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1 aterials with a twist and/or a difference in lattice constant.
2  due to their similar material chemistry and lattice constant.
3 ced a dose-related decrease in the hexagonal lattice constant.
4 s whose size can be controlled by tuning the lattice constant.
5 antized in odd multiples of the Si substrate lattice constant.
6  particle array have an approximately 200-nm lattice constant.
7 charge filling (the level of doping) and the lattice constant.
8 ty once surpassing the host crystal's atomic lattice constant.
9 (c) values correlating with smaller in-plane lattice constants.
10 al crystals with a variety of symmetries and lattice constants.
11  laminar growth, despite a large mismatch in lattice constants.
12  CH(3)-groups in a square arrangement with a lattice constant 0.55 nm from which we can identify abru
13 erials engineered to have artificially large lattice constants(4-6), such as those with moire superla
14 hick TiO2 simple cubic photonic crystal with lattice constant 450 nm was fabricated and used to exper
15 ck PhC's, first an Inverted Pyramid PhC with lattice constant a = 2,500 nm and second a Teepee PhC wi
16 es in a body-centered cubic lattice with the lattice constant a = 3.41(1) angstrom and exhibits phono
17 e paths l(mfp) shorter than their spin moire lattice constant a(spin), inhibiting miniband formation.
18                                     33) with lattice constants a = 11.8653(11) A, b = 5.8826(6) A, c
19                                     60) with lattice constants a = 8.3155(7), b = 13.3176(11), c = 11
20 rmal to the fiber (a-axis) direction, having lattice constants a = 9.69 A, b = 6.54 A, and c = 18.06
21  This observation is enabled by a very small lattice constant (a = 50 nm) of the nanofabricated AG pa
22 ted photonic crystals with a 5x reduction in lattice constants, achieving sub-100-nm features with a
23 reported nanolattice is the 500 nm unit-cell lattice constant, allowing the film to behave more like
24 repeat distance between them matches the ice lattice constant along the (1102) direction.
25 er unit layer, e(2)/ha(z), where a(z) is the lattice constant along the surface normal.
26  determine the array geometry, including the lattice constant and arrangement.
27  plasma frequency red-shifts with increasing lattice constant and blue-shifts as the network filling
28 The cell's dynamic control over the apparent lattice constant and dielectric contrast of these multil
29      Photomodulation of pitch, polarization, lattice constant and handedness inversion of chiral LCs
30                The WC possesses the expected lattice constant and is robust between filling factor nu
31 th increasing film thickness, affecting both lattice constant and MnO6 octahedral rotation.
32 two Pt(111) surfaces, one at the equilibrium lattice constant and the other laterally compressed by 2
33 growth, largely free from the constraints of lattice constant and thermal expansion coefficient misma
34 culations for the HEA structural properties (lattice constants and bulk moduli), relative stability,
35 based on the comparison between experimental lattice constants and lattice constants mainly obtained
36 hin 3D plasmonic photonic crystals that have lattice constants and nanoparticle diameters that can be
37 f their response as a function of changes of lattice constants and refractive index contrast are illu
38 try of the molecular distribution (i.e., the lattice constant) and the photophysics of fluorophores (
39 igher carrier mobilities than Si, a tuneable lattice constant, and a tuneable bandgap.
40 h the Cu-O bonds, with a periodicity of four lattice constants, and exhibits features characteristic
41 auses localization of electrons within a few lattice constants, and highlight the critical need for p
42 e transformation is solely determined by the lattice constants, and the conditions proposed for geome
43 ped to target desired lattice symmetries and lattice constants, and the occurrence of features such a
44 nd-triply periodic minimal surface geometry (lattice constant, approximately 30 micrometers), the [11
45  have similar crystallographic structure and lattice constants as NiFe2 O4 .
46 that cubic CdE and HgE have nearly identical lattice constants but very different band gap energies a
47 4) (M = Co/Fe) octahedral distortion and the lattice constant c.
48  constructed from expanded oxide rows with a lattice constant close to that of alpha-PtO2, either ass
49                               Therefore, the lattice constant contraction along this unique orientati
50 at the thinnest films are constrained to the lattice constants corresponding to the temperature at wh
51  evident from significant differences in the lattice constants, crystal packing, and overall conforma
52 dic one-dimensional diffraction grating with lattice constant d will be spatially refocused at distan
53 Cl, the dose-related change in the hexagonal lattice constant decreased but persisted.
54 e possessed by Ba(2)NaIO(6) and have similar lattice constants despite the nominally larger size of A
55 ic uniaxial heterostrain, which introduces a lattice constant difference in twisted homobilayers, lea
56 h-BN) have similar crystal structures with a lattice constant difference of only 2%.
57           However, constraining the in-plane lattice constants diminishes the energy gain associated
58 As the dimensionality of SCO is reduced, the lattice constant elongates over 10% along the growth dir
59                               The calculated lattice constants, equation of states, and atomic coordi
60 , if the relative difference between the two lattice constants for a specific material is greater tha
61 n the in-plane In(2)Se(3) and Fe(3-x)GeTe(2) lattice constants for both voltage polarities.
62 tion takes place when increasing the lateral lattice constant from a(LAO) to a(LNO).
63 pitaxy, the mismatch in lattice polarity and lattice constants has been limiting the quality of the g
64 (E(o)) ranging from 0.8 to 1.2 eV at a fixed lattice constant identical to that of Ge, as required fo
65 strain due to mismatch in the film-substrate lattice constants, (ii) possible variations in the bond
66 ry was obtained from the measurements of the lattice constant in the AFM images and from gel electrop
67   Peptide-induced Q(II) had strongly reduced lattice constants in comparison to the Q(II) phases that
68 roximately 8-10 A (where a, b, and c are the lattice constants in the H-bonding, chain, and intershee
69  a periodicity nearly commensurate with four lattice constants in-plane, eight out of plane, with lon
70 d charge separation, in contrast to a global lattice constant increase and lattice angle variations a
71 ng film thickness and the estimated in-plane lattice constant increasing with the film thickness.
72 stalline and perfectly epitaxial layers with lattice constants intermediate between those of Ge and a
73 observed InP concentration dependence of the lattice constant is closely reproduced by DFT simulation
74 , solid solution of ZrTiN was formed and the lattice constant is increased comparing with TiN and dec
75 n between experimental lattice constants and lattice constants mainly obtained from Materials-Project
76                   Defects and incommensurate lattice constants markedly change these properties.
77 hrates are energetically stable with relaxed lattice constants matching the experimental data.
78 o layered materials with a relative twist or lattice constant mismatch.
79  a two-dimensional triangular lattice with a lattice constant of 17 angstroms.
80        The square-like superstructure with a lattice constant of 2.68 nm features a periodic modulati
81 Square ice has a high packing density with a lattice constant of 2.83 A and can assemble in bilayer a
82 , crystallizes in space group Pm3n and has a lattice constant of 20.1994(9) angstrom at 130 degrees C
83                        However, the observed lattice constant of 5 nm was much larger.
84 nts of resistivity (here, a = 0.3 nm, is the lattice constant of Au).
85 nd band gaps of 41 and 38 meV at the lateral lattice constant of LaAlO(3), respectively.
86 , whose displacement distributions match the lattice constant of QDs, suggesting that the gold electr
87 ive voltage was applied; and (iv) the c-axis lattice constant of the film did not change in spite of
88 lts presented show how the modulation of the lattice constant of the LCP (triggered by the addition o
89 uctures can be tuned to 5.3% by altering the lattice constant of the matrix material, illustrating th
90                                              Lattice constant of the planar Sb honeycomb is found to
91  resonant wavelength is tuned by varying the lattice constant of the top perturbation layer.
92 acile formation of Im3m and Pn3m phases with lattice constants of 30-50 nm and 25-30 nm, respectively
93 the intrinsically distinct symmetries and/or lattice constants of each layer.
94  will be shown that the mismatch between the lattice constants of the nucleating crystal and the subs
95 ystem can be directly tuned by adjusting the lattice constants of the phases.
96 ces(6) because of the difference between the lattice constants of the two materials.
97  0.1% and 62 degrees C, but no change in the lattice-constants of the lamellar or cubic phases.
98 e formed by layer stacking without regard to lattice constants or symmetries of individual building b
99 tivity as the mean free path drops below the lattice constant, or as T -> 0, can be imperceptible, su
100 erior description of experimental values for lattice constants, polarization and bulk moduli, exhibit
101 otal plane and proved that the change in the lattice constant produced by the proteins resulted from
102 well suited for this task as their increased lattice constant provides access to intra-unit-cell phys
103 found to be epitaxial, with the out-of-plane lattice constant showing unanticipated decrease with inc
104                                It also has a lattice constant similar to that of graphite, and has la
105 tions reveal that the tuning of the in-plane lattice constant strongly modifies the interlayer magnet
106  the proteins had no effect on the hexagonal lattice constant, suggesting that the proteins fail to i
107 tria-stabilized zirconia substrates and have lattice constants that are a few percent larger than tha
108                  We show how to optimize the lattice constant to achieve efficient phase matching bet
109 ound state of LSMO is ferromagnetic, a large lattice constant together with an excess of La can stabi
110 d contracts with temperature; thus the array lattice constant varies with temperature, and the diffra
111                           By controlling the lattice constants, we tune the hopping amplitude and lon
112         This results in changes in the IPCCA lattice constants, which shifts the wavelength of light
113 ic arrays for different level structures and lattice constants, within the scope of currently realise

 
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