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O objetivo desta tese é demonstrar que para um subshift de Markov topologicamente transitivo com alfabeto enumerável e um potencial &#402 com pressão de Gurevic finita e variação limitada (&#402) < &#8734, existe um único estado de equilíbrio &#181t&#402 para cada t > 1, e a família (&#181t&#402)t>1 tem um ponto de acumulação quando t > &#8734. Além disso se também supomos que o &#402 é um potencial de Markov, demonstramos que a família de estados de equilíbrio (&#181t&#402)t>1 converge quando t > &#8734. Finalmente demonstramos a continuidade em &#8734 da entropia com respeito ao parâmetro t. Estes resultados não dependem da hipótese de existência de medidas de Gibbs. / The aim of this thesis is to prove that for a topologically transitive Markov subshift with countable alphabet and a summable potential &#402 with finite topological pressure Gurevic and bounded variation (&#402) < &#8734, there exists an equilibrium state &#181t&#402 tf for each t > 1 and the family of equilibrium states (&#181t&#402)t>1 associated to each potential tf has an accumulation point at t > &#8734. Moreover if we also assume that &#402 is a Markov potential we prove that the equilibrium states family (&#181t&#402)t>1 converges when t > &#8734. Finally we prove the continuity at &#8734 of the entropy with respect to the parameter t. These results do not depend on assuming the existence of Gibbs measures.

Les capteurs d’images CMOS sont de plus en plus utilisés dans le domaine industriel : la surveillance, la défense, le médical, etc. Dans ces domaines, les capteurs d?images CMOS sont exposés potentiellement à de grandes variations de température. Les capteurs d?images CMOS, comme tous les circuits analogiques, sont très sensibles aux variations de température, ce qui limite leurs applications. Jusquà présent, aucune solution intégrée pour contrer ce problème n’a été proposée. Afin de remédier à ce défaut, nous étudions, dans cette thèse, les effets de la température sur les deux types d?imageurs les plus connus. Plusieurs structures de compensation sont proposées. Elles reprennent globalement les trois méthodes existantes et jamais appliquées aux capteurs d’images. La première méthode utilise une entrée au niveau du pixel qui sera modulée en fonction de l’évolution de la température. La deuxième méthode utilise la technique ZTC (Zero Temperature Coefficient). La troisième méthode est inspirée de la méthode de la tension de référence bandgap. Dans tous les cas, nous réduisons de manière très intéressante l’effet de la température et nous obtenons une bonne stabilité en température de -30 à 125°C. Toutes les solutions proposées préservent le fonctionnement initial de l’imageur. Elles n’impactent également pas ou peu la surface du pixel / CMOS image sensors find widespread use in various industrial applications including military, surveillance, medical, etc. In these applications, CMOS image sensors are often exposed to large temperature variations. As analog circuits, these CMOS image sensors are very sensitive to temperature variations, which limit their applications. Until now, no integrated solution for this problem has been proposed. To solve this problem, we study, in this thesis, the temperature effects on the two most known types of CMOS image sensors. Several compensation structures are proposed. They generally return to the three existing methods and never applied to image sensors. The first method uses an entrance at the pixel level to be adjusted according to changes in temperature. The second method uses the ZTC (Zero Temperature Coefficient) technique. The third method is based on the method of the bandgap voltage reference. In all cases, we reduce a very interesting way the temperature effect and we get a good temperature stability of the sensor from -30 to 125°C. All the solutions preserve the initial operation of the imager. They also affect a little or not the surface of the pixel.

O objetivo desta tese é demonstrar que para um subshift de Markov topologicamente transitivo com alfabeto enumerável e um potencial &#402 com pressão de Gurevic finita e variação limitada (&#402) < &#8734, existe um único estado de equilíbrio &#181t&#402 para cada t > 1, e a família (&#181t&#402)t>1 tem um ponto de acumulação quando t > &#8734. Além disso se também supomos que o &#402 é um potencial de Markov, demonstramos que a família de estados de equilíbrio (&#181t&#402)t>1 converge quando t > &#8734. Finalmente demonstramos a continuidade em &#8734 da entropia com respeito ao parâmetro t. Estes resultados não dependem da hipótese de existência de medidas de Gibbs. / The aim of this thesis is to prove that for a topologically transitive Markov subshift with countable alphabet and a summable potential &#402 with finite topological pressure Gurevic and bounded variation (&#402) < &#8734, there exists an equilibrium state &#181t&#402 tf for each t > 1 and the family of equilibrium states (&#181t&#402)t>1 associated to each potential tf has an accumulation point at t > &#8734. Moreover if we also assume that &#402 is a Markov potential we prove that the equilibrium states family (&#181t&#402)t>1 converges when t > &#8734. Finally we prove the continuity at &#8734 of the entropy with respect to the parameter t. These results do not depend on assuming the existence of Gibbs measures.

量子擾動及挫折性兩者均可破壞絕對零溫的磁序，為近代凝態物 理關注的有趣現象。在外加橫場下的三角晶格易辛反鐵磁兼具量子臨 界現象(quantum criticality)及幾何挫折性，可謂量子磁性物質之一典 範理論模型。本論文利用平衡態及非平衡態量子蒙地卡羅(quantum Monte Carlo)方法探測三角晶格易辛反鐵磁之量子相變，其界定零溫 時無磁性的順磁態及具 Z6 對稱破缺的有序態(所謂時鐘態)。這裡的 量子蒙地卡羅方法為運用算符的零溫投射(zero-temperature projector) 及隨機序列展開(stochastic series expansion)演算法。在非平衡模擬 中，我們分別沿降溫過程及量子絕熱過程逼近量子相變點，藉此我們 得到動力學指數，及其它相關臨界指數。 / The destruction of magnetic long-range order at absolute zero temperature arising from quantum fluctuations and frustration is an interesting theme in modern condensed-matter physics. The triangular lattice Ising antiferromag- net in a transverse field provides a playground for the study of the combined effects of quantum criticality and geometrical frustration. In this thesis we use quantum Monte Carlo methods both in equilibrium and non-equilibrium setups to study the properties of the quantum critical point in the triangular lattice antiferromagnet, which separates a disordered paramagnetic state and an ordered clock state exhibiting Z6 symmetry breaking; The methods are based on a zero-temperature projector algorithm and the stochastic series ex- pansion algorithm. For the non-equilibrium setups, we obtain the dynamical exponent and other critical exponents at the quantum critical point approached by slowly decreasing temperature and through quantum annealing.