TCS 325B
TCS 325B
2.1 INTRODUCTION
With conditions such as these it leaves the transmitted signal very susceptible to
interception and interference. In order to circumvent such disastrous outcomes that could
arise from such vulnerabilities, the theory of spread spectrum was introduced.
Spread spectrum involves the deliberate variations in frequency of the transmitted signal
over a comparatively large segment of the electromagnetic spectrum. This variation is
done in accordance with a specific, complicated mathematical function. This frequency-
versus-time function must be „known‟ by both sender and receiver to ensure
synchronization.
Spread Spectrum uses wide band, noise-like signals. Because Spread Spectrum signals
are noise-like, they are hard to detect. Spread Spectrum signals are also hard to Intercept
or demodulate.
Further, Spread Spectrum signals are harder to jam (interfere with) than narrowband
signal because Spread Spectrum signals are so wide, they transmit at a much lower
spectral power density, measured in Watts per Hertz, than narrowband transmitters
It is imperative for the spread spectrum function be kept very confidential and out of the
hands of unauthorized persons
2.2 SPREAD SPECTRUM TECHNOLOGIES
There are two main types of spread spectrum techniques that are employed. These are
Direct Sequence Spread Spectrum (DSSS) and Frequency Hopping Spread Spectrum (FHSS).
Direct Sequence Spread Spectrum also known as Direct Sequence Code Division Multiple
Access (DS-CDMA) entails the division of the stream of information into small pieces, each
of which is allocated to a frequency channel across the spectrum
A data signal at the point of transmission is combined with a higher data-rate bit sequence,
also known as the „chipping code‟, which divides the data according to a spreading ratio.
The redundant chipping code helps the signal resist interference and enables the original data
to be recovered if data bits are damaged during transmission.
For a more practical example of the techniques employed by DSSS, consider a direct
sequence spread spectrum radio. A DSSS radio works by mixing a Pseudorandom Noise
(PN) sequence with the data. This mixing is done either by generating a wideband signal
which, in turn, is used to modulate the Radio Frequency (RF) carrier, or by modulating the
carrier source with the data and then spreading the signal prior to transmission. On the
receiving end, the incoming Direct Sequence (DS) signal is reconstructed by generating local
replica of the transmitter‟s PN code, and synchronizing the signal with this local PN
sequence.
By removing the effects of the spreading sequence through the second time modulation of the
incoming signal by the local PN sequence, the spread signal collapses into a data-modulated
carrier. Using correlation techniques the identity of a signal that has been spread with a
particular PN sequence can be discovered.
Frequency Hopping Spread Spectrum (FHSS) also known as Frequency Hopping Code
Division Multiple Access (FH-CDMA) involves a signal being transmitted across a
frequency band that is much wider than the minimum bandwidth required by the
information signal
The transmitter „spreads‟ the signal originally in the narrowband, across a number of
frequency band channels on a wider electromagnetic spectrum.
In a FHSS system, a transmitter „hops‟ between available frequencies according to a
spreading algorithm. The transmitter operates in synchronization with the receiver, which
remains tuned to the same center frequency as the transmitter.
The transmitter is therefore capable of hopping its frequency over a given bandwidth several
times a second, transmitting on one frequency for a certain period of time known as the
„dwell time‟, then hopping to another frequency in the same spreading bandwidth and
transmitting again.
Ideally each frequency should be occupied with equal probability and the probability of
hopping from one channel to any other channel should also be equal.
In DSSS, the data signal is directly spread by means of a wide spread code sequence. The
main idea is to spread the spectrum of the modulated (modulation that can be baseband or
digital) data signal a second time by the use of a wideband spreading signal.
The wideband spreading signal is selected in such a way as to make demodulation possible
only by the intended receiver and to make demodulation by an unintended receiver
impossible.
Direct sequence contrasts with the other spread spectrum process, in which a broad slice of
the bandwidth spectrum is divided into many possible broadcast frequencies.
In general, frequency-hopping devices use less power and are cheaper, but the performance
of DS-CDMA systems is usually better and more reliable.
The baseband DSSS system applies the direct sequence spread spectrum technique directly to
the baseband digital data
Similarly, the modulated DSSS applies the spread spectrum technique to the data that is
already modulated by some digital modulation technique. Different types of modulation are
used before the DSSS technique is applied. Most common are BPSK and QPSK modulation.
The baseband direct sequence spread spectrum system spreads the baseband digital signal using
the wide-bandwidth spreading-code signal. The spreading is done to the baseband signal directly
without any digital modulation. The technique and hence the system is called as baseband DSSS.
The block diagram of a baseband DSSS system is shown in Figure 2.1.
Figure 2.1 Block diagram of Baseband DSSS System
The original data signal which is of low bandwidth is multiplied with the wide-bandwidth direct
sequence spreading code. This operation widens the bandwidth of the data signal. Figure 2.2 a)
shows the original digital signal (NRZ bipolar +1, -1) and the spectrum of the signal is shown in
Figure 2.2 b). A sample digital bit pattern of 1010011 is used as the baseband digital signal. The
digital signal bandwidth is very narrow and the spectrum is wrapped-around FFT of the digital
signal. The spectrum shows that the signal is centered on zero frequency with a very narrow
bandwidth extending over a few frequency bins (approximately 100).
The resulting spread spectrum signal obtained as a result of multiplying the high chip-rate PN
code with the low-bit rate digital signal is shown in Figure 2.4 a) and the spectrum of the
resulting spread spectrum signal is shown in Figure 2.4 b). The bandwidth of the signal has
widened and has occupied almost the same bandwidth as the PN spreading code.
Despreading at the baseband DSSS receiver system is done by remultiplying the received signal
with the same PN code used at the transmitter. The chip rate is to be kept the same. Also, the
despreading has to be perfectly synchronized, as the PN codes have very good autocorrelation
properties. The despread signal using the same PN code used at the transmitter, however this
being the ideal case, the output is same as the digital signal is shown in Figure 2.5 a) and the
spectrum of the despread signal is shown in Figure 2.5 b). But in the presence of noise and other
channel disturbances, the signal has to undergo a couple of other processes for optimum
detection of the signals. However, one observation is that the spectrum of the signal is narrow
and so the signal is despread. The other two mandatory processes are correlation and decision.
The correlation-receiver output for the despread signal. The pulse-shaping signal used for
multiplication prior to integration is a rectangular pulse with one-bit duration. The correlator
output shown in the Figure 2.6 is sampled at every decision-time instant and is sent to the
decision circuit. The decision circuit contains a threshold detector that compares the sampled
correlator output with a reference value. A reference value of 0 can be used for determining the
bits. If the correlator output at the decision-time instant is greater than zero, then a bit is received,
else a bit of 0 is received.
Figure 2.6 Correlator Output Figure 2.7 Final Recovered Digital Signal
The output of the decision circuit for the sample bit pattern is shown in Figure 2.7. The
recovered digital signal is 1010011, which is the baseband signal sent from the transmitter.
Therefore, the signal is effectively recovered at the baseband direct-sequence spread spectrum
receiver system.
All the users in a spread spectrum communication system share the same bandwidth for
communication and hence it may appear as if the signals can be tapped by unintended users. The
privacy and secrecy of the information signal lies within the uniqueness of PN code used. With a
range of PN codes and other spreading codes that can be generated, it is not possible to identify
the PN code at the transmitter for spreading. Hence the reception of the signal at the unintended
receiver on using different PN codes with similar chip rate can be investigated. An incorrect PN
code that is used by an unintended user to despread and detects the signal is shown in Figure 2.8
a) and its spectrum is shown in Figure 2.8 b). The spectrum of the PN code is similar to that of
the original PN code used for spreading at the transmitter.
The despread signal and its spectrum are shown in Figure 2.9 a) and 2.9 b) respectively. From
the spectrum it is observed that the recovered signal is not effectively despread, as the frequency
of the despread signal appears to be high. The spectrum of the despread signal also extends along
a wide bandwidth and it is seen that the despreading is not effective with a PN code different
from the one used at the transmitter.
Figure 2.9 a) Despread Signal b) Spectrum of Despread signal
Correlator output for the despread signal using incorrect PN code is shown in the Figure 2.10.
The peak correlation magnitude obtained is about 100, whereas the peak correlation obtained
using incorrect PN code is about 600. Since the threshold reference value in the decision circuit
is zero, this correlator output may be used for detecting data bits. When the correlation output at
the decision-time instants is given to the decision circuit, the output of the decision circuit is
shown in the Figure 2.11.
The decoded digital sequence signal sequence is 0101100 and this is transmitted by the
transmitter. Hence the digital signal cannot be recovered when an incorrect PN code is
employed. The presence of the signal itself cannot be detected, as the signal detector has a high
reference value compared to the corrector output. So, the signal goes undetected. The signal that
is received contains not only the signal transmitted by this single transmitter, but a combined
signal of various signals from similar DSSS transmitters. Hence it is impossible to detect and
decode a particular DSSS signal without the exact PN code used in the transmitter.
PERFORMANCE IN NOISE
The performance of the baseband DSSS technique is analyzed in the presence of noise.
The AWGN channel model is used for analysis. Figure 2.12 shows the AWGN noise added by
the channel to the transmitted spread spectrum signal. The amplitude of the noise signal is
comparable to the magnitude of the spread spectrum signal.
The spread spectrum signal that is received at the baseband DSSS receiver system corrupted with
noise is shown in Figure 2.13 a) and its corresponding spectrum is shown in Figure 2.13 b).
When compared to the original spread spectrum signal, this signal appears to be corrupted
beyond recognition. The spectrum of the signal, even though it occupies the same bandwidth,
seems to be distorted uniformly by noise, as shown by the spikes at the top of the spectrum
envelope. AWGN affects all the frequency components alike and as the noise bandwidth is
infinite and uniform, the spectrum shape and width remain the same.
Even though the despread signal appears to be noisy, the correlator receiver output shown in
Figure 2.15 is similar to the noise free case. The correlator output at the decision-time instants is
unambiguous. Figure 2.16 shows the final decoded digital signal. The recovered digital pattern is
1010011, which is the transmitted sequence and hence the DSSS technique fares well in the
AWGN channels.
Figure 2.15 Correlator Output Figure 2.16 Final Recovered Digital Signal
PERFORMANCE OF BASEBAND SIGNAL IN JAMMER
The baseband signal as altered by the jammer on the channel. The signal that is received at the
baseband receiver system is shown in the Figure 2.18 a) and its spectrum is shown in Figure 2.18
b). The spectrum of the signal has not altered but has increased in its magnitude.
The correlator peak magnitude has also increased. The increase in the spectral-power magnitude
and the output of the peak correlator may inform the receiver about the jammed signal. The
correlator output for the received signal with jamming is shown in Figure 2.19. However the
jammer can also be an intelligent jammer that can vary the signal amplitude so that there is no
increase in the spectral power or correlator output. The output of the decision circuit for the
correlator output is shown in Figure 2.20.
The recovered digital signal is 1010001, which is not the digital signal transmitted by the
baseband digital communication system. Therefore, the baseband digital communication system
cannot recover the digital system in the presence of an intentional jammer signal. The system
needs advanced techniques to be able to combat the detrimental effects of the jammer.
The baseband signal is spread across the wide bandwidth of the spreading code. The spread
spectrum signal is sent down the channel by the DSSS system. The jammer signal then acts on
the spread spectrum signal. The spread spectrum signal that is sent down the channel by the
DSSS system is shown in Figure 2.21 and the Jammer signal is shown in Figure 2.22.
The resulting signal when the jammer signal is added the spread spectrum signal is shown in
Figure 2.24 a) and its spectrum is shown in Figure 2.24 b). The spectrum of the resulting signal
has a peak centered on the zero axis, which is the axis of the jammer signal.
The despread signal received at the receiver and its spectrum is shown in Figure 2.25 a) and b)
respectively. The spectrum of the despread is not similar to the original signal spectrum; but is
spread across the wide bandwidth.
Figure 2.25 a) Despread signal b) Spectrum of the Despread signal
The correlator output of the DSSS receiver is shown in the Figure 2.26. The jammer has no
effect on the correlator output when it comes to the detection of bits. It has gone undetected as
noise, as it is now spread across the whole bandwidth. Figure 2.27 shows the final demodulated
signal at the DSSS receiver in the presence of the jammer.
Figure 2.26 Correlator Output Figure 2.27 Final Digital Signal Output
The digital sequence recovered is 1010011, which is the digital signal at the transmitter.
Therefore, the DSSS technique has satisfactorily eliminated the negative effects of the jammer
which the baseband transmission alone could not handle.
PERFORMANCE OF SPREAD SPECTRUM IN NOISE AND JAMMER
The received signal at the DSSS baseband receiver when the spread spectrum signal is acted on
both by the jammer and the AWGN noise is shown in Figure 2.28 a) and its spectrum is shown in
Figure 2.28 b). The combined signal has been corrupted by both the jammer signal and the noise.
The spectrum of the combined signal, therefore, shows a central peak corresponding to the
jammer component, a wide spread spectrum corresponding to the spread spectrum signal and
noise along the whole spectrum corresponding to the AWGN.
Figure 2.28 a) SS signal acted on by both Noise and Jammer b) Spectrum of the signal
The result of despreading this combined signal at the receiver and its spectrum is shown in
Figure 2.29 a) and b) respectively. The spectrum of the despread signal has the central peak that
corresponds to the original digital signal component, the wide spread spectrum corresponds to
the jammer signal and the noise component.
Figure 2.30 Correlator Output Figure 2.31 Final Digital Signal Output
The digital signal is perfectly recovered at the receiver end even in the presence of noise and
jammer signal by the application of direct sequence spread spectrum technique to the baseband
digital signal.
Digital modulation techniques, due to their inherent advantages, are often employed to modulate
the baseband digital signal before sending it onto the channel. The performance of modulated
DSSS is analyzed with Binary Phase Shift Keying (BPSK) modulation technique. The general
block diagram of modulated DSSS system is shown in Figure 2.32.
In the first type, the digital signal is first BPSK modulated using the BPSK carrier. The
modulated signal is then spread across the wide bandwidth by means of the spreading
code. At the receiver end, the signal is first despread by multiplication with the spreading
code and then it is BPSK modulated.
In second type, the digital system is first spread using the spreading code, just as in the
baseband DSSS system. The resulting signal is then BPSK modulated using the BPSK
carrier. At the receiver, the signal is first BPSK demodulated and then it is despread using
the spreading code.
BPSK modulated DSSS of first type is shown in Figure 2.33. First the digital signal is BPSK
modulated and is then multiplied with the spreading code to obtain the BPSK DSSS signal. This
signal is then sent down the channel. At the receiver signal is despread by multiplication with the
spreading code. It is then demodulated using the correlator receiver and the same reference
carrier.
Figure 2.33 Block Diagram of BPSK Direct Sequence Spread Spectrum system
The original digital signal sequence is 1011001, which is BPSK DSSS modulated. The signal
and its spectrum are shown in Figure 2.34 a) and b). The spectrum of the digital signal is narrow
and is centered on the zero frequency. BPSK carrier signal and its spectrum are shown in Figure
2.35 a) and b) respectively.
Figure 2.34 a) Digital Signal b) Spectrum of Digital signal
The BPSK carrier is high frequency compared to the digital signal. The spectrum of the BPSK
carrier has two peaks that are mirror image of each other about the zero frequency. The spectrum
shows two plain peaks without any side bands of noise, as the carrier contained just a single
frequency. The spectrum of the digital power does not have a single frequency but a combination
of various frequencies.
BPSK modulated signal is shown in Figure 2.36 a) and its spectrum is shown Figure 2.36 b). The
phase reversal is clearly observed at the bit transitions. The digital signal used is NRZ bipolar;
the signal is simply multiplied with the BPSK carrier to obtain the BPSK modulated signal. The
digital signal has to pass through a level generator that will generate the (+1, -1) levels
corresponding to bits 1 and 0.
Figure 2.36 a) BPSK Modulated Signal b) Spectrum
PN code used for spreading and its spectrum is shown in Figure 2.37 a) and b) respectively. The
PN code is of high bit rate and its spectrum is very wide compared to the baseband signal and the
BPSK carrier.
The BPSK DSSS signal after the BPSK signal has been spread with the spreading code. This is
shown in Figure 2.38 a) and its spectrum is shown in Figure 2.38 b). The signal spectrum is
spread across a wide bandwidth. The BPSK components are also visible in the spectrum as two
low-frequency peaks. This BPSK DSSS signal is then sent into the channel.
Figure 2.38 a) BPSK DSSS Signal b) Spectrum
At the receiving end the received signal is first despread with the same PN code used at the
transmitting end. Figure 2.39 a) and b) shows the despread signal and its spectrum. The despread
signal is the BPSK modulated signal. The spectrum of the signal is also the same as that of the
BPSK signal generated at the transmitter end. This BPSK signal is demodulated to obtain the
original digital signal sequence.
The correlator output of the BPSK demodulator is shown in figure 2.40 and the final recovered
digital signal sequence is shown in Figure 2.41. The correlator output is then taken at the
decision-time instants and is sent to the decision circuit, where a reference value of zero can be
used as threshold value for detection.
Figure 2.40 Correlator Output Figure 2.41 Final Digital Signal Output
The unintended listener may not have the exact information about the chip rate of the PN code
used or the spectrum of the PN code. To provide the best possible interception, the listener has
this information and so is able to a PN code with the same chip rate and spectrum. However, the
code generated is different from the one used at the transmitter. The incorrect PN code and the
corresponding spectrum of the code is shown in figure 2.42 a) and b) respectively.
The despread signal using this incorrect PN code and the spectrum of the despread signal is
shown in figure 2.43 a) and b). The bit rate of the despread signal and its spectrum that the
signal is not despread correctly. The despread signal should have a spectrum that is narrow like
that of the original digital signal. But the spectrum is almost as wide as that of PN code.
Figure 2.43 a) Despread Signal Using Incorrect PN code b) Spectrum
The peak value of the correlator output is very less compared to the actual correlator output,
when the received signal is despread using the correct PN code. This is observed from the Figure
2.44 and Figure 2.45 shows the final recovered digital signal using the incorrect PN code.
Figure 2.44 Correlator Output Figure 2.45 Final Digital Signal Output
The final recovered digital signal is 0100110, which is not the original digital sequence sent from
the transmitter. Therefore, with an incorrect PN code, it is impossible to demodulate and decode
the original information signal in the BPSK DSSS system.
The performance of the BPSK DSSS system is analyzed in the presence of noise, which is the
AWGN. The noise that is added by the channel to the BPSK DSSS signal is shown in Figure
2.46.
Figure 2.46 AWGN Noise
The received BPSK DSSS signal at the receiver system is shown in figure 2.47 a) and its
spectrum is shown in Figure b). When compared to the original signal, the received signal
appears to be completely distorted beyond recognition. The spectrum occupies the same
bandwidth, with some added noise. The received signal is despread with the same PN code used
at the transmitter end and the resulting despread signal and its corresponding spectrum is shown
in Figure 2.48 a) and b) respectively.
The despread signal appears to be completely noisy. By looking at the signal, there is no way to
recognize the phase-reversal positions. The spectrum of the despread signal shows the two low-
frequency peaks that correspond to the BPSK signal. The noise that is spread cross whole
bandwidth is due to the AWGN noise. The noise has almost negligible effect when it comes to
recovering the digital signal. The correlator output for this despread signal is shown in Figure a)
and the final recovered digital signal. The recovered digital signal is the same as the one that is
transmitted. The BPSK system performed satisfactorily in the presence of AWGN noise.
Figure 2.47 a) Despread Signal b) Spectrum
Figure 2.48 Correlator Output Figure 2.49 Final Digital Signal Output
The correlator output for this received signal is shown in Figure 2.52 and the final demodulated
output is shown in Figure 2.53. The output of the correlator is, sent to the decision-sampling
instant. The demodulated output, when a zero reference is used as the threshold value. The final
demodulated digital sequence is 1010001, which is different from the original signal modulated
at the BPSK transmitter end. Hence BPSK modulation cannot effectively remove the effects of
the jammer signal.
Figure 2.52 Correlator Output Figure 2.53 Final Digital Signal Output
PERFORMANCE OF BPSK DSSS IN JAMMER
In BPSK DSSS system, the signal that is sent down the channel is the BPSK signal, which is
spread across a wide bandwidth. The jammer signal gets included to this wideband BPSK DSSS
signal. The spread spectrum signal sent along the channel is shown in figure 2.53 a) and
comparison of the jammer signal spectrum with the BPSK DSSS signal spectrum is shown in
Figure 2.53 b). The spectrum of the jammer is very narrow compared to the spectrum of the
spread spectrum signal because the jammer has information only about the frequency spectrum
of the BPSK carrier signal.
The resulting sum signal when this jammer signal is added to the spread spectrum and its
corresponding spectrum is shown in Figure 2.54 a) and b) respectively. The addition of the
jammer signal has changed the constant-amplitude envelope of the spread spectrum signal.
However the spectrum of the resulting signal is unchanged except for a couple of peaks in the
low-frequency region corresponding to the low-frequency jammer signal.
The correlator output of the BPSK demodulator is shown in Figure 2.56 a) and the final
demodulated digital signal at the BPSK DSSS receiver system is shown in Figure 2.56 b). Even
though the despread signal appears to be distorted, the jammer signal has negligible effect on the
correlator output of the BPSK demodulator, when the DSSS technique is used in conjunction
with the BPSK modulation.
Figure 2.56 Correlator Output Figure 2.57 Final Digital Signal Output
The digital sequence recovered is 1011001, which is the digital signal that is modulated at the
transmitter end. The BPSK alone cannot remove the negative effects of the jammer signal and
has failed to recover the original digital signal. However, when BPSK is coupled with DSSS
technique, it is able to recover the digital signal perfectly.
PERFORMANCE OF BPSK DSSS IN NOISE AND JAMMER
Figure 2.58 a) shows the resulting signal when both noise and jammer signal act on the BPSK
DSSS signal. The spectrum of the signal shown in Figure 2.58 b) shows the effect of AWGN in
the form of noise spread along the whole width of the spectrum. The jammer spectral component
is identified by the two low-frequency peaks.
Figure 2.58 a) Combined Signal of Spread Spectrum, Noise and Jammer b) Spectrum
The combined signal received at the BPSK DSSS receiver. The signal is then despread using the
PN code. The spectrum of the despread signal has two low-frequency components. These
correspond to the original digital signal that is despread by multiplication with the PN code.
However, the spectrum appears to be noisier than when only AWGN is present. This is because
the jammer that is added in the channel now gets spread across the whole bandwidth of the PN
code. The resulting despread signal is shown in figure 2.59 a) and the spectrum of the despread
signal is shown in Figure 2.59 b).
The correlator output seems to be without any obvious distortion that could cause error or
ambiguity in detecting the digital signal. The correlator output for this despread signal is shown
in Figure 2.60 and the final decoded digital signal after the correlator output is given to the
decision circuit. This is shown in figure 2.61 and the digital sequence recovered is 1011001,
which is the same as the actual digital signal modulated at the transmitted end. The BPSK DSSS
system performed well even in the presence of noise and a jammer signal.
Figure 2.60 Correlator Output Figure 2.61 Final Digital Signal Output
The second method of BPSK DSSS is also the digital system is first spread using the spreading
code, just as in the baseband DSSS system. The resulting signal is then BPSK modulated using
the BPSK carrier. At the receiver, the signal is first BPSK demodulated and then it is despread
using the spreading code.
The information signal undergoes primary modulation by PSK, FSK or other narrow band
modulation; but the most widely modulation scheme is BPSK (Binary Phase Shift Keying)
and secondary modulation with spread spectrum modulation
Spread spectra are obtained by multiplying the primary modulated signal and the square
wave, called the PN sequence. In Direct Sequence-Spread Spectrum the baseband waveform
is XOR by the PN sequence in order to spread the signal. After spreading, the signal is
modulated and transmitted
The equation 2.1 that represents this DS-SS signal and the block diagram of the BPSK DSSS
Transmitter is shown in Figure 2.62 a)
x(t) = √ (2 Es/Ts) [b(t) ⊗ c(t)] cos (2 π fc t + θ ) (2.1)
where
b(t) is the data sequence
Ts is duration of data symbol
c(t) is the PN spreading sequence
fc is the carrier frequency
θ is the carrier phase angle at t=0
Figure 2.62 a) Block Diagram of DS- SS Transmitter
The block diagram of the BPSK DSSS Transmitter is shown in Figure 2.62 b). The demodulator,
de-modulates the modulated (PSK) signal first, low Pass Filter the signal, and then de-spread the
filtered signal, to obtain the original message.
It is clear that the spreading waveform is controlled by a Pseudo-Noise (PN) sequence, which is
a binary random sequence. This PN is then multiplied with the original baseband signal, which
has a lower frequency, which yields a spread waveform that has noise-like properties. In the
receiver, the opposite happens, when the pass-band signal is first demodulated, and then de-
spread using the same PN waveform. An important factor here is the synchronization between
the two generated sequences.
If despreading is applied to the received diffuse wave, it returns to the PSK or FSK modulated
wave resulting from primary modulation. Then, as with narrowband demodulation, if the
despread wave and local signal are multiplied, and appropriate low pass processing is applied,
the information signal is obtained. Despreading involves multiplying the same PN code as that
used at the transmitting end for the receiving wave. At this time, it‟s necessary to synchronize the
receiving wave and PN code. The interference component power that falls into the demodulation
frequency band is reduced.
There are two processing methods on the receiving side, demodulation of the information signal
after despreading, and obtaining a positive and negative PN code by multiplying the local signal
by the receiving wave and despreading using correlation detection. With the former there is
process gain but the problem of synchronization remains. With the latter, the spectrum density of
the receiving wave itself is low and regeneration of the local carrier for performing synchronous
detection is a problem.
The occurrence of errors is calculated using a stochastic process, so ultimately, using a spread
spectrum results in fewer errors and this is why spread spectrum communication is resistant to
interference.
Far-Near Problem
Consider the situation, when a particular mobile is very far away from the mobile base-station.
Since the mobile is very far from the base-station, the effective power of the received signal is
very low. Consider another mobile, which is positioned right next to the first mobile. The power
of the signal from the second mobile is very high compared to the weak power signal of the first
mobile. Since two signals are positioned very close in the frequency spectrum, it is possible that
the high powered signal may completely overpower the low powered signal. As a result, the first
mobile will not be able to receive the signal from the mobile station. The problem repeats at the
base-station, when the base-station is trying to receive a low powered signal from a far-off
mobile and at the same time another mobile, which is in close proximity to the base-station sends
out a high powered signal that is close in spectrum to the weak signal frequency. This causes the
signal to be garbled and causes distortion. This situation is commonly referred as near-far
problem in wireless communication.
2.9 JAMMING CONSIDERATIONS
The goal of a jammer are to deny reliable communications to his adversary and to
accomplish this at minimum cost
The usual design goal for an anti-jam (AJ) communication system is to force a jammer to
expend its resources over
a wide-frequency band
for a maximum time
from a diversity of sites
Pulse Jammer
A pulse noise jammer is one that transmits pulses of band-limited white Gaussian noise with a
total average power of J. The effect of the jammer is more if it is successful in modelling its
central frequency and bandwidth to be identical with the communication channel.
Where,
Q(x) = 0.5*erfc(x/√2)
Eb - Energy per bit
N0 - Receiver front end thermal noise
While transmitting the noise pulse within the receiver bandwidth, the noise jammer will cause
the receiver front-end thermal noise power spectral density to increase.
N0′ = N0 + (Nj/ρ)
Where,
N0′ - New thermal noise power spectral density of the receiver
Nj - Jammer power spectral density
ρ - duty factor
The jammer power spectral density NJ is related to the total average noise power of the jammer
by the following relation:
NJ = J/BW
Where BW –bandwidth of the transmitted signal
The new increased average probability of error is
Compared to noise introduced by jammer, the thermal noise of RADAR, the first term in the
above equation is negligible. The probability of bit error is given by
Using the Q function and maximizing the resultant error probability with respect to ρ, the
maximum value of the duty factor is
ρ = Nj / 2Eb
The corresponding error probability is
As a result, the maximized new error probability is proportional to NJ, the jammer noise power
spectral density.
The partial-band noise jammer, which consists of noise whose total power, is evenly spread over
some frequency band that is a subset of the total spread bandwidth. Owing to the smaller
bandwidth, the partial-band noise jammer is easier to generate than the barrage noise jammer. A
PBNJ where the jammer transmits noise over a fraction of the total spread spectrum signal band
spreads noise of total power J evenly over some frequency range of bandwidth Wj, which is a
subset of the total spread bandwidth Wss.
The fraction ρ is defined as the ratio
where r is (0, 1) which is the fraction of the total spread spectrum band that has noise of power
spectral density
A Gaussian noise jammer is chosen to restrict its total power J to a fraction r of the full SS
bandwidth Wss. A corresponding degraded SNR level
It is assumed that the jammer hops the jammed band over Wss, relative to the FH dwell time
1/Rh, but often enough to deny the FH system the opportunity to detect that it is being jammed in
a specific portion of Wss and take remedial action.
Multitone Jammer
In tone jamming (TM), one or more jammer tones are strategically placed in the spectrum where
they are placed and their number affects the jamming performance. Two types of tone jamming
are
Single-tone jamming (STJ) places a single tone where it is needed
Multiple-tone jamming (MTJ) which distributes the jammer power among several tones
Figure 2.63 Power spectral density of (a) STJ and (b) MTJ
Where:
A is the amplitude
f0 is frequency of STJ and
θ is the initial phase which is uniform distribution between (0, 2π).
Where PJ and NT are total jamming power and the number of multi tone jamming respectively. PJ is
divided into same power equally depending on the number of multi tone jamming and fj is jamming
frequency. All phases are assumed to be independent and uniformly distributed over (0, 2π).