CMOS Architectures for NOR & NAND Logic Gates … Architectures for NOR & NAND Logic Gates Using...

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CMOS Architectures for NOR & NAND Logic Gates Using Single Electron Transistors A. Venkataratnam and A.K. Goel Department of Electrical & Computer Engineering Michigan Technological University Houghton, MI 49931, USA Email: [email protected] ABSTRACT Single electron transistor (SET) is one of the nano devices suitable for developing nano-scale logic circuits. In this paper, CMOS architectures for NOR and NAND gates have been proposed using SET’s and their operational characteristics have been verified by using the simulation model SET-SPICE. First, a two-input NOR gate was designed and verified and then the design was extended to implement a NOR3 gate and a NAND2 gate. The basic layout of a SET is a small conducting island coupled to the source and drain leads by tunnel junctions that are capacitively coupled to a control gate and one or more input gates. Operation of an SET as an “n” and a “p” device was achieved by controlling the charge on the SET island. This charge is related to the capacitance at the island, capacitance at the gate electrode and the voltage applied to the gate. The effects of temperature, island capacitance and the ability of the proposed gate to drive load capacitance have also been studied. Keywords: single electron transistors (SET), CMOS, logic devices 1 INTRODUCTION Nano-scale devices show potential for low power, high speed at a size much lower than current day CMOS [1, 2]. The popular nano-devices that are explored for logic circuit applications are carbon nanotube transistors, nanowire FETs, quantum dots and single electron transistors (SET). Quantum dots and single electron transistors can be combined into a single category called Single Electron Devices, which work on the principle of controlling the movement of a single electron. Single electron transistors use quantum effects to perform operations similar to conventional CMOS transistors. In order to use these devices to perform logic operations it is required to realize operation identical to the MOSFET. Earlier logic designs [3-6] based on SET’s have used architectures different from CMOS to realize simple logic gates, except to an inverter [7]. This will require developing architectures different from CMOS for each logic gate/operation. In this paper CMOS architecture based NOR and NAND gate has been proposed and operation verified using the simulation model SET-SPICE [8]. This model, developed by researchers at Delft University in Netherlands, makes use of the most popular circuit simulator called SPICE and incorporates a text- based model for single electron transistors. The basic layout of an SET (Fig. 1) is a small conducting island coupled to the source and drain leads by tunnel junctions that are capacitively coupled to one or more gates. Single electron movement deals with a small amount of excess electrons on islands changing their distribution over time. The charges in single-electron devices are transported in a quantized way rather than continuously. Complementary operation of these devices can be achieved by controlling the charge on the island. The charge on the island is related to the capacitance at the island, capacitance at the gate electrode and the voltage applied to the gate. In-order to obtain biasing voltage at the gate for complementary operation of the SET, current oscillations where observed for V cc = 15 mV and V ee = 0 V with C j1 = C j2 =C g1 =C g2 =C 0 = 10 -18 F and R t = 10 9 . Voltage at the gate was varied from 0 to 1V and the corresponding current oscillations where observed. Based on this simulation it was found that gate bias has to be around 0.1V for the SET to operate as NMOS and it has to be around 0.3V for PMOS operation. Fig. 1: A Schematic Diagram of a SET 2 DESIGN OF A NOR2 GATE The NOR2 gate consists of four single electron transistors and was based on the complementary logic as shown in Fig. 2. Device parameters including V cc and V ee were set to values as mentioned in the previous section. All possible logic combinations for a two-input NOR gate were tested at the input. Logic ‘1’ is represented by a 25 mV signal and the logic ‘0’ is represented by ground at the input. The waveforms corresponding to the input and output as in SET-SPICE are shown in Fig. 3, which verify the NOR2 operation. At the output, logic ‘1’ charges up to V cc , while logic ‘0’ is pulled down to ground. Based on these results, this design was extended to a 3-input NOR gate. These simulations where done at a temperature of 4.2 o K. Tunnel Junctions Source Drain Gate Tuning Gate Contacts Island Cg1 Cg2 Cj1,Rt Cj2,Rt V g1 Vg2 Q0 C0 NSTI-Nanotech 2005, www.nsti.org, ISBN 0-9767985-2-2 Vol. 3, 2005 176

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Page 1: CMOS Architectures for NOR & NAND Logic Gates … Architectures for NOR & NAND Logic Gates Using Single Electron Transistors A. Venkataratnam and A.K. Goel Department of Electrical

CMOS Architectures for NOR & NAND Logic Gates UsingSingle Electron Transistors

A. Venkataratnam and A.K. GoelDepartment of Electrical & Computer Engineering

Michigan Technological UniversityHoughton, MI 49931, USAEmail: [email protected]

ABSTRACT

Single electron transistor (SET) is one of the nano devicessuitable for developing nano-scale logic circuits. In thispaper, CMOS architectures for NOR and NAND gates havebeen proposed using SET’s and their operationalcharacteristics have been verified by using the simulationmodel SET-SPICE. First, a two-input NOR gate wasdesigned and verified and then the design was extended toimplement a NOR3 gate and a NAND2 gate. The basiclayout of a SET is a small conducting island coupled to thesource and drain leads by tunnel junctions that arecapacitively coupled to a control gate and one or more inputgates. Operation of an SET as an “n” and a “p” device wasachieved by controlling the charge on the SET island. Thischarge is related to the capacitance at the island,capacitance at the gate electrode and the voltage applied tothe gate. The effects of temperature, island capacitance andthe ability of the proposed gate to drive load capacitancehave also been studied.

Keywords: single electron transistors (SET), CMOS, logicdevices

1 INTRODUCTION

Nano-scale devices show potential for low power, highspeed at a size much lower than current day CMOS [1, 2].The popular nano-devices that are explored for logic circuitapplications are carbon nanotube transistors, nanowireFETs, quantum dots and single electron transistors (SET).Quantum dots and single electron transistors can becombined into a single category called Single ElectronDevices, which work on the principle of controlling themovement of a single electron.

Single electron transistors use quantum effects to performoperations similar to conventional CMOS transistors. Inorder to use these devices to perform logic operations it isrequired to realize operation identical to the MOSFET.Earlier logic designs [3-6] based on SET’s have usedarchitectures different from CMOS to realize simple logicgates, except to an inverter [7]. This will requiredeveloping architectures different from CMOS for eachlogic gate/operation. In this paper CMOS architecturebased NOR and NAND gate has been proposed andoperation verified using the simulation model SET-SPICE[8]. This model, developed by researchers at DelftUniversity in Netherlands, makes use of the most popularcircuit simulator called SPICE and incorporates a text-based model for single electron transistors.

The basic layout of an SET (Fig. 1) is a small conductingisland coupled to the source and drain leads by tunneljunctions that are capacitively coupled to one or more gates.Single electron movement deals with a small amount ofexcess electrons on islands changing their distribution overtime. The charges in single-electron devices are transportedin a quantized way rather than continuously.Complementary operation of these devices can be achievedby controlling the charge on the island. The charge on theisland is related to the capacitance at the island, capacitanceat the gate electrode and the voltage applied to the gate.

In-order to obtain biasing voltage at the gate forcomplementary operation of the SET, current oscillationswhere observed for Vcc = 15 mV and Vee = 0 V with Cj1 =Cj2 = Cg1 = Cg2 = C0 = 10-18 F and Rt = 109 Ω. Voltage at thegate was varied from 0 to 1V and the corresponding currentoscillations where observed. Based on this simulation itwas found that gate bias has to be around 0.1V for the SETto operate as NMOS and it has to be around 0.3V forPMOS operation.

Fig. 1: A Schematic Diagram of a SET

2 DESIGN OF A NOR2 GATE

The NOR2 gate consists of four single electron transistorsand was based on the complementary logic as shown in Fig.2. Device parameters including Vcc and Vee were set tovalues as mentioned in the previous section. All possiblelogic combinations for a two-input NOR gate were tested atthe input. Logic ‘1’ is represented by a 25 mV signal andthe logic ‘0’ is represented by ground at the input. Thewaveforms corresponding to the input and output as inSET-SPICE are shown in Fig. 3, which verify the NOR2operation. At the output, logic ‘1’ charges up to Vcc, whilelogic ‘0’ is pulled down to ground. Based on these results,this design was extended to a 3-input NOR gate. Thesesimulations where done at a temperature of 4.2oK.

Tunnel Junctions

Source Drain

Gate Tuning Gate

Contacts

Island

Cg1

Cg2

Cj1, Rt Cj2, Rt

Vg1

Vg2

Q0

C0

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3 DESIGN OF A NOR3 GATE

This design consists of three P-SET’s in series and three N-SET’s in parallel with a total of six transistors in similar tothe CMOS based NOR3 gate. The parameters and thevoltage levels at the input were similar to the previoussimulation. The I/O waveforms for this circuit are shown inFig. 4, which verifies a NOR3 logic operation.

Fig. 2: NOR2 gate architecture

4 DESIGN OF A NAND2 GATE

CMOS architecture equivalent NAND2 gate was designedwith SET’s using four transistors. The NAND2 gate wasalso simulated with identical bias conditions as of theNOR2 gate. The device parameters for junction capacitanceand resistance were also identical to the NOR2. The I/Owaveforms of the NAND2 gate are shown in Fig. 5.

5 SIMULATION RESULTS

5.1 Dependence on Island Capacitance

The island capacitance was varied from 10-20 F to 10-18 Fand the output was observed. A C0 = 10-19 F providedoptimal results for both the NOR and NAND gates. Thisvalue translates to an island size of about 2 nm. The I/Owaveforms of the NOR2 gate at C0 = 10-19 F are shown inFig. 6.

5.2 Dependence on Load Capacitance

Similarly the load capacitance at the output was also variedbetween 10-18 F and 10-12 F. The results showed that thedevices could drive a load of about 10-15 F. When the loadcapacitance was increased between 10-14 F and 10-12 F the

waveform did not match with the normal gate operation asearlier.

5.3 Dependence on Temperature

The simulation temperature was at 4.2°K for the initialsimulations. When the operating temperature wasincreased, useful results were obtained till about 10°K. Ifthe temperature was increased further the logic ‘0’ voltagelevel at the output shifted further away from zero andsimilarly the voltage level of logic ‘1’ shifted downwardsaway from Vcc. The I/O waveforms for the NOR2 gate at20°K having undesirable voltage level shifts at the outputare shown in Fig. 7.

6 SUMMARY AND CONCLUSION

The CMOS architecture based NOR2, NOR3 and NAND2gates have been designed with SET’s and simulated usingSET-SPICE model. The effects of the temperature, islandand load capacitance were also studied.

ACKNOWLEDGEMENT ANDDISCLAIMER

The research reported in this document was performed inconnection with contract DAAD17-03-C-0115 with theU.S. Army Research Laboratory. The views andconclusions contained in this document are those of theauthors and should not be interpreted as presenting theofficial policies or position, either expressed or implied, ofthe U.S. Army Research Laboratory or the U.S.Government unless so designated by other authorizeddocuments. Citation of manufacturer’s or trade name doesnot constitute an official endorsement or approval of the usethereof. The U.S. Government is authorized to reproduceand distribute reprints for Government purposesnotwithstanding any copyright notation hereon.

REFERENCES

[1] D.G. Gordon, M.S. Montemerlo, J.C. Love, G.J.Opiteck and J.C. Ellenbogen, “Overview ofNanoelectronic Devices,” Proceedings of the IEEE,Volume: 85, No. 4, pp. 521 – 540, April 1997.

[2] K.K. Likharev, “Single-electron devices and theirapplication”, Proceedings of the IEEE, Volume: 87Issue: 4, pp. 606 –632, April 1999.

[3] A. Venkataratnam and A. Goel, “Simulation of LogicCircuits Based on the Single Electron Technology,”Proceedings of the International Workshop on Physicsof Semiconductor Devices, Chennai, India, Dec. 2003.

[4] C. Lageweg, S. Cotofana and S. Vassiliadis,, “Digitalto analog conversion performed in single electrontechnology,” Proceedings of the 2001 1st IEEEConference on Nanotechnology, pp. 105 –110, 2001.

[5] C.H. Hu, J.F. Jiang and Q.Y. Cai, “A single electrontransistor based Analog/Digital Converter,”Proceedings of the 2002 IEEE Conference onNanotechnology, pp. 487 – 490, 2002.

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Time0s 100ms 200ms 300ms 400ms 500ms 600ms 700ms 800ms

V(Vin1) V(Vin2) V(Cload)

0V

10mV

20mV

30mV

Fig. 3: I/O waveforms for the NOR2 gate at 4.2oK using SET-SPICE, C0=10-18F

Fig. 4: I/O waveforms for the NOR3 gate at 4.2oK using SET-SPICE, C0=10-18F

Time

0s 100ms 200ms 300ms 400ms 500ms 600ms 700ms 800msV(Vin1) V(Vin2) V(Cload)

0V

10mV

20mV

30mV

Fig. 5: I/O waveforms for the NAND2 gate at 4.2oK using SET-SPICE, C0=10-19F

Time0s 0.2s 0.4s 0.6s 0.8s 1.0s 1.2s 1.4s 1.6s

V(Vin1) V(Vin2) V (Vin3) V(Cload)

0V

10mV

20mV

30mV

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Time0s 100ms 200ms 300ms 400ms 500ms 600ms 700ms 800ms

V(Vin1) V(Vin2) V(Cload)

0V

10mV

20mV

30mV

Fig. 6: I/O waveforms for the NOR2 gate at 4.2oK using SET-SPICE, C0=10-19F

Time0s 100ms 200ms 300ms 400ms 500ms 600ms 700ms 800ms

V(Vin1) V(Vin2) V(Cload)

0V

10mV

20mV

30mV

Fig. 7: I/O waveforms for the NOR2 gate at 20oK using SET-SPICE, C0=10-19F

[6] C. Lageweg, S. Cotofana and S. Vassiliadis, “StaticBuffered SET Based Logic Gates,” Proceedings of theIEEE-NANO 2002, pp. 491 – 494, Aug 2002.

[7] C.P. Heij, P. Hadley and J.E. Mooij, “Single ElectronInverter,” Applied Physics Letter, Volume: 78, Issue:8,pp. 1140 – 1142, February 2001.

[8] G. Lientschnig, I. Weymann and P. Hadley,“Simulating Hybrid Circuits of Single-ElectronTransistors and Field-Effect Transistors,” JapaneseJournal of Applied Physics, Vol. 42, pp. 6467–6472,2003.

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