between successive optoelectronic gates (101, 102) to sequentially convey information internally in the form of electrical, rather than optical, signals. Illustratively, the transmission gate is optoelectronic and comprises two back to back p-i-n photodiodes each including a quantum well region. The first and second optoelectronic gates are S-SEEDs comprising p-i-n photodiodes also each including a quantum well region. The transmission gate is responsive to a first level of an optical control signal ( 109, 119) for substantially blocking current, and to a second level of the optical control signal for substantially passing current. Applicarions of the apparatus include its use in a shift register, 2 x 1 switch, 1 x 2 switch, and an exclusive OR gate.

Description: Technical Field This invention relates to optoelectronic apparatus, and more particularly to an optical shift register. Background and Problem To make competitive optical computers and photonic switches, optical devices are required that perform functions that are similar to the functions performed by electronic devices in electronic systems. By using optoelectronic devices, such as the quantum well self electro-optic effect devices (SEEDs) disclosed in U. S. Patent Re32,893 issued to D. A. B. Miller on March 21, 1989, many such corresponding functions can be achieved. The symmetric SEEDs (S-SEEDs) disclosed in U. S. Patent 4,754,132 issued to H. S. Hinton et al. on June 28, 1988 have been shown to operate as set-reset latches, differential logic gates, or optical tri-state logic devices (U. S. Patent 4,800,262 issued to A. L. Lentine on January 24, 1989). More recently, S-SEEDs have been applied as logic gates capable of implementing any boolean logic function in a single combinational circuit with a single clock cycle of delay (U. S. Patent No. 4,967,068, issued October 30, 1990, and U. S. Patent No. 4,959,534, issued September 25, 1990, of A. L. Lentine et al.). This is important because it avoids the optical cascading otherwise needed to perform more complex logic functions; the approach is lacking, however, in that there is no apparent way to implement sequential circuits, such as shift registers, counters, multiplexers and demultiplexers. U. S. Patent No. 4,952,791, issued August 28, 1990, of H. S. Hinton et al. discloses one known sequential optical circuit apparatus comprising optically cascaded S-SEEDs in an integrated structure; while the monolithic structure eliminates the need for the bulk optics of free space optically interconnected subsystems, the structure is complex, and adds capacitance thereby reducing system speed. Because the devices are optically cascaded, it is not possible in some applications to use short pulses to rapidly switch the devices because of saturation of the first device of a cascaded pair. In view of the foregoing, a recognized deficiency in the art is the lack of an apparatus for implementing optical sequential logic without requiring optical cascading. In the article entitled "Programmable hybrid parallel processing for real-time digital logic operations", Optics Letters, Vol. 12, No. 11, November 1987, pages 965 to 967, S. Fukushima and T. Kurokawa describe an optoelectronic logic circuit which has an optoelectronic phototransistor gate matrix stage which is coupled by electrical or optical switches to controllably transmit electrical signals from the gate matrix to an optoelectric output stage (in this case an LED). This system uses LED arrays to encode and decode logic signals. US-A-4 904 858 teaches that symmetric self electro optic effect devices (S-SEEDs) can be used as logic devices, including an arrangement that implements an R-S flip-flop which exploits the bi-stable behavior of S-SEEDs. The devices of this patent, however, use optical inputs and optical outputs exclusively. Solution This deficiency is eliminated and a technical advance is achieved in accordance with the principles of the invention in an apparatus as set out in claim 1. Information is communicated to and from the apparatus in the optical domain, but where the apparatus includes a transmission gate advantageously interposed between successive optoelectronic gates to sequentially convey information internally, significantly in the form of electrical, rather than optical, signals. Since there is no need to optically cascade component gates, the apparatus construction is simplified because there is no need to align the optical output of one gate for transmission as the optical input to a second gate. Switching speed is improved since the structure is of reduced size and therefore reduced capacitance compared to the known Hinton et al. monolithic structure and since there is no tendency to overdrive and thereby saturate a first gate in order to provide sufficient optical input power to a second gate. An apparatus in accordance with the invention includes first and second optoelectronic gates and a transmission gate. The first optoelectronic gate has a logical state controllable by an optical input signal and generates an electrical signal representative of the logical state. The transmission gate is electrically coupled to the first optoelectronic gate and selectively transmits the electrical signal. The second optoelectronic gate is electrically coupled to the transmission gate and has an optical state controllable by the selectively transmitted electrical signal. In the embodiment, the transmission gate comprises two back to back p-i-n photodiodes each including a quantum well region. The first and second optoelectronic gates are S-SEEDs comprising p-i-n photodiodes also each including a quantum well region. The transmission gate is electrically coupled from a point between the p-i-n photodiodes of the first S-SEED gate to a point between the p-i-n photodiodes of the second S-SEED gate. The transmission gate is responsive to a first level of the optical control signal for substantially blocking current, and to a second level of the optical control signal for substantially passing current. To provide a cascaded mode of operation, the optical control signal is applied after the optical input signal is applied. With the first optoelectronic gate implemented as an S-SEED, an optical clock signal is applied to the first gate during the application of the optical control signal to the transmission gate. An optical shift register in accordance with the invention comprises N optoelectronic processing gates arranged in sequence and N-1 optoelectronic transmission gates each being electrically interposed between successive ones of the N processing gates, N being a positive integer greater than two. Each processing gate has an optical state controllable by an optical input signal and controllable by an electrical input signal, and generates an electrical signal representative of optical state. Each transmission gate is responsive to an optical control signal and selectively transmits an electrical signal between the successive processing gates. The shift register is responsive to optical control signals applied sequentially to successive transmission gates for shifting information represented by the optical state of one processing gate to successive processing gates of the shift register. Drawing Description FIG. 1 is a circuit diagram of a circuitry forming part of a shift register in accordance with the invention comprising two optoelectronic signal processing gates and an electrically interposed, optoelectronic transmission gate; FIG. 2 is a circuit diagram of an illustrative optical shift register in accordance with the invention; Detailed Description FIG. 1 is a circuit diagram of a circuitry employed in an embodiment of the invention, comprising two optoelectronic signal processing gates, 101, 102 and an optoelectronic transmission gate 151 electrically connected between gates 101 and 102. In this embodiment gates 101, 102 are implemented using symmetric self electro-optic effect devices (S-SEEDs). The logical state of optical processing gate 101 is represented by an internal voltage V 1 , which controls the voltage across the multiple quantum well (MQW) intrinsic regions in the S-SEED of gate 101. Each of the optical gates 101, 102 has one or more optical outputs that also represent the logical state of the device. The logical state of gate 102 is represented by an internal voltage V 2 , which controls the voltage across the MQW regions in the S-SEED of gate 102. Thus, the logical states of gates 101, 102 are represented by both electrical and optical states although the optical output beams from gates 101, 102 are not used in the present embodiment. Optoelectronic transmission gate, 151 operates as an open circuit without incident light and as a short circuit with incident light. The optoelectronic processing gates are SEEDs and if the transmission gate is implemented using back to back quantum well p-i-n diodes, the entire apparatus may be implemented with only one type of device (i. e. MQW diodes), making circuit fabrication simple. In the present embodiment, optical processing gates 101, 102 are S-SEEDs comprising serially connected p-i-n diodes with quantum wells in the intrinsic region, and transmission gate 151 comprises two back to back p-i-n photodiodes which may be identical to the quantum well diodes used in the S-SEEDs. In cascaded operation, a complementary set of input beams, 104, 114, first sets the state of S-SEED 101. Input beams 104, 114 essentially determine V 1 . A set of clock beams, 105, 115, is then applied to S-SEED 101 to provide output beams, 108, 118. Clock beams 105, 115, do not substantially alter the optical state or the voltage V 1 of S-SEED 101. At the same time a set of transfer beams, 109, 119, is applied to transmission gate 151 to transfer the voltage V 1 on the center node of S-SEED 101 to the center node of S-SEED 102. Now V 2 =V 1 . In this implementation, if the transfer beams 109, 119, are applied without the clock beams, 105, 115, S-SEED 101 will likely lose its state; however if the optical processing gates are more complex than S-SEEDs and hold their state indefinitely without incident light beams, only the transfer beams would need to be applied. Lastly, a set of clock beams, 106, 116, incident on S-SEED 102 provides a set of output beams, 107, 117, representative of the optical state of S-SEED 102. This operation provides the functional equivalent of cascading optical processing gates. The cascading is not done by routing the optical outputs from one gate to the inputs of the next gate, but is electrical in that the voltage representing the state of the first gate is applied directly to the second gate. The operation of optoelectronic transmission gates may be better understood by considering their application in several exemplary optical systems. As a first example, consider an optical shift register comprising N optical processing gates with N-1 transmission gates as illustrated in FIG. 2. Operation of the shift register is an extension of the cascaded operation described above. As above, first the input beams 104, 114 set the state of S-SEED 101. Clock beams 105, 115 and transfer beams 109, 119 are then applied transferring the data from S-SEED 101 to S-SEED 102. Clock beams 106, 116 and transfer beams 110, 120 are subsequently applied and the data is transferred to S-SEED 103. This process continues until the data is transferred to the last S-SEED 160 in the shift register. Like other shift registers, half of the data transfers take place during one half clock cycle and the other half take place during the complement half clock cycle. Thus clock beams 106, 116 are complements of clock beams 105, 115; transfer beams 110, 120 are complements of transfer beams 109, 119. Data can be read in or out in parallel to every other S-SEED thereby performing serial to parallel or parallel to serial conversion. Note that the shift register can shift data from left to right as described above by having the odd (even) numbered transfer beams applied concurrently with the odd (even) numbered clock beams. The shift register can shift data from right to left by having the odd (even) numbered transfer beams applied concurrently with the even (odd) numbered clock beams.

Claims: An optical shift register having first and second optical processing gates (101, 102), each of said first and second optical processing gates (101, 102) comprised of S-SEEDs having a pair of p-i-n diodes with quantum wells in the intrinsic region serially connected across a voltage source, each of said S-SEEDs having an electrical junction between the two serial connected p-i-n diodes thereof, said optical shift register comprising: an optically controlled transmission gate (151) comprised of two back to back p-i-n photodiodes which may be quantum well diodes as used in said optical processing gates (101, 102) connected from the electrical junction of said first optical processing gate (101) to the electrical junction of said second optical processing gate (102); wherein a first state of said first optical processing gate (101) is set by a complementary set of input beams, (104, 114), thereby determining a first voltage (V1) at said electrical junction of said first optical processing gate (101); said first optical processing gate (101) subsequently has a first set of clock beams, (105, 115), applied thereto and produce a first set of output beams (108, 118) from said first optical processing gate (101) without affecting the state of said first optical processing gate (101) or said first voltage (V1) corresponding to said first state; said transmission gate (151) has a set of transfer beams (109, 119) concomitantly applied with said first set of clock beams (105, 115) thereto for transferring said first voltage (V1) to said electrical junction of said second optical processing gate (102) thereby setting a second voltage (V2) at said electrical junction of said second optical processing gate (102) equal to said first voltage (V1); and said second optical processing gate (102) has a second set of clock beams, (106, 116) applied thereto to produce a set of second set of output beams, (107, 117) from said second optical processing gate (102) that represent an optical state of said second optical processing gate (102); wherein a state set by said first set of input beams (104, 114) in said first optical processing gate (101) is cascaded to said second optical processing gate (102) by control of said first set of clock beams (105, 115) and said set of transmission beams (109, 119), and affects said second set of output beams (107, 117) produced by said second set of clock beams (105, 115) that is subsequently applied to said second optical processing gate (102).

Inventors: LENTINE ANTHONY LODOVICO, LENTINE, ANTHONY LODOVICO
Applicants: AT & T CORP, AT&T CORP.
Application year: 1991
Main classification: H03K19
IPC codes: G11C19, G06E1, H03K19, G02F3