ライフサイエンスコーパス: twist angle

1 quencies that are largely independent of the twist angle.

2 of hexagonal boron nitride stacked at small twist angle.

3 of moire excitons can be controlled via the twist angle.

4 ode whose coupling increases with decreasing twist angle.

5 istance, which is tuneable by the interlayer twist angle.

6 ulator at moire half-filling over a range of twist angle.

7 t density, are examined as a function of the twist angle.

8 oire potential that can be controlled by the twist angle.

9 of GB character, defined in this work by the twist angle.

10 nfigurations, for example via control of the twist angle.

11 (MoSe(2)/WSe(2)) heterobilayer with a small twist angle.

12 sional moire optics through variation of the twist angle.

13 nked arylene diimide dimer with a 76 degrees twist angle.

14 on between the layers is at a photonic magic twist angle.

15 t potential changes in bend angle as well as twist angle.

16 perpendicular electric fields in a range of twist angles.

17 boratory frame as a function of the tilt and twist angles.

18 mise unique properties with their 90 degrees twist angles.

19 of twisted bilayer WSe(2) (tWSe(2)) at small twist angles.

20 moire physics beyond those formed with small twist angles.

21 ch parallel laminae are stacked with varying twist angles.

22 es of the structures, particularly for small twist angles.

23 bilayer has a type I band alignment at large twist angles.

24 in WSe(2)/WS(2) heterostructures with large twist angles.

25 bilayer graphene devices with highly uniform twist angles.

26 atomically sharp interfaces with a range of twist angles.

27 -systems and sterically regulated inter-aryl twist angles.

28 smaller but constant redshift for all other twist angles.

29 s available on the distribution of the local twist angles.

30 nd the receptor, but showed variation in D23 twist angles.

31 ive Poisson's ratios can be tuned by the pre-twisting angles.

32 s physical parameters by adjusting the layer twist angle(1-3), electrical field(4-6), moire carrier f

33 der Waals heterostructures with a controlled twist angle(1-3)-enable the engineering of electron band

34 ectronically decoupled from them via a large twist angle (~10-30 degrees ).

35 G2*U16 and U7*G11/C8*G10, while the smallest twist angles (28.24 and 27.27 degrees ) are at G2*U16/G3

36 The largest twist angles (37.70 and 40.57 degrees ) are at steps G1*

37 rmations appear clearly separated by a large twist angle (~40 degrees ) and depend mainly on the comp

38 gles are better hydrated than steps with low twist angles, 6.9 H2O vs 0 H2O; negative roll angles are

39 r excitons near the commensurate 21.8-degree twist angle(7).

40 superconductor-insulator transition at magic twist angles(8).

41 hromophores reveals large ring-ring dihedral twist angles (80-89 degrees) and a highly charge-separat

42 featuring three rows of KSM at a 30 degrees twist angle, achieving a 1.6-fold increase in the Sherwo

43 as the enforcement of consecutive 90 degrees twist angles along the polyimide backbone.

44 A bilayer graphene stack featuring a tunable twist angle and a tubular edge connection between the la

45 ene moire superlattice depend sensitively on twist angle and are completely different from those in t

46 The twist angle and base roll combine to significantly affec

47 e construct a phase diagram as a function of twist angle and displacement field, incorporating intera

48 nge of 0.4 eV, expanding the combinations of twist angle and doping where they can be placed at the F

49 stortions may be exploited to manipulate the twist angle and interfacial strain in bulk heterostructu

50 ndence of exciton oscillator strength on the twist angle and interlayer coupling is analyzed.

51 rs in the filament was optimized in terms of twist angle and local packing using Rosetta.

52 nsitions are highly tunable also by choosing twist angle and material combination our results open up

53 exes are further sensitive to the interlayer twist angle and offer opportunities to explore emergent

54 aged vibrational amplitudes as a function of twist angle and position.

55 iption of the evolution the moire bands with twist angle and reveals the topological nature.

56 ically switched only over a limited range of twist angle and sample hetero-strain values.

57 Beyond twist angle and strain, the dependence of the TBG phase

58 ty of the correlated ground states and local twist angle and strain.

59 ce of these interlayer exciton resonances on twist angle and temperature.

60 states that are highly sensitive to both the twist angle and the application of an electric displacem

61 a and constant phase, is tunable by both the twist angle and the illumination frequency.

62 phonon dynamics in MoS(2)/WS(2) at 4 degrees twist angle and WSe(2)/MoSe(2) heterobilayers with twist

63 This causes a decrease in the inter-ring twist angle and, together, these changes are responsible

64 us or heterogeneous 2D layers stacked with a twist angle and/or lattice mismatch.

65 superconductivity in a significant range of twist angles and fillings.

66 formations and causes distortions in related twist angles and helical rises.

67 erogeneous interactions can we reproduce the twist angles and related properties.

68 tions also indicate that the actin propeller twist-angle and nucleotide cleft-angles are influenced b

69 st angle, spatial inhomogeneity in the local twist angle, and distortions caused by random strain.

70 ice resistance peaks, tunable by varying the twist angle, and Hofstadter butterfly physics under a ma

71 degrees C</=T</=198 degrees C) and bicrystal twist angle, and insensitive to impurities from the atmo

72 moire potential is primarily governed by the twist angle, and its dynamic tuning remains a challenge.

73 frontier bands change sign as a function of twist angle, and this change is driven by the competitio

74 crystals by varying the number of layers and twist angles, and by using different two-dimensional com

75 d, pristine interfaces, precisely controlled twist angles, and macroscopic scale (up to centimeters)

76 chains, as evidenced by the decrease in the twist-angle, and consequent increase in the cholesteric

77 Our results could enable the exploration of twist-angle- and electric-field-controlled correlated ph

78 The presence of the bulge induces very large twist angles (approximately +50 degrees) between the bas

79 e pairs, 2.5 H2O vs 1.3 H2O; steps with high twist angles are better hydrated than steps with low twi

80 ons reveal that energy fluctuations at small twist angles are dominated by an interference-like inter

81 The twist angles are reversed (37 degrees and 26 degrees) in

82 al phases can form only for a small range of twist angles around the magic angle, which further diffe

83 These results establish twist angle as an effective way to control energy relaxa

84 monolayer and bilayer phosphorene even for a twist angle as large as 19 .

85 significant changes in the opening, roll and twist angles as compared to the normal A:T base pair.

86 s with frequencies strongly dependent on the twist angle, as well as resonances with frequencies that

87 For larger twist angles, Au has only a small misorientation with th

88 magnetic coupling and estimate the critical twist angle below which moire magnetism with mixed ferro

89 the correlated phases in bilayer WSe(2) with twist angle between 2 and 3 degrees.

90 Recently, the twist angle between adjacent sheets of stacked van der W

91 A remarkable example is the control over the twist angle between artificially-stacked vdW crystals, e

92 multilayer graphene by the introduction of a twist angle between different layers to create van Hove

93 Techniques to control the twist angle between graphene layers have led to rapid ex

94 The relative twist angle between layers of near-lattice-matched van d

95 rization and is only weakly dependent on the twist angle between layers.

96 While twist angle between the bilayer has been shown to be a c

97 Such reconstruction strongly depends on the twist angle between the crystals, which has received gro

98 nversion efficiency from 2.6% to 6.4% as the twist angle between the monomeric building blocks in the

99 (11+) was used to gauge the influence of the twist angle between the p-orbital at Si+ and the C-Si bo

100 re of the RNA is characterized by a very low twist angle between the two G.U base-pairs, providing a

101 ve singularities whose energy depends on the twist angle between the two layers.

102 ance is expected to change with the relative twist angle between the two rings, with the planar confo

103 The twist angle between the wobble pairs, 38.1 degrees, is a

104 onal boron nitride (hBN), formed by a minute twist angle between two hBN monolayers assembled on a gr

105 ng field of twistronics, which harnesses the twist angle between two-dimensional materials, represent

106 Yet, ortho branching causes large twist angles between the core and the arms that are detr

107 ls form mobile bulges causing a variation of twist angles between the helix pairs.

108 atomic periodicities, which can be tuned by twist angles between the layers, leading to moire-of-moi

109 the aromatic bridges gradually increases the twist angles between the two PDI planes, leading to a va

110 ray scattering, respectively, from which the twist-angle between DNA molecules can be calculated.

111 Manipulating the 'twist angle' between the two layers enables fine control

112 re excitons robust in bilayers of even large twist angles, but also properties of the moire excitons

113 thin van der Waals crystals with a relative twist angle can give rise to notable new physical proper

114 er than the imaginary part, with the highest twist angle chromophore giving |Re(gamma)/Im(gamma)| app

115 nce for the series decreases with increasing twist angle, consistent with a cosine-squared relation p

116 way for manipulating 2D magnetism with layer twist angle control.

117 ional plasmonic nanoparticle lattices enable twist-angle-controlled directional lasing emission, even

118 Twist-angle-controlled interlayer electronic hybridizati

119 antiferromagnetic (AF) ground state in small-twist-angle CrI(3) bilayers.

120 This novel twist angle degree of freedom and control should be gene

121 Here, we report a strong twist-angle dependence of heterogeneous charge transfer

122 From the twist-angle dependence, we furthermore obtain the effect

123 attracted growing interest due to its unique twist-angle-dependent electronic properties.

124 ces in which electrons directly experience a twist-angle-dependent periodic potential.

125 ent is attributed to the emergence of unique twist-angle-dependent van Hove singularities, which are

126 The reduction in twist-angle disorder reveals the presence of insulating

127 are particularly fragile with respect to the twist-angle disorder.

128 ts with the general band flattening at small twist angle due to the moire interference.

129 At extremely low twist angles (e.g. below 0.25 degrees ) the amplitude in

130 hermal properties that can be manipulated by twist-angle engineering.

131 etwork can be tuned by the adjustment of the twist angles, establishes TTG as a platform for explorin

132 f two graphene monolayers with an interlayer twist angle, exhibits a strong light-matter interaction

133 relaxation introduces an array of localized twist-angle faults, termed twistons and moire solitons,

134 We also identify twist angles favorable for quantum spin Hall insulators

135 temperature scanning tunneling microscopy at twist angles for which superconductivity has been observ

136 junctures, only slightly relaxes the biaryl twist angle from 89.6 degrees to approximately 80 degree

137 om 46 degrees to 22 degrees ), inter-helical twist angle (from 66 degrees to -18 degrees ), and inter

138 HSs in bilayer graphene over a wide range of twist angles (from 5 degrees to 31 degrees ) with wide t

139 ntional type of disorder enabling the use of twist-angle gradients for bandstructure engineering, for

140 recent focus on manipulating the interlayer twist angle has led to the observation of out-of-plane r

141 that can be precisely controlled through the twist angle have emerged as exciting platforms for study

142 uous variation of twist angles with improved twist-angle homogeneity and reduced random strain, resul

143 stic constant K2 and for assessing the total twist angle in a standard nematic twist cell.

144 ir evolution are systematically studied with twist angle in bilayer and trilayer graphene sheets.

145 NOE NMR measurements of the twist angle in solution confirm that the solid-state twi

146 y-layer stacking, yet controlling interlayer twist angles in a bulk solid remains an outstanding chal

147 te the evolution of interlayer coupling with twist angles in as-grown molybdenum disulfide bilayers.

148 tigate moire band topology across a range of twist angles in both materials.

149 ries have been observed in tDBG devices with twist angles in the range 1.2-1.3 degrees , but the topo

150 ion of van der Waals structures with defined twist angles, in which interlayer moire patterns are rea

151 The twist angle increases with the increase of deformation a

152 found that differences in electric field and twist angle induced trends in exciton transition strengt

153 for the design of quantum materials, as the twist-angle-induced superlattices offer means to control

154 fer from low efficiency and reproducibility, twist angle inhomogeneity, interfacial contamination, an

155 Close to a magic twist angle, insulating behavior is observed, which give

156 The dependence of the TMR on the twist angle is calculated from the electron-parallel mom

157 When the twist angle is near 60 degrees , no such correlations ar

158 c velocity crosses zero several times as the twist angle is reduced.

159 The twist angle is significantly altered by the interaction

160 stematic experimental study as a function of twist angle is still missing.

161 e TS structure of ribozyme reaction while no twisted angle is found in TS of the reaction in water.

162 o Bernal bilayer graphene are stacked with a twist angle, is such a moire system with tunable flat ba

163 We induce superconductivity at a twist angle larger than 1.1 degrees -in which correlated

164 d EPC of twisted bilayer graphene (TBG) with twist angles larger than 6 degrees .

165 he Raman G peak area initially increases for twist angles larger than a critical angle and decreases

166 van der Waals bilayers(1-4) created at small twist angles lead to a long wavelength pattern with appr

167 soscopic modulation of local strain and spin twist angles, leading to twisto-magnetic stripes, arises

168 In twisted bilayer graphene, at certain twist angles, long-range periodicity associated with moi

169 olanes exist, and they all suffer from small twist angles (<35 degrees ).

170 Enabled by the twist angle measurements of the spontaneous twist, we de

171 e dynamics, indicates a peak-to-trough local twist angle modulation of 0.6 degrees , correlated with

172 Here we use near-0 degrees -twist-angle MoSe(2)/MoSe(2) bilayers with large rhombohe

173 and the TBG stabilizes superconductivity at twist angles much smaller than the magic angle.

174 ce twisted double bilayer (TDB) WSe(2), with twist angles near 60 degrees , as a controllable platfor

175 At the average twist angle o ~ 1.56 , a theoretically predicted "magic

176 At small twist angle o, due to atomic reconstruction, the moire s

177 We reveal the rich physics at small twist angles o < 4( ), and identify a particular magic a

178 ree graphene layers stacked with alternating twist angles o.

179 anded supramolecular polymers with a helical twist angle of -26.7 per hexad are formed when the pure

180 ent at the WSe(2)/SiP heterointerface with a twist angle of 0 degrees , whose amplitude is electrical

181 For the smallest twist angle of 0.79 degrees, superconductivity is still

182 A twist angle of 12.2 degrees is selected such that the su

183 erizable conformation is its reduced helical twist angle of 22 degrees.

184 II (G x U/U x G) structure stack with a low twist angle of 25.3 degrees in contrast to that of motif

185 5'-side of the first C6.A27(+) wobble has a twist angle of 27 degrees compared to the 3'-side U7.A28

186 adopts a twisted backbone with an end-to-end twist angle of 28 degrees that was unambiguously confirm

187 t the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for al

188 rystal structure of 17 reveals that it has a twist angle of 45.2 degrees for the carbon-carbon double

189 the molecule's backbone, with an end-to-end twist angle of 51 degrees , consistent with computationa

190 a collinear FM ground state above a critical twist angle of about 3 .

191 a collinear FM ground state above a critical twist angle of about 3 degrees .

192 roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positio

193 roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positio

194 roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positio

195 At a twist angle of approximately 5 degrees, we find that hol

196 the same g-factor as the heterobilayer at a twist angle of approximately 60 degrees.

197 phenylimidazol-1-yl)purine nucleoside, and a twist angle of approximately 61 degrees was measured bet

198 gest that the CTD may constrain the relative twist angle of proteins within the ssDNA filament such t

199 y between the top and bottom MoS(2) when the twist angle of the bilayer is small (<~7 degrees ).

200 that varies approximately sinusoidally with twist angle of the bilayer MoS(2).

201 ent, achieved by adjusting the thickness and twist angle of the bilayer.

202 ees with respect to the surface normal and a twist angle of the CCC plane relative to the tilt plane

203 These results show that maps of the twist angle of the LC constructed from families of optic

204 he stack of images into a spatial map of the twist angle of the LC on the analytic surface.

205 different ring substitutions that alter the twist angle of the molecules.

206 ith the ruffling deformation and the average twist angle of the pyrrole rings.

207 0 mK, spontaneously formed in tWTe(2) with a twist angle of ~ 3(o).

208 twisted four-layer WS(2) at high interlayer twist angles of >=4 degrees .

209 ural relaxation of the moire superlattice at twist angles of <2 degrees , and 'topological defect' AA

210 t-handed or left-handed helical stacks, with twist angles of +15 or -15 per hexad, respectively.

211 s, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectiv

212 , -15.9 and 6.7, in samples with approximate twist angles of 60 degrees and 0 degrees, respectively.

213 angle and WSe(2)/MoSe(2) heterobilayers with twist angles of 7 degrees , 16 degrees , and 25 degrees

214 anophanes containing a malonyl tether, where twist angles of almost 80 degrees were reached.

215 G7 (roll angles of approximately 42 degrees, twist angles of approximately 16 degrees ), but is much

216 G7 (roll angles of approximately 20 degrees, twist angles of approximately 17 degrees).

217 At twist angles of approximately 20 degrees the emitters be

218 e layer with respect to the other at 'magic' twist angles of around 1 degree leads to the emergence o

219 Furthermore, the twist angles of the LC can be used to quantify the energ

220 At very small twist angles of ~0.1 degrees , bilayer graphene exhibits

221 he cell-wall polysaccharides lead to a fixed twisting angle of cellulose helicoids in the cell wall.

222 overies demonstrate that bilayers with large twist angles offer a design platform to explore moire ph

223 , such as twisted bilayer graphene by tuning twist angle or applying pressure, and trilayer graphene

224 etermining effects of nucleotide sequence on twist angle or rise at individual bp steps does not prov

225 ted properties without the need for invoking twist angles or moire domains.

226 lic rotation rate, P =0.05 and P =0.006; net twist angle, P=0.02) movement were significantly reduced

227 the remarkably strong moire physics in large-twist-angle phosphorene heterostructures.

228 ntinuum and can be made with widely tuneable twist angle, pitch, width, thickness and length.

229 re including base stacking energy, propeller twist angle, protein deformability, bendability, and pos

230 entation of their basal planes with a mutual twist angle ranging from 0 degrees to 60 degrees .

231 on of tBLGs in bilayer graphene domains with twist angles ranging from 0 to 30 was found to be improv

232 tion with electron density, temperature, and twist angle) showing good quantitative agreement with re

233 ge twist angles, while in samples with small twist angles, signals from two distinct long-lived excit

234 suffer from imprecise control of the average twist angle, spatial inhomogeneity in the local twist an

235 The twist angle strongly affects the electronic states, exci

236 esulting from correlated changes in bend and twist angles such that the p53-DNA tetrameric complex is

237 an be tuned over 235 meV by twisting, with a twist-angle susceptibility of 8.1 meV/ , an order of mag

238 Furthermore, in the regime of lower twist angles, TBBG shows multiple sets of flat bands nea

239 ppear over arrays of moire supercells in low-twist-angle tDT CrI(3).

240 bust chemical knob, and from the interphenyl twist angle that acts as a fine-tunable knob.

241 The filaments also exhibit random twist angles that are broadly distributed.

242 nnier orbital size of 15 nanometres and with twist angles that deviate slightly from the magic angle

243 agreement with our experiments that consider twist angles that vary from 0 degrees to 90 degrees .

244 extensive ab initio simulations, we identify twist angles that yield flat conduction bands, provide a

245 escribe DNA deformations (i.e., the bend and twist angles), the translational parameters describing t

246 To explain this behavior with twist angle, the energy separation of the van Hove singu

247 tudy, we demonstrate that in addition to the twist angle, the interlayer coupling can be varied to pr

248 wo sheets of graphene are stacked at a small twist angle, the resulting flat superlattice minibands a

249 For small twist angles, the material undergoes a self-organized la

250 In contrast, at small twist angles, there exist simultaneous spatially modulat

251 ling pairs of mono-twin films with a 'magic' twist angle theta(*) that provides commensurability betw

252 ted by a network of partial dislocations for twist angles theta < 2 degrees .

253 At large twist angles (theta(t)), moire patterns are, in general,

254 TBG)(1,2) crucially depend on the interlayer twist angle, theta.

255 recover a similar equation for the internal twist angle to that of classical vortex tubes.

256 n state geometry requires adjustment for the twist angles to those of the relaxed ground state to pro

257 ptical twisted bilayer photonic crystal with twist angle-tunable dispersion and great simulation-expe

258 by, the moire reciprocal lattice period via twist-angle tuning.

259 In the limit of small twist angles, two competing structural orders-rhombohedr

260 terostructures, the interference of multiple twist angles ubiquitously leads to tunable ultralong-wav

261 rgy superlattice structures as a function of twist angle using InterMatch.

262 e homobilayers, focusing on WSe(2), at small twist angles using a combination of first principles den

263 prominent in moire graphene, where at magic twist-angle values, flat bands feature [Formula: see tex

264 This potential disorder is distinct from the twist angle variation which has been studied elsewhere.

265 alley polarization for the specific range of twist angles we investigate, and instead may plausibly r

266 Near 45 degrees twist angle, we observe fractional Shapiro steps and Fra

267 three layers of graphene with two different twist angles, we form two mutually incommensurate moire

268 mension in a controlled setup by varying the twist angle, which provides an intriguing benchmark with

269 r MoS(2) single crystal with zero interlayer twist angle, which retains monolayer-like exciton proper

270 olarization of the same helicity for a given twist angle, which suggests that the trapping potential

271 ricate network of domain structures at small twist angles, which can harbour exotic electronic behavi

272 electron population in only MoSe(2) at large twist angles, while in samples with small twist angles,

273 tile DNA sublattices, achieving seed-defined twist angles with deviations below 2 degrees , along wit

274 s technique achieves continuous variation of twist angles with improved twist-angle homogeneity and r

275 ration continues to decrease with decreasing twist angle, with a lowest value of 7 to 13 millielectro

276 At small twist angles, ZrS(2) heterostructures give rise to an em