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Optically-switched microwave filter with the use of photovaractors in self-bias mode

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OPTICALLY-SWITCHED MICROWAVE FILTER WITH THE USE OF

PHOTOVARACTORS IN SELF-BIAS MODE

Zenon R. Szczepaniak*, Bogdan A. Galwas& and Sergei A. Malyshev#

*& Institute of Microelectronics and Optoelectronics, Warsaw University of Technology Nowowiejska 15/19, 00-665 Warsaw, Poland

Phone/Fax: (+48 22) 825 03 93

* [email protected] , & [email protected]

# Institute of Electronics, National Academy of Sciences of Belarus

22 Lagoiski Trakt, 220090 Minsk, Republic of Belarus [email protected]

Phone: (375-17) 265-22-13, Fax: (375-17) 265-25-41

ABSTRACT

A new type of semiconductor optoelectronic device, which is called as photovaractor, was used in a self-bias mode of operation to obtain an optically-variable impedance. This approach allowed designing an optically-switched microwave band-pass filter. The use of the photovaractor in the microwave structure was investigated. The measurements of the photovaractor, the idea of the self-bias mode, and the simulations of the filter have been presented.

INTRODUCTION

The fast development in the microwaves and the photonic fields causes the merging of these two branches. The microwave-driven optical devices as well as the optically-controlled microwave circuits are needed. Especially, the optically-controlled microwave signal processing is now under the interest, because of the development in the new radar, and fibre-radio systems. It is worth to point out the approach using the microwave planar structures, for example resonators, made on the semiconductor substrate – Cabon et al (1). Another approach to design the optically-controlled microwave circuits is to use two coupled semiconductor devices, when the first one is photosensitive, and the second one is controlled. The examples of such a solution are the following devices couples: PIN photodiode-varactor diode – by Szczepaniak and Galwas (2), photovoltaic cell-varactor diode, by Nagra et al (3), photovoltaic cell-FET – Sun et al (4). An alternative approach is to design and made the semiconductor device which parameters can be optically changed. The examples of this idea are microwave phototransistors and photovaractors.

PHOTOVARACTOR IN SELF-BIAS MODE

A new type of special microwave junction device is a photovaractor. Generally, it is for example, a PIN photodiode, which is specially designed, and optimised to obtain very high capacitance changes under the optical illumination. Idea, measurements and modelling of the photovaractor were described in previous papers – Malyshev et al (5). However the device provides the impedance change dependent on the bias voltage and the illuminating power level, the new proposal of the operation is a bias-free configuration. The assumption is that the external bias circuit is not used, and moreover, the device has its pins (anode and cathode) short-circuited by a very large resistor – for example 1 MΩ. It means that the photodiode is terminated by almost open. Then the optical illumination causes the generation of a voltage across the device. This mode of the operation can be described as a self-bias mode.

In this setup even relatively small optical illumination causes the significant change of the photovaractor impedance. The change of the capacitance as well as resistance is observed.

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An example of the photovaractor impedance changes under the optical illumination for the frequency band from 300 kHz to 3 GHz is shown in Fig. 1, and at the frequency equal to 900 MHz is shown in Fig. 2.

It can be seen that with the use of the optical power equal to about 0.112 mW it is possible to obtain two photovaractor impedance states: almost open (ON) and almost 50Ω match (OFF) – Fig. 2. This capability allows to design several microwave circuits working with the use of the two-state impedance.

OPTICALLY-SWITCHED MICROWAVE FILTER

The possibility of the optical control of the photovaractor impedance was considered to design an optically-switched microwave filter. The first design was the microwave band-pass filter at the centre frequency about 900 MHz. The filter structure consists of two coupled sections of the microstrip line. The second step of the design was the optimisation of the filter structure with two photovaractors connected to it. The general topology and the idea of the filter (it is not real scale) were shown in Fig. 3. The transmission characteristics of the filter with and without the photovaractors were shown in Fig. 4. The filter is in the ON state when the photovaractors are not illuminated. Then the photovaractors impedance is almost open, and the microwave signal can be transmitted through the filter structure. When the photovaractors are illuminated by the optical power, their impedance approaches to 50 ohms and causes the attenuation of the microwave signal, resulting in decreasing of the transmission. The Q-factor of the resonant filter structures is then very low. It corresponds to the OFF state. The transmission characteristics of the microwave filter with the photovaractors in the ON and OFF states were shown in Fig. 5.

CONCLUSIONS

However the filter without photodiodes can be designed with minimal losses in the pass-band, the filter with photovaractors has higher losses because the photovaractor impedance is not the ideal open. The OFF state can be obtain with the use of the optical power illuminating the photovaractors equal to 0.112 mW. The resistors loading the photovaractors influence on the speed of reaction of the photovaractor impedance under the optical illumination. The decrease of the resistors values will cause the improvement of the switching speed. However, the lower values of the resistors, the higher optical power required to achieve the same photovaractor impedance changes under the illumination. The optically-variable impedance of the photovaractor can be used in other different microwave applications.

REFERENCES

1. B. Cabon, A. Vilcot, S. Chouteau, B. Boyer, J. Haidar, M. Bouthinon, and J. Boussey - „Optical control of microwave passive devices integrated on silicon”, Proc. 10TH MICROCOLL Conference 1999, Budapest Hungary March 21-24, 1999.

2. Z. Szczepaniak and B.Galwas, “Optically-Controlled Microwave Phase Shifter”, Proc.

EDMO’99, King’s College London, UK, 22-23 November 1999, pp.290-294.

3. A.S Nagra, O. Jerphagnon, P. Chavarkar, M. VanBlaricum, and R.A. York, "Indirect optical control of microwave circuits using monolithic optically variable capacitors," IEEE Trans. on

MTT, Vol. 47, No.7, July 1999, pp. 1365-1372.

4. C. K. Sun, R. Nguyen, C. T. Chang, and D. J. Albares, “Photovoltaic-FET for optoelectronic RF/µwave switching,” IEEE Trans. on MTT, Vol. 44, No. 10, October 1996,pp. 1747-50, 1996. 5. S.Malyshev, B.Galwas, V.Andrievski, A.Chizh, L.Dobrzanski, and Z.Szczepaniak, “Analysis of

photovaractors for microwave photonic application”, Proc. 30TH EuMC’2000, France, Paris, 3-5

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0 1.0 1.0 -1.0 10.0 10.0 -10.0 5.0 5.0 -5.0 2.0 2.0 -2.0 3.0 3.0 -3.0 4.0 4.0 -4 .0 0.2 0.2 -0.2 0.4 0.4 -0.4 0.6 0.6 -0 .6 0.8 0.8 -0.8 Swp Max 3GHz Swp Min 0.0003GHz S[1,1] 0 mW S[1,1] 0.004 mW S[1,1] 0.04 mW S[1,1] 0.185 mW S[1,1] 1.885 mW

Fig. 1. Photovaractor impedance vs. frequency for different illumination powers in self-bias mode.

0 1.0 1.0 -1.0 10.0 -10.0 5.0 5.0 -5.0 2.0 2.0 -2.0 3.0 3.0 -3.0 4.0 -4.0 0.2 0.2 -0.2 0.4 0.4 -0.4 0.6 0.6 -0.6 0.8 0.8 -0.8 Swp Max 900MHz Swp Min 900MHz 0 mW 0.004 mW 0.005 mW 0.04 mW 0.112 mW 0.185 mW 0.552 mW 1.412 mW ON OFF Popt

Fig. 2. Photovaractor impedance at 900 MHz for different illumination powers in self-bias mode.

IN

O U T

C

R

R

C

P IN - p h o to va ra cto r

P IN - p h o to va ra cto r

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550 750 950 1150 1300 Frequency [MHz] -30 -25 -20 -15 -10 -5 0 T ra n sm is sio n [ d B ] DB(|S[2,1]

filter without photodiodes filter with photodiodes DB(|S[2,1]

Fig. 4. Transmission characteristics of the filter without photovaractors and optimised filter with photovaractors. 550 750 950 1150 1350 1450 Frequency [MHz] -30 -25 -20 -15 -10 -5 0 T ran sm iss io n [ d B ] DB(|S[2,1]|) Popt = 0 mW DB(|S[2,1]|)Popt = 0.112 mW ON - STATE OFF - STATE

Fig. 5. Transmission characteristics of the microwave filter with the photovaractors in ON (not illuminated) and OFF (illuminated) states.

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