Nesta tese apresentamos uma extensão da técnica de espalhamento hiper-Rayleigh (HRS) e sua aplicação para o estudo dos mecanismos que interferem na primeira hiperpolarizabilidade molecular (). Utilizamos um laser Nd:YAG, Q-switched e mode-locked como bombeio para excitar as amostras. Este laser emite pulsos de 100 ps modulados por uma envoltória de Q-switch. A saída é uma seqüência de pulsos com intensidades que acompanham a forma da envoltória. Usamos este trem de pulsos para excitar as amostras na medida de espalhamento hiper-Rayleigh, e um sistema de detecção com resolução temporal suficiente para resolver cada pulso independentemente. Esta modalidade de bombeio permitiu eliminar o controle mecânico da intensidade, o que reduziu o tempo necessário para a medida e melhorou a estabilidade nas condições experimentais. O método com trem de pulsos proporciona meios de identificar contribuições luminescentes e evitar valores superestimados para a primeira hiperpolarizabilidade. Realizamos testes medindo a molécula de paranitroanilina em vários solventes e verificamos muito boa reprodutibilidade dos valores da literatura. Comparamos os resultados medidos com valores calculados a partir do método de Hartree-Fock e corrigimos o engrandecimento por ressonância utilizando um modelo de dois níveis. A comparação entre valores teóricos e experimentais teve uma diferença média de 15%. Um estudo análogo para a molécula de dianilina não reproduziu os valores experimentais e atribuímos a falha à inaplicabilidade do modelo de dois níveis para medidas no regime ressonante. Também estudamos a primeira hiperpolarizabilidade nas porfirinas TDMImP e TPPS4, sob a forma base livre e formando complexos com Zn2+, Fe3+ e Mn3+. Para a TPPS4 estendemos o estudo para observar os efeitos da protonação na base livre e da formação de oxo dímeros na FeTPPS4 e as alterações causadas pela presença de micelas de CTAB. A comparação direta entre os resultados é dificultada em muitos casos pela diferença no engrandecimento por ressonância. Foi possível verificar que a presença de micelas tem o efeito de diminuir o valor de na H2TPPS4 pH 7. As medidas de HRS em ambiente ácido (pH 4) corroboram com a literatura, indicando que a ocorre desprotonação na presença de micelas. Um estudo teórico e experimental dos três isômeros do aminofenol permitiu analisar os efeitos da posição relativa dos grupos radicais e do comprimento da conjugação sobre a primeira hiperpolarizabilidade. Verificamos que a alteração no caráter doador/aceitador para diferentes posições dos grupos radicais tem influência maior no valor de do que o comprimento da conjugação. Utilizamos compostos com o ligante salen, com grupos laterais etano e DR1 e com ligantes H2, Cu2+, Ni2+ e VO2+, para estudar como os diferentes grupos e complexos refletem diferenças no valor de . Foi possível verificar que diferentemente da absorção linear e da seção de choque para dois fótons, o ligante com grupos radicais DR1 causam um aumento na primeira hiperpolarizabilidade que é muito maior do que a soma das contribuições individuais. Os complexos têm primeiras hiperpolarizabilidades maiores do que o ligante com H2 e a comparação entre os dois grupos com diferentes radicais mostra que existe uma correlação entre os aumentos causados por diferentes complexos. / This thesis reports an extension of the Hyper-Rayleigh scattering technique (HRS) and its application to study the mechanisms that contribute to the molecular first hyperpolarizabilities (). We use a Nd:YAG laser, Q-switched and mode-locked, as pumping beam to excite the samples. The laser delivers 100 ps pulses modulated by a Q-switch envelope, and the output is a pulse sequence which intensities follow the shape of the envelope. This pulse train is used to excite the samples in a Hyper-Rayleigh scattering experiment and the signal for each mode-lock pulse is detected independently. This modality of pumping allows the removal of the mechanical intensity control, therefore reducing measurement time and improved experimental stability. The method with pulse train also provides means to identify luminescent contributions and avoid overestimated values for the first hyperpolarizability. We performed test measurements with para-nitroaniline in several solvents and verified very good reproducibility of literature values. We also compared the measured and calculated values, obtained with the Hartree-Fock method and corrected for resonance enhancement with a two level model. The comparison between theoretical and experimental values results in an average difference of 15%. Similar studies for the dianiline molecule failed to reproduce experimental values and we attributed the failure to the inadequacy of the of the two-level model to correct resonance enhancement. We also studied the first hyperpolarizability of the TDMImP and TPPS4 porphyrins, in the free-base form and in complex with Zn2+, Fe3+ and Mn3+. For TPPS4 we extended the study to observe the protonação effects in the free-base and the formation of oxo dimmers in FeTPPS4 complexes. The comparison between results from different compounds is hindered in most cases by different contributions from resonance enhancement. However, it was possible to verify that the presence of micelles has the effect of reducing the value of on H2TPPS4 pH 7. The HRS measurements in acid environment (pH 4) corroborates with the literature, indicating that desprotonation occurs in the presence of CTAB micelles. A theoretical and experimental study of three aminofenol isomers allowed to verify the effects of the relative positions of radical groups and the conjugation length on the first hyperpolarizability. The results show that in this case the change in the donor/acceptor character for different positions of the radical groups is more important than the increase in one unit in the conjugation length. We also studied compounds with the salen ligant, observing the effects of different lateral groups (ethane and DR1) and different complexes (H2, Cu2+, Ni2+ and VO2+) on the value of . It was possible to verify that, differently than the linear absorption the two-photon cross section, the compounds with DR1 shows an increase in the first hyperpolarizability that is much larger than the sum of the individual contributions of DR1 groups. The metal complexes have larger first hyperpolarizabilities than the ligant and the enhancement produced by different complexes follows the same pattern for both radical groups. Even after the strong increase in produced by the DR1 group, the much weaker effect of the complexes is preserved and measurable.

In this thesis we use pulse shaping system to generate pulse train. Using empirical mode decomposition(EMD) and short-time Fourier transform(STFT) to analyze the signal of terahertz radiation. we use pulse shaping system to modulate the amplitude and phase of light which provide for pulse train generation. Compare with other method, first, our method will improve the stability of time delay control. Second this method is easier to control the time delay and number of pulse in the pulse train. In the past, people find the occur time of high frequency by observed the time domain of terahertz radiation directly, but if the occur time near the time of the peak power of terahertz radiation, we can¡¦t find out the occur time of high frequency. Using STFT can find out the relationship between intensity and time, but if the modes in signal have different width of frequency STFT have to use different time window to get the best frequency resolution and time resolution. However the time window with different width will have different frequency resolution, and the relationship between intensity and time will change with different frequency resolution, therefore using different frequency resolution will get different result, so we need a new signal analysis method. To solve this problem we use EMD to decompose different mode in the signal of terahertz radiation into different intrinsic mode function(IMF), and analyze the signal of terahertz by STFT to find the occur time of high frequency of terahertz radiation. Because the modes are separated in to different IMF, we can use STFT with the same time window. We expect this method applied to narrow-band frequency-tunable THz wave generation will be better.

Nesta tese apresentamos uma extensão da técnica de espalhamento hiper-Rayleigh (HRS) e sua aplicação para o estudo dos mecanismos que interferem na primeira hiperpolarizabilidade molecular (). Utilizamos um laser Nd:YAG, Q-switched e mode-locked como bombeio para excitar as amostras. Este laser emite pulsos de 100 ps modulados por uma envoltória de Q-switch. A saída é uma seqüência de pulsos com intensidades que acompanham a forma da envoltória. Usamos este trem de pulsos para excitar as amostras na medida de espalhamento hiper-Rayleigh, e um sistema de detecção com resolução temporal suficiente para resolver cada pulso independentemente. Esta modalidade de bombeio permitiu eliminar o controle mecânico da intensidade, o que reduziu o tempo necessário para a medida e melhorou a estabilidade nas condições experimentais. O método com trem de pulsos proporciona meios de identificar contribuições luminescentes e evitar valores superestimados para a primeira hiperpolarizabilidade. Realizamos testes medindo a molécula de paranitroanilina em vários solventes e verificamos muito boa reprodutibilidade dos valores da literatura. Comparamos os resultados medidos com valores calculados a partir do método de Hartree-Fock e corrigimos o engrandecimento por ressonância utilizando um modelo de dois níveis. A comparação entre valores teóricos e experimentais teve uma diferença média de 15%. Um estudo análogo para a molécula de dianilina não reproduziu os valores experimentais e atribuímos a falha à inaplicabilidade do modelo de dois níveis para medidas no regime ressonante. Também estudamos a primeira hiperpolarizabilidade nas porfirinas TDMImP e TPPS4, sob a forma base livre e formando complexos com Zn2+, Fe3+ e Mn3+. Para a TPPS4 estendemos o estudo para observar os efeitos da protonação na base livre e da formação de oxo dímeros na FeTPPS4 e as alterações causadas pela presença de micelas de CTAB. A comparação direta entre os resultados é dificultada em muitos casos pela diferença no engrandecimento por ressonância. Foi possível verificar que a presença de micelas tem o efeito de diminuir o valor de na H2TPPS4 pH 7. As medidas de HRS em ambiente ácido (pH 4) corroboram com a literatura, indicando que a ocorre desprotonação na presença de micelas. Um estudo teórico e experimental dos três isômeros do aminofenol permitiu analisar os efeitos da posição relativa dos grupos radicais e do comprimento da conjugação sobre a primeira hiperpolarizabilidade. Verificamos que a alteração no caráter doador/aceitador para diferentes posições dos grupos radicais tem influência maior no valor de do que o comprimento da conjugação. Utilizamos compostos com o ligante salen, com grupos laterais etano e DR1 e com ligantes H2, Cu2+, Ni2+ e VO2+, para estudar como os diferentes grupos e complexos refletem diferenças no valor de . Foi possível verificar que diferentemente da absorção linear e da seção de choque para dois fótons, o ligante com grupos radicais DR1 causam um aumento na primeira hiperpolarizabilidade que é muito maior do que a soma das contribuições individuais. Os complexos têm primeiras hiperpolarizabilidades maiores do que o ligante com H2 e a comparação entre os dois grupos com diferentes radicais mostra que existe uma correlação entre os aumentos causados por diferentes complexos. / This thesis reports an extension of the Hyper-Rayleigh scattering technique (HRS) and its application to study the mechanisms that contribute to the molecular first hyperpolarizabilities (). We use a Nd:YAG laser, Q-switched and mode-locked, as pumping beam to excite the samples. The laser delivers 100 ps pulses modulated by a Q-switch envelope, and the output is a pulse sequence which intensities follow the shape of the envelope. This pulse train is used to excite the samples in a Hyper-Rayleigh scattering experiment and the signal for each mode-lock pulse is detected independently. This modality of pumping allows the removal of the mechanical intensity control, therefore reducing measurement time and improved experimental stability. The method with pulse train also provides means to identify luminescent contributions and avoid overestimated values for the first hyperpolarizability. We performed test measurements with para-nitroaniline in several solvents and verified very good reproducibility of literature values. We also compared the measured and calculated values, obtained with the Hartree-Fock method and corrected for resonance enhancement with a two level model. The comparison between theoretical and experimental values results in an average difference of 15%. Similar studies for the dianiline molecule failed to reproduce experimental values and we attributed the failure to the inadequacy of the of the two-level model to correct resonance enhancement. We also studied the first hyperpolarizability of the TDMImP and TPPS4 porphyrins, in the free-base form and in complex with Zn2+, Fe3+ and Mn3+. For TPPS4 we extended the study to observe the protonação effects in the free-base and the formation of oxo dimmers in FeTPPS4 complexes. The comparison between results from different compounds is hindered in most cases by different contributions from resonance enhancement. However, it was possible to verify that the presence of micelles has the effect of reducing the value of on H2TPPS4 pH 7. The HRS measurements in acid environment (pH 4) corroborates with the literature, indicating that desprotonation occurs in the presence of CTAB micelles. A theoretical and experimental study of three aminofenol isomers allowed to verify the effects of the relative positions of radical groups and the conjugation length on the first hyperpolarizability. The results show that in this case the change in the donor/acceptor character for different positions of the radical groups is more important than the increase in one unit in the conjugation length. We also studied compounds with the salen ligant, observing the effects of different lateral groups (ethane and DR1) and different complexes (H2, Cu2+, Ni2+ and VO2+) on the value of . It was possible to verify that, differently than the linear absorption the two-photon cross section, the compounds with DR1 shows an increase in the first hyperpolarizability that is much larger than the sum of the individual contributions of DR1 groups. The metal complexes have larger first hyperpolarizabilities than the ligant and the enhancement produced by different complexes follows the same pattern for both radical groups. Even after the strong increase in produced by the DR1 group, the much weaker effect of the complexes is preserved and measurable.

Current cochlear implant systems use fast pulsatile stimulation to deliver the temporal modulations of speech and to, potentially, improve the neural representation of such modulations by restoring the independence of neural firing. The realization of these benefits may vary with other pulse rate-dependent temporal interactions that occur at the neural membrane, e.g., per(i)stimulatory adaptation and its post-stimulatory or forward masking effects. This study attempted to characterize adaptation and recovery of the electrically evoked compound action potential (ECAP) using probe pulses delivered within and following brief (100 ms) high-rate masker (1800 pps) pulse trains at various current levels in adults and children. With this stimulus paradigm, the ECAP amplitude typically achieved a steady state during the course of pulse train stimulation. The ECAP amplitude at steady state was, on average, a similar proportion (50-70%) of the amplitude at onset for various stimulus levels and in both age groups. However, long-term adaptation effects, evidenced by the decrease in onset ECAP amplitude, were greater in adults particularly at lower levels in the ECAP dynamic range. Instances of alternation in ECAP amplitude were seen at stimulus levels that were higher in the ECAP dynamic range. The forward masking effects of pulse train stimulation were quantified by the ECAP amplitude in response to a subsequent probe pulse normalized by the response to the same pulse presented alone. Pulse train forward masking increased with the level of the masker pulse train and decreased with the level of the probe stimulus. The recovery of the ECAP for probes that were lower in level than the masker pulse train was incomplete at 600 ms after masker offset, consistent with long-term cumulative effects observed in the response to the probe alone. Masker pulse trains that are lower in level than the probe pulse produced proportionally small decrements in the ECAP amplitude with complete recovery within 250 ms of pulse train offset particularly in adults. ECAP recovery of a probe preceded by a masker pulse train of equal level followed a monotonic or non-monotonic pattern consistent with a hypothesis of both adaptation and facilitation occurring with pulse train stimulation. The various patterns of recovery may attest to the occurrence of more than a single process in the same subset of nerve fibers or in different fibers. We hypothesize that the variations in the recovery patterns may be attributable to individual differences in the status of the auditory nerve and possibly, the variations in temporal interactions across the spatial domain at different stimulus levels. Finally, the probe-evoked ECAP amplitude at steady state in children and briefly, e.g., 20 ms, after pulse train offset in both age groups could be predicted by the ECAP amplitude in response to the same probe pulse when preceded at a brief interval (1.2 or 2 ms) by a single masker pulse of the same level as the masker pulse train. Further investigation may reveal if the observed differences in neural responsiveness to pulsatile stimulation, among individuals account for differences in psychophysical measures, including speech perception and whether there may be an "optimal" neural output that could be evoked by an individually "optimized" signal.

No description available.

To advance the understanding of electric hearing, from both a theoretical and practical perspective, the present study employs an engineering approach to examine whether a fundamental stochastic link exists between neural stimulation and perception. Through the use of custom-developed psychophysics software, temporal gap-detection experiments were carried out and compared with simulation results of a theoretical model. The results are informative, and the suggested modeling principles may be a step forward to a clearer understanding of how the hearing system perceives temporal stimuli. To enable the implementation of psycho-electric experiments involving cochlear implants, a software framework was developed for Matlab version 6.5, called the Psychoacoustics Toolbox, which can present stimuli either acoustically or (for interfacing with cochlear implants) using Cochlear Ltd. hardware. This toolbox facilitates easy setup of experiments based on extensible markup language (XML) templates, and allows for both adaptivestaircase procedures and presentation of a fixed set of stimuli to a participant. Multi-track interleaving of stimuli is also supported, as put forward by Jesteadt (1980), to allow for capturing of subjective responses (such as loudness perception). As part of this research, experiments were performed with three subjects, with a total of four cochlear implants. For the temporal gap-detection experiments, the rate of electrical stimulation varied over a range from 100 to 2700 pulses per second; both periodic stimulus sequences and stimuli reflecting a dead-time-modified Poisson process were used. Also, three spatially distinct stimulation sites were used with each implant to allow comparison among basal, central and apical cochlear responses. A biologically plausible psychophysical model (in contrast with a phenomenological one) was developed for predicting temporal gap-detection thresholds in electric hearing. The model was applied to both periodic and Poisson stimuli, but can easily be used with other kinds of stimuli. For comparison with experimental results, model predictions were made over the same range of stimulus rates. As a starting point, the model takes the neural stimuli, runs them through a neural filter, and then draws statistical interspike-interval (ISI) distribution data from the generated spikes. From the ISI statistics, psychometric curves can be calculated using the principles of Green and Swets (1966), from which predictions can be made for threshold measurements based on the percentage-correct mark for the specific experimental setup. With a model in place, simulations were executed to compare the model results with experimental measurements. In addition to the simulations, mathematical equations for the periodic types of stimuli were derived, given that numerical calculations could be made with higher computational e ciency for this kind of stimulus. These equations allowed for an investigation into the implications of varying the values of different neuron-model parameters. Clear similarities were found between the shapes of gap-threshold curves for experimental and modeled data, and qualitative links have been identified between model parameters and features recognized in threshold curves. For periodic stimuli, quantitative predictions of gap thresholds are close to experimental ones, although measured values cover a larger range. The results of experimental measurements using Poisson stimuli are generally somewhat larger than model predictions, although the shapes of the curves show resemblance. A possible explanation is that participants may find decision tasks involving Poisson stimuli, as opposed to periodic stimuli, confusing. Overall, model predictions and experimental results show close correspondence, suggesting Department of Electrical, Electronic and Computer Engineering. University of Pretoria. ii that the principles underlying the model are fundamentally correct. Copyright 2007, University of Pretoria. All rights reserved. The copyright in this work vests in the University of Pretoria. No part of this work may be reproduced or transmitted in any form or by any means, without the prior written permission of the University of Pretoria. Please cite as follows: Geldenhuys, TA 2007, Temporal gap detection in electric hearing : modelling and experiments, MEng dissertation, University of Pretoria, Pretoria, viewed yymmdd < http://upetd.up.ac.za/thesis/available/etd-02232012-131459 / > E1091/gm / Dissertation (MEng)--University of Pretoria, 2012. / Electrical, Electronic and Computer Engineering / Unrestricted

No description available.

In this work, the interference sensitivity of an FMCW radar has been evaluated by studying the impact on a simulated detection chain. A commercially available FMCW radar was first characterized and its properties then laid the foundation for a simulation model implemented in Matlab. Different interference methods have been studied and a selection was made based on the results of previous research. One method aims to inject a sufficiently large amount of energy in the form of pulsed noise into the receiver. The second method aims to deceive the radar into seeing targets that do not actually exist by repeating the transmitted signal and thus giving the radar a false picture of its surroundings. The results show that if it is possible to synchronize with the transmitted signal then repeater jamming can be effective in misleading the radar. In one scenario the false target even succeeded in hiding the real target by exploiting the Cell-Averaging CFAR detection algorithm. The results suggests that without some smart countermeasures the radar has no way of distinguishing a coherent repeater signal, but just how successful the repeater is in creating a deceptive environment is highly dependent on the detection algorithm used. Pulsed noise also managed to disrupt the radar and with a sufficiently high pulse repetition frequency the detector could not find any targets despite a simulated object in front of the radar. On the other hand, a rather significant effective radiated power level was required for the pulse train to achieve any meaningful effect on the radar, which may be due to an undersampled signal in the simulation. It is therefore difficult based on this work to draw any conclusions about how suitable pulsed noise is in a non-simulated interference context and what parameter values to use.