Neste trabalho foi desenvolvido um Espectrômetro de Correlação Angular Gama- Gama Perturbada Diferencial em Tempo (CAP) constituído por seis detectores cintiladores de BaF2, para realização de medidas de interações hiperfinas (campo hiperfino magnético e gradiente de campo elétrico) em diversos materiais e propiciar estudos na área da física da matéria condensada. O espectrômetro desenvolvido possui um sistema de aquisição não convencional em comparação aos demais equipamentos destinados a medidas de CAP. Ao invés do tradicional Analisador Multicanal (MCA), este espectrômetro utiliza um sistema de aquisição de dados constituído, basicamente, por um Conversor Analógico Digital (ADC) rápido, uma placa digital (I/O) convencional e um roteador construído no laboratório de Interações Hiperfinas (LIH) do IPEN. Este versátil e eficiente sistema, controlado por um software também criado no LIH em LabVIEW, permite a geração simultânea de 30 espectros de coincidências γ - γ atrasadas, número superior em comparação aos 12 espectros do antigo espectrômetro de quatro detectores. Além de medidas de linearidade, resolução em tempo e tempo morto, o funcionamento e o desempenho do espectrômetro foram comprovados através de medidas de CAP utilizando os núcleos de prova 111In -> 111Cd e 181Hf -> 181Ta, cujos resultados são bem conhecidos da literatura. Foram feitas medidas de interação quadrupolar do 181Ta em háfnio metálico e do 111Cd em cádmio metálico, e de campo hiperfino magnético do 111Cd e do 181Ta em níquel. Os resultados destas medidas se mostraram em concordância com a literatura. Adicionalmente foram realizadas medidas inéditas de interações hiperfinas magnéticas no composto intermetálico LaMnSi2 utilizando os núcleos de prova 111Cd e 140Ce. As medidas foram realizadas na faixa de temperatura de 10 K a 400K. No caso das medidas utilizando a sonda 111In -> 111Cd, os resultados mostram uma variação do campo magnético com a temperatura que segue a função de Brillouin. Já no caso das medidas com o núcleo de prova 140La -> 140Ce, o resultado apresentou um comportamento anômalo do campo hiperfino em função de temperatura. Os resultados evidenciam uma forte hibridização da banda 4f do Ce com a banda 3d do Mn, fato verificado e estudado em trabalhos anteriores com compostos semelhantes. / In this work a Perturbed gama-gama Angular Correlation (PAC) spectrometer was constructed consisting of six BaF2 scintillator detectors to perform measurements of hyperfine interactions (magnetic hyperfine field and electric field gradient) in different materials to study condensed matter physics. The spectrometer developed has an unconventional acquisition system compared to other equipment for PAC measurements. Instead of a traditional multichannel analyzer (MCA), the spectrometer utilizes a data acquisition system consisting of basically a fast analog to digital converter (ADC), a conventional digital card (I/O) and a router constructed in the hyperfine interactions laboratory (LIH) of IPEN. This versatile and efficient system, controlled by software, also developed in the LIH using LabVIEW, allows simultaneous generation of 30 delayed γ - γ coincidence spectra compared to 12 spectra in the old 4 detector spectrometer in our laboratory. In addition to the tests of system linearity, time resolution and dead time, the operational performance of this spectrometer was demonstrated by PAC measurements using 111In -> 111Cd and 181Hf -> 181Ta nuclear probes, for which the results are well known from the literature. The quadrupole interaction of 181Ta in metallic hafnium, and 111Cd in metallic cadmium, and magnetic hyperfine field of 111Cd in nickel, were measured and the results are in agreement with the literature. Additionally the measurements were carried out, with the new spectrometer, to study the hyperfine field in the intermetallic compound LaMnSi2 using 111Cd and 140Ce nuclear probes. The measurements were carried out in the temperature range from 10 K to 400 K. While the temperature dependence of hyperfine field measured with 111In -> 111Cd probe, follows the Brillouin function the behaviour of the hyperfine field measured with 140La -> 140Ce is anomalous. This behavior has been explained in terms of a strong hybridization of 4f band of Ce with the 3d band of Mn, a fact verified in previous studies with similar compounds.

We have built a spectrometer to investigate the Near-Infrared (NIR) range of this radiation, which is used for bunch diagnostics at the European X-ray Free-Electron Laser. This could give information on the development of microbunching, periodic features in the longitudinal charge profile of the bunches which have a negative impact on the operation of the facility. In general it offers an ability to investigate the influences of the laser heater, the compression, and other factors that affect the structure of the bunches. The CDR is generated 1934 m after the injector, at full acceleration. The spectrometer is based around the KALYPSO detector system, able to read out from a 256 pixel linear array detector at MHz frequencies, making it possible to obtain single bunch readings during current user operation of the facility, at 1.1 MHz. KALYPSO has an InGaAs sensor, sensitive in the range 0.9 – 1.7 μm. A 40 mm N-SF11 equilateral prism is used for dispersion. First measurements have been taken, and CDR has been detected. The spectrometer needs further calibration and resolution was lacking, but it can offer insight in to relative changes, and bunch-to and can be used as for fingerprinting the beam. A reduction in signal in the sensitive range and a skew towards longer wavelengths was seen when going from uncompressed to compressed beam. When varying the power of the laser heater the behavior varied from run to run, with changing machine settings. In some cases the CDR was attenuated, while FEL intensity initially increased, until the induced energy spread from the laser heater was large enough to inhibit the FEL process. Another, less expected, behaviour was also observed, where the initially low CDR intensity at first increased, while FEL intensity stayed the same, before it then followed the same pattern as in the first case.

Neutron are emitted from a deuterium plasma with energies around 2.5 MeV. The neutron spectrum is intimately related to the ion velocity distribution of the plasma. As a consequence, the analysis of neutron energy spectra can give information of the plasma rotation, the ion temperature, heating efficiency and fusion power. The upgraded magnetic proton recoil spectrometer (MPRu), based on the thin-foil technique, is installed at the tokamak JET. The upgrade of the spectrometer was done to allow for measurements of deuterium plasmas. This thesis describes the hardware, the data reduction scheme and the kind of fusion plasma parameters that can be estimated from the data of the MPRu. The MPRu data from 3rd harmonic ion cyclotron resonance and beam heating are studied. Other neutron spectrometer techniques are reviewed as well, in particular in the aspect of suitability for neutron emission spectrometry at ITER. Each spectrometer technique is evaluated using synthetic data which is obtained from standard scenarios of ITER. From this evaluation, we conclude that the thin-foil technique is the best technique to measure, e.g., the ion temperature in terms of time resolution.

Diese Dissertation ist innerhalb eines Teilprojekts des Schwerpunktprogramms SPP1233 ”Megacities Megachallenge - Informal Dynamics of Global Change“ entstanden. Thema der vorliegenden Arbeit ist die Untersuchung der heterogenen Reflexion der Sonnenstrahlung an urbanen Bodenoberflächen, sowie deren Einfluss auf die Bestimmung der optischen Dicke von Aerosolpartikeln aus Satellitendaten. Zu diesem Zweck wurden flugzeuggetragene Messungen der spektral aufgelösten, reflektierten solaren Strahlung durchgeführt. In dieser Arbeit werden Messungen mit dem SMART-Albedometer (Spectral Modular Airborne Radiation measurement sysTem) präsentiert, die im Rahmen zweier Messkampagnen in Leipzig im September 2007 und in Zhongshan, China im Dezember 2009 erfasst wurden. Die spektrale Bodenreflektivität und Bodenalbedo wurden aus den spektralen Messungen der aufwärtsgerichteten Stahldichte (Radianz) und Strahlungsflussdichte (Irradianz) bestimmt. Dazu wurden eindimensionale Strahlungsübertragungsrechnungen durchgeführt. Der Einfluss der Flughöhe auf die Bodenreflektivität und Bodenalbedo wird anhand eines Messbeispiels, sowie einer Modellstudie mit ein- und dreidimensionalen Strahlungsübertragungsrechnungen diskutiert. Für beide Untersuchungsgebiete, Leipzig und Zhongshan, wird die Heterogenität der Reflexion solarer Strahlung an urbanen Oberflächen gezeigt. Der Einfluss der im operationellen Aerosolalgorithmus des satellitengetragenen Instrumentes MODIS (MODerate resolution Imaging Spectroradiometer) getroffenen Annahmen zur Bodenreflektivität auf die optische Dicke von Aerosolpartikeln, wurde mittels der gemessenen spektralen Bodenreflektivität und einer auf Strahlungsübertragungsrechnungen basierenden Modellstudie quantifiziert. Ein linearer Zusammenhang zwischen Bodenreflektivität und optischer Dicke von Aerosolpartikeln wird für beide Fallbeispiele gezeigt. Mittels der Messungen in Zhongshan kann bestätigt werden, dass die Bodenreflektivität für urbane Oberflächen im Aerosolalgorithmus unterschätzt wird. Im Rahmen der Modellstudie wird die Sensitivität des Aerosolalgorithmus auf die programminternen Annahmen zur Bodenreflektivität quantifiziert.

Fourier transform infrared emission spectra of MnH and MnD were observed in the ground <em>X</em>⁷&sigma;⁺ electronic state. The vibration-rotation bands from <em>v</em> = 1 to 0 to <em>v</em> = 3 to 2 for MnH, and from <em>v</em> = 1 to 0 to <em>v</em> = 4 to 3 for MnD were recorded at an instrumental resolution of 0. 0085 cm^-1. Spectroscopic constants were determined for each vibrational level and equilibrium constants were found from a Dunham-type fit. The equilibrium vibrational constant <em>&omega;_e</em> for MnH was found to be 1546. 84518(65) cm^-1, the equilibrium rotational constant <em>B_e</em> was found to be 5. 6856789(103) cm^-1 and the equilibrium bond distance <em>r_e</em> was determined to be 1. 7308601(47) Å. <br /><br /> New high resolution emission spectra of CoH and CoD molecules have been recorded in the 640 nm to 3. 5 <em>µ</em>m region using a Fourier transform spectrometer. Many bands were observed for the <em>A</em>^'3&phi;-<em>X</em>³&phi; electronic transition of CoH and CoD. In addition, a new [13. 3]4 electronic state was found by observing the [13. 3]4- <em>X</em>³&phi;₃ and [13. 3]4-<em>X</em>³&phi;₄ transitions in the spectrum of CoD. Analysis of the transitions with &delta;&omega; = 0, ±1 provided more accurate values of spin-orbit splittings between &omega; = 4 and &omega; = 3 components. The ground state for both molecules was fitted both to band and Dunham-type constants. The estimated band constants of the perturbed upper states were also obtained. <br /> <br /> The emission spectrum of gas-phase YbO has been investigated using a Fourier transform spectrometer. A total of 8 red-degraded bands in the range 9 800 ? 11 300 cm^-1 were recorded at a resolution of 0. 04 cm^-1. Because of the multiple isotopomers present in the spectra, only 3 bands were rotationally analyzed. Perturbations were identified in two of these bands and all 3 transitions were found to terminate at the <em>X</em>¹&sigma;⁺ ground electronic state. The electronic configurations that give rise to the observed states are discussed and molecular parameters for all of the analyzed bands are reported. <br /><br /> Electronic spectra of the previously unobserved EuH and EuD molecules were studied by means of Fourier transform spectroscopy and laser-induced fluorescence. The extreme complexity of these transitions made rotational assignments of EuH bands impossible. However, the spin-spin interaction constant, &lambda;, and Fermi contact parameter, <em>b</em>_F, in the ground <em>X</em>⁹&sigma;^- electronic state were estimated for the ¹⁵¹EuH and ¹⁵³EuH isotopologues. <br /><br /> Electronic spectra of SmH, SmCl, TmH and ErF molecules were recorded for the first time using Fourier transform spectrometer. The poor signal to noise ratio of the observed bands coupled with their complexity prevented a rotational analysis. The electronic states that may be involved in the observed transitions are discussed.

Fourier transform infrared emission spectra of MnH and MnD were observed in the ground <em>X</em>⁷&sigma;⁺ electronic state. The vibration-rotation bands from <em>v</em> = 1 to 0 to <em>v</em> = 3 to 2 for MnH, and from <em>v</em> = 1 to 0 to <em>v</em> = 4 to 3 for MnD were recorded at an instrumental resolution of 0. 0085 cm^-1. Spectroscopic constants were determined for each vibrational level and equilibrium constants were found from a Dunham-type fit. The equilibrium vibrational constant <em>&omega;_e</em> for MnH was found to be 1546. 84518(65) cm^-1, the equilibrium rotational constant <em>B_e</em> was found to be 5. 6856789(103) cm^-1 and the equilibrium bond distance <em>r_e</em> was determined to be 1. 7308601(47) Å. <br /><br /> New high resolution emission spectra of CoH and CoD molecules have been recorded in the 640 nm to 3. 5 <em>µ</em>m region using a Fourier transform spectrometer. Many bands were observed for the <em>A</em>^'3&phi;-<em>X</em>³&phi; electronic transition of CoH and CoD. In addition, a new [13. 3]4 electronic state was found by observing the [13. 3]4- <em>X</em>³&phi;₃ and [13. 3]4-<em>X</em>³&phi;₄ transitions in the spectrum of CoD. Analysis of the transitions with &delta;&omega; = 0, ±1 provided more accurate values of spin-orbit splittings between &omega; = 4 and &omega; = 3 components. The ground state for both molecules was fitted both to band and Dunham-type constants. The estimated band constants of the perturbed upper states were also obtained. <br /> <br /> The emission spectrum of gas-phase YbO has been investigated using a Fourier transform spectrometer. A total of 8 red-degraded bands in the range 9 800 ? 11 300 cm^-1 were recorded at a resolution of 0. 04 cm^-1. Because of the multiple isotopomers present in the spectra, only 3 bands were rotationally analyzed. Perturbations were identified in two of these bands and all 3 transitions were found to terminate at the <em>X</em>¹&sigma;⁺ ground electronic state. The electronic configurations that give rise to the observed states are discussed and molecular parameters for all of the analyzed bands are reported. <br /><br /> Electronic spectra of the previously unobserved EuH and EuD molecules were studied by means of Fourier transform spectroscopy and laser-induced fluorescence. The extreme complexity of these transitions made rotational assignments of EuH bands impossible. However, the spin-spin interaction constant, &lambda;, and Fermi contact parameter, <em>b</em>_F, in the ground <em>X</em>⁹&sigma;^- electronic state were estimated for the ¹⁵¹EuH and ¹⁵³EuH isotopologues. <br /><br /> Electronic spectra of SmH, SmCl, TmH and ErF molecules were recorded for the first time using Fourier transform spectrometer. The poor signal to noise ratio of the observed bands coupled with their complexity prevented a rotational analysis. The electronic states that may be involved in the observed transitions are discussed.

This thesis presents results of investigations that have been carried out to understand dynamics in nonlinear Paul trap mass spectrometers. Of the three problems that have been taken up for study in this thesis, the first concerns understanding early/delayed ejection of ions in mass selective boundary ejection experiments. The second looks at the differential resolution observed in forward and reverse scan resonance ejection experiments. The third study explores a coupled nonlinear resonance within the nominally stable region of trap operation. The method of multiple scales has been to elucidate dynamics associated with early and delayed ejection of ions in mass selective ejection experiments in Paul traps. We develop a slow flow equation to approximate the solution of a weakly nonlinear Mathieu equation to describe ion dynamics in the neighborhood of the stability boundary of ideal traps (where the Mathieu parameter qz = qz* = 0.908046). For positive even multipoles in the ion trapping field, in the stable region of trap operation, the phase portrait obtained from the slow flow consists of three fixed points, two of which are saddles and the third is a center. As the qz value of an ion approaches qz*, the saddles approach each other, and a point is reached where all nonzero solutions are unbounded, leading to an observation of early ejection. The phase portraits for negative even multipoles and odd multipoles of either sign are qualitatively similar to each other and display bounded solutions even for qz > qz*, resulting in the observation of delayed ejection associated with a more gentle increase in ion motion amplitudes, a mechanism different from the case of the positive even multipoles. The second study investigates constraints on pre-ejection dynamical states which cause differential resolution in resonance ejection experiments using Paul traps with stretched geometry. Both analytical and numerical computations are carried out to elucidate the role of damping and scan rate in influencing coherence in ion motion associated with the forward and reverse scan. It has been shown that in the forward scan experiments, for a given damping, low scan rates result in coherent motion of ions oof a given mass at the jump point. At this point, the amplitude and phase of ions of a given mass, starting at different initial conditions, become effectively identical. As the scan rate is increased, coherence is destroyed. For a given scan rate, increasing damping introduces coherence in ion motion, while decreasing damping destroys this coherence. In reverse scan experiments, for a given damping, very low scan rates will cause coherent ion motion. Increasing the scan rate destroys this coherence. The effect of damping in reverse scan experiments is qualitatively similar to that in the forward scan experiments, but settling times in the forward scan are shorter, leading to improved coherence and resolution. For mass spectrometrically relevant scan rates and damping values, significantly greater coherence is obtained in the forward scan. In the third study we investigate the weakly coupled and nonlinear Mathieu equations governing ion motion in axial and radial directions in a Paul trap in the neighborhood of a nonlinear resonance point at az* = -0.2313850427 and qz* = 0.9193009931$. Using harmonic balance based approximate averaging up to second order; we obtain a slow flow that, we numerically demonstrate, approximates the actual ion dynamics. We find that the slow flow is Hamiltonian. We study the slow flow numerically with the objective of exploring and displaying some of the possible types of interesting ion motions. In particular, we choose specific but arbitrary parameter values; study the stability of the individual radial and axial motion invariant manifolds; examine the rather large times associated with escape of ions; notice regions in the averaged phase space wherein trajectories do not, in fact, escape; observe apparently chaotic dynamics preceding escape for ions that do escape; and note that trajectories that do not escape appear to be confined to 4-tori. We conclude with some comments on the implications for practical operation of the Paul trap near this resonant point.

<p>Conventional mass spectrometry sensing has isomorphic nature, which means measure the input mass spectrum abundance function by a resemble of delta function to avoid ambiguity. However, the delta function nature of traditional mass spectrometry sensing approach imposes trade-offs between mass resolution and throughput/mass analysis time. This dissertation proposes a new field of mass spectrometry sensing which combines both computational signal processing and hardware modification to break the above trade-offs. We introduce the concept of generalized sensing matrix/discretized forward model in mass spectrometry filed. The presence of forward model can bridge the cap between sensing system hardware design and computational sensing algorithm including compressive sensing, feature/variable selection machine learning algorithms, and stat-of-art inversion algorithms. </p><p>Throughout this dissertation, the main theme is the sensing matrix/forward model design subject to the physical constraints of varies types of mass analyzers. For quadrupole ion trap systems, we develop a new compressive and multiplexed mass analysis approach mutli Resonant Frequency Excitation (mRFE) ejection which can reduce mass analysis time by a factor 3-6 without losing mass spectra specificity for chemical classification. A new information-theoretical adaptive sensing and classification framework has proposed on quadrupole mass filter systems, and it can significantly reduces the number of measurements needed and achieve a high level of classification accuracy. Furthermore, we present a coded aperture sector mass spectrometry which can yield a order-of-magnitude throughput gain without compromising mass resolution compare to conventional single slit sector mass spectrometer.</p> / Dissertation

The work presented here develops a gamma-ray spectral construction and analysis software tool that was used to analyze multi-detector data collected using a digital spectrometer with list mode capabilities. The tool was used to parse the output from three detectors and generate new spectra that the user chooses from post-processing suppression routines, such as simulated anticoincidence and coincidence spectra. Part of this research was also to characterize the improvements in the detection limits and the various detector efficiencies from this method as opposed to creating these spectra using traditional electronic gating systems. A focus is placed on the detection capability improvements for nuclear forensics purposes, particularly the identification and quantification of fission product samples, and structuring the code framework for handling these types of time-dependent samples while increasing the versatility of the detector system. Improvements to the minimum detectable activity for a series of fission products was accomplished through post-processing suppression methods and multi-dimensional spectral data structures are now achievable. / text

Plasma enhanced chemical vapor deposition systems are massively deployed to grow numerous thin film coatings including hydrogenated amorphous silicon. A new deposition chamber was designed, procured, and constructed to investigate the plasma properties of a 100% silane (SiH4) glow discharge with varying chamber pressure and inter-electrode spacing. A Hiden EQP1000 ion mass spectrometer sampled the plasma from the substrates point of view. Ion energy distributions were obtained using four different excitation sources +DC, –DC, radio frequency (at 13.56 MHz), and the DC Saddle Field (DCSF) in the tetrode configuration. The shape of the ion energy distributions was constant for the capacitively coupled +DC, –DC, and rf (at higher pressures of 75 and 160 mTorr) glow discharges. The shape of the ion energy distributions for the DCSF plasma exhibited a double peak or saddle structure analogous to radio frequency plasmas. The width between the peaks (peak separation) was controlled by the pressure and the semi-transparent cathode to semi-transparent anode distance. Ion energy distributions from the DCSF plasma concurred with rf and +DC ion energy distributions at specific pressures and inter-electrode distances. This result demonstrates the versatility of the DCSF glow discharge system. Moreover, control of the peak separation is modeled to be iii equivalent to controlling the critical ratio (ion transit time in the sheath to the electron oscillating period), and/or the inferred electron oscillating sheath potential. The DCSF possesses a fusion of rf and +DC methods. The long high energy tail or constant background are indicative of a +DC high voltage sheath in which there is an increasing fraction of collisionless ions as the anode-cathode distance increases. These collisionless ions are provided by the oscillating electrons (or rf nature) of the DCSF method. Higher order silane (silicon containing) ions increase in relative intensity with increasing inter-electrode spacing for the +DC, –DC, and rf plasmas. These higher order silane ions are also detected in the DCSF plasma, and can be reduced at either lower pressure or lower cathode to anode or cathode to substrate distances.