Design Of Low Power VLSI Circuits Using Energy Efficient . - IJSER

1y ago
10 Views
2 Downloads
990.30 KB
10 Pages
Last View : 18d ago
Last Download : 3m ago
Upload by : Harley Spears
Transcription

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518349Design of Low Power VLSI Circuits usingEnergy Efficient Adiabatic LogicAmit Shukla, Arvind Kumar, Abhishek Rai and S.P. SinghAbstract—In this paper, a new design of adiabatic circuit, called energy efficient adiabatic logic (EEAL) is proposed. Earlier various diodebased adiabatic logic families have been proposed. To achieve minimum energy consumption, this paper proposes a technique in whichdiode is replaced by MOS transistor at charging and discharging path whose gate is controlled by the power clocks. By using thistechnique non adiabatic loss and power consumption of the diode is eliminated. In the proposed circuit, the input and output logic levels arenearly the same and can be used for building cascaded logic circuits. The split level sinusoidal power supply is used to achieve low powerhigh speed adiabatic circuits. In this paper we have designed and simulated NOT, NAND, NOR gates, Half Adder and Full adder circuit. Allsimulations in this paper have been implemented by VIRTUOSO SPECTRE simulator of cadence with the 0.18 μm UMC technology MOStransistor model under 1.8-volt peak to peak split level sinusoidal power clock supply. From the simulation result, we find that proposedlogic circuits can save significant amount of energy compared to CMOS circuits and GFCAL circuits with similar parameters up to 500MHz.Index Terms— Adiabatic logic, Energy efficient, Low power, Power delay product, Power dissipation, Recovery logic, Split level powerclock—————————— ——————————1 INTRODUCTIONIJSERIndia (corresponding author email amitshukla33@gmail.com) Arvind kumar is Asst. Professor with the Department of Electronics andCommunication engg. MNNIT Allahabad India(emailarvindk@mnnit.ac.in)Demands for low power electronics have motivateddesigners to explore new approaches to VLSI circuits. Theclassical approaches of reducing power consumption inconventional CMOS circuits included reducing the supplyvoltages, node capacitances, and switching frequencies. Thepower consumption in conventional CMOS is proportionalto the square of the power supply voltage; therefore,voltage scaling is one of the important methods used toreduce power consumption. To achieve a high transistordrive current and improve the circuit performance, thetransistor threshold voltage (Vt) must be scaled down inproportion to the supply voltage. However, scaling downof the transistor threshold voltage (Vt) results inproportional increase in subthreshold leakage current [1].Adiabatic systems have been applied to low powerdevices. Various adiabatic logic families have beenproposed [2-15] emphasizing on the energy recoveryprinciple. There are two types of adiabatic circuits; fullyadiabatic and quasi adiabatic circuits. Fully adiabaticcircuits are more complex then quasi adiabatic circuits, andhence not grown in popularity as quasi adiabatic circuits,which have simpler architecture and power supply �� Amit Shukla,Abhishek Rai and S.P.Singh are with the Department ofElectronice and Communication engg. (VLSI Design) MNNIT AllahabadFully adiabatic circuits suffer from adiabatic loss due to theleakage current through non-ideal switches. Quasiadiabatic circuits suffer from adiabatic and non-adiabaticloss. Non-adiabatic loss is proportional to the capacitancedriven and square of the threshold voltage. Adiabatic lossis proportional to frequency but non-adiabatic loss isindependent on frequency. The term ‘adiabatic’ meansreversible thermodynamic process where a transformationtakes place in such a way that no gain or loss of energyoccurs [3]. Some energy recovery logic has been proposed[4-7]. They have achieved significant energy savingcompared with conventional logic but output of thesecircuits are valid only during a particular phase of powerclock. Hence, multiple-phase clocking is required to drive achain of cascaded adiabatic logic circuits. Younis andKnight have proposed adiabatic logic families with lessdissipation but each gate requires 16 times the number ofdevices compared with conventional logic [8].Dickinsonand Denker have used a diode based adiabatic dynamiclogic circuits [9]. The drawbacks are that the gates aredynamic and require four phase clocking for cascading thegates. Antonio and Saletti proposed a positive feedbackadiabatic logic gate, but this requires four phase powerclock and requires the input in its complement form [10].Recently diode based adiabatic logic circuits have beenIJSER 2013http://www.ijser.org

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518proposed [11-15]. Most of them achieve significant powersaving but they have several disadvantage such as outputamplitude degradation, large delay, complex circuitstructure and power dissipation across the diode in thecharging path.In this paper, we propose energy efficient adiabatic logiccircuits. EEAL inherits all the advantages of recentlyreported adiabatic logic circuits with additionalimprovement in power saving. By using the EEAL circuits,we can achieve high output amplitudes and reduce powerdissipation. To minimize the dynamic power consumptionin this circuit, we apply a split level sinusoidal supplyvoltage. Further we have also proposed various EEALbased logic circuits and compare their performances withthe recently reported (GFCAL) glitch free cascadebleadiabatic logic circuits and conventional CMOS circuit.This paper is divided into five sections. Section 1 dealsthe introduction part. Section 2 describes the differencesbetween conventional CMOS and adiabatic circuits. Section3 describes the proposed energy efficient adiabatic logic(EEAL) circuit operation and its analysis. In section 4discusses about EEAL based various circuit. Conclusion isgiven in the section 5.350QW 0 v(t)dq(1)At any instant, the voltage across the capacitor v(t)So equation (1) becomesQ q(t)W 0Cdq 12CV2E QV CV2𝐶(2)(3)So energy dissipated by resistor is during charging1Ediss E – W CV22IJSERIn conventional CMOS circuits, load capacitor (C) is chargefrom a dc power supply and discharging it to ground,whereas, in adiabatic circuits, the load capacitor is chargethrough the varying power supply and it discharge to thevarying power supply instead of discharging it to ground.Power dissipation in logic circuits primarily occurs duringswitching. The inverter can be considered to consist of apull-up (PMOS) and pull-down (NMOS) networksconnected to the load capacitance (C). Both pull-up andpull-down networks can be modeled by an ideal switch inseries with resistor (R) which is equal to correspondingchannel resistance of the transistor. For understanding thecharging and discharging process, inverter can be modeledas simple RC circuit.𝑞(𝑡)The energy drawn from the power supply(4)RV2 Conventional CMOS Circuits VersesAdiabatic Logic Circuits CDC / varyingpower supplyFigure 1 Simple RC circuitThis shows that one half of the energy is dissipated as heatduring charging through pull-up networks (PMOS) andhalf of energy is stored in load capacitor. Hence inconventional CMOS, during a complete charge-dischargecycle, the energy CV2 is withdrawn from power supply andis dissipated as heat. Half of this energy dissipated duringcharging and half of energy dissipated during discharging.2.2 Conventional ChargingConsider a simple RC circuit as shown in figure 1.Assume that initially the charge on the capacitor is 0 and itstarts charging at time t 0 from constant power supplyvoltage V. At any instant of time the voltage on thecapacitor is v(t). A small amount of charge dq to thecapacitor requires an amount of work dW v(t)dq. Thetotal work done in charging the capacitor from 0 to Qcoulombs is2.2 Adiabatic ChargingIn adiabatic charging, capacitor is charge by the timevarying power supply. For convenient we take ramp typeVvoltage source V(t) , where V is the peak voltage ofTpower supply and T is the time period. At any instant oftime the currentIJSER 2013http://www.ijser.org

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518i(t) VCT351(1- e 𝑡/𝑅𝐶 ).Energy dissipated across the resistor during chargingTEdiss 0 i2 (t)Rdt ((T RC)RCT) CV2,(5)Compare equation (4) & (5), it has been seen that if timeperiod of charging/discharging T is much greater then RC,then energy dissipation in adiabatic is less thanconventional CMOS. That is, energy dissipation can bemade arbitrarily small by increasing the charging time T.3 Proposed Energy Efficient Adiabatic Logic(EEAL) Inverter3.1 Circuit The basic schematic of energy efficient adiabatic logiccircuit is shown in fig. 2(a). This circuits involve an Nnetwork, P-network and one charging NMOS transistor(T1) and one discharging PMOS (T2) whose gate arecontrolled by power supply. The EEAL circuits use twocomplementary split level sinusoidal power supply (Vc & ). The voltage level of Vc exceeds that of Vc by a factor ofVcVdd/2. One power supply is in phase while other supply isout of phase which has peak-to-peak voltages of 1.8V in a180nm CMOS process. The power supply design still meetsthe requirement in, where the voltage difference betweencurrent carrying electrodes must be zero when thetransistor switches to the ON State. The power supplyexpression is given as follows:IJSERVcSinDCFigure 2(b)waveformsP1INPUTVC T1T2OUTPUTCLGNDFigure 2(a) Proposed EEAL inverter circuitsVdd43sin(ω t θ) Vdd4 - Vdd sin(ω t θ) 1 VddVc44The NMOS transistor (T1) is in the pull-up network andPMOS transistor (T2) in the pull-down network are use inthe place of diode for the charging and discharging. At thecharging and discharging path, channel resistance is sameso, circuit is balanced. The power dissipation due to ONresistance is significantly lower than the power dissipationdue to the threshold voltage drop through diodes. Henceusing MOS transistor, power dissipation is reducedcompare to the diode based adiabatic circuits. Thesimulated waveform of proposed inverter in fig 2(b) showsthat logic level difference between input and output is verysmall and can be used for building cascaded logic circuits.IJSER 2013http://www.ijser.org

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-55183.4 Comparison of power, delay and PDP withfrequency at fixed load capacitanceFor understanding the circuit operation of proposedinverter, first let’s assume that the output capacitor isinitially uncharged state and input is logic ‘0’. In this case,the transistor P1 will be ON while the transistor N1 is OFF. decreasing, at some pointWhen Vc is increasing and Vcwhere power supply Vc exceeds the threshold voltage Vtnof the transistor T1, the transistor T1 turns ON and startscharging the capacitor. So logic ‘0’ gives logic ‘1’ at theoutput.The input and supply frequencies are variedsimultaneously from 1 MHz to 500 MHz. For betterperformance power supply frequency should be greaterthan two time of input supply frequency.When output capacitor is initially charged and input islogic ‘1’. In this case the transistor N1 will be ON while thetransistor P1 is OFF, since the gate of the transistor T2 is , the transistor T2 will ON at the pointconnected to Vc where the Vc exceeds the threshold voltage Vtp of thattransistor. The output capacitor starts discharging. So logic‘1’ gives logic ‘0’ at the output. Hence the output is thecomplement of the input.109876543210CMOSPower dissipation (μW)3.2 Circuit Operation352110GFCAL2550IJSERWhen output capacitor is initially charged and input islogic ‘0’. In this case the transistor P1 will be ON andtransistor N1 will be OFF. At the charging path transistorT1 will be OFF, this is because due to large thresholdvoltage Vtn of the transistor and thus prevents charging. Socapacitor remains unchanged. Thus logic ‘0’ gives logic ‘1’at the output.In last two cases, no transitions occur at the output sodynamic switching is reduce and thus energy dissipation isalso reduce in proposed logic circuits.Frequency (MHz)(a)1.2CMOS1Here we check the performance of the Proposed EEAL,GFCAL and conventional CMOS inverter. The circuit of theinverter is simulated using VIRTUOSO SPECTRE circuitsimulator of cadence EDA tools. The length and width ofthe transistor are 180 nm and 240 nm, respectively the valueof load capacitance is 5 fF; we have been simulated theirpower and delay and compared with the variation intransition frequency.IJSER 1102550 100 250 333 500Frequency (MHz)(b)3.3 Efficiency of proposed inverter circuit withfrequency100 250 333 500Delay (nS)When output capacitor is initially uncharged state andinput is logic ‘1’. In this case the transistor N1 will be ONand transistor P1 will be OFF. At the discharging pathtransistor T2 will be OFF, this is because power clock doesnot exceed the threshold voltage Vtp of the transistor andthus prevents discharging. So the capacitor remainsunchanged. Thus logic ‘1’ gives logic ‘0’ at the output.Proposed

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518Power -Delay Product (fJ)1CMOSGFCALsimulate the proposed inverter by adding different one byone load capacitor at the output node. Input supplyfrequency kept 50 MHz and for better performance, powersupply frequency kept 100 MHz. As the load capacitancetakes time to charge or discharge based on its capacitancevalue, a large capacitance will lead to slow charging anddischarging and small capacitance values give very fastcharge and discharge times. However a disadvantage ofusing smaller capacitance is the ripple observed in theoutput waveform.Proposed0.80.60.40.201102550353100 250 333 5007Frequency (MHz)CMOS6Power-Delay Product (fJ)(c)Figure 3 Simulation result of inverter compare in term of(a) Power dissipation with varying frequency, (b) Delaywith varying frequency, (c) Power-delay-product withvarying frequencyGFCAL5432IJSERIn the graph, we have seen that as input frequency increase,power dissipation of both the inverter increases whereasproposed (EEAL) inverter have lesser power dissipation ateach frequency in comparison to conventional CMOS andGFCAL. The output logic levels up to frequencies of50MHz are 1.65 V corresponding to logic ‘1’ and 0.25 Vcorresponding to logic ‘0’. It has been observed that asfrequencies increases then 50 MHz, the logic valuecorresponding ‘1’ is decreases and logic valuecorresponding ‘0’ is increases. At frequencies higher than500 MHz, the difference between logic‘1’ and logic ‘0’becomes small. This is because the time period of thesupply waveform is small compared with the time constantof charging and discharging, and the capacitor is unable tocharge and discharge to the required levels. However acontinuous decrease in delay for both the inverter withinput frequency is observed. Initially proposed EEALinverter has larger delay then conventional CMOS but lessthan GFCAL. When input frequency reaches around 50MHz the difference between their delays are minimized.Thus from given observation it is observed that powerefficiency and overall power delay product (PDP) isimproved 50% in comparison to conventional CMOS and20% in comparison to GFCAL throughout the wholefrequency range.3.5 Efficiency of proposed inverter circuits with loadcapacitanceDiode using MOS transistors are weak in drivingcapability. Here we observe the driving capability of theproposed EEAL inverter without using any diode; weProposed105102030405060Load Capacitor (fF)Figure 4 simulation result of inverter compare in term ofPDP with varying load capacitorHere we observed that when load capacitance is increasesthe power dissipation of both inverters correspondinglyincreases but a very small delay increase in comparison toconventional CMOS but less than GFCAL. However ourproposed EEAL inverter has better energy efficient thanconventional CMOS at all load capacitor. From simulationresult it is observed that power efficiency and overallpower delay product (PDP) is significant improved incomparison to conventional CMOS and GFCAL throughoutthe all load capacitor.4 Proposed EEAL based logic circuitsThe NAND and NOR gates are universal gates and usedto design complex digital circuits. As we cannot buildadiabatic circuits by simply using conventional methodtherefore an optimized design of these gates can certainlybenefit the performance of the larger circuits. In theIJSER 2013http://www.ijser.org

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518354following subsections, various logic such as NAND, NOR,Half adder and Full adder circuits have been implementedbased on proposed EEAL design. The simulation at 25 MHzis done by VIRTUOSO SPECTRE circuit simulator ofcadence EDA tools. The length and width of the transistorare 180 nm and 240 nm.4.1 Proposed EEAL NAND gateVcAVcSinSinDCDCN1P1BP2(b)Figure 5 Proposed EEAL NAND logic gate (a) Circuitdiagram, (b) Simulation waveformN2IJSERThe simulated timing waveforms for input string A 10001000100010001000, B 11001100110011001100 andoutput 01110111011101110111 are shown in Fig 5(b).When any input has logic ‘0’, then output give logic ‘1’otherwise output give logic ‘0’. Thus a NAND operation isrealized. From the simulation result, it has been seen thatthe power dissipation in the proposed NAND gate is about60% of that of a CMOS and about 15% of that of GFCALNAND gates.T1T2CLOUTPUTGND(a)Circuit diagram of proposed adiabatic NAND gate isshown in Fig 5(a). This circuit consists of two branches. Thefirst branch consists of two parallel P-channels MOSFET (P1& P2) and a N-channel MOSFET (T1) connected in series.The second branch consist of two series N-channelMOSFET (N1 & N2) and a P-channel MOSFET (T2)connected in series. The output of load capacitance OS/pMOS) T1 & T2 whose gate is directly connected ). Gate ofwith split level sinusoidal power clock (Vc and VcP1 & N1 are tied together with an input A and P2 & N2with another input B.4.2 Proposed EEAL NOR gateVcVcASinSinDCDCN1N2P1BP2T2T1GNDIJSER 2013http://www.ijser.orgCLOUTPUT

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518355to the inverter. The OR gate is realized by connecting theoutput of a NOR gate as input to the yA.BCLBProposedSUM A BNORProposedNORCL(a)(b)IJSERFigure 6 Proposed EEAL NOR logic gate (a) Circuitdiagram, (b) Simulation waveformCircuit diagram of proposed adiabatic NOR gate is shownin Fig 6(a). This circuit consists of two branches. The firstbranch consists of two series P-channel MOSFET (P1 & P2)and a N-channel MOSFET (T1) connected in series. Thesecond branch consists of two parallel N-channel MOSFET(N1 & N2) and a P-channel MOSFET (T2) connected arged through charging/discharging (nMOS/pMOS) T1 & T2 whose gate is directly connected ). Gate ofwith split level sinusoidal power clock (Vc and VcP1 & N1 are tied together with an input A and P2 & N2with another input B. The simulated timing waveforms forinput string A 10001000100010001000,B 11001100110011001100 and output 00110011001100110011are shown in Fig 6(b). When any input has logic ‘1’, thenoutput give logic ‘0’ otherwise output give logic ‘1’. Thus aNOR operation is realized. From the simulation result, ithas been seen that the power dissipation in the proposedNOR gate is about 60% of that of a CMOS and about 15% ofthat of GFCAL NOR gates.4.3 Proposed EEAL Half AdderThe half adder circuit is realized using two NOR gates andone AND gate as shown in Fig 7(a). The AND gate isrealized by connecting the output of a NAND gate as input(b)Figure 7 Proposed EEAL Half Adder (a) Block diagram, (b)Simulation waveformIn order to realize a operation, consider the truth table forhalf-adder. The outputs namely the SUM and CARRY .It isrequired that the SUM should be logic ’0’ when both inputsare same i.e logic 0. For the logic ‘1’ output, the inputs canbe any of the two combinations i.e. 01, 10, i.e input are notsame. The CARRY is taken at the output node, whichfollow as the AND gate. The combination of inputs ‘00,01, 10, 11’ are given in the form of strings A ‘10001000100010001000’ and B ‘11001100110011001100’.The outputs namely the SUM and CARRY are obtained asIJSER 2013http://www.ijser.org

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518strings SUM ‘01000100010001000100’ and CARRY ‘10001000100010001000’, respectively. Simulated waveformis shown in Fig 7(b) at different input frequency. From thesimulation result, it has been seen that CMOS half addertakes double power consumed by the proposed adiabatichalf adder.4.4 Proposed EEAL Full AdderThe Full adder circuit is realized using two half adders andan OR gate as shown in Fig 8 (a). The OR gate is realized byconnecting the output of a NOR gate as a input of inverter.The supply for all the circuits is used split level sinusoidalpower clock.356The performance of full adder circuit is same as that of thehalf adder. Full adder has three input and output is SUMand CARRY. The combination of input for all state aregiven in the form of string A ‘1000100010001000’ B ‘1100110011001100’ and C ‘1110111011101110’. The outputnamely the SUM and CARRY are obtained as strings SUM ‘1010101010101010’ and CARRY ‘1100110011001100’respectively. Simulated waveform is shown in Fig 8(b) atdifferent input frequency. For better performance, Powerclock frequency should take more than two times of inputfrequency.4.5 Comparison of power dissipation for theproposed EEAL full adder, GFCAL full adder andCMOS full adder at different transition osedfull adderPowerdissipationin(µW)GFCALfull adderPowerdissipationin(µW)CMOS fulladder1 CarryAProposedProposed HAORBSUMIJSERProposed HACCarrySUM(a)30Power dissipation (μW)25(b)CMOSSimulation waveformIJSER 2013http://www.ijser.orgProposed201510501Figure 8 Proposed EEAL Full Adder (a) Block diagram, (b)GFCAL51025Frequency (MHz)50100

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518Figure 9 Power dissipation of Full adder circuitHere we check the performance of the proposed fulladder, GFCAL full adder and conventional CMOS fulladder. The circuit is simulated using VIRTUOSO SPECTREcircuit simulator of cadence EDA tools. The length andwidth of the transistor are 180 nm and 240 nm, respectivelythe value of load capacitance is 5 fF. We have beensimulated their power dissipation and compared with thevariation in transition frequency. From the simulationresult we find that power dissipation in proposed fulladder is about 50% compare with that of the CMOS fulladder.5 ConclusionsIn this paper we have presented energy efficient adiabaticlogic circuits in which power delay product is improvedmore than 50% compared with that of conventional CMOScircuits. The simulation result and comparativeperformance revealed that power dissipation in proposedlogic are considerably lower than conventional CMOSlogic. Previously adiabatic logic circuits use of diode whichlimit the direction of current. It is not only difficult tofabricate diodes in CMOS technology but also consumemore power. In this circuit, input and output logic levelsare approximately same so it can be used in buildinghierarchical circuits. Further, the proposed circuits havelow power density on chip and thus it can be used in poweraware high performance VLSI circuitry.357logic circuit”. Proc. Intern. Symp. Low power design, 1995,pp. 191-196.[5] Moon Y., Jeong D.K., “An efficient charge recovery logiccircuits”. IEEE Journal of Solid-State Circuits, 1996, SC-31,(4) pp.514-522.[6] Liu F., Lau K.T., “Pass transistor adiabatic logic withNMOS pull-down configuration”, Electron. Lett., 1998, 34,(8) pp.739-741.[7] Maksimovic D., Oklobdzija V.G., Nikolic B., CurrentK.W., “Clocked CMOS adiabatic logic with integratedsingle phase power clock supply”. IEEE Transaction onvery large scale integration system, 2000, 8,(4), pp.460-463.[8] Younis S., Knight T., “Asymptotically zero energy splitlevel charge recovery logic”. Proc. Workshop on low powerdesign, Napa Valley, California, 1994, pp. 177-182.IJSERREFERENCES[1] K. Roy, S. Mukhopadhyay and H. mahmoodi-Meimand,“A leakage current mechanism and leakage reductiontechniques in deep sub-micrometer CMOS circuits,” Proc.IEEE, Vol.91, Issue2, Feb, 2003, pp.305-327.[2] Hu Jianping; Cen Lizhang; Liu Xiao; “ A new type oflow power adiabatic circuit with complementary passtransistor logic” ASIC,2003. Proc. 5th internationalConference on Vol.2, Oct.2003, pp.1235-1238.[3] K.A.Valiev and V.I. Starosel’ ski, “A model andproperties of a thermodynamically reversible logic gate”Mikroelektronika, 29(2), 83-98(2000).[4] Kramer A.Denker J.S., Flower B., Moroney J., “Secondorder adiabatic computation with 2N-2P and 2N-2N-2P[9] Dickinson A.g., Denker J.S., “Adiabatic dynamic logic”,IEEE Journal of Solid State Circuits, 1995, 30,(3), pp.311-315.[10] Antonio B., Saletti R., “Ultra low power adiabaticcircuit semi-custom design”, IEEE Transaction on verylarge scale integration Systems, 2004,12, (11), pp. 1248-1253.[11] N.S.S. Reddy, M .Satyam, and K.L. Kishore, “Caacadable adiabatic logic circuits for low powerapplications” IET circuit, Devices & System, 2(6), 518526(2008).[12] Nazarul Anuar, Yashuhiro Takahashi, and ToshikazuSekine, “LSI implementation of a low power 4x4 bit arraytwo phase clocked adiabatic static CMOS logic multiplier”Microelectronics Journal, Elsevier,43,244-249(2012).[13] Wang Pengjun and Yu Junjun, “ Design of two phasesinusoidal power clock and clocked transmission gateadiabatic logic circuit” Journal of Electronics (China), 24(2).225-231(2007).[14] A. Blotti, R. Saletti, “Ultralow power adiabatic circuitsemi custom design” IEEE Transaction on VLSI system,12(11), 1248-1253(2004).[15] Nazarul Anuar, Yashuhiro Takahashi, and ToshikazuSekine, “ Two phase clock adiabatic static CMOS logic andits logic family” Journal of semiconductor technology andscience, 10(1),1-10(2010).IJSER 2013http://www.ijser.org

International Journal of Scientific & Engineering Research, Volume 4, Issue 6, June-2013ISSN 2229-5518IJSERIJSER 2013http://www.ijser.org358

Adiabatic logic, Energy efficient, Low power, Power delay product, Power dissipation, Recovery logic, Split level power clock —————————— —————————— 1 INTRODUCTION . Demands for low power electronics have motivated designers to explore new approaches to VLSI circuits. The classical approaches of reducing .

Related Documents:

VL2114 RF VLSI Design 3 0 0 3 VL2115 High Speed VLSI 3 0 0 3 VL2116 Magneto-electronics 3 0 0 3 VL2117 VLSI interconnects and its design techniques 3 0 0 3 VL2118 Digital HDL Design and Verification 3 0 0 3 VL2119* Computational Aspects of VLSI 3 0 0 3 VL2120* Computational Intelligence 3 0 0 3

VLSI Design 2 Very-large-scale integration (VLSI) is the process of creating an integrated circuit (IC) by combining thousands of transistors into a single chip. VLSI began in the 1970s when complex semiconductor and communication technologies were being developed. The microprocessor is a VLSI device.

VLSI IC would imply digital VLSI ICs only and whenever we want to discuss about analog or mixed signal ICs it will be mentioned explicitly. Also, in this course the terms ICs and chips would mean VLSI ICs and chips. This course is concerned with algorithms required to automate the three steps “DESIGN-VERIFICATION-TEST” for Digital VLSI ICs.

Dr. Ahmed H. Madian-VLSI 3 What is VLSI? VLSI stands for (Very Large Scale Integrated circuits) Craver Mead of Caltech pioneered the filed of VLSI in the 1970’s. Digital electronic integrated circuits could be viewed as a set

15A04604 VLSI DESIGN Course Objectives: To understand VLSI circuit design processes. To understand basic circuit concepts and designing Arithmetic Building Blocks. To have an overview of Low power VLSI. Course Outcomes: Complete Knowledge about Fabrication process of ICs Able to design VLSIcircuits as per specifications given.

55:131 Introduction to VLSI Design 10 . Simplified Sea of Gates Floorplan 55:131 Introduction to VLSI Design 11 . SoG and Gate Array Cell Layouts 55:131 Introduction to VLSI Design 12 . SoG and Gate Array 3-in NAND 55:131 Introdu

Principles of VLSI Design Introduction CMPE 315 Principles of VLSI Design Instructor Chintan Patel (Contact using email: cpatel2@cs.umbc.edu). Text CMOS VLSI Design: A Circuits and Systems Perspective, Third Edition. by Neil H.E. Weste and David Harris. ISBN: 0-321-14901-7, Addison Wesl

VLSI Fabrication Process Om prakash 5th sem ASCT, Bhopal omprakashsony@gmail.com Abstract VLSI stands for "Very Large Scale Integration". This is the field which involves packing more and more logic devices into smaller and smaller areas. Thanks to VLSI, circuits that would have