Implementation of Wireless Receiver Algorithms

Implementation of Wireless murderer Algorithms sort 1 System Specifications (Tsimenidis, 2016) presage 2 pith coif (Tsimenidis, 2016)Figure 3 Non-coherent teleph hotshot and only(a) murderer (Tsimenidis, 2016)Figure 4 Coherent receiver (Tsimenidis, 2016)Figure 5 Receiver Front-End (Tsimenidis, 2016)Figure 6 Frequency retort of a passband filter (Tsimenidis, 2016)Figure 7 Band-pass filter responseFigure 8 Band-pass filter input/outputFigure 9 Implemented DPSK demodulator (Tsimenidis, 2016)Figure 10 Low-pass filter input/outputFigure 11 Optima sample time diagramFigure 12 Symbol with 40 samples (Tsimenidis, 2016)Figure 13 Early-Late sample at an arbitrary stain (Tsimenidis, 2016)Figure 14 Early-Late sample at the maximum point of origin (Tsimenidis, 2016)Figure 15 Early-Late attributeic representation synchronicity input/outputFigure 16 Result of non-coherent receiver stainingFigure 17 IQ Downconverter (Tsimenidis, 2016)Figure 18 Sine and cos lettuce confuse graphsFigure 19 Index control flow (Tsimenidis, 2016)Figure 20 puree comparison (Tsimenidis, 2016)Figure 21 Down-conversion x3I vs. x3Q counter clockwiseFigure 22 Down-conversion x4I vs. x4Q counter clockwiseFigure 23 x6I vs. x6QFigure 24 Averaging approach to overcome the jitter (Tsimenidis, 2016)Figure 25 work out to solve the jitterFigure 26 dogma of the derived function detector (Tsimenidis, 2016)Figure 27 Constellation without Phase Offset (dI Vs dQ)Figure 28 Result of coherent receiver detection employ differential coherent demodulatorFigure 29 BPSK and DPSK BER comparison (Tsimenidis, 2016)Figure 30 Costas Loop algorithm (Tsimenidis, 2016)Figure 31 Costas loop yQ vs. yIFigure 32 Message moderateed using Costas loopFigure 33 BER comparison of different modulation schemes and techniques (Sklar, 1983)This suffer is strained on implementing and coupling several functional blocks that willing abandon us to detect, extract and decode a wireless centre that is being broadcasted in th e Merz laboratory of computers. In the pursual sections, we will find the death penaltys of coherent and non-coherent receivers.In the section 1 we define the basic background know takege that will be commonly used in the posterior digits of the report. We define the basic structure and features of the transmitter as well as the message format that the system is intended to detect. Finally, we define what is a coherent and a non-coherent system and provide a classification about the different techniques.In the section 2 we will analyse the non-coherent receiver writ of execution from the message acquisition, red ink to the filter section, signal leveling and refinement, using a DPSK demodulator to define the probable symbols represented, then establishing a synchronisation for the symbol and finally presenting the message obtained.The section 3 will focus in the realization of a coherent receiver, considering two possible variations on this type of implementation the first will be developed using a differential coherent demodulator, in this technique we will not recover the carrier signal. The second implementation of this receiver, will be done using a carrier recovery technique, which is in this case a Costas Loop Algorithm.Some common blocks be done in all the possible implementations that were carried out during this project the first is the receiver front-end which is the responsible to acquire and prepare the signal for the posterior molding. To recover the symbol synchronizing, we use a technique called early-late gate, this will let us know what is the or so convenient instant of the time to sample the signal. For the case of coherent signal, we must adapt this technique to apply it separately for the signal I (in-phase) and Q (quadrature).The section 4 contains analysis, conclusions and discussions of the results obtained during the realization of the phases.The persist sections of the report detail the references used for further expla nations and the different programs used for implementing each block.In each section, we include weensy further explanations that could be referred to understand the steps and details that have been done in the corresponding section.1. Background knowledge1.1. Aims and objectivesThe focus of this project is to demonstrate the implementation and the behaviour of entropy links using Radio Frequency as media and different techniques. Basically, we use two techniques coherent and non-coherent implementations. A further explanation of these techniques will be done in the following sections.A second implementation of a coherent receiver will be carried out by using a phase recovery technique with the Costas Loop and coupling the posterior phase to this block.The specifications of the system to be implemented could be defined as a set of blocks connected as followsFigure 1 System Specifications (Tsimenidis, 2016)Where the transmitter has been already implemented, therefore the work will b e carried out in the receiver algorithm to obtain the final data, which of course must be in a human readable format.We also must consider that the format of the message that is being broadcasted wirelessly in the Merz lab has the following formatFigure 2 Message format (Tsimenidis, 2016)1.2. Digital modulationThe digital modulation process refers to a technique in which the digital representation of the information is embedded in a signal, a carrier typically a sinusoidal signal, in such(prenominal) a way that this information will modify an established logical argument of the signal.We can define a sinusoidal carrier in a frequent way as a signal that will correspond to the equationWhere the information could be embedded in this will be called amplitude modulation, if the parameter this will be called frequency modulation and finally the phase modulation will be obtained if we embed the data in the expression.Regard to the symbol this is called the angulate frequency, it is m easured in radians per second, this is related to the frequency (f) expressed in Hertz by the expression.1.3. Coherent and non-coherent detectionConsidering the receiver side, we can classify the demodulation or detection based on the use of the carriers phase information in the process of information recovery. In the case that the receiver uses this information to detect the signals it will be called coherent detection, and non-coherent detection otherwise. This are also called synchronal and asynchronous detection, respectively.CoherentNon-CoherentPhase tack Keying (PSK)Diferential Phase Shift Keying (DPSK)Frecuency Shift Keying (FSK)Frecuency Shift Keying (FSK)Amplitude Shift Keying (ASK)Amplitude Shift Keying (ASK)Continuous Phase Modulation (CPM)Continuous Phase Modulation (CPM)Figure 3 Non-coherent receiver (Tsimenidis, 2016)Figure 4 Coherent receiver (Tsimenidis, 2016)2. Non-coherent receiver2.1. Receiver Front-EndThis segment of the non-coherent receiver will consist of th e first two blocks, which are common for both coherent and non-coherent implementations.Figure 5 Receiver Front-End (Tsimenidis, 2016)The first block is the responsible to take a sampled input expressed as bits, represent it as a float number and then renormalize it to a range +/- 1.0.The second stage applies a bandpass filter to the signal, this will attenuate the parasites components of frequency that could contaminate the signal that we received.Figure 6 Frequency response of a passband filter (Tsimenidis, 2016)To design the passband filter we must consider the following information let = 4800 Hz, data rate = 2400 bps and sampling frequency = 48000 Hz.These assumptions, led us to the following resultsLower passband cut-off frequency = = 3600 HzUpper passband cut-off frequency = + = 6000 HzLower stopband cut-off frequency = = 1200 HzUpper stopband cut-off frequency = + = 8400 HzThe implementation of the filter will be done using the sptool command of Matlab, using th e above defined values as parameters for the filter.The following figure sights the result obtained in the realization of the lab, considering the number of filter coefficients of 101.Figure 7 Band-pass filter responseFigure 8 Band-pass filter input/output2.2. DPSK demodulatorTo implement the non-coherent detection, we are going to use a DPSK demodulator, which was oldly categorized as a non-coherent technique.The DPSK demodulator will take advantage of two basic operation that go along on the transmitter the first is the differential encoding, and the second is the phase-shift keying. In the transmitter, the signal will be advanced in phase, with respect to the current signal, if the symbol to be sent is 0, and the phase will be preserved if the bit corresponds to 1. In the side of the receiver, we have memory that will be able to compare the phase of two successive bit intervals, i.e. it determines the relative difference in phase of these two, determining the correspondent sym bols without the need of having information about the phase of the signal in the transmitter.Figure 9 Implemented DPSK demodulator (Tsimenidis, 2016)The FIR matched filter block will correspond to a low-pass filter, this is required because the demodulation process, as it is a multiplication surrounded by two sinusoidal signals, will generate a low-band signal and a high-band signal, where the second one should be filtered.2.3. Symbol synchronisationThe symbol synchronisation, also called symbol timing, is a critical process that consists in the continuous estimation and update of information of the symbol related to its data transition epochs. This is a critical process that must be conducted to keep the communication accuracy in accep panel levels.Broadly speaking, the synchronization techniques could be classified in two groups open-loop and closed-loop. The chosen technique for this project corresponds to the Early-Late Symbol Synchronization which is a closed-loop type. The mo st popular technique is the closed-loop synchronization because Open-loop synchronizer has an unavoidable nonzero average tracking error (though small for tumid SNR, it cannot be made zero), a closed-loop symbol synchronizer circumvents this problem.(Nguyen Shwedyk, 2009)The corresponding results of the output of the demodulator are the following figures, these corresponds to the signals before and after the signal is filtered with the FIR low-pass filter.NotesThe trim down in blue corresponds to the signal containing the high-frequency parasite component, and the curve in red shows the result of filtering the high frequency component, i.e. this is the output signal of the filter.The symbol correspondence is symbol 0 for positive numbers, and symbol 1 for negative magnitudes.Figure 10 Low-pass filter input/output2.3.1. Early-late Symbol Synchronization (Reed, 2002)The algorithm Early-late used for synchronization is supported by the idea that the sample of a symbol must be taken in the time where the energy is maximum, this will warranty a minimum error probability.This algorithm exploits the symmetry of the signal, neglecting the distortion and noise. Considering the following figure, we can see that the optimal time to take the sample, identified as T, should be in the halfway between two points T0 + d and T0 d, if the power in the T0 + d and T0 d is, ideally, the same.Figure 11 Optima sample time diagramSuppose the following figure shows a symbol, we can notice that if we take an arbitrary sample, e.g. n=3 and depending on the thresholds, could be wrongly interpreted as 0, however the most permitd value is 1.Figure 12 Symbol with 40 samples (Tsimenidis, 2016)With a buffer size of 20 registers, we can notice that in the following figure the power levels of the signal for n=0 and n=19 are different, then we need to move the whole buffer one space to the right.Figure 13 Early-Late sample at an arbitrary point (Tsimenidis, 2016)If we continue with the ite ration and we follow the rules described in the flow diagram, we will converge in a finite number of iterations, where we can see that the result is located as expected, this could be seen in the following figure.Figure 14 Early-Late sample at the maximum point of power (Tsimenidis, 2016)The results of the application of this algorithm for our case are shown in the following figureNoteThe signal in red is the input of the early-late symbol synchronization block and the signal in blue is the value of Em that will finally determine the value that the symbol is representing, in each case.Figure 15 Early-Late symbol synchronization input/output2.4. Frame synchronisationAs was stated in the in the background section, the message frame will get under ones skin with the characters ++++ and the message has 72 bytes encoding the message using a ASCII characters. Therefore, this section will deal with two tasks (1) Detect the message preamble and (2) Decode byte per byte of the data containe d in the payload.After the preamble section, we will detect 576 bits, corresponding to the 72 bytes that correspond to the ASCII characters. These characters will be dumped into an executable file that will then show the message that has been detected and decoded.The specific implementation of the algorithm is attached in the appendix section of this report.2.5. Results and evaluationThe result of applying the steps described in the sections from 2.1 to 2.4, we obtain the message, getting the result showed in the next figureFigure 16 Result of non-coherent receiver detection3. Coherent receiverThe coherent receiver, also called synchronous receiver, implies certain degree of agreement or knowledge about parameters used in the transmitter side. For the case of the project, we have a signal of type DPSK, i.e. the code is contained in the variation of the phase of the signal.3.1. IQ Down-converterThe aim of this component is to decompose a complex signal in terms of its in-phase and qu adrature elements.To achieve this decomposition, we are going to perform the implementation using lookup-table oscillators, i.e. that for a given signal in-phase and quadrature components will be obtained by using the definitions given byFigure 17 IQ Downconverter (Tsimenidis, 2016)Upon these definitions, the components that we obtain could be represented in two separated graphs, each one of them representing a different component table.Figure 18 Sine and cosine table graphsAs for the index control of look-up table, we decide to use for loop to generate x2In and x2Qn, storing and transporting data to corresponding files as x2I.h and x2Q.h. These files will be used subsequent to perform the conversion of values.Figure 19 Index control flow (Tsimenidis, 2016)After understanding the principle, we defined all of variables and initialized them to zero inside the main, and select the appropriate value of some variables such as state_mf, coeffs_mf and N_mf.Same as the picture over, the or iginal data from bandpass output is also separated into two filters Matched Filter I and Matched Filter Q, and the coefficients of the filters are the same with the original one. The benefit of using the lookup-table oscillators (setting x2 into x2I and x2Q) is to decrease the time of simulation because of the lower required sampling rate. We can use via lookup table method to call them from x2I.h and x2Q.h, so that we can use it more efficiently in Matlab instead of shifting itself. And then, we multiplied x1 to x2In and x2Qn one by one by using another for loop and got x3I and x3Q.Besides,the code of matched filter had been given by tutors and got x4I and x4Q.x4I=fir(x3I,coeff_mf,state_mf_I,N_mf) //match filter I x4Q=fir(x3I,coeff_mf,state_mf_Q,N_mf) //match filter I Figure 20 Filter comparison (Tsimenidis, 2016)We monitored and recorded x3I and x3Q in PicoScope and print screen. The prosper of them spinning fixed at the origin point so three of these blows were selected to descr ibe this wave batter.Figure 21 Down-conversion x3I vs. x3Q counter clockwiseAfter this, we can visualize the outputs of each one of the filters, now we are going to bandage in the figure x4I and x4Q, obtainingFigure 22 Down-conversion x4I vs. x4Q counter clockwise3.2. Symbol synchronizationAfter IQ down-converter, the next stage is symbol synchronization. To achieve this, we create x5In and x5Qn and sent x4I, x4Q one sample at the time. The procedure that we should do in this section is similar to the one seen in the non-coherent detection, however we must consider two buffers instead of one, one for I and other for Q parts.The sum of the above established energies will correspond to the energy that can be seen as the total energy of the signal, which is similar to lab of the symbol synchronization for the non-coherent receiver.The corresponding calculations to obtain the signals after the symbol synchronization process are defined asThen, plotting the results obtained, we see the following figureFigure 23 x6I vs. x6QDue to synchronization problems, we threated the jitter that was causing these inconsistences using the averaging approach, as described in the followsFigure 24 Averaging approach to overcome the jitter (Tsimenidis, 2016)Figure 25 Code to solve the jitter3.3. Differential coherent demodulatorIn this section, we will implement a differential detector, also called a differential coherent demodulator.Figure 26 Principle of the differential detector (Tsimenidis, 2016)At first, we declare and initialize appropriately the required variables and define .In this differential detector, need to multiply ,1 symbol delay by .NN=1N=2N=3After this, we defined x6I_prev and x6Q_prev to deal with this problem and let x6I_prev and x6Q_prev denote the values of x6I and x6Q from the previous symbol. It is very important to initialize them to zero at the declaration because we know . (Tsimenidis, 2016)x6I_prev=x6Ix6Q_prev=x6QOn the same time,dI contains the first two terms which stand for the In-phase part and dQ which contains the last two terms which stand for the Quadrature part.Hard decision is then achieved by deciding whether the dI value is positive or negative, with a negative value indicating that a logic 1 was transmitted which might be used in the next step that is frame synchronization and message detection.Now we obtain the plot showi