written 8.5 years ago by | • modified 8.5 years ago |
Mumbai University > Electronics Engineering > Sem7 > Optical Fiber Communication
Marks: 10M
Year:May2014
written 8.5 years ago by | • modified 8.5 years ago |
Mumbai University > Electronics Engineering > Sem7 > Optical Fiber Communication
Marks: 10M
Year:May2014
written 8.5 years ago by | • modified 8.5 years ago |
The photodiode converts the optical bit stream into an electrical time-varying signal. The role of the preamplifier is to amplify the electrical signal for further processing.
An equalizer is sometimes used to increase the bandwidth. The equalizer acts as a filter that attenuates low-frequency components of the signal more than the high-frequency components, thereby effectively increasing the front-end bandwidth.
The amplifier gain is controlled automatically to limit the average output voltage to a fixed level irrespective of the incident average optical power at the receiver. The low-pass filter shapes the voltage pulse. Its purpose is to reduce the noise without introducing much Intersymbol interference
The pulses sent by the transmitter arrive distorted at the receiver. This digital pulse train incident on the photodetector is given by:
$$P(t)= \sum_{n = -∞}^∞b_n h_p (t-nT_b)$$
P(t) is the received optical power
$T_b$ is the bit period
$b_n $ is the amplitude parameter of the nth message bit
$h_p t$ is the received pulse shape
$$∫_{-∞}^∞ h_p(t) dt=1$$
$$i(t)= \frac{ηq}{hν } M P(t)= R.M ∑_{n=-∞}^∞b_n h_p (t-nT_b)$$
Where, $R= \frac{ηq}{hν}$ is photodiode responsivity
M = Mean gain of photodetector.
This current is then amplified and filtered to produce a mean voltage at the output of the equalizer given by convolution of current with amplifier impulse response
$$v_{out} (t)= A.R.M.P(t)h_B (t)h_{eq} (t) \ \; \ v_{out} (t)= R.G.P(t)* h_B (t)*h_{eq} (t) ....(1) \ \; \$$
Here, A is the amplifier gain, and G is total gain. ∴ G = AM
$h_B (t)$ is the impulse response of bias circuit
$h_eq (t)$ is the equalizer impulse response
$H_B (f)$ is the Fourier transform of $h_B$ (t)
$$h_B (t)= F^{-1} [H_B (f)]= ∫_{-∞}^∞H_B (f) e^{j2πft} df$$
The bias current transfer function $H_B$ (f) is simply impedance of parallel combination of $R_b,R_a,C_d $ and $C_a$
$$H_B (f)= \frac{1}{1⁄R+ j2πfC}$$
Where, $ \frac1{R}= \frac1{R_a} + \frac1{R_b} $
$$C= C_a+ C_b$$
Where, $h_{out} (t)$ is the shape of an isolated amplified and filtered pulse.
The Fourier transform equation is given as:
$$H_{out} (f)= ∫_{-∞}^∞h_{out} (t).e^{-j2πft} dt=R.G.H_p f.H_B (f).H_{eq} (f)$$
Where, $H_p$ (f) is the Fourier transform of received pulse and $H_{eq} (f)$ is the transfer function of the equalizer.