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Three-dimensional superlattices

Two-Dimensional and Three-Dimensional Superlattices Syntheses and Collective Physical Properties... [Pg.315]

Chapter 8 presents evidence on how the physical properties of colloidal crystals organized by self-assembly in two-dimensional and three-dimensional superlattices differ from those of the free nanoparticles in dispersion. [Pg.690]

Oonishi, T., Sato, S., Yao, H. and Kimura, K. (2007) Three-dimensional gold nanopartide superlattices Structures and optical absorption characteristics. Journal of Applied Physics, 101, 114314. [Pg.346]

Crystalline phases (truncated octahedra) of 5 nm silver particles, thiolate protected as well, have been detected by means of high-resolution transmission electron microscopy (HRTEM) [26-28]. Three-dimensional architectures of 5-6 nm thiolate-stabilized gold particles have also been described [29]. Several other reports on 3D superlattices of metal nanoparticles have become known during the last few years [30-33]. [Pg.11]

Lead nitrate complexed with EDTA and lead perchlorate and sodium sulphide have been used for PbS ECALE-deposition.158159 The films were cubic and highly (200) oriented, and AFM images showed the same cubic structure.158159 PbSe films were also cubic, and the band gap of a film after 50 deposition cycles was 8000cm-1.160 PbSe/PbTe superlattices, with 4.2-nm and 7.0-nm periods, have been grown by ECALE.161 The (111) reflection in the XRD pattern showed a first-order satellite peak and one second-order peak, indicating the formation of the superlattice. AFM images of the superlattice structure showed a small amount of three-dimensional growth.161... [Pg.269]

Talapin, D. V. Shevchenko, E. V. Kornowski, A. Gaponik, N. Haase, M. Rogach, A. L. Weller, H. 2001. A new approach to crystalhzation of CdSe nanoparticles into ordered three-dimensional superlattices. Adv. Mater. 13 1868-1871. [Pg.343]

Murray, C. B. Kagan, C. R. Bawendi, M. G. 1995. Self-organization of CdSe nanocrystallites into three-dimensional quantum dot superlattices. Science 270 1335-1338. [Pg.343]

Figure 1 2 1. The different types of 2.5 Lifshitz electronic topological transition (ETT) The upper panel shows the type (I) ETT where the chemical potential EF is tuned to a Van Hove singularity (vHs) at the bottom (or at the top) of a second band with the appearance (or disappearance) of a new detached Fermi surface region. The lower panel shows the type (II) ETT with the disruption (or formation) of a neck in a second Fermi surface where the chemical potential EF is tuned at a vHs associated with the gradual transformation of the second Fermi surface from a two-dimensional (2D) cylinder to a closed surface with three dimensional (3D) topology characteristics of a superlattice of metallic layers... Figure 1 2 1. The different types of 2.5 Lifshitz electronic topological transition (ETT) The upper panel shows the type (I) ETT where the chemical potential EF is tuned to a Van Hove singularity (vHs) at the bottom (or at the top) of a second band with the appearance (or disappearance) of a new detached Fermi surface region. The lower panel shows the type (II) ETT with the disruption (or formation) of a neck in a second Fermi surface where the chemical potential EF is tuned at a vHs associated with the gradual transformation of the second Fermi surface from a two-dimensional (2D) cylinder to a closed surface with three dimensional (3D) topology characteristics of a superlattice of metallic layers...
Luther, P. K., and Squire, J. M. (1980). Three-dimensional structure of the vertebrate muscle A-band. II. The myosin filament superlattice. / Mol. Biol. 141,... [Pg.83]

Luther, P. K., and Squire, J. M. (1980). Three-dimensional structure of the vertebrate muscle A-band. II. The myosin filament superlattice./. Mol. Biol. 141, 409-439. Luther, P. K., and Squire, J. M. (2002). Muscle Z-band ultrastructure Titin Z-repeats and Z-band periodicities do not match./. Mol. Biol. 319, 1157-1164. [Pg.251]

Redl, F. X., Cho, K. S., Murray, C. B. O Brien, S. Three-dimensional binary superlattices of magnetic nanocrystals and semiconductor quantum dots. Nature (London) 423, 968—971 (2003). [Pg.238]

In general, unlike for the perfect epitaxial structures of fully strained materials, for nitride heteroepitaxial layers it is essential to perform not a single scan for a symmetrical reflection, but a set of two- or even three-dimensional maps of symmetrical and asymmetrical reflections. Additionally, for some applications, an intense beam is needed and therefore low-resolution X-ray diffractometry can be sometimes a preferable technique to the commonly used high-resolution XRD. For example, if we examine a heterostructural nitride superlattice, low resolution diffractometry will give us a broader zeroth-order peak (information on the whole layer) but more satellite peaks (information on the sublayers). Therefore, multipurpose diffractometers with variable configurations are the most desirable in nitride research. [Pg.254]

Fig. 21.4 Temperature dependencies of normalized Raman intensities of TO2 (solid triangles) and TO4 (open triangles) phonons for (a) SLs [(BaTi03)2(SrTi03)4] x 40 and [(BaTi03)5(SrTi03)4] x 25 (b) SLs [(BaTi03)g(SrTi03)4] x 40 and [(BaTi03)8(SrTi03)4] x 10. The dash-dotted lines are fits to linear temperature dependence, (c) and (d) - three-dimensional phase-field model calculations of polarization as a function of temperature in the same superlattice... Fig. 21.4 Temperature dependencies of normalized Raman intensities of TO2 (solid triangles) and TO4 (open triangles) phonons for (a) SLs [(BaTi03)2(SrTi03)4] x 40 and [(BaTi03)5(SrTi03)4] x 25 (b) SLs [(BaTi03)g(SrTi03)4] x 40 and [(BaTi03)8(SrTi03)4] x 10. The dash-dotted lines are fits to linear temperature dependence, (c) and (d) - three-dimensional phase-field model calculations of polarization as a function of temperature in the same superlattice...
Fig. 21.5 Tc dependence on layer thicknesses n and m in superlattices (BaTi03) / (SrTi03) j. Blue triangles and red circles are for m = 4 and m = 13, respectively. Open squares show the values obtained from variable temperature X-ray diffraction measurements. Solid lines are from the three-dimensional phase-field model calculations, dashed lines -simulations assuming a single domain in the BaTi03 layers. The dash-dotted line shows in bulk BaTi03 (After Li et al. [150])... Fig. 21.5 Tc dependence on layer thicknesses n and m in superlattices (BaTi03) / (SrTi03) j. Blue triangles and red circles are for m = 4 and m = 13, respectively. Open squares show the values obtained from variable temperature X-ray diffraction measurements. Solid lines are from the three-dimensional phase-field model calculations, dashed lines -simulations assuming a single domain in the BaTi03 layers. The dash-dotted line shows in bulk BaTi03 (After Li et al. [150])...
The way in which the nanocrystals organize themselves depends critically on the core diameter, the nature of the ligand, substrate and even the dispersive medium used [101]. Thiolized metal nanocrystals readily arrange into two-dimensional arrays on removal of the solvent [29]. Using suitable methods, they can also be put into one-dimensional organization in the form of strings or assembled in a stepwise fashion in a three-dimensional superlattice (see Figure 4.8). [Pg.61]

Fig. 4.15. Three-dimensional superlattices of 4.8 nm CdSe nanocrystals (a) along orientation (b) along <101) orientation (c) along orientation. High resolution... Fig. 4.15. Three-dimensional superlattices of 4.8 nm CdSe nanocrystals (a) along orientation (b) along <101) orientation (c) along <m> orientation. High resolution...
The distance between metal ion clusters and the orientation of the clusters in zeolite cages depends on the zeolite hosts, and as a result the three-dimensional arrays can be described in different ways. They can be called cluster crystals or superlattices. The Na/ Na-Y cluster crystal formed by accommodation of one Na43+ cluster in each sodalite cage is written as in Equation (9.2) ... [Pg.610]


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