ライフサイエンスコーパス: face-centered cubic

1 s are atypical for PBAs, which are typically face centered cubic.

2 s are atypical for PBAs, which are typically face centered cubic.

3 free from disorder, unlike the well-studied face-centered cubic A3C60 alkali metal fulleride superco

4 dynamics simulations, to elucidate a twinned face-centered-cubic alloy in an experiment with hardness

5 the six <100> preferred growth directions in face centered cubic alloys.

6 bute the deformation mechanism of metastable face-centered cubic alloys to unstable martensite fault

7 ndentation strain rates (10(4) s(-1)), using face-centered cubic aluminum and body-centered cubic mol

8 truncated octahedral grains into fully dense face-centered cubic and body-centered cubic "granular cr

9 nontrivial behavior due to the existence of face-centered cubic and body-centered cubic crystal stru

10 istributions are controlled by motion of the face-centered cubic and body-centered cubic phase bounda

11 Herein, we report how face-centered-cubic and hexagonal close-packed structure

12 on from an ordered monoclinic structure to a face-centered-cubic arrangement of orientationally disor

13 NpN(2) crystallizes in a face-centered cubic CaF(2)-type structure with a space g

14 e. the body-centered cubic AlCoMnNiV and the face-centered cubic CoFeMnNiZn, which are successfully s

15 hemical ordering in nearly random equiatomic face-centered cubic CoFeNi solid solution.

16 stabilize the Au{111} to fulfill a complete face-centered-cubic core.

17 The data were consistent with a face-centered cubic crystal having a unit crystal cell s

18 Twin nucleation in a face-centered cubic crystal is believed to be accomplish

19 the swap motion is a phonon eigenmode of the face-centered cubic crystal structure of Pb, and it is e

20 n form with the approximate periodicity of a face-centered cubic crystal, as the spontaneous product

21 The identification of new face-centered cubic crystallographic structure of Ru nan

22 k waves in three-dimensional 10-million atom face-centered cubic crystals with cross-sectional dimens

23 o this success, pure metals that freeze into face-centered cubic crystals with little to no activatio

24 s this fundamental question by examining the face-centered-cubic Cu-Zn alpha-brasses.

25 ty in bulk nanolayered composites of a model face-centered-cubic (Cu)/body-centered-cubic (Nb) system

26 Our predicted spectrum for the face-centered cubic delta phase agrees well with experim

27 ing metals inter-diffuse, ultimately forming face-centered-cubic equiatomic CoCrFeNi alloy.

28 aller grain size, and optimized fractions of face-centered cubic (f.c.c., gamma) and hexagonal close-

29 Ruthenium nanocrystals with both a face-centered cubic ( fcc) structure and well-controlled

30 The face centered cubic (fcc) alloy NiCoCrx with x approxima

31 alysis leads to asymptotic states resembling face centered cubic (FCC) and hexagonal close packed (HC

32 Electrodeposited Pt and CuO exhibited face centered cubic (fcc) and monoclinic crystal structu

33 e cubic (SC), body centered cubic (BCC), and face centered cubic (FCC) crystal structures and show th

34 Chemically disordered face centered cubic (fcc) FePt nanoparticles (NPs) show

35 corporation into the Pd lattice, the overall face centered cubic (FCC) lattice is maintained; however

36 Recent successes in forming different shaped face centered cubic (fcc) metal nanostructures has enabl

37 ften adopt the body centered cubic (bcc) and face centered cubic (fcc) structures.

38 he bead surface expressing a complete set of face centered cubic (fcc) surface structures represented

39 sition from cubic solid solution [denoted as face centered cubic (fcc)] structure to tetragonal inter

40 xperimental observations with a close-packed face-centered cubic (fcc) (111), hexagonal close-packed

41 mately proved the complete transformation of face-centered cubic (fcc) Ag-NPs into monoclinic Ag(2)S-

42 vis the archetypal dislocation mechanisms in face-centered cubic (FCC) and body-centered cubic (BCC)

43 n(6)Fe(34)Co(34)Ni(6) alloy, comprising both face-centered cubic (fcc) and hexagonal closed packed (h

44 ted a multiphase structure composed of major face-centered cubic (fcc) and minor hexagonal close-pack

45 to fabricate porous PhCs with an underlying face-centered cubic (fcc) arrangement.

46 composed of a hydrogel polymerized around a face-centered cubic (fcc) array of monodisperse, highly

47 iolate ligands and one sulfido ligand with a face-centered cubic (FCC) Au22 kernel.

48 e nC60-stir was a superstructure composed of face-centered cubic (fcc) close-packing of near-spherica

49 rtion (due to its larger atomic radius) in a face-centered cubic (FCC) CoFeNi solid solution, and a c

50 -methylbenzenethiol) nanocluster featuring a face-centered cubic (fcc) core in a square shape (edge l

51 s were used to create an interface between a face-centered cubic (FCC) crystal and its liquid.

52 thways between body-centered cubic (bcc) and face-centered cubic (fcc) crystal structures can be enco

53 ssembly of the base-centered cubic (bcc) and face-centered cubic (fcc) crystalline nanoparticle latti

54 tals: body-centered cubic (BCC) crystals and face-centered cubic (FCC) crystals.

55 ination of the phonon dispersion curves in a face-centered cubic (fcc) delta-plutonium-0.6 weight % g

56 Unlike the previously synthesized disordered face-centered cubic (fcc) FePt nanoparticles with diamet

57 overcome the strength-ductility tradeoff in face-centered cubic (FCC) high-entropy alloys (HEAs).

58 dening ability and fracture toughness of the face-centered cubic (fcc) high-entropy alloys render the

59 ns of icosahedral (Ih), decahedral (Dh), and face-centered cubic (fcc) isomers within a set of popula

60 Face-centered cubic (fcc) lattice is the only known crys

61 g, which is the Delaunay tessellation of the face-centered cubic (fcc) lattice, and its closely relat

62 med the nature of single supercrystal with a face-centered cubic (fcc) lattice.

63 -bridged honeycomb structure consisting of a face-centered cubic (fcc) matrix and an interwoven hexag

64 e growth is developed and applied to a model face-centered cubic (fcc) metal that undergoes phase tra

65 in plastic deformation of low stacking-fault face-centered cubic (Fcc) metals but rarely found in bod

66 We observed solid compressed face-centered cubic (fcc) Ni up to at least 332 +/- 30 G

67 into superlattice (SL) allotropes of either face-centered cubic (fcc) or body-centered cubic (bcc) s

68 local atomic structure is consistent with a face-centered cubic (fcc) or Marks decahedral arrangemen

69 izes in the space group R3 and adopts pseudo face-centered cubic (fcc) packing, whereas other MOSCs,

70 behavior of lattice dislocations for the SI face-centered cubic (fcc) phase.

71 atomic volume, cerium adopts three distinct face-centered cubic (fcc) phases driven by different phy

72 hexagonal close-packed (hcp) and metastable face-centered cubic (fcc) phases, respectively, regardle

73 ing between hexagonal close-packed (hcp) and face-centered cubic (fcc) sites, was seen when the tip w

74 e nanoparticles do not show the bulk iridium face-centered cubic (fcc) structure but show decahedral

75 ditions, high-entropy alloys (HEAs) with the face-centered cubic (FCC) structure have drawn enormous

76 Among these, equatomic CrMnFeCoNi with the face-centered cubic (FCC) structure is noteworthy becaus

77 re transformation from chemically disordered face-centered cubic (fcc) structure to chemically ordere

78 noble metal typically stable as a solid in a face-centered cubic (FCC) structure under ambient condit

79 ple, LaH10 is found to adopt a sodalite-like face-centered cubic (fcc) structure, stable above 200 GP

80 re to an intermediate gamma-phase, then to a face-centered cubic (fcc) structure, while others instea

81 Gold is well known to adopt face-centered cubic (fcc) structure.

82 duced Frank loops can unveil their nature in face-centered cubic (fcc) structure: Circular loops are

83 NCs with dense ligand coverage assemble into face-centered cubic (fcc) superlattices whereas NCs with

84 structure from body-centered cubic (BCC) to face-centered cubic (FCC) through a series of body-cente

85 triggering a localized phase transition from face-centered cubic (FCC) to hexagonal close-packed (HCP

86 It is face-centered cubic (fcc) to low temperatures with Na(+)

87 of this hypothesis requires the synthesis of face-centered cubic (fcc) trivalent fulleride anion salt

88 gy, simple cubic, body-centered cubic (bcc), face-centered cubic (fcc), and cesium chloride (CsCl)-ty

89 ydride nanoparticle, a structure that is not face-centered cubic (fcc), formed through coreduction of

90 c (bcc), body-centered tetragonal (bct), and face-centered cubic (fcc)--as confirmed by synchrotron s

91 The actual ground state is face-centered cubic (fcc).

92 S NCs in toluene self-assemble into a single face-centered-cubic (fcc) and body-centered-cubic (bcc)

93 d, we characterize SRO in three CoCrNi-based face-centered-cubic (FCC) MPEAs.

94 the transformation of Pd nanomaterials from face-centered-cubic (fcc) phase into amorphous phase wit

95 depletion of dislocations from submicrometer face-centered-cubic (FCC) pillars provides a plausible e

96 revealed, in which the original single-phase face-centered-cubic (FCC) structure partially transforms

97 nner core has a monotwinned/stacking-faulted face-centered-cubic (fcc) structure.

98 oparticle ligands; these NCTs initially form face-centered-cubic (FCC) structures in solvents that ar

99 iously reported body-centered cubic (BCC) or face-centered-cubic (FCC) types, the major structure was

100 s a ligand-deficient layered analogue of the face-centered cubic fcu UiO-67(Hf).

101 h the organic linker and the metal node in a face-centered cubic (fcu) MOF, we tune the adsorption of

102 lloy transformed upon hydrogenation into the face-centered-cubic fluorite Mg1-yTiyHx phase with favor

103 ca synthesized under typical conditions is a face-centered cubic Fm3m structure with 3-dimensional he

104 is a high-temperature phase which reverts to face centered cubic gold on cooling to 295 K.

105 ects that connect this layer to the adjacent face-centered cubic grains, we explain the geometric ori

106 rigins of fatigue strength in a large set of face-centered cubic, hexagonal close-packed, and body-ce

107 alloy (MEA) featuring a fully recrystallized face-centered cubic/hexagonal close-packed dual-phase ul

108 mmetry, which reduces the frustration of the face centered cubic lattice of Os(VI) ions.

109 preferably interact with vacant sites of the face-centered cubic lattice above the metal surface.

110 s, it has only recently been proved that the face-centered cubic lattice has the highest possible pac

111 cies that move freely in three dimensions, a face-centered cubic lattice is best.

112 hedral structure, which is a fragment of the face-centered cubic lattice of bulk gold with a small st

113 rystals arranged within a silica matrix in a face-centered cubic lattice with cell dimensions that ar

114 of the four possible 111 glide planes in the face-centered cubic lattice, begins with junction format

115 del or backbone model on either the cubic or face-centered cubic lattice.

116 nd the X-ray structure is best-fitted onto a face-centered cubic lattice.

117 aining a truncated octahedral core with bulk face-centered cubic-like arrangement, yet a nanomolecule

118 uring the FSA process, grains of the as-cast face-centered cubic matrix were refined by high-temperat

119 = 1,4,8,11-tetraazacyclotetradecane) afford face-centered cubic [(Me(3)tacn)(8)Mo(8)Ni(6)(CN)(24)](1

120 Iridium is unique among the face-centered cubic metals in that it undergoes brittle

121 The (643) and (six four three) planes of face-centered cubic metals such as Cu have kinked and st

122 These observations in two dissimilar face-centered cubic metals suggest that strain recovery

123 winning should thus be highly unfavorable in face-centered cubic metals with high twin-fault energy b

124 e evolution of plasticity in heavily twinned face-centered cubic metals, with the potential for optim

125 cubic nanometer) tetradecahedral cavities in face-centered cubic metals.

126 tetrahedra (SFTs) are ubiquitous defects in face-centered cubic metals.

127 large as ~30%, at the same level of ductile face-centered-cubic metals.

128 bble growth arguably applies to various FCC (face-centered cubic) metals such as Au, Ag, Ni, and Al.

129 At further compressions and in face-centered cubic Na above 64 GPa, the linear relation

130 We illustrate these concepts with face-centered cubic nanocrystals, demonstrating diverse

131 S(*)R or involves direct binding of RS(*) to face-centered-cubic or hexagonal-close-packed sites.

132 In some oblate plasmas, a mixture of bcc and face-centered cubic ordering was seen.

133 Although pristine C60 prefers to adopt a face-centered cubic packing arrangement in the solid sta

134 ody-centered cubic phase, differing from the face-centered cubic phase of both bulk solid xenon and s

135 perature between 300 K and 4800 K), only the face-centered cubic phase of platinum has been observed.

136 ticle structure from a chemically disordered face-centered cubic phase to the chemically ordered face

137 y exploiting the decreasing stability of the face-centered cubic phase with increasing Mn content, we

138 However, stable non-face-centered cubic phases have not been reported in nob

139 l lattice may induce distortions to form non-face-centered cubic phases when the lateral dimensions o

140 ly 1 J/m(2), which is expected for bulk fcc (face centered cubic) silver.

141 CC SLs can undergo dynamic transformation to face-centered-cubic SLs in response to post-assembly mol

142 lloy, CrMnFeCoNi, which forms a single-phase face-centered cubic solid solution, and found it to have

143 lectron diffraction patterns of concentrated face-centered cubic solid solutions have been widely att

144 ll free energy difference separating it from face-centered cubic spheres usually results in phase coe

145 ent method, we show that the icosahedron and face-centered cubic SRO increase upon cooling.

146 few than three atoms energetically prefers a face-centered-cubic stacking, to serve as a nucleus of s

147 he crystal symmetry changes from a distorted face centered cubic structure to a lower symmetry orthor

148 even though the nucleus core is dominated by face-centered cubic structure corresponding to the stabl

149 entered cubic structure to 52 GPa and in the face-centered cubic structure from 64 to 97 GPa, and stu

150 to form crystalline silver nanoparticles of face-centered cubic structure with a mean size of 10 nm.

151 [Sb(0.76)I(6)](2).25H(2)O (HSbOI), forming a face-centered cubic structure with cationic Sb(32)O(44)

152 Both materials are nanocrystalline (face-centered cubic structure) and show reversible volta

153 clusters (NCs) in addition to the well-known face-centered cubic structure, including hexagonal close

154 structures in a stable single-phase HEA with face-centered cubic structure, thus resulting in enhance

155 EA) of CrMnFeCoNi is a solid solution with a face-centered cubic structure.

156 rming successful synthesis and a crystalline face-centered cubic structure.

157 eas along the nanowire axis, with a textured face-centered cubic structure.

158 Comparing it to similarly face-centered cubic-structured Au(36)(TBBT)(24), Au(44)(

159 in the high-symmetry crystal phase, such as face centered cubic structures, reducing the symmetry is

160 ess, of planar-extended core dislocations in face-centered cubic structures.

161 or proton-irradiated structural metals with face-centered cubic structures.

162 gle elements only, occupying three different face-centered-cubic sublattices.

163 toric stress drives SC(110) orientation in a face-centered-cubic supercrystal (SC), rocksalt (RS) NPs

164 d a strong tendency to form multiply twinned face-centered cubic superlattices with decahedral and ic

165 rns are observed on various superhydrophilic face-centered cubic surfaces.

166 6)(SR)(24) nanocluster reveals an unexpected face-centered-cubic tetrahedral Au(28) kernel (magenta).

167 chanisms of room temperature rolling induced face-centered cubic titanium (fcc-Ti) in polycrystalline

168 ystal exhibits a phase transformation from a face-centered cubic to a body-centered tetragonal struct

169 pted non-close-packed structures (e.g., from face-centered cubic to body-centered cubic) and changed

170 faults that change the local structure from face-centered cubic to hexagonal close packed.

171 displayed a superlattice transformation from face-centered cubic to lamellar structures, while no cle

172 cking faults, twins, transformation from the face-centered cubic to the hexagonal close-packed struct

173 e crystals, whereby a body-centered cubic to face-centered cubic transformation is found to proceed s

174 We studied a combination of eight face-centered cubic transition metals and 18 common surf

175 iates on two different facets of these eight face-centered-cubic transition metals, combined with a s

176 toms per primitive unit cell (1140 atoms per face-centered cubic unit cell).