# Temporal Response of MSM-LED Optical Integrated Device

Authors: Sh. M. Eladl; M. A. Ashour
Journal: Journal of Atomic, Molecular, and Optical Physics
 (2011)

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## Abstract

The temporal response of an optical integrated device is theoretically analysed. The device is composed of a Metal-Semiconductor-Metal (MSM) Photodetector and a Light Emitting Diode (LED). The analysis is based on the frequency response of the constituent devices without any optical feedback within the device structure. All expressions describing the frequency response, time response, output derivatives, and rise time are outlined. The results show that the temporal response of MSM detectors is similar to the LED response if the cutoff frequency of the LED is lower than that of MSM, while it is similar to MSM detector if the cutoff frequency of the MSM is lower than that of LED.


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## Body

## 1. Introduction

There is an increased interest in Metal-Semiconductor-Metal (MSM) photodetectors recent years as they offer an attractive alternative to the traditional choice of PIN photodetectors. The MSM Photodetectors are very suitable for high-speed photodetection. This increased interest is because of their ease of fabrications, larger bandwidth, and flexibility with other electronic circuit technologies. Monolithic integration of such types of devices onto several semiconducting materials allows them to be integrated with other semiconducting devices to obtain other enhanced functions [1, 2].Planar metal-semiconductor-metal light-emitting diodes with InGaN/GaN multiquantum wells (MQWs) as the active layer have been demonstrated for the first time. The diodes with interdigitated Schottky electrodes fabricated on p-GaN contact layer exhibit symmetrical current-voltage characteristic with a turn-on voltage of ~13 V at 20 mA. The violet light emission centred at 408 nm is generated by radiative recombination taking place in the MQWs. The evolution of light output power against injection current reveals an enhanced carrier collecting efficiency of the active MQWs at higher injection current level [3, 4].The reliable n+-ZnSSe metal-semiconductor-metal (MSM) blue-green light emitting diodes (LEDs) have been fabricated. The contact metal was CuGe/Pt/Au. The current transport mechanisms agree very well with the back to back tunneling diodes. The kink phenomena were observed in the MSM current-voltage curves. In the metal-semiconductor interface, the element Zn in ZnSSe can be replaced by Cu results in some acceptor levels as radiative recombination centers in the MS interface. The peak wavelength in the LED electroluminescent (EL) spectra was strongly dependent on the injection currents from 5 to 40 mA. The peak wavelength and full width at half maximum are 510 and 10 nm, respectively, at 10 mA injection current. When the injection current increases to 15 mA, the peak wavelength shifted to 530 nm due to different recombination centers. Further increasing the injection currents, the peak wavelength shifted slightly to the long wavelength side [5–7]. No previous attention has been focused to analyze the MSM-LED integrated device.In this paper, a proposed integrated optical device is composed of a Metal-Semiconductor-Metal (MSM) photodetector as a detecting part at the input side of the device and a Light Emitting Diode (LED) as an emitting part at the output side of the device. A schematic view of the proposed structure is shown in Figure1; the device consists of MSM detector with interdigitated contacts each separated by a distance L. The other part of the device is 3 layers of LED. The aim is to study the dynamic characteristics of this integrated device based on the frequency response concerning this two constituent parts. An optical feedback will take place due to the back light from the LED side to the MSM photodetector side within the structure of the device. The analytical expressions are carried out by neglecting this optical feedback effect within the device due to the difference in the optical spectra of both input and output sides.Figure 1
A schematic view of MSM-LED integrated device.


## 2. Theoretical Analysis

The frequency response of the quantum efficiency of MSM photodetector is outlined in [8]
(1)ηMSM(ω)=hντtr∑k=1∞Ck,nζk,n+jω,
where h is blank’s constant, ν is the frequency of the input light, and Ck,n, ζk,n, τtr are described in [8].And the frequency response of LED is reduced as(2)ηLED(ω)=η01+jω/ωLED.
For MSM-LED integrated structure,(3)ηMSM-LED(ω)=(hντtr,n∑k=1∞Ck,nζk,n+jω)(η01+jω/ωLED).
Assuming a unit impulse response of the input light power
(4)ηMSM-LED(s)=hντtr,n(1s)(∑k=1∞Ck,nζk,n+s)(η01+s/ωLED).
Taking the inverse Laplace,forωLED>ςk,n,
(5)ηMSM-LED(t)=hνCk,nτtr,nζk,n[1-∑k=1∞η0e-ςk,nt],
for ωLED<ςk,n,(6)ηMSM-LED(t)=Ck,nζk,n[1+η0e-ωLEDt].
The output derivative of MSM-LED as a measure of speed can be derived as
(7)ddt(ηMSM-LED(t))=hν[Ck,n]2τtr,nζk,n[∑k=1∞η0e-ςk,nt].
And for ωLED<ςk,n, it will reduce as (8)ddt(ηMSM-LED(t))=-ωLEDCk,nζk,n[η0e-ωLEDt].
Rise time can be calculated as follows:
(9)T=ln⁡[0.2[hνCk,n]-0.9ηζk,nτtr,n/η0[hν(Ck,n)2]]-1.


## 3. Results and Discussions

The device parameters used in the following calculations are as follows:τ = 1 ns, k=20, μn=8500 cm2/V.s, and μp=400 cm2/V.s. The input light is assumed as a step function in time. The transient response of the quantum efficiency of MSM photodetector for carriers of electrons, holes, and total photocurrents is shown in Figure 2. This curve is calculated by 20 terms of the Fourier series concerning  (1). The steeply sloped curve is for the electron and the much less sloped curve, appearing almost as constant for this current scale, is for the holes. The total photocurrent appears approximately as the electron current offset by a constant. In this regime, it is evident because of their higher mobility. The dependence of quantum efficiency on the contact spacing L is clear in Figure 3.  It can be seen that the high quantum efficiency of the device can be achieved by choosing the contact spacing L to be large.  The calculated transient response of the MSM-LED integrated device is shown in Figure 4. It can be noticed that the contact spacing L has a major effect on controlling the quantum efficiency of the device. Also shown in the figure as the contact spacing L is increased, which in turn increases the width of the barrier, the quantum efficiency of the considered device is also increased.  In addition, the quantum efficiency value initially increases linearly with time until approaching a definite value; this definite value mainly depends on the input power intensity, operating wavelength, and the contact spacing L. The parameters used for calculation are shown in the figures.Figure 2
Temporal response of MSM atL = 0.3 μm.Figure 3
Temporal response of MSM atL = 0.1 μm.Figure 4
Temporal response of MSM-LED at different values ofL and μ = 8500 vcm−2.The value of carrier mobilityμ has a significant effect on the performance evaluation of the MSM-LED integrated device. Figure 5 shows the temporal response of the quantum efficiency of the developed device when carrier mobility μ is taken into account. From the figure, as the value of carrier mobilityμ increases the quantum efficiency of the proposed device decreases.Figure 5
Temporal Response of MSM-LED at different values ofL and μ = 400 vcm−2.The dependence of the output derivative as a measure of the device speed on time is shown in Figure6. Also the effect of contact spacing L on the output derivative is shown in the same figure.  It has been shown from the figure that the device output changes with decreasing derivative and thus will approach zero, also the output derivative increases with the increase of contact spacing L at any time.Figure 6
Output derivative of MSM-LED at different values ofL and μ = 8500 vcm−2.Again, the value of carrier mobilityμ has a significant effect on the output derivative of the MSM-LED integrated device. Figure 7 shows the variation of the output derivative of the considered model with time when μ is taken into account to be considered. From the figure, as the value of carrier mobility μ increases the device output changes with decreasing derivative.Figure 7
Temporal Response of MSM-LED at different values ofL and μ = 400 vcm−2.The variation of the rise time with the desired quantum efficiency at different values ofL is shown in Figure 8.  It can be noticed that the rise time increases with the increase of quantum efficiency and the contact spacing L of the device. With the increase in the desired quantum efficiency, the difference between the final state quantum efficiency and the initial one will increase; this increased difference will take more time and hence the increase in rise time. Also, the quantum efficiencies of both MSM photodetector and LED cause an enhancement of the output, and hence the rise time is increased as a result.Figure 8
Rise time against quantum efficiency of MSM-LED at different values ofL.


## 4. Conclusion

Analytical modeling of the temporal performance of an integrated device is presented. The device under study is composed of a Metal-Semiconductor-Metal (MSM) Photodetector and a Light Emitting Diode (LED). The modeling is based on the frequency response of the constituent devices. The analytical expressions describing the transient performance are derived. The results show that the quantum efficiency of LED causes an enhancement of the output and rise time is increased as a result. As a future extension to this study, modeling of this device by the use of its equivalent circuit is planned to show the effect of all interesting parameters on the static characteristics



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*Source: 756758-2011-03-29.xml*