Le futur collisionneur du CERN (le LHC) possède un fantastique potentiel de découverte à condition d'avoir une prédiction quantitative de la QCD. Pour ce faire, il est nécessaire d'effectuer des calculs dans l'approximation NLO de manière à réduire la dépendance de la section efficace en fonction des échelles non physiques. Pour obtenir des résultats dans cette approximation, il faut calculer les sections efficaces des sous-processus partoniques contribuant à la réaction étudiée à l'ordre le plus bas ainsi que les corrections virtuelles (une boucle) et réelles. Le calcul des corrections virtuelles reste très compliqué si le nombre de particules externes est supérieur à quatre ou si les particules externes (internes) sont massives.<br />Dans cette thèse est proposée une méthode automatique pour effectuer les calculs à une boucle et à cinq pattes, et qui peut être généralisée aux cas de particules massives.<br />Dans une première partie, nous décrirons divers outils et méthodes nécessaires à de tels calculs. Nous les appliquerons ensuite au calcul de la réaction (gluon + gluon -> photon + photon + gluon), qui intéresse les expérimentateurs des expériences ATLAS et CMS comme bruit de fond à la recherche du Higgs, notamment pour décrire correctement la queue de la distribution transverse du boson de Higgs. Sera alors présenté le résultat explicite de cette amplitude pour chaque configuration d'hélicités sous une forme compacte et une représentation clairement invariante de jauge. Nous terminerons par une étude phénoménologique de cette réaction.

Le contexte de cette thèse est la théorie de l'élasticité non linéaire, appelée également "élasticité finie". On y présente des résultats concernant la propagation d'ondes d'amplitude finie dans des matériaux élastiques non linéaires soumis à une grande déformation statique homogène. Bien que les matériaux considérés soient isotropes, lors de la propagation d'ondes un comportement anisotrope dû à la déformation statique se manifeste. Après un rappel des équations de base de l'élasticité non linéaire (Chapitre 1), on considère tout d'abord la classe générale des matériaux incompressibles. Pour ces matériaux, on montre que la propagation d'ondes transversales polarisées linéairement est possible pour des choix appropriés des directions de polarisation et de propagation. De plus, on propose des généralisations des modèles classiques de "Mooney-Rivlin" et "néo-Hookéen" qui conduisent à de nouvelles solutions. Bien que le contexte soit tri-dimensionnel, il s'avère que toutes ces ondes sont régies par des équations d'ondes scalaires non linéaires uni-dimensionelles. Dans le cas de solutions du type ondes simples, on met en évidence une propriété remarquable du flux et de la densité d'énergie. Dans les Chapitres 3 et 4, on se limite à un modèle particulier de matériaux compressibles appelé "modèle restreint de Blatz-Ko", qui est une version compressible du modèle néo-Hookéen. En milieu infini (Chapitre 3), on montre que des ondes transversales polarisées linéairement, faisant intervenir deux variables spatiales, peuvent se propager. Bien que la théorie soit non linéaire, le champ de déplacement de ces ondes est régi par une version anisotrope de l'équation d'onde bi-dimensionnelle classique. En particulier, on présente des solutions à symétrie "cylindrique elliptique" analogues aux ondes cylindriques. Comme cas particulier, on obtient aussi des ondes planes inhomogènes atténuées à la fois dans l'espace et dans le temps. De plus, on montre que diverses superpositions appropriées de solutions sont possibles. Dans chaque cas, on étudie les propriétés du flux et de la densité d'énergie. En particulier, dans le cas de superpositions il s'avère que des termes d'interactions interviennent dans les expressions de la densité et du flux d'énergie. Finalement (Chapitre 4), on présente une solution exacte qui constitue une généralisation non linéaire de l'onde de Love classique. On considère ici un espace semi-infini, appelé "substrat" recouvert par une couche. Le substrat et la couche sont constitués de deux matériaux restreints de Blatz-Ko pré-déformés. L'onde non linéaire de Love est constituée d'un mouvement non atténué dans la couche et d'une onde plane inhomogène dans le substrat, choisies de manière à satisfaire aux conditions aux limites. La relation de dispersion qui en résulte est analysée en détail. On présente de plus des propriétés générales du flux et de la densité d'énergie dans le substrat et dans la couche. The context of this thesis is the non linear elasticity theory, also called "finite elasticity". Results are obtained for finite-amplitude waves in non linear elastic materials which are first subjected to a large homogeneous static deformation. Although the materials are assumed to be isotropic, anisotropic behaviour for wave propagation is induced by the static deformation. After recalling the basic equations of the non linear elasticity theory (Chapter 1), we first consider general incompressible materials. For such materials, linearly polarized transverse plane waves solutions are obtained for adequate choices of the polarization and propagation directions (Chapter 2). Also, extensions of the classical Mooney-Rivlin and neo-Hookean models are introduced, for which more solutions are obtained. Although we use the full three dimensional elasticity theory, it turns out that all these waves are governed by scalar one-dimensional non linear wave equations. In the case of simple wave solutions of these equations, a remarkable property of the energy flux and energy density is exhibited. In Chapter 3 and 4, a special model of compressible material is considered: the special Blatz-Ko model, which is a compressible counterpart of the incompressible neo-Hookean model. In unbounded media (Chapter 3), linearly polarized two-dimensional transverse waves are obtained. Although the theory is non linear, the displacement field of these waves is governed by a linear equation which may be seen as an anisotropic version of the classical two-dimensional wave equation. In particular, solutions analogous to cylindrical waves, but with an "elliptic cylindrical symmetry" are presented. Special solutions representing "damped inhomogeneous plane waves" are also derived: such waves are attenuated both in space and time. Moreover, various appropriate superpositions of solutions are shown to be possible. In each case, the properties of the energy density and the energy flux are investigated. In particular, in the case of superpositions, it is seen that interaction terms enter the expressions for the energy density and the energy flux. Finally (Chapter 4), an exact finite-amplitude Love wave solution is presented. Here, an half-space, called "substrate", is assumed to be covered by a layer, both made of different prestrained special Blatz-Ko materials. The Love surface wave solution consists of an unattenuated wave motion in the layer and an inhomogeneous plane wave in the substrate, which are combined to satisfy the exact boundary conditions. A dispersion relation is obtained and analysed. General properties of the energy flux and the energy density in the substrate and the layer are exhibited.

The speech signal is inherently characterized by its variations in time, which get reflected as variations in frequency. The specto temporal changes are due to changes in vocaltract, intonation, co-articulation and successive articulation of different phonetic sounds. In this thesis we are looking for improving the speech recognition performance through better feature parameters using a non-stationary model of speech. One effective means of modeling a general non-stationary signal is using the AM-FM model. AM-FM model can be extended to speech through a sub-band analysis, which can be mimic the auditory analysis. In this thesis, we explore new methods for estimating AM and FM parameters based on the non-uniform samples of the signal. The non-uniform sample approach along with adaptive window estimation provides for important advantage because of multi-resolution analysis. We develop several new methods based on ZC intervals, local extrema intervals and signal derivative at ZC’s as different sample measures of the signal and explore their effectiveness for instantaneous frequency (IF) and instantaneous envelope (IE) estimation. To deal with speech signal for automatic speech recognition, we explore the use of auditory motivated spectro temporal information through the use of an auditory filter bank and signal parameters (or features) are derived from the instantaneous energy in each band using the non-linear energy operator over a larger window length. The temporal correlation present in the signal is exploited by using DCT and keeping the lower few coefficients of DCT to keep the trend in the energy in each band. The DCT coefficients from different frequency bands are concatenated together, and a further spectral decorrelation is achieved through KLT (Karhunen-Loeve Transform) of the concatenated feature vector. The changes in the vocaltract are well captured by the change in the formant structure and to emphasize these details for ASR we have defined a temporal formant by using the AM-FM decomposition of sub-band speech. A uniform wideband non-overlaping filters are used for sub-band decomposition. The temporal formant is defined using the AM-FM parameters of each subband signal. The temporal evolution of a formant is represented by the lower order DCT coefficients of the temporal formant in each band and its use for ASR is explored. To address the robustness of ASR performance to environmental noisy conditions, we have used a hybrid approach of enhancing the speech signal using statistical models of the speech and noise. Use of GMM for statistical speech enhancement has been shown to be effective. It is found that the spectro-temporal features derived from enhanced speech provide further improvement to ASR performance.

The cooperative relaying scheme is a promising technique for increasing the capacity and reliability of wireless communication. Even though extensive research has performed in information theoretical aspect, there are still many unresolved practical problems of cooperative relaying system. This dissertation analyzes the performance of cooperative decode-and-forward (DF) relaying systems in the presence of multiple interferers and improve network throughput for these systems. We propose and summarize various systems in the view of network topology, transmission structure, and slot allocation. We present closed-form expressions for the end-to-end outage probability, average symbol-error-probability, average packet-error-probability, and network throughput of the proposed systems. This dissertation shows that the robustness of the destination against interference is more important than robustness of the relay against interference from an interference management perspective, and increasing the number of branches yields better outage and error performance improvements against shadowing than increasing the number of hops. In cellular networks, the cooperative diversity systems can outperform the dual-Rx antenna system, but only when the relay is located in a relatively small portion of the total cell area with respect the the destination mobile terminal. The results also show that since the effective regions of the uplink and the downlink do not overlap, different relays should be utilized for cell sectorization in the uplink and the downlink. Finally, the proposed variable-slot selection DF scheme can reduce the system complexity and make the maximum throughput point in the low and moderate signal-to-interference-plus-noise ratio region.

There is a growing demand for the high quality TV programs such as High Definition TV (HDTV). The CATV network is often a suitable solution to address this demand using a CATV modem delivering high data rate digital signals in a cost effective manner, thereby, utilizing a complex digital modulation scheme is inevitable. Exploiting complex modulation schemes, entails a more sophisticated modulator and distribution system with much tighter tolerances. However, there are always distortions introduced to the modulated signal in the modulator degrading signal quality.<p> In this research, the effect of distortions introduced by the RF band pass filter in the modulator will be considered which cause degradations on the quality of the output Quadrature Amplitude Modulated (QAM) signal. Since the RF filter's amplitude/group delay distortions are not symmetrical in the frequency domain, once translated into the base band they have a complex effect on the QAM signal. Using Matlab, the degradation effects of these distortions on the QAM signal such as Bit Error Rate (BER) is investigated.<p> In order to compensate for the effects of the RF filter distortions, two different methods are proposed. In the first method, a complex base band compensation filter is placed after the pulse shaping filter (SRRC). The coefficients of this complex filter are determined using an optimization algorithm developed during this research. The second approach, uses a pre-equalizer in the form of a Feed Forward FIR structure placed before the pulse shaping filter (SRRC). The coefficients of this pre-equalizer are determined using the equalization algorithm employed in a test receiver, with its tap weights generating the inverse response of the RF filter. The compensation of RF filter distortions in base band, in turn, improves the QAM signal parameters such as Modulation Error Ratio (MER). Finally, the MER of the modulated QAM signal before and after the base band compensation is compared between the two methods, showing a significant enhancement in the RF modulator performance.

The structure of 11S cruciferin has been solved; however, how the individual subunits contribute to its physico-chemical and functional properties are not well known. The cruciferin isoforms in Arabidopsis thaliana, CRUA, CRUB, and CRUC, were investigated with respect to their molecular structures and the relationship of structural features to the physico-chemical and functional properties of cruciferin using homology modeling and various analytical techniques. Comparison of these models revealed that hydrophobicity and electrostatic potential distribution on the surface of the CRUC homotrimer had more favorable interfacial, solubility, and thermal properties than those of CRUA or CRUB. Flavor binding and pepsin digestion were associated with hypervariable regions (HVRs) and center core regions, respectively, moreso for CRUA and CRUB homotrimers than for CRUC. Chemical imaging of a single cell area in wild type (WT) and double-knockout seeds (CRUAbc, CRUaBc, and CRUabC) using synchrotron FT-IR microscopy (amide I band, 1650 cm-1, νC=O) showed that seed storage proteins were concentrated in the cell center and protein storage vacuoles, whereas lipids were closer to the cell wall. Secondary structure components of proteins of double-knockout lines did not show major differences. Changes in protein secondary structure components of pepsin-treated CRUabC (CRUC) mutant were minimal, indicating low enzyme accessibility. A three-step chromatographic procedure allowed isolation of the hexameric form of cruciferin with high purity (>95%). Fourier transform infrared (FT-IR) and circular dichroism (CD) spectroscopic analysis of the secondary structure of these proteins revealed cruciferins were folded into higher order secondary structures; 44−50% β-sheets and 7−9% α-helices. The relative subunit ratio was approximately 1:3:6 (CRUA:CRUB:CRUC) in the WT cruciferin. The Tm values of purified cruciferin at pH 7.4 (μ = 0.0) were in the order of WT = CRUA = CRUB < CRUC. The order of surface hydrophobicity as determined by ANS (1-anilinonaphthalene-8-sulfonate) probe binding was CRUA > CRUB = WT >> CRUC. Intrinsic fluorescence studies revealed a compact molecular structure for the CRUC homohexamer compared to the CRUA and CRUB homohexamers. The order of emulsion forming abilities was CRUA = CRUB > WT > CRUC (no emulsion formation) and the order of heat-induced network structure strength was WT > CRUA = CRUB > CRUC (no gel formation). The inability of CRUC to form gels or emulsions may be attributed to its low surface hydrophobicity and molecular compactness. At pH 2.0, CRUC hexamers dissociated into trimers which allowed the formation of an O/W emulsion and heat-induced network structures. Solubility of cruciferin as a function of pH at low ionic strength gave two minima around pH 4 and 7.4 yielding a “W” shape solubility profile deviating from the typical “U” or “V” shape solubility profile of other 11S globulins. The high ionic strength (μ = 0.5) was not favorable for emulsification, heat-induced gel formation, or solubilization for all cruciferins. Furthermore, the CRUA and CRUB homohexamers exhibited rapid pepsinolysis, while the CRUC homohexamer and WT heterohexamer were digested more slowly. Although fairly well conserved regions were found in the primary structure of these three cruciferin subunits, differences were found in the hypervariable regions and extended loop regions resulting in slight differences in 3D structures and interactions that occur during association to form superstructures, such as hexamers. These differences were reflected in the physico-chemical and techno-functional properties of hexamers and trimers composed of each subunit. In silico predictions for certain functionalities were highly correlated with empirical data from laboratory experiments.

An electrostatic actuator driven by conventional voltage control and charge control requires high actuation voltage and suffers from the pull-in phenomenon that limits its operation range, much less than its entire gap. To provide effective solutions to these problems, we present complete analytical and numerical models of various electrostatic actuators coupled with resonant drive circuits that are able to drive electrostatic actuators at much lower input voltage than that of conventional actuation methods and to extend their operation range beyond their conventional pull-in points in the presence of high parasitic capacitance. Moreover, in order to validate the analytical and numerical models of various electrostatic actuators coupled with the resonant drive circuits, we perform the experiment on the microplate and the micromirror coupled with the resonant drive circuit. For instance, using a high voltage amplifier, we manage to rotate the micromirror with sidewall electrodes by 6 ° at 180 V. However, using the resonant drive circuit, we are able to rotate the same micromirror by 6 ° at much lower input voltage, 8.5 V. In addition, the presented work also facilitates the stability analysis of electrostatic actuators coupled with the resonant drive circuits and provides how the effect of the parasitic capacitance can be minimized. For example, the resonant drive circuit placed within a positive feedback loop of a variable gain amplifier is able to extend the operation range much further even in the presence of very high parasitic capacitance. The resonant drive circuit with the proposed feedback controllers is also able to minimize the detrimental effects of the parasitic capacitance and to displace a parallel-plate actuator over its entire gap without the saddle-node bifurcation. Finally, we present a new displacement measurement method of electrostatic actuators coupled with the resonant drive circuits by sensing the phase delay of an actuation voltage with respect to an input voltage. This new measurement method allows us to easily implement feedback control into existent systems employing an electrostatic actuator without any modification or alteration to the electrostatic actuator itself. Hence, this research work presents the feasibility of electrostatic actuators coupled with the resonant drive circuit in various industrial and medical applications, in which the advantages of miniaturization, low supply voltage, and low power consumption are greatly appreciated.

There is a growing demand for the high quality TV programs such as High Definition TV (HDTV). The CATV network is often a suitable solution to address this demand using a CATV modem delivering high data rate digital signals in a cost effective manner, thereby, utilizing a complex digital modulation scheme is inevitable. Exploiting complex modulation schemes, entails a more sophisticated modulator and distribution system with much tighter tolerances. However, there are always distortions introduced to the modulated signal in the modulator degrading signal quality.<p> In this research, the effect of distortions introduced by the RF band pass filter in the modulator will be considered which cause degradations on the quality of the output Quadrature Amplitude Modulated (QAM) signal. Since the RF filter's amplitude/group delay distortions are not symmetrical in the frequency domain, once translated into the base band they have a complex effect on the QAM signal. Using Matlab, the degradation effects of these distortions on the QAM signal such as Bit Error Rate (BER) is investigated.<p> In order to compensate for the effects of the RF filter distortions, two different methods are proposed. In the first method, a complex base band compensation filter is placed after the pulse shaping filter (SRRC). The coefficients of this complex filter are determined using an optimization algorithm developed during this research. The second approach, uses a pre-equalizer in the form of a Feed Forward FIR structure placed before the pulse shaping filter (SRRC). The coefficients of this pre-equalizer are determined using the equalization algorithm employed in a test receiver, with its tap weights generating the inverse response of the RF filter. The compensation of RF filter distortions in base band, in turn, improves the QAM signal parameters such as Modulation Error Ratio (MER). Finally, the MER of the modulated QAM signal before and after the base band compensation is compared between the two methods, showing a significant enhancement in the RF modulator performance.

Timing offsets result from the use of real clocks that are non-ideal in sampling intervals. These offsets also known as timing jitter were shown to degrade the performance of the two forms of UWB systems impulse radio and orthogonal frequency division multiplexing (OFDM)-based UWB. It was shown that for impulse radio, timing jitter distorts the correlation property of the transmitted signal and the resulting performance loss is proportional to the root-mean-square (RMS) value of the timing jitter. For the OFDM-based UWB, timing jitter introduced inter-channel interference (ICI) and the performance loss was dependent on the product of the bandwidth and the RMS of the timing jitter. A number of techniques were proposed for mitigating the performance degradation in each form of UWB. Specifically, for impulse radio, the methods of pulse shaping and sample averaging were provided, whereas for OFDM-based UWB, oversampling and adaptive modulation were given. Through analysis and simulation, it was shown that substantial gain in signal power-to-noise ratio can be achieved using these jitter-reduction methods.

This thesis reports the development of various high performance readout and control electronics for implementing angular rate sensing systems using MEMS gyroscopes developed at METU. First, three systems with open loop sensing mechanisms are implemented, where each system has a different drive-mode automatic gain controlled (AGC) self-oscillation loop approach, including (i) square wave driving signal with DC off-set named as OLS_SquD, (ii) sinusoidal driving signal with DC off-set named as OLS_SineD, and iii) off-resonance driving signal named as OLS_OffD. A forth system is also constructed with a closed loop sensing mechanism where the drive mode automatic gain controlled (AGC) self-oscillation loop approach with square wave driving signal with DC off-set named as CLS_SquD. Sense and drive mode electronics employ transimpedance and transresistance amplifiers as readout electronics, respectively. Each of the systems is implemented with commercial discrete components on a dedicated PCB. Then, the angular rate sensing systems are tested with SOG (Silicon-on-Glass) gyroscopes that are adjusted to have two different mechanical bandwidths, more specially 100 Hz and 30 Hz. Test results of all of these cases verify the high performance of the systems. For the 100 Hz bandwidth, the OLS_SquD system shows a bias instability of 4.67 &amp / #730 / /hr, an angle random walk (ARW) 0.080 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 22.6 mV/(&amp / #730 / /sec). For the 30 Hz bandwidth, the OLS_SquD system shows a bias instability of 5.12 &amp / #730 / /hr, an ARW better than 0.017 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 49.8 mV/(&amp / #730 / /sec). For the 100 Hz bandwidth, the OLS_SineD system shows a bias instability of 6.92 &amp / #730 / /hr, an ARW of 0.049 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 17.97 mV/(&amp / #730 / /sec). For the 30 Hz bandwidth, the OLS_SineD system shows a bias instability of 4.51 &amp / #730 / /hr, an ARW of 0.030 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 43.24 mV/(&amp / #730 / /sec). For the 100 Hz bandwidth, the OLS_OffD system shows a bias instability of 8.43 &amp / #730 / /hr, an ARW of 0.086 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 20.97 mV/(&amp / #730 / /sec). For the 30 Hz bandwidth, the OLS_OffD system shows a bias instability of 5.72 &amp / #730 / /hr, an ARW of 0.046 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 47.26 mV/(&amp / #730 / /sec). For the 100 Hz bandwidth, the CLS_SquD system shows a bias instability of 6.32 &amp / #730 / /hr, an ARW of 0.055 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 1.79 mV/(&amp / #730 / /sec). For the 30 Hz bandwidth, the CLS_SquD system shows a bias instability of 5.42 &amp / #730 / /hr, an ARW of 0.057 &amp / #730 / /&amp / #8730 / hr, and a scale factor of 1.98 mV/(&amp / #730 / /sec). For the 100 Hz bandwidth, the R2 nonlinearities of the measured scale factors of all systems are between 0.0001% and 0.0003% in the &plusmn / 100 &amp / #730 / /sec measurement range, while for the 30 Hz bandwidth the R2 nonlinearities are between 0.0002% and 0.0062% in the &plusmn / 80&amp / #730 / /sec measurement range. These performance results are the best results obtained at METU, satisfying the tactical-grade performances, and the measured bias instabilities and ARWs are comparable to the best results in the literature for a silicon micromachined vibratory gyroscope.