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Molecular dynamics simulation study on the phase behavior of the Gay Berne model with a terminal dipole and a exible tail J Chem Phys 120(16):7792 7800 Funamoto K, Ozaki M, Yoshino K 2003 Discontinuous shift of lasing wavelength with temperature in cholesteric liquid crystal Jpn J Appl Phys, Part 2: Letters 42(12B):L1523 L1525 Furumi S, Yokoyama S, Otomo A, Mashiko S 2003 Electrical control of the structure and lasing in chiral photonic band gap liquid crystals Appl Phys Lett 82(1):16 18 Goossens WJA 1971 Molecular theory of the cholesteric phase and of the twisting power of optically active molecules in a nematic liquid crystal Mol Cryst Liq Cryst 12(3):237 244 Gottarelli G, Spada GP 1985 Induced cholesteric mesophases: origin and application Mol Cryst Liq Cryst 123(1 4):377 388..

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Fig. 2.11 Concentration distribution in the case of linear diffusion with c = 0 for x = 0 (see Eq. 2.5.6), where D = 10"' s , time in seconds is indicated at each curve and the effective diffusion layer thickness is shown for t = 100 s

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In the past, clustered solutions were composed of homogeneous computing nodes. They used identical processor, memory, and OS configurations on each of the nodes. This is still prevalent, especially in HPC clusters. With HA clusters, it is a requirement. The homogeneous environment makes managing the environment as a single entity much easier, especially when HPC clusters grow to support more than four nodes (there are HPC clusters supporting over 1,000 nodes). Load balancing clusters are also often homogeneous, especially when the cluster is performing many iterations of the same task. More recently, however, with the concept of on-demand computing, much of the load-balancing software can pair tasks with appropriate node configurations. Grid clusters are more frequently heterogeneous, performing a multitude of independent tasks.

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(see Table 2.3). Figure 2.11 depicts the concentration distribution. It can be seen from Eq. (2.5.6) that the ratio c/c is independent of the concentration but only depends on the distance from the reference plane, on the time and on the diffusion coefficient. Assuming that the solution of the diffusing substance is dilute, the diffusion coefficient does not depend on its concentration. The material flux through the reference plane is given by the concentration gradient for x = 0. In the present case the concentration gradient is dc dx'~

Gottarelli G, Samori B, Stremmenos C, Torre G 1981 Induction of cholesteric mesophases in nematic liquid crystals by some chiral aryl alkyl carbinols A quantitative investiga tion Tetrahedron 37(2):395 399 Gottarelli G, Hibert M, Samori B, Solladie G, Spada GP, Zimmermann R 1983 Induction of the cholesteric mesophase in nematic liquid crystals: mechanism and application to the determination of bridged biaryl con gurations J Am Chem Soc 105(25):7318 7321 Haas WE, Nelson KF, Adams JE, Dir GA 1974 The uv imaging with nematic chlorostilbenes J Electrochem Soc 121(12):1667 1669 John S 1987 Strong localization of photons in certain disordered dielectric superlattices Phy Rev Lett 58(23):2486 2489 Kopp VI, Fan B, Vithana HKM, Genack AZ 1998 Low threshold lasing at the edge of a photonic stop band in cholesteric liquid crystals Opt Lett 23(21):1707 1709 Kopp VI, Zhang Z Q, Genack AZ 2003 Lasing in chiral photonic structures.

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With the advent of virtual machines (as described in 8, Virtualization ), virtual clusters can be created within a single blade or across blades.

Prog Quantum Electron 27(6):369 416 Kumaresan S, Mallia VA, Kida Y, Tamaoki N 2005 Thermal and photooptical properties of azoxybenzene/alkyloxy azobenzene cholesterol dimesogens with alkyl diacetylene linker J Mater Res 20(12):3431 3438 Kurihara S, Nomiyama S, Nonaka T 2000 Photochemical switching between a compen sated nematic phase and a twisted nematic phase by photoisomerization of chiral azobenzene molecules Chem Mater 12(1):9 12 Kurihara S, Nomiyama S, Nonaka T 2001 Photochemical control of the macrostructure of cholesteric liquid crystals by means of photoisomerization of chiral azobenzene molecules Chem Mater 13(6):1992 1997 Kurihara S, Hatae Y, Yoshioka T, Ogata T, Nonaka T 2006 Photo tuning of lasing from a dye doped cholesteric liquid crystals by photoisomerization of a sugar derivative having plural azobenzene groups Appl Phys Lett 88(10):103121/1 103121/3 Lee H K, Doi K, Harada H, Tsutsumi O, Kanazawa A, Shiono T, Ikeda T 2000.

(2.5.7)

Photochemical modulation of color and transmittance in chiral nematic liquid crystal containing an azobenzene as a photosensitive chromophore J Phys Chem B 104(30):7023 7028 Lin T H, Chen Y J, Wu C H, Fuh AY G, Liu J H, Yang P C 2005 Cholesteric liquid crystal laser with wide tuning capability Appl Phys Lett 86(16):161120/1 161120/3 Mallia VA, Tamaoki N 2003 Photoresponsive vitri able chiral dimesogens: photo thermal modulation of microscopic disordering in helical superstructure and glass forming properties J Mater Chem 13(2):219 224 Matsuhisa Y, Huang Y, Zhou Y, Wu S T, Ozaki R, Takao Y, Fujii A, Ozaki M 2007 Low threshold and high ef ciency lasing upon band edge excitation in a cholesteric liquid crystal Appl Phys Lett 90(9):091114/1 091114/3 Matsui T, Ozaki R, Funamoto K, Ozaki M, Yoshino K 2002 Flexible mirror less laser based on a free standing lm of photopolymerized cholesteric liquid crystal.

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