Noise Margin analysis of Efficient CNTFET- based Standard Ternary Inverter

An ultra-thin natural-source-based cellulose derivate is used in a bilayer gate dielectric for organic complementary inverters. Extraordinarily high small-signal gains up to 1600, a very sharp transition region (as low as 40 mV), a full rail-to-rail swing, a balanced noise margin of 92.5%, and “long-time” stability are shown, revealing that these inverters are highly suitable for complex circuit designs. For more than a decade now the research in organic electronics was driven by unique consumer markets demanding for electronic circuits on flexible substrates over large areas and ideally at low cost. Meanwhile, versatile macroelectronic applications with attractive form factors such as flexible displays,1-4 large-area sensor arrays,5-11 e-paper,12, 13 low-cost radio-frequency identification tags,14-18 and bendable microprocessors19 have been realized using organic thin-film transistors (OTFTs) as the essential element. In the majority of these applications OTFTs are integrated either in the form of arrays or as digital logic. The fundamental building block of digital logic is the inverter, a circuit that inverts an input signal. Much work has been devoted in the last five years to design unipolar inverters using p-type-only OTFTs.18-23 Unfortunately, unipolar logic based on single gate OTFTs always suffers from high power consumption and low noise margin coupled with high noise margin variability and therefore impedes the fabrication of complex circuits having hundreds or more logic gates.19, 22, 23 In this context, it stands beyond doubt that the integration of both n-type and p-type transistors in complementary organic-based circuits12 is very advantageous due to a lower power dissipation, higher noise margin, better operational stability, and easier design of the circuit.24-27 To date, several major obstacles complicated the development of organic complementary circuits, which are as follows: i) the lack of n-channel OTFTs with a performance comparable to the p-channel OTFTs, ii) the challenge of device stability (difficulty in fabricating OTFTs with hysteresis-free characteristics), and iii) the difficulty in fabricating sufficiently thin gate dielectrics allowing for low supply voltages. Although many recently reported complementary organic inverters are impressive with respect to their low operation voltages (≤5 V),27-36 high static gains (>100 V/V),25, 28, 30, 32 and large noise margins (>80%),25, 35, 37, 38 only few of those can combine low-voltage operation with high gain and sufficient immunity against electrical noise.39 Moreover, there have been few investigations of the influence of hysteresis and threshold voltage shifts on the inverter characteristics, which typically gives rise to electrical instabilities and performance limitations of those devices.32, 39 The inverter's noise margin is the most critical parameter, since it directly determines the maximum complexity of circuits.22 Particularly, interesting applications of organic electronic circuits are found in analog electronics that allow for the read-out and processing of signals from printed large-area sensors and form an interface to silicon electronics. Examples are analog-to-digital (A/D) converters, operational amplifiers, and comparators, all including several tens of transistors, thus requiring both high gain and a large noise margin to be functional as well as sufficient processability. It is interesting to note that the majority of organic complementary inverters already mentioned24-34, 36-40 relied on pentacene as the p-type semiconductor (14 incidences), fluorinated copper phthalocyanine (6 incidences), or N,N′-ditridecylperylene-3,4,9,10-tetracarboxylic diimide (5 incidences) as the n-type material. On the contrary, the variation in gate dielectric materials that are used is much higher with an emphasis on hybrid dielectric systems. Hybrid systems allow accounting for both a high dielectric breakdown voltage and an engineered interface to the semiconductor. Moreover, the implementation of biodegradable and biocompatible materials represents a new niche in the organic electronics research, aimed to address the issues of cost and toxicity to humans and environment posed by nowadays electronics, a topic that was recently reviewed elsewhere.41-43 Accordingly, we have demonstrated the usage of a novel hybrid and biodegradable high-k gate dielectric material system based on a cellulose derivative for low-voltage complementary organic circuits with exceptional high noise margins.35 Previous work done in our laboratories demonstrated the fabrication feasibility of complex circuits, where the electrode patterning was performed by a self-aligned photolithography technique.44, 45 This process can easily be transferred to an anodized aluminum (Al2O3) + trimethylsilyl cellulose (TMSC) based bilayer system; the respective results will be published soon. To follow on this preliminary work we have developed an extraordinarily well-performing complementary inverter technology based on a hybrid dielectric composed of a bilayer of alumina (Al2O3) and trimethylsilyl cellulose (TMSC) and pentacene or C60 for the p-channel and the n-channel organic semiconductor, respectively. It outperforms any inverter reported so far with respect to the combination of excellent key parameters, such as record DC gain of above 500 V/V, low operation voltage of only 4 V, and large noise margin up to 92.5%. In order to clarify the origin for this high performance, special attention is given to the investigation of the semiconductor–dielectric interface, the semiconductor morphology, the nature of traps, the influence of mobility levels on the inverter performance and its long-term stability. This article is not meant to report new materials and systems, but rather find explanations and present a thorough analysis of the extraordinary performance of the cellulose derivative (TMSC) dielectric and the TMSC to semiconductor interface in organic field-effect transistors and simple inverter circuits. All OTFTs presented in this work have a bottom gate, top contact device architecture, as illustrated in Figure 1a. The transistor fabrication process is described in detail in the Experimental Section. The semiconducting layer is pentacene for p-type and C60 (fullerene) for n-type conduction. For the gate dielectric, an inorganic (Al2O3)–organic (TMSC) bilayer is chosen with 28 and 30 nm layer thickness, respectively. The dielectric properties of both single-layer TMSC films and bilayer Al2O3 + TMSC films, were investigated by current–voltage (I(V)), capacitance–frequency (C(f)), and capacitance–voltage (C(V)) measurements in appropriate capacitor structures with 72 nm insulator layer thickness of pure TMSC and 28 + 30 nm of bilayer film of Al2O3 + TMSC, respectively. In Figure 1b, the I(V) curves of a representative capacitor formed by a single layer cellulose dielectric is shown, whereas in Figure S1a (in the Supporting Information) the curve with bilayer dielectric is displayed. A comparison of I(V) curves of a single layer and bilayer dielectric is displayed in Figure 1c. At an electric field of 3.0 MV cm−1 (equivalent to ≈22 V) a current density on the order of 10−6 A cm−2 is observed for the single-layer TMSC. A breakdown field of 4.5 ± 0.3 MV cm−1 is extracted from eight appropriate capacitor structures. One representative C(V) measurement is displayed in Figure 1d. Its capacitance of about 29 nF cm−2 corresponds to a dielectric constant of εR = 2.4 ± 0.2 at 1 kHz with an excellent stability at frequencies down to 0.5 mHz (virtually flat dielectric constant and low dielectric losses which are indicative of a high purity and negligible amount of mobile ionic species) as illustrated in Figure 1e.46 In comparison, capacitors based on the bilayer dielectric have three orders of magnitude lower leakage currents (≈10−9 A cm−2) at an electric field of 3.0 MV cm−1 corresponding to ≈17.5 V and an effective capacitance of 53 nF cm−2 at 1 kHz (see Figure S1a,b, Supporting Information). As can be derived from Figure S1c (in the Supporting Information) the permittivity of the bilayer dielectric also shows excellent stability over the tested frequency range (1 mHz to 10 kHz). The measured capacitance value of the dielectric is in good agreement with calculations by assuming a permittivity of 9 and a thickness of 28 nm for the Al2O3 layer as well as a measured permittivity of 2.4 ± 0.2 (Figure 1e) and 30 nm thickness for the TMSC layer (see the Experimental Section). In any OTFT with bottom gate architecture the surface properties of the gate dielectric (surface energy, surface roughness) decisively affect the arrangement and growth of small molecule semiconductors. The surface energy of spin-coated TMSC thin films was determined by contact angle measurements. With a water contact angle of 98.5°, TMSC can be regarded as a hydrophobic, low energy surface material with a total surface energy of γ = 24.2 ± 0.6 mN m−1, separable in a small polar component γP = 1.8 ± 0.5 mN m−1 and a dispersive component γD = 22.4 ± 0.1 mN m−1. The average surface roughness, indicated by the root mean square (rms)–roughness values, was found to be only 0.77 ± 0.1 nm by atomic force microscopy (AFM) measurements. On this smooth and low energy TMSC surface, a small-grain growth mode with average grain sizes between 150 and 300 nm for pentacene (shown in Figure 1a) and 50 nm for C60 was observed by AFM measurements. In Figure 2, typical electrical characteristics of OTFTs with either C60 or pentacene as the semiconducting layer are plotted. Both p- and n-type transistors are based on the inorganic–organic bilayer gate dielectric composed of Al2O3 and TMSC. The output characteristics ID(VDS) are displayed in Figure 2a,b, whereas the transfer characteristics ID(VGS) are shown in Figure 2c,d. Both transistor types display very small hysteresis between forward and reverse voltage sweeps. The output characteristics show clear saturation, but for the pentacene-based OTFT a non-linear behavior of the drain current at very low drain voltages is observable (Figure 2b). Such an S-shape of the output curve has been already observed and reported for many different device configurations and has sometimes been attributed to a lateral field dependent contact resistance.47-55 In Table 1, the critical device parameters Von (onset voltage), Vthr (threshold voltage), S (subthreshold swing), μlin (charge carrier mobility in the linear regime), and μsat (charge carrier mobility in the saturation regime) are compiled and averaged over eight devices for each transistor type. On average, C60-based OTFTs show a charge carrier mobility of 0.7 cm2 V−1 s−1 in the saturation regime, a threshold voltage of 1.3 V, and a small subthreshold swing of 305 mV dec−1. Pentacene-based OTFTs have on average a mean threshold voltage of −4.7 V, a very small subthreshold swing of 225 mV dec−1, and a field-effect mobility of 0.22 cm2 V−1 s−1 in the saturation regime. The gate leakage currents are very low and in the range of 10−10 A. The balanced performance of our p- and n-type OTFTs, as well as the fact that both transistor types strictly behave as normally off transistors at zero applied gate voltage is a good base for integrating them in complementary organic inverters. A schematic image of such a complementary inverter circuit is displayed in Figure 3a together with the voltage transfer characteristics (VTCs) of a typical device and the static gain measured for operation voltages of VDD = 4, 5, 6, and 7 V. The inverter exhibits extraordinarily high small-signal gains; for all operation voltages, gains above 500 V/V are measured with a maximum value of about 1000 V/V for VDD = 7 V. The best performing device even has a maximum gain value of 1600 V/V. Moreover, a very sharp transition regime (ΔVin ≤ 40 mV) and a full rail-to-rail swing are observed. The extracted inverter parameters are compiled in Table 2. The switching threshold voltages VM are found to be very close to the ideal value of VDD/2 at all operation voltages with a nearly perfect fit (e.g., VM = 2.04 V at VDD = 4 V). In Figure 3b, the mismatches of the threshold voltages to the ideal values (ΔVM) are plotted as a function of VDD revealing a linear increase of ΔVM with the supply voltage. This means that the asymmetry of the VTCs increase with increasing the operation voltages. Additionally, the noise margins (NM) are plotted in Figure 3b as a function of VDD, illustrating the linear decrease of the NM with increasing operation voltage. Such a behavior reveals the direct correlation between ΔVM and NM and is an indication of the deviation of the VTCs from perfect symmetry. The noise margin is an important figure of merit of an inverter stage and measures the immunity against inevitable transistor parameter variations and electrical noise.56 There are several ways to determine the noise margin of an inverter. One convenient way is called the “maximum equal criterion” (MEC), where the NM is found by the maximum square that fits between inverter transition curve and the mirrored inverter curve as shown in Figure 3c.22, 35 The NM values for all the supplied voltages are listed in Table 2. The noise margin is mainly limited by the steepness of the transition ΔVin and the position of the switching threshold voltage VM (VM = Vin = Vout) as shown in Figure 3c. High and balanced noise margins are found when the ideal condition VM = VDD/2 is met, thus when VM = Vin =VDD/2 = Vout. The inverter in Figure 3c has a NM of 1.79, which is 90% of the maximum theoretical value for a supply voltage of 4 V, determined by the “maximum equal criterion.” Additionally, the “negative slope criteria” reveals a balanced NM of 1.85 V (92.5%) for a supply voltage of 4 V. The OTFTs with pentacene and C60 semiconductor layers (as used in the complementary inverters) were also analyzed with regard to their long-term stability. The dependence of their onset voltage and charge carrier mobility on the time period after preparation is plotted in Figure 4 based on measurements of at least five devices for each transistor type. The error bars display the standard deviations. p- and n-type devices exhibit an onset voltage shift of +1.3 and +0.95 V, respectively, over a period of 45 days. The main part of the shift occurred either after the first or after the second measurement and then the onset voltage shift tended to saturate. It seems that both pentacene- and fullerene-based devices stabilized their electrical properties after few days. Between day 8 and day 45 no significant change in the transfer characteristics was observed. Concerning the subthreshold swing, no significant change was observed over 45 days (S = 215 mV dec−1 (0 days), 210 mV dec−1 (8 days), and 225 mV dec−1 (45 days)) in the pentacene OTFTs, indicating that the interface trap density is stable. On the contrary, after 8 days an increase of the swing was observed for the C60 devices from 305 mV dec−1 (0 days), to 410 mV dec−1 (8 days), to 430 mV dec−1 (45 days). The mean value of the charge carrier mobility of the pentacene OTFTs showed no significant variation over 45 days: 0.22 cm2 V−1 s−1(fresh sample), 0.19 cm2 V−1 s−1 (after 8 days), 0.21 cm2 V−1 s−1 (after 45 days). In contrast, a strong reduction of about one order of magnitude (from 0.7 to 0.06 cm2 V−1 s−1 within the first 8 days and to 0.05 cm2 V−1 s−1 after 45 days) was observed for the fullerene transistors. In order to test the reliability of our OTFT devices we have also performed negative and positive bias stress tests. The bias stress was done 1 day after fabrication, on devices which had been previously measured only once. A reversible negative onset voltage shift of about 400 mV was observed under negative bias of −7.5 V over 21 hours stress (see Figure 5a,b) The main part of the negative voltage shift occurred during the first 2 hours (300 mV) whereas shift saturation was reached after 6 hours. The positive bias stress resulted in a significantly smaller positive onset voltage shift (ca. +100 mV over 4 hours stressing the device). Devices that were stored for seven months in the glovebox showed no bias stress effect at all (i.e., shift of the onset voltage) when their transistor characteristics were measured at regular intervals during the storage period. In order to investigate the “long-time” behavior of complementary inverters, electrical measurements were done after 1, 4, 8, and 45 days of the respective device preparation. Inverters were measured 1 day after device stabilization (see Figure 4a,b). The “long-time” behavior of complementary inverters is shown in Figure 4c,d where the VTC and gain curves are plotted as a function of time. For the lowest VDD of only 4 V, a small shift of the switching threshold voltage was measured: starting from 2.04 V after 1 day to an identical value of 2.17 V after 8 and 45 days, respectively, with a related exceptional high noise margin of 1.79 V (90% of the theoretical maximum) after 1 day and 1.74 V (87%) after 8 and 45 days. It is interesting to note that, after 8 days of storage time, the hysteresis in inverter characteristics was virtually negligible (<100 mV, see Figure 4d) and moreover, repeated measurements did not change the inverter transition, although the gain was somewhat reduced (from 503 (0 days) to 320 (8 days) and 195 (45 days)). The operational stability of the VTC was shown over a period of at least 45 days (Figure 4c for VDD = 4 V). Furthermore, the remarkable long-term stability of these TMSC-based complementary inverters was demonstrated by 16 consecutively recorded inverter curves that are virtually superimposed over one another (Figure 5c). The current–voltage characteristics show that the Al2O3 + TMSC bilayer capacitors have substantially lower leakage currents than the single TMSC layer devices. Due to the roughness of the aluminum bottom electrode with spikes up to 10 nm, the anodization process is a convenient method to reduce the leakage currents for at least three orders of magnitude at an electric field of 3 MV cm−1 as displayed in Figure 1d and make the dielectric layer more robust.57 Another advantage of the anodization step is the substitution of the hydroxide of the native oxide layer. Finally, the subsequent short oxygen plasma treatment (see the Experimental Section) is sufficiently removing all residuals left after the anodization process. This procedure allows for the generation of a pure and trap-reduced dielectric interface to the organic semiconductors, by measurements at low revealing a virtually flat permittivity in the mHz to kHz frequency range and low dielectric losses which both are indicative of a high purity and negligible amount of mobile ionic The generation of this excellent interface is in virtually hysteresis-free characteristics of all the One important that the performance of OTFTs, and in the charge carrier is the of the As shown by several the of the surface energy of the to that of the is one important the growth For a low surface energy material with a smooth surface TMSC, a growth mode is and with a rather high density and small grain sizes are formed (see Figure The high density of grain a significant decrease of the charge carrier since grain as charge On the a better between pentacene on low surface energy materials TMSC with and better reduce the of trap thus the mobility of charge in the In there is an between grain related and interface with regard to their influence on charge carrier The low subthreshold swing observed in all our pentacene-based OTFTs is indicative of a low interface trap density which the influence of the large grain trap density on the charge carrier Accordingly, a mobility 0.2 cm2 V−1 s−1 is observed in the p-type devices. In C60 films, the influence of on the charge carrier mobility is by far not as significant as in pentacene films, which is attributed to the of the fullerene In the pentacene OTFTs (see Figure a non-linear current increase in the linear regime of the ID(VDS) output characteristics is at higher gate have been in to such a which can be observed in bottom gate The explanations i) the of the charge carrier mobility for semiconductor ii) currents that the of the mobile by an effective under the drain and iii) large at the electrode from an energy between the work of contact material and semiconductor films, a gate or large contact are found in our of these it has been shown that a mobility in combination with a small contact in a non-linear drain voltage dependence of the current due to The from a of from trap and a dependence of on the drain A respective of the pentacene output curve in Figure the dependence in the regime 2 V, thus indicating that a mobility has to be The of any hysteresis in the I(V) curves and the low and value of the subthreshold swing a low density of interface in the pentacene are not for the observed and the of the as by the of the pentacene layer gives rise to which to a field dependence of the charge carrier This is all the more given that the pentacene grain sizes are 300 nm at a large density of grain As by Figure 4 the characteristics of both pentacene- and C60-based OTFTs show a positive onset voltage shifts storage which after a of measurements. The virtually subthreshold swing in pentacene as well as the negligible hysteresis as the origin of the On the contrary, it seems that trap are for the positive onset voltage shift in are either over time or during the first measurements by the applied positive gate be easily by the gate bias and therefore are not to the swing, but the small onset voltage in pentacene-based It has been reported by many that the of the of trap in pentacene trap also be due to such as at the a at the or a at the fabrication and transfer from the to the measurement stage the semiconductor layer and rise to such For oxygen can even the devices are to but transferred directly and measured in a glovebox with reduced oxygen and water have also observed that the of oxygen with pentacene is in the that these are under device operation with the of oxygen in the grain observed that the storage of devices in and their subsequent measurement in did not a change in their I(V) also observed that the storage time to the first measurement has influence on the device (i.e., on the onset voltage in this of and the first measurement the of to the of oxygen or with the which in a second are by Moreover, also are are not as in the as the (see and This an for the positive shift of the onset voltage between first and second measurement (Figure and also for the saturation of the onset voltage shift in In order to clarify which of are present in our we performed measurements on pentacene films (in and after storage in for (see Figure Supporting Information). storage under a small increase of the at energy is observed that can be attributed to the to and The analysis reveals an increase of the from 0.2 to At the position no change is that trap in our devices for bias stress and the positive onset voltage can mainly be attributed to It be that the of any mobility in pentacene OTFTs against an of pentacene both are to oxygen For the C60 transistors, one a strong decrease of the charge carrier mobility during 8 days of storage which is by all over the device grain This is a effect of The decrease in charge carrier mobility and the at the interface that the subthreshold swing is in a positive onset voltage shift of the C60 transistors. With respect to the complementary inverters, noise margin values beyond from the maximum theoretical value for all supply voltages are and the high operational of the OTFT devices. At a very low supply voltage of 4 V, our bilayer organic complementary inverters have a static gain of more than 500 V/V with a noise margin of 92.5%, which is already reported devices with architecture (see the of inverter performance given in 38 and also gain values above 1000 V/V values up to 1600 were measured for our devices. This is all the most as the charge carrier mobility values of the transistors are not thus the that the of the mobility values between p- and n-channel with the virtually hysteresis are the factors for high gain and high noise margin Accordingly, a mobility 1 be the the is not high ≤ it can be by and p-channel transistors with different In our the mobility is The static of a complementary inverter is determined by technology parameters, the parameters of p- and n-type transistors. A good of these parameters a good saturation of both output can to a significant increase of the gain A is shown in the Supporting Furthermore, high gain values are also determined by the interface An insulator with an low trap density (as this is the for is in having I(V) curves with virtually zero Accordingly, it is to measurements with a very high voltage small voltage thus one to the high gain value of the complementary inverter it by hysteresis The noise margin with increasing VDD due to their strong this is also for the of the VTCs by see Figure A for this behavior can be found in the bias stress that was observed for both types of transistors. The negative shift of Von under negative gate and the positive

In this paper, standard ternary logic gates are initially designed to considerably reduce static power consumption. This study proposes novel ternary gates based on two supply voltages in which the direct current is eliminated and the leakage current is reduced considerably. In addition, ST-OR and ST-AND are generated directly instead of ST-NAND and ST-NOR. The proposed gates have a high noise margin near V_(DD)/4. The simulation results indicated that the power consumption and PDP underwent a~sharp decrease and noise margin showed a considerable increase in comparison to both one supply and two supply based designs in previous works. PDP is improved in the proposed OR, as compared to one supply and two supply based previous works about 83% and 63%, respectively. Also, a memory cell is designed using the proposed STI logic gate, which has a considerably lower static power to store logic ‘1’ and the static noise margin, as compared to other designs.

In complementary metal–oxide–semiconductor (CMOS) high-speed buffer design, leakage power dissipation, complex routing area, and low-power consumption are the most common challenges. To overcome these challenges, the BiCMOS technology and CMOS multi-valued logic (MVL) are used to maintain the yield and the performance of the high-speed buffers. In this paper, performance comparison of different types of buffers: Schmitt trigger, tristate and bidirectional buffer with BiCMOS and CMOS MVL logic are presented. Cadence virtuoso editor and ADE spectre simulator at gpdk 180 nm technology node are used for simulation setup. The results show that CMOS MVL logic delay, power dissipation, low and high noise margin are better than BiCMOS by 20, 43, 19, and 39%, respectively. Based on these results, CMOS MVL logic outperforms BiCMOS for low-power applications at comparable speed.

Power consumption measurement and temperature recording during granulation

Flexible inkjet-printed dual-gate organic thin film transistors and PMOS inverters: Noise margin control by top gate

A number of novel voltage-mode multiple-valued logic circuits are introduced. Adopting the main features of the true single-phase clocked logic, efficient quaternary logic dynamic and pseudo-static latches, dynamic and static master-slave storage units, and uni-signal controlled pass gates are proposed. These circuits use two kinds of MOS transistors, i.e., enhancement and depletion mode, each of which has two threshold voltages. The proposed circuits exhibit regular, modular, and iterative structure, which means that the MVL circuits are VLSI implementable and can be easily re-designed for any radix of an arithmetic system. Since we use only clock signal, the derived circuits have low power dissipation. Comparisons with existing circuits prove substantial improvements in terms of speed, power consumption, and transistor count.

In this paper, Photonic crystal based all optical XOR and OR gate is proposed. 2D hexagonal lattice of Photonic crystal is being used. The defects are introduced for the designing of efficient gates. The photonic band gap is optimized with the proper selection of r/a ratio i.e. ratio of radius of cell and lattice constant. The structure is investigated through Plane wave expansion (PWE) method and Finite Difference time domain (FDTD). The band-gap of perfect crystal lies in C band. The performance of gates is analyzed through contrast ratio and Noise margin. The Contrast ratio for XOR gate is as high as 15.37 dB and Noise Margin is 0.68 and 0.655 for OR and XOR gate respectively.

Ambipolar π-conjugated polymers may provide inexpensive large-area manufacturing of complementary integrated circuits (CICs) without requiring micro-patterning of the individual p- and n-channel semiconductors. However, current-generation ambipolar semiconductor-based CICs suffer from higher static power consumption, low operation frequencies, and degraded noise margins compared to complementary logics based on unipolar p- and n-channel organic field-effect transistors (OFETs). Here, we demonstrate a simple methodology to control charge injection and transport in ambipolar OFETs via engineering of the electrical contacts. Solution-processed caesium (Cs) salts, as electron-injection and hole-blocking layers at the interface between semiconductors and charge injection electrodes, significantly decrease the gold (Au) work function (∼4.1 eV) compared to that of a pristine Au electrode (∼4.7 eV). By controlling the electrode surface chemistry, excellent p-channel (hole mobility ∼0.1-0.6 cm(2)/(Vs)) and n-channel (electron mobility ∼0.1-0.3 cm(2)/(Vs)) OFET characteristics with the same semiconductor are demonstrated. Most importantly, in these OFETs the counterpart charge carrier currents are highly suppressed for depletion mode operation (I(off) < 70 nA when I(on) > 0.1-0.2 mA). Thus, high-performance, truly complementary inverters (high gain >50 and high noise margin >75% of ideal value) and ring oscillators (oscillation frequency ∼12 kHz) based on a solution-processed ambipolar polymer are demonstrated.

We report on flexible organic complementary inverters using pentacene and C60 as active semiconductors fabricated on a plastic substrate. Individual transistors as well as inverters show good operational stability with negligible hysteresis. The threshold voltages are comparable for p-channel pentacene and n-channel C60 organic field-effect transistors, and noise margins larger than 80% of the maximum theoretical values were obtained at a supply voltage VDD as low as 3 V. A high dc gain of 180 was achieved at VDD=5 V. The inverters demonstrated good mechanical stability when tested after bending under both tensile and compressive stress.

Static Random Access Memory (SRAM) technology is the latest technology must advance to satisfy the high-speed performance and low power consumption requirements of contemporary devices. The design, testing, and validation of SRAM cells with configurations ranging from six transistors (6T) to ten transistors (10T) are thoroughly examined in this research work. The study's main goal is to pinpoint the crucial elements that affect SRAM cell performance, such as data retention voltages, power consumption, delay factors, stability measures, and noise margins. Existing SRAM designs and their drawbacks are assessed through a thorough literature review, emphasizing the need for innovative SRAM design techniques. The process includes a thorough examination of important variables and the design and testing of several SRAM cell designs using sophisticated simulation tools. To guarantee robustness and reliability, every design from 6T to 10T is painstakingly created, simulated, and verified against a series of predetermined scenarios. The findings show how several SRAM layouts compare in terms of power efficiency, delay, stability, noise margin, and area efficiency. The study's conclusions offer helpful recommendations for improving SRAM designs in the future by weighing the trade-offs between stability, speed, and power consumption. By providing tested design methodologies that improve the performance and efficiency of SRAM cells, this research makes a substantial contribution to the field of semiconductor technology and meets the expanding demands of contemporary electronic gadgets.

Compared to binary logic, the multi-valued logic circuits provide very small chip size, higher speed, and considerably small number of interconnections and simpler realization of logic functions. However, the main drawback of these circuits is the lower noise margin. The noise margin decreases as the radix of multi-valued system increases. Due to the low noise margins, it is necessary to restore or recover the nominal levels of the signal after a certain number of cascaded stages. In this paper a new current mode CMOS restoration circuit is presented and evaluated.

In the last decade, we have seen how Moore's law has lost its validity because it has reached the physical limit of miniaturization of components and the problem of thermal dissipation increasing with the chip’s clock frequency. For this reason, multi-core architectures were born, and quantum computing is being looked at as a possible solution for more computing power. The aim of this article is to demonstrate the possibility to realize computer architectures using multi-value logic. The objective is reached when we are able to translate any MVL function into the corresponding MVL circuit. The method proposed is completely independent of the basis adopted in the MVL domain and the physical quantity used to represent or transfer the domain values. Thus, this approach provides a new theoretical and practical context for applying new technologies or polymorphic materials, which can represent multiple values. In order to give concreteness to the analyzed theoretical aspects, we will represent a case study based on a classical combinational circuit, the summing circuit using LTspice® XVII (© Analog Device Corporation) as simulation environment has been carried out. The results show that it is possible to build MVL combinatorial circuits, although there are limitations because the proposed solution is just a proof of concept. The method can also be successfully applied to sequential MVL circuits, which are not the subject of the present article.

Welcome to the 11th ACM/IEEE International Symposium on Low Power Electronics and Design!.The 2006 edition of the ACM/IEEE International Symposium on Low Power Electronics and Design (ISLPED) welcomes you to the beautiful, on-the-lake setting of the Tegernsee area in Germany, within a one hour drive from Munich. On a par with this great location, a strong and diverse technical program features two keynote talks from leaders in the field, a technical panel, four embedded tutorials, and, new for this year, three half-day tutorials scheduled for the last day of the symposium.Dr. Christoph Kutter, Senior VP Products and Systems, Infineon Technologies, will give a keynote on design challenges for mobile communication devices. The Thursday keynote is given by Barry Dennington, Senior Vice President, NXP Semiconductors/CTO/SoC Design Technology, who will present an industrial view on the demands of a convergent communications, consumer and automotive market, the technology challenges a semiconductor company faces and the solutions that lead to actual products with a few examples. The Friday panel is titled "Flexibility and Low Power; a Contradiction in Terms?". Moderated by Peter Wintermayr, Editor in Chief of Markt and Technik, panelists Reiner Hartenstein, Univ. Kaiserslautern; Heinrich Meyr, RWTH Aachen Univ. and Chief Scientific Officer CoWare; and Steve Leibson, Tensilica, will discuss whether configurable or re-configurable computing offer solutions for low power design.The four embedded tutorials during the first two days of the conference are organized around two major themes: (1) low power circuit design and technologies; and (2) low power systems and energy management. Two embedded tutorials on sub-threshold design and variability/low power design from experts from MIT, University of Michigan, and IBM Research are paired with two others on energy harvesting for battery limited systems and low power portable applications from researchers from NEC Labs and University of California. New for this year, ISLPED will offer three half-day tutorials on hot topics such as leakage aware design, micropower analog design, and addressing fault-tolerance/variability and power issues from system to circuit levels. The tutorials feature presenters from OFFIS, Intel, University of North Carolina, Carnegie Mellon University, and IBM Research.Out of 214 submissions received in early March, only 75 strong technical papers were accepted for presentation in paper or poster sessions, yielding an acceptance rate of 26% for regular and short papers (56 papers), or 35% including 19 posters. Topics range from low power analog and RF design, power aware circuit design and tools, and architecture techniques for low power, to system and application level power management. The program is organized in twelve technical sessions featuring long (30 min) and short (20 min) paper presentations, as well as two interactive poster sessions that will provide an additional venue for authors and symposium attendees to interact in an informal setting. Following the tradition of ISLPED, this year's event also includes exhibits featuring tools and methodologies from leading vendors of low power or power-aware design tools. New for this year, the program includes an industry session that will highlight contributions showcased by companies participating in the ISLPED exhibits. Winning entries to the annual Low Power Design Contest will also be featured in a separate technical session.

As the development of binary systems forecasted to reach to its end, ternary system is gaining more attention. However, most ternary logic circuits were not considered to be a ‘true’ competitor to binary systems. To counter this common belief on ternary logic, in this study, we propose a ternary logic system based on depletion-mode MOSFETs and conventional MOSFETs that can truly compete with binary systems in terms of power and delay. Based on our novel circuitry of 11 logic gates, we illustrate that (1) our circuits consume near-zero static current on all logic states (−1, 0, +1), (2) our standard ternary inverter (STI) shows improved PDP of 71× and 245× compared to conventional CNTFET or memristor and MOSFET based ternary circuits, and (3) our balanced ternary full adder (BTFA) shows 48× improved power consumption compared to other ternary-device based adders and 5.3× improved power compared to the same devices. With our results, we highlight that ternary logic is now competitive to binary.

In this seminal, a low-power conditional discharging-flip flop (Modified CD-FF) has been presented. A clock-pulse by single feedback through scheme is proposed for use in the Modified CD-FF. Two inverters in clock-pulse generator circuit have been removed to optimize delay in clock path. In this low-power circuit design, the clock pulse is designed by a single inverter and pass-transistor logic (PTL). The proposed circuit (MCD-FF) reduces the additional switching activity of certain internal nodes as well as generates less glitch in the output with a lesser transistor count. As a consequence, the width of transistor is increased to manage the delay for clock pulse. Overall performances of circuit design provides better optimized area, delay and power consumption (average power) than earlier flip flop designs compared to 90nm technology.