Design of High Performance SRAM Based Memory Chip

The semiconductor memory SRAM uses bi-stable latch circuit to store the logic data 1 or 0. It differs from Dynamic RAM (DRAM) which needs periodic refreshment operation for the storage of logic data. Depending upon the frequency of operation SRAM power consumption varies i.e. it consumes very high power at higher frequencies like DRAM. The Cache memory present in the microprocessor needs high speed memory hence SRAM can be used for that purpose in microprocessors. The DRAM is normally used in the Main memory of processors, where importance is given to the density than its speed. The SRAM is also used in industrial subsystems, scientific and automotive electronics. In this thesis 16-Kb Memory is designed by using memory banking method in UMC 90nm technology ,which operates at a frequency of 1GHz.The post layout simulation for the complete design is performed and also obtained power analysis for the overall design. All peripherals like pre-charge, Row Decoder, Word line driver, Sense amplifier, Column Decoder/Mux and write driver are designed and layouts of all the above peripherals also drawn in an optimised manner such that their layout occupies minimum area. The 6T SRAM cell is designed with operating frequency of 8 GHz and stability analysis are also performed for single SRAM cell. The layout of Single SRAM cell is drawn in a symmetric manner, such that two adjacent cells can share same contact, which results reduction in the area of cell layout. The Static Noise Margin, Read noise margin and Write Noise Margin of single cell are found to be 240mV, 115mV and 425mV respectively for a supply voltage of 1V.The effect of pull-up ratio and cell ratio on the stability of SRAM cell is observed

Journal of Telecommunications and Information Technology, 2007, nr 2

kwartalni

Low-frequency noise in downscaled silicon transistors: Trends, theory and practice

By the continuing downscaling of sub-micron transistors in the range of few to one deca-nanometers, we focus on the increasing relative level of the low-frequency noise in these devices. Large amount of published data and models are reviewed and summarized, in order to capture the state-of-the-art, and to observe that the 1/area scaling of low-frequency noise holds even for carbon nanotube devices, but the noise becomes too large in order to have fully deterministic devices with area less than 10nm×10nm. The low-frequency noise models are discussed from the point of view that the noise can be both intrinsic and coupled to the charge transport in the devices, which provided a coherent picture, and more interestingly, showed that the models converge each to other, despite the many issues that one can find for the physical origin of each model. Several derivations are made to explain crossovers in noise spectra, variable random telegraph amplitudes, duality between energy and distance of charge traps, behaviors and trends for figures of merit by device downscaling, practical constraints for micropower amplifiers and dependence of phase noise on the harmonics in the oscillation signal, uncertainty and techniques of averaging by noise characterization. We have also shown how the unavoidable statistical variations by fabrication is embedded in the devices as a spatial “frozen noise”, which also follows 1/area scaling law and limits the production yield, from one side, and from other side, the “frozen noise” contributes generically to temporal 1/f noise by randomly probing the embedded variations during device operation, owing to the purely statistical accumulation of variance that follows from cause-consequence principle, and irrespectively of the actual physical process. The accumulation of variance is known as statistics of “innovation variance”, which explains the nearly log-normal distributions in the values for low-frequency noise parameters gathered from different devices, bias and other conditions, thus, the origin of geometric averaging in low-frequency noise characterizations. At present, the many models generally coincide each with other, and what makes the difference, are the values, which, however, scatter prominently in nanodevices. Perhaps, one should make some changes in the approach to the low-frequency noise in electronic devices, to emphasize the “statistics behind the numbers”, because the general physical assumptions in each model always fail at some point by the device downscaling, but irrespectively of that, the statistics works, since the low-frequency noise scales consistently with the 1/area law

The 1991 3rd NASA Symposium on VLSI Design

Papers from the symposium are presented from the following sessions: (1) featured presentations 1; (2) very large scale integration (VLSI) circuit design; (3) VLSI architecture 1; (4) featured presentations 2; (5) neural networks; (6) VLSI architectures 2; (7) featured presentations 3; (8) verification 1; (9) analog design; (10) verification 2; (11) design innovations 1; (12) asynchronous design; and (13) design innovations 2

Modeling EMI Resulting from a Signal Via Transition Through Power/Ground Layers

Signal transitioning through layers on vias are very common in multi-layer printed circuit board (PCB) design. For a signal via transitioning through the internal power and ground planes, the return current must switch from one reference plane to another reference plane. The discontinuity of the return current at the via excites the power and ground planes, and results in noise on the power bus that can lead to signal integrity, as well as EMI problems. Numerical methods, such as the finite-difference time-domain (FDTD), Moment of Methods (MoM), and partial element equivalent circuit (PEEC) method, were employed herein to study this problem. The modeled results are supported by measurements. In addition, a common EMI mitigation approach of adding a decoupling capacitor was investigated with the FDTD method

Topical Workshop on Electronics for Particle Physics

The purpose of the workshop was to present results and original concepts for electronics research and development relevant to particle physics experiments as well as accelerator and beam instrumentation at future facilities; to review the status of electronics for the LHC experiments; to identify and encourage common efforts for the development of electronics; and to promote information exchange and collaboration in the relevant engineering and physics communities