Novel Voltage-Controlled Oscillator Design byMOS

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Novel Voltage-Controlled Oscillator Design byMOS-NDR Devices and

Circuits

Dong-Shong Liang*, Kwang-Jow Gan, Chung-Chih Hsiao, Cher-Shiung Tsai, Yaw-Hwang

Chen,Shih-Yu Wang, Shun-Huo Kuo, Feng-Chang Chiang, and Long-Xian Su

Department of Electronic Engineering, Kun Shan University of Technology, Taiwan, R.O.C.

suln@mail.ksut.edu.tw

This paper describes the design of a voltagecontrolled oscillator (VCO) based on the negative differential resistance (NDR) devices. The NDR devices used in the work is fully composed by the metal-oxide- semiconductor field-effect-transistor

(MOS) devices. This MOS-NDR device can exhibit the

NDR characteristic in its current-voltage curve by suitably arranging MOS parameters. The VCO is constructed by three low-power MOS-NDR inverter.

This novel VCO has a range of operation frequency from 151MHz to 268MHz. It consumes 24.5mW in its central frequency of 260MHz using a 2V power supply.

This VCO is fabricated by 0.35µm CMOS process and occupied an area of 120 x 86 µm

2

.

1. Introduction

Abstract

In recent years, several new applications based on resonant tunneling diode (RTD) have been reported

[1]-[4]. The negative-differential-resistance (NDR) current-voltage (I-V) characteristics of the RTD devices have several advantages, and they may have high potential as functional devices due to their unique folding I-V characteristics. However these RTD devices are fabricated by the compound semiconductor and process. Therefore this kind of NDR device is difficult to combine with other devices and circuits to achieve the system-on-a-chip (SoC).

Therefore, we proposed a new MOS-NDR device that is fully composed of metal-oxide-semiconductor field-effect-transistor (MOS) devices. During suitably arranging the MOS parameters, we can obtain the NDR characteristic in its I-V curve. We call this NDR device as MOS-NDR device. Because this NDR device is consisted of the MOS devices, yet it is much more convenient to combine other devices and circuits to achieve the SoC by standard CMOS process.

We will demonstrate a novel voltage-controlled oscillator (VCO) designed based on the MOS-NDR devices and circuit. The VCO is constructed by three cascading low-power MOS-NDR inverters. The basic inverter is composed by two series-connected MOS-

NDR devices according to the monostable-bistable transition logic element (MOBILE). The signal will be feedback from the output of the third MOS-NDR inverter to the input of the first MOS-NDR inverter.

Under suitable design, we can obtain an oscillator with its frequency proportional to the magnitude of input bias. We design and implement this VCO by the

0.35µm CMOS process.

2.MOS-NDR Device and Inverter Design

Figure 1 shows a MOS-NDR device which is composed of three NMOS transistors. This circuit can show the ȁ -type NDR I-V characteristic by suitably arranging the MOS parameters. Figure 2 shows the I-V curve, measured by Tektronix-370B curve trace, with the width parameters of the three MOS devices as

1µm, 10µm, and 40µm, respectively. The MOS length is fixed at 0.35µm. The V

GG is fixed at 3.3V.

Fig. 1 The circuit configuration of a ӛ -type MOS-NDR device.

Proceedings of the 9th International Database Engineering & Application Symposium (IDEAS’05)

1098-8068/05 $20.00 © 2005

IEEE

2

1.6

(1)

1.2

0.8

0.4

W

1

=1u,W

2

=10u,W

3

=40u

V

GG

=3.3V

(2) (3) (4)

0

0 0.5

1 1.5

2 2.5

Voltage(V)

Fig. 2 The measured I-V characteristic for a MOS-NDR device..

If we connect a NMOS with a MOS-NDR device in parallel, we can modulate the peak current of MOS-

NDR device’s I-V curve through the gate voltage of

NMOS. The circuit is shown in Fig. 3. The total current I

Total is the sum of the currents through the

MOS-NDR and NMOS devices: I

Total

=I

NDR

+I

MOS

. Since

I

MOS

is modulated by the gate voltage (V

G

), so is I

Total

.

Our inverter circuit design is based on two seriesconnected MOS-NDR devices as shown in Fig. 4. This circuit is called as monostable-bistable transition logic element (MOBILE) [5]-[6]. The input node is located at the V

G

gate. The output node is located between the two MOS-NDR devices. When the bias voltage is smaller than twice the peak voltage (2V

P

), there is one stable point (monostable) in the series circuit.

(corresponding to “0” and “1”), respectively, are shown in Fig. 5. A small difference between the peak currents of the two devices determines the state of the circuit. If the peak current of the driver device is smaller than that of the load device, the operation point will be located at the high state. On the other hand, if the peak current of the driver device is bigger than that of the load device through the V

G

voltage, the operation point will be located at the low state.

Fig. 4 The MOS-NDR inverter designed by MOBILE theory.

Fig. 3 The peak current of MOS-NDR device can be controlled by the VG voltage.

However when the bias voltage is larger than two peak voltages but smaller than two valley voltages (2V

V

), there will be two possible stable points (bistable). The intersection point located at the NDR region for two I-

V curve will be regarded as unstable point. The two stable points that respect the low and high states

Fig. 5 The bistable states when V

S

is bigger than 2V

P but smaller than 2V

V

.

By suitably determining the parameters of devices and circuits, we can obtain the inverter result as shown in Fig. 6. Figure 7 illustrates the relationship between the input bias V

S

and the power dissipation for a MOS-

NDR inverter. The power dissipation of this inverter is

5.75mW using a 2V power supply.

Proceedings of the 9th International Database Engineering & Application Symposium (IDEAS’05)

1098-8068/05 $20.00 © 2005

IEEE

The circuit configuration of the novel VCO is shown in Fig. 8. The oscillator circuit is composed of three cascading MOS-NDR inverters. The signal will be feedback from the output of the third MOS-NDR inverter to the input of the first MOS-NDR inverter.

This VCO is designed and fabricated by the standard

0.35µm CMOS process and occupied an area of 120 x

86 µm

2

. Figure 9 shows the layout of VCO.

6

4

10

Fig. 6 The MOS-NDR inverter result.

8

2

0

1.6

2

Input Bias (V)

2.4

Fig. 7 The power dissipation for a MOS-NDR inverter.

3. VCO DESIGN

Fig. 9 The layout of VCO.

4. SIMULATION RESULTS

Under suitable parameters design, we can obtain an oscillator with its frequency proportional to the magnitude of input bias V

S

. Figure 10 shows the simulated waveform of the oscillator under 2V bias voltage by HSPICE program. Figure 11 shows its spectrum.

Figure 12 illustrates the relationship between the input bias and the oscillation frequency. This VCO has a range of operation frequency from 151MHz to

268MHz. The relationship between the power dissipation and input bias is shown in Fig. 13. It consumes 24.5mW in its central frequency of 260MHz using a 2V power supply.

Fig. 8 The circuit configuration of the VCO

Fig. 10 The simulated waveform of the oscillator.

Proceedings of the 9th International Database Engineering & Application Symposium (IDEAS’05)

1098-8068/05 $20.00 © 2005

IEEE

Fig. 11 The simulated waveform of the oscillator. power MOS-NDR inverters. For chip area die consideration, we use fully MOS devices instead of

LC-tank structure. The oscillation frequency is from

151MHz to 268MHz. This VCO is designed by the standard 0.35µm CMOS process. If we fabricated this

VCO by 0.18µm CMOS process, the oscillation frequency will be increased above GHz.

Acknowledgments

The authors would like to thank the Chip

Implementation Center (CIC) of Taiwan for their great effort and assistance in arranging the fabrication of this chip. This work was supported by the National Science

Council of Republic of China under the contract no.

NSC93-2218- E-168-002.

280

240

200

160

120

1.6

2

Input Bias (V)

2.4

Fig. 12 The relationship between the input bias and the oscillation frequency.

40

30

20

10

0

1.6

2 2.4

Input Bias (V)

Fig. 13 The power dissipation for a VCO.

5. Conclusions

We have designed a voltage-controlled oscillator

(VCO) based on the ȁ -type MOS-NDR devices and circuits. The VCO is composed of three cascading low-

References

[1] S. Sen, F. Capasso, A. Y. Cho, and D. Sivco, Ϙ

Resonant tunneling device with multiple negative differential resistance: digital and signal processing applications with reduced circuit complexity, ϙ IEEE

Trans. Electron Devices , vol. 34, pp. 2185-2191, 1987.

[2] T. H. Kuo, H. C. Lin, R. C. Potter, and D. Shupe, Ϙ A novel A/D converter using resonant tunneling diodes, ϙ

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[3] L.O. Chua, “Simplicial RTD-Based Cellular Nonlinear

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[4] Y. Kawano, Y. Ohno, S. Kishimoto, K. Maezawa, T.

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Electron. Lett ., vol 39, no. 21, pp. 1546-48, 2003.

[5] K. J. Chen, K. Maezawa, and M. Yamamoto, “InPbased high-performance monostable-bistable transition logic elements (MOBILE's) using integrated multipleinput resonant-tunneling devices”, IEEE Electron

Device Lett.

, vol. 17, pp. 127-129, 1996.

[6] K. Maezawa, H. Matsuzaki, M. Yamamoto, and T.

Otsuji, “High-speed and low-power operation of a resonant tunneling logic gate MOBILE,” IEEE Electron

Device Lett ., vol. 19, pp. 80-82, 1998.

Proceedings of the 9th International Database Engineering & Application Symposium (IDEAS’05)

1098-8068/05 $20.00 © 2005

IEEE

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