We designed a superconducting random access memory (RAM) in which all component circuits can be operated with dc-bias currents. A dc-powered superconducting loop driver and a dc-powered sense circuit are effectively combined with single flux quantum (SFQ) circuits. We proposed a pipeline structure for the memory cell array composed of the dc-powered loop drivers, the dc-powered sense circuits, passive transmission lines (PTLs), and SFQ gates. This pipeline structure enables a clock operation of 10 GHz even in a large-scale RAM. An effective device structure for the RAM based on a planarized multi-layer device structure was proposed. A dc-power layer and two PTL layers were placed under the ground plane. This structure is indispensable to create the pipeline structure using PTLs. The large inductance formed in the power layer enables low power dissipation of the RAM. We found from the estimations that 10 GHz clock operation with extremely low power dissipation can be achieved even in a large-scale RAM of 1 Mbit.
We designed a superconducting random access memory (RAM) in which all component circuits can be operated with dc-bias currents. A dc-powered superconducting loop driver and a dc-powered sense circuit are effectively combined with single flux quantum (SFQ) circuits. We proposed a pipeline structure for the memory cell array composed of the dc-powered loop drivers, the dc-powered sense circuits, passive transmission lines (PTLs), and SFQ gates. This pipeline structure enables a clock operation of 10 GHz even in a large-scale RAM. An effective device structure for the RAM based on a planarized multi-layer device structure was proposed. A dc-power layer and two PTL layers were placed under the ground plane. This structure is indispensable to create the pipeline structure using PTLs. The large inductance formed in the power layer enables low power dissipation of the RAM. We found from the estimations that 10 GHz clock operation with extremely low power dissipation can be achieved even in a large-scale RAM of 1 Mbit.
We present the design and test results of components for a superconductor Cryogenic Random Access Memory (CRAM). The 16-Kb RAM design consists of four 4-Kb sub-arrays (blocks) with a 400 ps access time (latency) and a 100 ps cycle time (throughput). Each 4-Kb RAM block comprises a row-accessed 32/spl times/128 memory cell array, bipolar line drivers, row decoders, and column sense circuits. The implementation of specially designed distributed Josephson junctions in the sensing circuits reduces the overall size of the blocks and allows the use of smaller dc control currents.
A new design concept for the Josephson-junction random access memory (RAM) has been developed. In contrast to previous RAMs based on single flux quantization (SFQ), in our system READ and WRITE operations employ ballistic transfer of SFQ pulses along bit lines (either Josephson transmission lines, or passive superconducting microstrip lines, or their combination). The basic memory cells are the single-junction SQUIDs, connected serially by the bit lines and inductively coupled to word lines. READ and WRITE operations are performed by sending SFQ pulses in appropriate directions along bit lines, and DC currents of appropriate polarity into word lines. This approach allows design of very dense memories with n/spl les/2 Josephson junctions per bit, memory cell area smaller than 80 /spl lambda//sup 2/ (where /spl lambda/ is the minimum feature size), and the critical parameter margin well above /spl plusmn/20%. In this paper we present the general structure of the RSFQ RAM, as well as design and results of testing of the basic memory cell and decoder circuitry using Hypres' 3.5-/spl mu/m, 1-kA/cm/sup 2/ Nb-trilayer technology.>
Superconductor electronics offers logic circuits for high-speed data processing and high-performance computing. The main barrier to practical application is the lack of high-speed and low-power memory. It is widely believed that the most reliable and functional bit cell for superconducting memory is the vortex transitional bit cell, which was successfully used by Nagasawa in a 4-kb memory. This paper reviews existing challenges in this type of Josephson memory devices and discusses engineering issues in implementing a model single flux quantum random access memory. We evaluate the contributions that various components of the memory system make to delay and power dissipation. The 256-bit memory provides an experimentally confirmed read access time of 190 ps. As a result, we found that delay and power dissipation are found largely in the address decoder, line drivers, bit-selection scheme, and the data readout circuitry. With these circuits being similar for various magnetic memory devices, our findings provide essential data for a comprehensive assessment of new concepts for bit cells, readout, and write in superconducting memories.
An experimental memory model for investigating the feasibility of a 16K RAM memory with Josephson junctions was fabricated and tested. There are nearly 4500 Josephson junctions in the design which includes array, line drivers, and address decoders. Storage element is a single flux-quantum (SFQ) cell arranged in a 2K array. Drivers and decoders are based on the principle of current steering in superconducting loops, which is a medium speed but low power approach. The measured read-access time of the model is approximately 10 ns. Power dissipation of the unselected chip is zero, whereas for a read/write cycle time of 30 ns, it amounts to about 10 /spl mu/W. Results indicate that a 16K chip is feasible electrically. The estimated access time and power dissipation are 15 ns and 40 /spl nu/W, respectively.
We have designed a 16 kbit superconducting latching/SFQ hybrid (SLASH) RAM, which enables high-frequency clock operation up to 10 GHz. The 16 kbit SLASH RAM consists of four 4 × 4 matrix arrays of 256 bit RAM blocks, block decoders, latching block drivers, latching block senses, impedance matched lines and the powering circuits. The 256 bit RAM block is composed of a 16 × 16 matrix array of vortex transitional memory cells, latching drivers, SFQ NOR decoders and latching sense circuits. We have also designed and implemented an SFQ NOR decoder that is composed of magnetically coupled multi-input OR gates and RSFQ inverters.
The address decoders, address line drivers, and sense circuits of the fully decoded memory consist of resistor-coupled Josephson logic circuits to realize fast access. The memory cell is constructed from two three-junction symmetric SQUID (superconducting quantum interface device) gates, and a four-flux-quanta storage loop for enabling bipolar current drive. This memory configuration has intrinsic advantages in regard to magnetic flux trapping in address lines and a gate circuit latch-up problem over a DC-powered memory constructed from inductor coupled gates. Individual control and cell circuits were fabricated, using a lead-alloy process, and their operation was verified. A 570-ps read access time is estimated as the sum measured 280-ps decoding time, and calculated 130-ps address line current rising time, 110-ps sense time, and 50-ps signal propagation time. The 1-kb chip is designed to consume 9 mW without voltage regulators.>