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Blue phase liquid crystals (BPLCs) have a delicate lattice structure existing between chiral nematic and isotropic phases, with a stable temperature range of about 2 K. But due to short coherent length, these self-assembled nano-structured BPLCs have a fast response time. In the past three decades, the application of BPLC has been rather limited because of its narrow temperature range. In 2002, Kikuchi et al. developed a polymer stabilization method to extend the blue-phase temperature range to more than 60 K. This opens a new gateway for display and photonic applications. In this dissertation, I investigate the material properties of polymer-stabilized BPLCs. According the Gerber’s model, the Kerr constant of a BPLC is linearly proportional to the dielectric anisotropy of the LC host. Therefore, in the frequency domain, the relaxation of the Kerr constant follows the same trend as the dielectric relaxation of the host LC. I have carried out experiments to validate the theoretical predictions, and proposed a model called extended Cole-Cole model to describe the relaxation of the Kerr constant. On the other hand, because of the linear relationship, the Kerr constant should have the same sign as the dielectric anisotropy of the LC host; that is, a positive or negative Kerr constant results from positive (∆ε > 0) or negative host LCs (∆ε < 0), respectively. BPLCs with a positive Kerr constant have been studied extensively, but there has been no study on negative ∆ε polymer-stabilized BPLCs. Therefore, I have prepared a BPLC mixture using a negative ∆ε LC host and investigated its electro-optic properties. I have demonstrated that indeed the induced birefringence and Kerr constant are of negative sign. Due to the fast response time of BPLCs, color sequential display is made possible without color breakup. By removing the spatial color filters, the optical efficiency and resolution density are both tripled. With other advantages such as alignment free and wide viewing angle, polymer-stabilized BPLC is emerging as a promising candidate for next-generation displays. However, the optical efficiency of the BPLC cell is relatively low and the operating voltage is quite high using conventional in-plane-switching electrodes. I have proposed several device structures for improving the optical efficiency of transmissive BPLC cells. Significant improvement in transmittance is achieved by using enhanced protrusion electrodes, and a 100% transmittance is achievable using complementary enhanced protrusion electrode structure. For a conventional transmissive blue phase LCD, although it has superb performances indoor, when exposed to strong sunlight the displayed images could be washed out, leading to a degraded contrast ratio and readability. To overcome the sunlight readability problem, a common approach is to adaptively boost the backlight intensity, but the tradeoff is in the increased power consumption. Here, I have proposed a transflective blue phase LCD where the backlight is turned on in dark surroundings while ambient light is used to illuminate the displayed images in bright surroundings. Therefore, a good contrast ratio is preserved even for a strong ambient. I have proposed two transflective blue phase LCD structures, both of which have single cell gap, single gamma driving, reasonably wide view angle, low power consumption, and high optical efficiency. Among all the 3D technologies, integral imaging is an attractive approach due to its high efficiency and real image depth. However, the optimum observation distance should be adjusted as the displayed image depth changes. This requires a fast focal length change of an adaptive lens array. BPLC adaptive lenses are a good candidate because of their intrinsic fast response time. I have proposed several BPLC lens structures which are polarization independent and exhibit a parabolic phase profile in addition to fast response time. To meet the low power consumption requirement set by Energy Star, high optical efficiency is among the top lists of next-generation LCDs. In this dissertation, I have demonstrated some new device structures for improving the optical efficiency of a polymerstabilized BPLC transmissive display and proposed sunlight readable transflective blue-phase LCDs by utilizing ambient light to reduce the power consumption. Moreover, we have proposed several blue-phase LC adaptive lenses for high efficiency 3D displays.

Ce travail se place dans le cadre de la mesure ultrasensible d’anisotropie de phase optique que permet l’emploi adapté des cavités de très haute finesse. Pour stabiliser la fréquence laser sur une résonance de la cavité, un schéma d’asservissement reposant sur la rétroaction optique est utilisé.Une première partie décrit le couplage optique entre le laser et la cavité à travers l’analyse du comportement de la fréquence d’émission du laser auto-réinjecté. Une comparaison analytique théorie expérience a permis d’identifier les signaux d’erreur nécessaires au maintien durable de la fréquence du laser à l’exacte résonance d’un mode de la cavité. Après une description détaillée du dispositif d’asservissement, sa réalisation expérimentale sur une cavité de finesse de quelques milliers (F = 3 000)a démontré la possibilité de stabiliser la fréquence laser sur plus de dix heures avec une excursion résiduelle à la seconde de 375 Hz.Dans la deuxième partie, le développement précédent a été mis en œuvre sur une cavité de très haute finesse (F = 250 000) et a permis la mesure ultrasensible de biréfringence induite dans des gaz par effet Kerr. L’originalité du dispositif repose sur la mise à profit de la biréfringence résiduelle des miroirs de haute réflectivité.Elle est utilisée d’une part comme source à la rétroaction optique, et d’autre part comme biais optique à la mesure de la biréfringence du gaz. Une étude théorique et expérimentale détaillée des sources de bruit présent dans la chaîne de détection en fonction de la valeur du biais optique a permis de réaliser la mesure de déphasage au niveau du bruit de photons avec quelques mW de puissance laser. Ainsi, une sensibilité référence sur la mesure de déphasage Kerr de 3.10−13 rad a été démontrée pour un temps de mesure de 800 sec. Cette valeur record améliore de trois ordres de grandeur les déphasages Kerr précédemment mesurés. Le dispositif a été de plus mis à profit pour la mesure à faible champ électrique (< 40 V /mm) et à pression atmosphérique, des constantes de Kerr de différents gaz moléculaires et atomiques jusqu’à l’He. / The context of the work is the ultra-sensitive measurement of phase anisotropy permits by well-used of very high finesse cavity. To stabilize the laser frequency at the exact resonance of one cavity mode, a servo control based on optical feedback is used.In the first part, the optical coupling between laser and cavity is described through the comportment of the frequency of the self-locked laser. A comparison between experience and theory has permitted to identify the error signals in order to keep enduringly the laser frequency at the exact resonance. The experimental realization of the servo control into a 3 000 finesse cavity had demonstrated the stabilization of the laser frequency during more than ten hours with a residual one second excursion of 375 Hz.In the second part, the previous development has been used with a very high finesse cavity (F=250 000) to measure static Kerr birefringence in gases. The originality of the set-up is the use of the residual high reflectivity mirrors birefringence, firstly as the source of the optical feedback and secondly as an optical bias to measure the weak gas birefringence. An experimental and theoretical study of the noise according to the value of the optical bias has permitted a photon noise limited measurement (laser intensity of few mW). A record sensitivity of the phase shift induced by Kerr effect has been demonstrated at 3.10-13 rad with 800 s integration time. The scheme has been used to measure, in weak electric field (<40 V/mm) and in standard condition of pressure and temperature, the Kerr constant of molecular and atomic gases, even He gas