ライフサイエンスコーパス: twist

1 ngle-sided surface (e.g. by ends with a half-twist).

2 ructure (knitted, short staple fibers, lower twist).

3 lament, which exhibits an intrinsic bend and twist.

4 stics including structure, type of yarn, and twist.

5 compared with RS experienced increased mean TWiST.

6 ing the normal mode analysis, to a series of twists.

7 as a rigid ribbon that becomes flexible when twisted.

8 e switched off or inverted by conformational twisting.

9 lowing flexural deformation under bending or twisting.

10 petitive deformations, including bending and twisting.

11 fication of ovarian tumors based on CBX7 and TWIST-1 expression, which predicts clinical outcomes and

12 TWIST-1 is however transcriptionally nonfunctional in th

13 of CBX7 in sEOC was sufficient to reactivate TWIST-1-induced transcription, prompt mesenchymal transf

14 high expression of the mesenchymal effector, TWIST-1.

15 trans retinal in photoexcited bR to a highly twisted 13-cis conformation.

16 For twisted 2H bilayers, stable 2H domains dominate, with nu

17 For twisted 3R bilayers, a tessellated pattern of mirror-ref

18 le, a trefoil (3(1)) knot(6-15), and a three-twist (5(2)) knot-were each selectively prepared from th

19 -rebound mechanism in which the nucleophilic twisted amide is quaternized and subsequently ring-opene

20 affinities of a diverse set of Troger's base twisted amides and compare them with related nonplanar b

21 The first living polymerization of twisted amides is reported, achieved using simple primar

22 t may be formed as a result, including splay-twist analogues of blue phases.

23 Q-TWiST analyses were performed defining TOX as the mean d

24 e(1-) (x) Sn(x) S) nanoribbons with an axial twist and deep subwavelength thickness are demonstrated

25 ucleosome, coupling different degrees of DNA twist and DNA movement to distinct nucleotide-bound stat

26 Additional twist and pinch motions were observed in an open ORC con

27 assessed were Snail-1, Snail-2, N-cadherin, Twist and vimentin.

28 Our results highlight the importance of twist and writhe in unknotting processes, providing guid

29 The twist and writhe of these braided coils are coupled with

30 y generation and storage systems that can be twisted and folded to multiple deformations while retain

31 als, and hemithioacetals is demonstrated for twisted and planarized mechanophores in solution and mem

32 ctrochemical cell array can be readily bent, twisted and stretched without affecting its device perfo

33 trapped chromophore with characteristic ring twisting and bridge-H bending motions enables rational d

34 fferent structural motifs upon physiological twisting and stretching.

35 n this work, we demonstrate that in TBG, the twisting and substrate induced symmetry breaking allow a

36 can be applied to structures with different twists and number of layers.

37 no doubt the road ahead will reveal further twists and turns for this fascinating pathway crucial fo

38 Here, we follow the twists and turns on their road to success and highlight

39 G(2)/M arrest; reduced expression of Snail, Twist, and Notch1; and inactivated several profibrotic s

40 r aim was to assess LV cardiac mechanics, LV twist, and the prevalence of rigid body rotation, using

41 multiple conformations (i.e. J-elongated, S-twisted, and O-circular).

42 rbated foreshortening, SmartFlex exacerbated twisting, and SmartControl restricted bending of the FPA

43 d twisting; SmartFlex and Innova exacerbated twisting; and Supera and Viabahn restricted bending.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

68 Twist-angle-controlled interlayer electronic hybridizati

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

70 , -15.9 and 6.7, in samples with approximate twist angles of 60 degrees and 0 degrees, respectively.

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

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

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

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

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

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

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

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

79 perpendicular electric fields in a range of twist angles.

80 Mobius aromaticity was developed for twisted annulenes with electron counting rules opposite

81 of nucleosome motions such as breathing and twisting are enhanced in nucleosomes with multiple TF bi

82 ignment between adjacent layers ('interlayer twist') are of interest because of electronic structure

83 This is accompanied by an extra core twist, as the peripheral dihedral angle increases from 1

84 of baseline FPA foreshortening, bending, and twisting associated with each posture.

85 tifying and modeling the force-extension and twisting behavior of single ethidium-complexed DNA molec

86 create actuators that can extend, contract, twist, bend, and perform a combination of these motions

87 ence, niraparib treatment resulted in a mean TWiST benefit of 2.95 years and 1.34 years, respectively

88 e in the series of nonplanar amides are less twisted benzofused 1-azabicyclo[3.3.1]nonan-2-one deriva

89 e superlattice potentials from an interlayer twist between crystals(1,2).

90 han four-fold and two-fold increases in mean TWiST between niraparib and RS in the gBRCAmut and non-g

91 unit in the CT state instead of displaying a twist between the donor and acceptor; it is TICT-like.

92 layer graphene for certain 'magic' angles of twist between the orientations of the two layers(6).

93 We thus establish twisted bilayer GeSe as an intriguing inroad into the st

94 ds with topological character in magic-angle twisted bilayer graphene (MATBG) has created a unique op

95 ed and superconducting phases in magic-angle twisted bilayer graphene (MATBG)(1,2) crucially depend o

96 Magic-angle twisted bilayer graphene (TBG), with rotational misalign

97 Twisted bilayer graphene (tBLG) is a metallic material w

98 We report the observation of a QAH effect in twisted bilayer graphene aligned to hexagonal boron nitr

99 the spectroscopic properties of magic-angle twisted bilayer graphene as a function of electron filli

100 Magic-angle twisted bilayer graphene exhibits a variety of electroni

101 Recent experiments on twisted bilayer graphene have shown a high-temperature p

102 Twisted bilayer graphene is a key material in this regar

103 Twisted bilayer graphene near the magic angle(1-4) exhib

104 topological nature of the band structure of twisted bilayer graphene plays an important role in this

105 Our results demonstrate twisted bilayer graphene to be a distinctively tunable p

106 l doping on the electronic band structure of twisted bilayer graphene using a back-gated device archi

107 states and superconductivity in magic-angle twisted bilayer graphene(1,2) has enabled the experiment

108 correlated insulating states in magic-angle twisted bilayer graphene(1-11) prompts fascinating quest

109 topological insulators(3-9) and magic-angle twisted bilayer graphene(10,11).

110 Hall effect in the flat band of magic-angle twisted bilayer graphene(4-8) has sparked the exploratio

111 led view of the phenomenology of magic-angle twisted bilayer graphene, adding to our evolving underst

112 In twisted bilayer graphene, at certain twist angles, long-

113 Similarly to magic-angle twisted bilayer graphene, TDBG shows energy gaps at the

114 Unlike in 'magic angle' twisted bilayer graphene, theoretical calculations show

115 und states, in stark contrast to magic-angle twisted bilayer graphene.

116 y induce new correlated electronic phases in twisted bilayer graphene.

117 es emerge at low temperatures in magic-angle twisted bilayer graphene.

118 h spontaneous ferromagnetism was observed in twisted bilayer graphenes (TBG) near 3/4 filling.

119 nable correlated system based on small-angle twisted bilayer-bilayer graphene (TBBG), consisting of t

120 perconducting states observed in magic-angle twisted-bilayer graphene and ABC trilayer graphene/boron

121 tuning required to obtain the magic angle in twisted-bilayer graphene poses challenges to fabrication

122 red light for imaging moire superlattices of twisted bilayers graphene encapsulated by hexagonal boro

123 In particular, we analyze in detail twisted bilayers of Neel antiferromagnets on the honeyco

124 copy to reveal the lattice reconstruction in twisted bilayers of the transition metal dichalcogenides

125 Moire lattices in twisted bilayers of transition metal dichalcogenides (TM

126 The twisted bodipy shows intense long wavelength absorption

127 ead-to-tail polymeric interactions and local twisting, both of which depart from strict superhelical

128 signature in the form of spectral flow under twisted boundary conditions.

129 rmed the hypothesis of chromatin fibers as a twist buffer.

130 ved the electrical harvesting performance of twisted carbon nanotube yarn, which was previously repor

131 c field created by Floquet engineering(18) a twisted cavity(11,19) and by Rydberg-mediated interactio

132 both N and O atoms (i.e., crown, boat-chair, twist chair-chair, and boat-boat for the oxaza[3.3.2]-,

133 We show that high cooling results from twist changes for twisted, coiled, or supercoiled fibers

134 high cooling results from twist changes for twisted, coiled, or supercoiled fibers, including those

135 P<0.001), whereas esmolol+hypoxia augmented twist compared with esmolol alone (16.5+/-3.3 degrees ;

136 pulse irradiation on the Si substrate, and a twisted cone structure with a height of 3.5 um was creat

137 between the fluorescent planar and the dark twisted configurations.

138 The significant differences in QA-PFS and Q-TWiST confirm the benefit of rucaparib versus placebo in

139 broad absorption in the visible range, and a twisted conformation make them good candidates as non-fu

140 he luminescence properties of a high-energy, twisted conformation of the previously well-studied chro

141 that shows a transition between relaxed and twisted conformations in the absence and presence of gua

142 ecular topologies associated with planar and twisted conformations of TT, respectively.

143 he mechanical response of DNA to bending and twisting constraints, both of which are important in def

144 cleotide and membrane binding; the degree of twisting correlates with the length and orientation of M

145 The growth of spontaneously twisted crystals is a common but poorly understood pheno

146 An analysis of the formation of twisted crystals of a metastable benzamide polymorph (fo

147 r parameters from zero-stress elongation and twisting data.

148 erhelical location (SHL) +2, supporting the 'twist defect' model of chromatin remodeling.

149 ity, as well as insensitivity to bending and twisting deformations-features that are important for so

150 re brittle and fragment at small bending and twisting deformations.

151 tip-patched prisms assemble into unexpected twisted dimers due to the patch-patch interactions.

152 s to adopt a distinct morphology with longer twist distance than variants lacking this substitution.

153 osome occupancy and high predicted propeller twist DNA shape value.

154 ions, surprisingly including those with over-twisted DNA.

155 but different system with reduced symmetry - twisted double bilayer graphene (TDBG), consisting of tw

156 ere, using van der Waals heterostructures of twisted double bilayer graphene (TDBG), we demonstrate a

157 ulated by a physical interaction with FKBP42/Twisted Dwarf1 (TWD1), a peptidylprolyl cis-trans isomer

158 s (LCLCs) have revealed an anomalously small twist elastic constant compared to the splay and bend co

159 ue in general for thermotropic nematics, the twist elastic constant is found to be one order of magni

160 These results demonstrate that a small twist elastic constant is not restricted to the special

161 The reason for this extremely small twist elastic constant very likely originates with the f

162 of elastic constants and do not include the twist elastic constant.

163 e the axial and spring-index dependencies of twist-enhanced cooling and its origin in a phase transfo

164 yered crystals-in which a tunable interlayer twist evolves naturally during synthesis.

165 anchoring points, thereby constraining their twist, experience a mechanical torque upon cofilin bindi

166 including parallel fiber electrodes (PFEs), twisted fiber electrodes (TFDs), wrapped fiber electrode

167 aterial compositions, fabric structure, yarn twist, fiber type, and hairiness.

168 Understanding and use of twisted fibres implies the use of complex multi-componen

169 Individual twisted fibres on stone tools from the Abri du Maras led

170 Twisted fibres provide the basis for clothing, rope, bag

171 on, resulting in propagation of an sRPT-like twisted fibril morphology, unlike the rodlike structure

172 or the synthesis of molecular knots focus on twisting, folding and/or threading molecular building bl

173 Herein, we report a "Twisted-Planar-Twisted" framework, the hexaphyrin dimer D that exists i

174 Polymorphism and twisting frequently concur as they are both associated w

175 A helically twisted, fully BNB-embedded PAH 11 was prepared by combi

176 al targets and downstream responses, such as twist, function as molecular ratchets.

177 Moreover, esmolol+normalized Spo(2) lowered twist further than esmolol alone (10.5+/-3.1 degrees ; P

178 X-ray crystallography revealed a slightly twisted geometry for the phenyl-substituted cisoid squar

179 re-containing building block adopts a highly twisted geometry relative to its free form, leading to t

180 erating characteristics curve showed that LV twist had optimal predictive value to discriminate patie

181 s heterostructures obtained via stacking and twisting have been used to create moire superlattices(1)

182 The ability of the twisted helicene frame to delocalize the negative charge

183 Structurally, these twisted heterostructures feature atomic reconstruction a

184 Previously, such twisted heterostructures have involved a single planar i

185 In an unusual twist, human cytomegalovirus co-opts the antiviral radic

186 nd peripheral O(2) saturation (Spo(2)) on LV twist in acute and chronic hypoxia and (2) elucidate whe

187 However, the propagation of twist in condensed chromatin remains yet unresolved.

188 nces in quantum yields can be explained by a twist in the chromophore upon coordination of platinum o

189 rity of the nucleus of neutrophils and a new twist in the interplay of cofilin, Wdr1, and coronin in

190 The LPC maps indicate presence of a twist in the lattice planes that increases after epitaxi

191 ine/threonine-rich stretch causes a backbone twist in the N-terminal beta strand, stabilizing the mon

192 By introducing a rotational twist in their geometry, asymmetric transmission with th

193 ally coherent sources that are statistically twisted in the space-frequency and space-time domains.

194 in Tpm flexibility and prominent coiled-coil twisting in pseudorepeat 4.

195 the sharp kinks and additional inter-segment twisting in target DNA and thus attenuates unwanted tran

196 ated, flexible conformation, not circular or twisted, in which the N-terminal domain I (DI) and the C

197 Interestingly, fibril helical twists increased upon the removal of C-terminal residues

198 lved electron diffraction shows that Eshelby twist, induced by a torque on the ends of a cylindrical

199 Theoretical studies suggest that these twist-induced phenomena are common to layered materials

200 density functional theory shows a 67 degrees twist inside an acceptor unit in the CT state instead of

201 trilayer structure with one aligned and one twisted interface.

202 ned to donor torsion, acceptor wag, acceptor twist, intermolecular stretch, donor torsion overtone, a

203 bulk polar solution, DMABN forms an excited twisted intramolecular charge-transfer (TICT) state that

204 Distinct from twisted intramolecular charge-transfer (TICT) states, ex

205 cal studies indicate that the formation of a twisted intramolecular charge-transfer species enables t

206 ults demonstrated that left ventricular (LV) twist is abnormal in LVNC, but it has not been investiga

207 These findings suggest LV twist is augmented in hypoxia via beta(1)-AR-dependent a

208 ural analysis shows that the crystal lattice twist is consistent with the geometric twist of the laye

209 gregation experiments, suggesting the fibril twist is modulated by N-terminal residues outside the am

210 d-exchange and the redox steps a hypervalent twist is required for the reaction to proceed via an ene

211 erritin (40 wt%) in carbon nanotube yarn and twisting it into a coiled structure, which provides stre

212 As an illustration, we consider twisted kagome lattices(9-15), reconfigurable mechanical

213 We hypothesized that PHA twisting led to torsion of the residual primordial commo

214 Left ventricular (LV) twist mechanics are augmented with both acute and chroni

215 Activation occurs through a clamp-twisting mechanism, in which Dip1 forces two core subuni

216 model, we extracted values of the chromatin twist modulus and the linking number per stacked nucleos

217 that the ISC of the bodipy results from its twisted molecular structure and reduced symmetry.

218 of lamellae is shown to be able to create a twist moment that is responsible for the observed non-cl

219 ics of the interconversion between the major twisted-monomeric conformation and a more regular beta s

220 Quiescent Abeta42 fibrils adopt a long and twisted morphology, while agitated fibrils are short and

221 simulations recapitulate the characteristic twist motion of the suppressor domain (SD) and reveal co

222 h clearly corroborate the suppression of the twisting motion of thiadiazole core in the presence of a

223 hat substantially affected helix bending and twisting motions in the entire TMD.

224 faces and show that it leads to continuously twisted multilayer superstructures.

225 ll rearrangement in both wild-type and snail twist mutant embryos, where our theoretical prediction i

226 Due to the strongly donating and highly twisted nature of the TTAC donor as well as the spatiall

227 D(2) -symmetric molecule with an end-to-end twist of 97 degrees .

228 Their photophysics is governed by the twist of lateral phenyl rings and intramolecular and int

229 We argue that in vivo the total twist of linker DNA could be modulated by interaction wi

230 of few-layer materials stacked at a relative twist of small angle have recently shown the emergence o

231 eploying N-acyl-glutarimides to achieve full twist of the acyclic amide bond, and results in the disc

232 The stammer, which locally alters the twist of the helix, significantly increases copper-catal

233 ttice twist is consistent with the geometric twist of the layers, leading to moire superlattices betw

234 rrangement with a rise of ~65 angstrom and a twist of ~180 degrees .

235 In particular, a G545S mutation may hinder twisting of beta3 because its side chain hydroxyl forms

236 lass of PSs, which exhibit stimuli-initiated twisting of conjugated backbone.

237 me, characterized by abnormal flattening and twisting of hair shafts (pili torti) and hearing problem

238 nd contradicts the predominant hypothesis of twisting of microfibrils in plant primary cell walls.

239 In bilayer graphene, the twisting of one layer with respect to the other at 'magi

240 modes of isolated superatom, 2D synchronized twisting of superatoms in layers, and 3D acoustic interl

241 if to contact the cephalosporin carboxylate, twisting of the beta3 strand to form the oxyanion hole,

242 electron microscopy showed that in yeast the twisting of the opposing distribution bands is echoed by

243 tools to synthetic topological matter (here twisted optical resonators). Combined with advances in R

244 Here, we studied the effect of Twist or Snail deficiency in endothelial cells on EndMT

245 onditional deletion of Twist1 (which encodes Twist) or Snai1 (which encodes Snail) in VE-cadherin(+)

246 flip pathway or via a volume-conserving hula-twist pathway.

247 two distinct S(1) decay pathways: a reactive twisting pathway and an unreactive planar pathway.

248 A rich phase diagram with noncollinear twisted phases is obtained, and spin waves are further c

249 K(S)) turned into nanohelices with a regular twisting pitch, while the other (C'EK(S)K(S)) remained a

250 th overall planarity, referred to as "Planar-Twisted-Planar" and "Planar-Planar-Planar", respectively

251 Herein, we report a "Twisted-Planar-Twisted" framework, the hexaphyrin dimer

252 It is observed that the helical twisting power of this chiral molecular switch increases

253 the linker, from a coplanar arrangement to a twisted, previously unseen conformer.

254 ins, capable of zinc-dependent assembly into twisted, rope-like intercellular filaments in the biofil

255 This ask1 mutant produces twisted rosette leaves, a reduced number of petals, fewe

256 g grade >= 3 TEAEs, the difference in mean Q-TWiST (rucaparib v placebo) was 6.88 months (95% CI, 5.7

257 ich moire-lattice induced phenomena in angle-twisted semiconductor van der Waals heterostructures.

258 dimensional system emerges upon stacking two twisted sheets of GeSe, in marked contrast to all moire

259 ra, SmartControl, and AbsolutePro restricted twisting; SmartFlex and Innova exacerbated twisting; and

260 c plane has been visualised and a new spiral twisting solidification phenomena observed.

261 D) and mutual coherence functions (MCFs) for twisted space-frequency and space-time Gaussian Schell-m

262 the generation and subsequent propagation of twisted space-frequency and space-time GSM beams.

263 ly, we describe how to physically synthesize twisted space-frequency and space-time partially coheren

264 hods indicate that these HOPs, which feature twisted spikes and other morphologies, display higher co

265 The twist spinning mode (TSM) protocol described here enable

266 suggest that the accumulation of bending and twisting stresses as the filament elongates on the membr

267 rrelated phases of matter in multi-flat-band twisted superlattices.

268 tates, with between <5 and 70% lower helical twist than nonsupercoiled DNA.

269 of the actin monomer have significantly less twist than their crystal structures and that the ATP mon

270 ouble protofilaments can exhibit left-handed twisting that is dependent on the bound nucleotide and m

271 dergo PCP-directed apical rotation, inducing twisting that results in a helical structure of defined

272 trike," a ballistically rapid, overhead back-twist, that seems not to rely on visual cues [4, 5, 8].

273 ing of the in-between relationships, we have twisted the problem as a supervised learning one and inv

274 ey must block the diffusion of the excess of twist through the two binding sites on the DNA molecule

275 This mosaic zone provides a new twist to our understanding of the Atlantic-Mediterranean

276 structures hold the potential to bring a new twist to the field of spatial-domain optical analog comp

277 The ability to manipulate the twisting topology of van der Waals structures offers a n

278 From this, we assess how the measured twist-torque profiles develop with increasing stretching

279 We argue that combining the twist-torque profiles for various stretching forces effe

280 expression can be supported by action of the Twist transcription factor, specifically, through one en

281 EMTs are driven by SNAIL, ZEB and TWIST transcription factors(5,6) together with microRNAs

282 atomic coupling for carbon atoms by studying twisted trilayer graphene and show that the result can b

283 Twisted two-dimensional bilayer materials exhibit many e

284 cyl-glutarimide amide with an almost perfect twist value, tau = 89.1 degrees .

285 Moire lattices formed in twisted van der Waals bilayers provide a unique, tunable

286 sub-5-nm spatial resolution in a variety of twisted van der Waals heterostructures including, but no

287 ons in tunable flat-band systems realized in twisted van der Waals heterostructures(3-6).

288 could provide an alternative means to create twisted van der Waals structures.

289 Q-TWiST was calculated as muTOX x TOX + TWiST, with muTOX

290 pared with baseline (14.8+/-3.0 degrees ) LV twist was reduced with esmolol (11.2+/-3.3 degrees ; P=0

291 serve that the structural changes induced by twist were reversible, indicating that chromatin has a l

292 Q-TWiST with TOX defined using select grade >= 2 TEAEs als

293 fraction revealed that the actin filament is twisted with a larger radius, that tropomyosin and tropo

294 ing of two Bernal stacked bilayer graphenes, twisted with respect to one another.

295 estimated time without symptoms or toxicity (TWiST) with niraparib compared with routine surveillance

296 Q-TWiST was calculated as muTOX x TOX + TWiST, with muTOX calculated using EQ-5D-3L data.

297 e involves previously unknown stretching and twisting within individual solenoid segments and loosens

298 the unique demand to maintain stems that can twist without breaking.

299 findings by modeling double-helical DNA as a twisted wormlike chain with a finite width, intrinsic cu

300 th a very compact woven structure and highly twisted yarns made of continuous filaments, compared wit