ライフサイエンスコーパス: critical temperature

1 eir physiological temperature limits (their 'critical temperatures').

2 he superconductor, eventually depressing its critical temperature.

3 the 2D Ising model of ferromagnetism at the critical temperature.

4 rring at temperatures notably below the bulk critical temperature.

5 rgy of solvation changes above and below the critical temperature.

6 essary for the thermal protocol to cross the critical temperature.

7 rgy, Fermi surface, and even superconducting critical temperature.

8 identified, each of which possesses its own critical temperature.

9 nertia of the confined solid below a certain critical temperature.

10 CuO4 at temperatures significantly above the critical temperature.

11 state at temperatures up to 3,300 times the critical temperature.

12 a ferroelectric transition at an x-dependent critical temperature.

13 with the emergence of long-range order at a critical temperature.

14 region where pairs form above the superfluid critical temperature.

15 mperature, reaching values near unity at the critical temperature.

16 versal jump in the superfluid density at the critical temperature.

17 ise to the spin reorientation at such a high critical temperature.

18 r left- or right-handed nanocrystals below a critical temperature.

19 in exfoliated flakes, although with a lower critical temperature.

20 varying substrate and temperature below the critical temperature.

21 e quantum oscillation of the superconducting critical temperature.

22 temperature of the environment falls below a critical temperature.

23 aterial for a temperature range close to its critical temperature.

24 which scales as [Formula: see text] near the critical temperature.

25 ropy, domain structure, spin polarization or critical temperatures.

26 mall fermion pairs for superfluidity at high critical temperatures.

27 culations including a narrow distribution of critical temperatures.

28 50 kelvin compared with the previous highest critical temperature(1) is an encouraging step towards t

29 surface in the 'normal' state above the bulk critical temperature(1).

30 have been found to show unprecedentedly high critical temperatures(1-4), stimulating investigations i

31 f elemental sulfur by ODE, which possessed a critical temperature (~180 degrees C).

32 ficantly reduced baseline drifting and lower critical temperature (259.4 K and 261 K depending on the

33 er potential, a parallel magnetic field or a critical temperature ~36 K.

34 Instead, at temperatures above the critical temperature a range of unusual properties, coll

35 e of temperatures can be calculated from the critical temperature and a single measurement of the int

36 owth of a nitride superconductor with a high critical temperature and a subsequent nitride semiconduc

37 -layer topological semimetal TaIrTe4 below a critical temperature and bias current.

38 ons, while keeping the upper critical field, critical temperature and electronic mass anisotropy unch

39 Above the critical temperature and extending to biases much larger

40 the thermodynamic and environmental screens (critical temperature and global warming potential), we s

41 o provide a window on fluctuations above the critical temperature and hence, in principle, can also p

42 By incorporating the critical temperature and local symmetry breaking, it int

43 ing gap that vanishes at the superconducting critical temperature and magnetic field and a higher-ene

44 The predicted critical temperature and pressure for [C(4)mim][BF(4)] w

45 e subsequently denatured from the beads at a critical temperature and selectively separated from wild

46 approximately (Tc-T)(beta), where Tc is the critical temperature and the exponent beta was close to

47 pproach, based on experimental evidence of a critical temperature and the parameterization of the equ

48 e the superconducting properties such as the critical temperature and the superfluid density across i

49 cy increases when the temperature approaches critical temperature and the working frequency goes near

50 Further increasing the critical temperature and/or decreasing the stabilized pr

51 may lead to new superconductors with higher critical temperatures and novel properties.

52 at low temperatures (close to the dynamical critical temperature) and becomes symmetric at high temp

53 n that hatching success increased up to some critical temperature, and then declined when AGMT exceed

54 rate (the difference between lower and upper critical temperatures, and between optimum and upper cri

55 d the nature of the 'normal' state above the critical temperature are widely debated.

56 GPMV miscibility critical temperatures are also lowered to a similar exte

57 The very high critical temperatures are attributed to an unusually lar

58 known for oxide materials, where much higher critical temperatures are offered by copper oxide-based

59 simulated under historical conditions, since critical temperatures are rarely exceeded during the gro

60 res of a superconductor, which appear at the critical temperature, are the formation of an energy gap

61 tic ordering with a drastic variation of the critical temperature as a function of the guest molecule

62 on the magnesium-based surface band up to a critical temperature as high as 30 K for merely six mono

63 model of thermoregulation defines the lower critical temperature as threshold of the thermoneutral z

64 Above a critical temperature associated with a structural phase

65 hydrides indeed can maintain relatively high critical temperature at relatively modest pressures acce

66 omponent's respective boiling temperature or critical temperature at sub- and supercritical pressures

67 otosynthetic heat tolerance is T(crit) - the critical temperature at which incipient damage to photos

68 Studies describing critical temperatures at which spring freeze damage occu

69 ated organisms only marginally elevate their critical temperatures because they have a fixed amount o

70 the pre-compacted SiC powder specimens to a critical temperature before applying any voltage to the

71 We observed a critical temperature, below which the peptide folds into

72 The difference in critical temperature between the two samples having nomi

73 f superconductivity is predicted to occur at critical temperatures between 240 and 320 kelvin at mega

74 The critical temperature beyond which photosynthetic machine

75 e, the Meissner state is destroyed above the critical temperature by strong phase fluctuations (as op

76 surface carrier density enable shifts in the critical temperature by up to 30 K.

77 a temperature significantly higher than the critical temperature (by 100-220 K).

78 n over by superconducting domes that feature critical temperatures comparable to those in devices wit

79 strain values and at temperatures below the critical temperature, consistent with a drop in spin pol

80 more thermally sensitive, with lower maximum critical temperatures (CTmax ).

81 The upper critical temperatures (Ctmax) of both populations are ve

82 to differences in thermal tolerance (maximum critical temperatures: CTmax ).

83 High-critical temperature cuprate superconductors set the pre

84 in thin-film tricrystal samples of the high-critical-temperature cuprate superconductor YBa(2)Cu(3)O

85 Here we report a critical temperature dependence on magnetic configuratio

86 nd reverse domain superconductivity with the critical temperature depending upon the location.

87 we present Differential Strand Separation at Critical Temperature (DISSECT), a method that enriches u

88 idly along the isotherm corresponding to the critical temperature, enabling such a plate to act as a

89 can be understood if the lipid mixture has a critical temperature equal to 75 degrees K.

90 and the quest for superconductors with high critical temperature equates to a search for systems wit

91 urs under external conditions that cause the critical temperature for a competing order to go to zero

92 The critical temperature for complete oxidative decompositio

93 presented to support the hypothesis that the critical temperature for fusion of two LUV populations d

94 isfavour ordered phases, leading to an upper critical temperature for magnetism, superconductivity an

95 stable up to 873 kelvin, which is above the critical temperature for many applications in extreme en

96 e potential could also strongly increase the critical temperature for s-wave superfluidity.

97 effects, even at temperatures well above the critical temperature for spontaneous phase separation, a

98 the oscillations is strongly peaked near the critical temperature for superconductivity and decreases

99 ced, we delineate a strategy to increase the critical temperature for superconductivity.

100 As pressure is increased, the critical temperature for the hcp-to-fcc transformation a

101 Bose-Hubbard model and find that the maximum critical temperature for the supersolid phase tends to b

102 The lower critical temperature for thermoregulation was about 8.0

103 temperature may indicate the existence of a critical temperature for transition from H(2) dominated

104 ch are predicted to exhibit promisingly high critical temperatures for superconductivity.

105 osely related to the gap that appears at the critical temperature (for example, the variation of the

106 own to possess reliably high superconducting critical temperatures ([Formula: see text]), which corre

107 Optically heating above a critical temperature [Formula: see text] = 32 degrees C

108 f the three-dimensional (3D) superconducting critical temperature [Formula: see text] and a full reco

109 g is observed just above the superconducting critical temperature [Formula: see text] due to Cooper p

110 temperatures, and between optimum and upper critical temperatures) generally represents the same ran

111 0) cm(-2), and the flow of a supercurrent at critical temperatures greater than 2 K.

112 ries, such as the optical enhancement of the critical temperature in certain superconductors and the

113 nct from thermal phase fluctuations near the critical temperature in equilibrium.

114 recovery of self-field critical current and critical temperature in irradiation-annealing process.

115 ed to domain walls, all occuring at a higher critical temperature in relative scales.

116 e what local and global mechanisms limit the critical temperature in unconventional superconductors.

117 rconducting cerium superhydride and the high critical temperature in yttrium superhydride, we carry o

118 to investigate the magnetic transitions and critical temperatures in Fe(2)O(3) polymorphs(7) at pres

119 cs provide an experimental tool for lowering critical temperatures in plasma membranes of intact cell

120 ero-resistance state with the detected onset critical temperatures in the range of 97-141 K.

121 Below a critical temperature, in a membrane composed of modified

122 Owing to their high critical temperatures, iron oxides are the only potentia

123 rings is particularly intriguing because the critical temperature is an oscillatory function of magne

124 periodic array of holes and observe that the critical temperature is controlled by the total fraction

125 ropy upon increasing the pressure, while the critical temperature is defined by the 'reaction' equili

126 t of coarsening following a quench below the critical temperature is domain growth.

127 row parameter window in which the supersolid critical temperature is enhanced by disorder.

128 The superconducting critical temperature is largest at low density below a L

129 or the other gamma-crystallins for which the critical temperature is located above the freezing point

130 ially important at magnetic fields where the critical temperature is suppressed.

131 second order magnetic phase transition whose critical temperature is tunable from 100 K to well above

132 Since the critical temperature is typically on the order of room t

133 metabolic rate) to explain the plasticity of critical temperatures is complicated by the need to acco

134 conductors, and the wide range of associated critical temperatures, is readily understood in terms of

135 Above a critical temperature known as the Leidenfrost point (LFP

136 ght on 1T-TiSe(2) while cooling it below the critical temperature leads to the preferential formation

137 cal." We found that women had a cooler lower critical temperature (mean +/- SD: 21.9 +/- 1.3 degrees

138 rve two distinct temperature regimes, with a critical temperature near 250 K.

139 er, superfluidity and superconductivity with critical temperatures near 10(10) kelvin, opaqueness to

140 tes show that this mechanism may explain the critical temperatures observed in doped SrTiO(3).

141 ments reveal a gap of 2 meV (or 25 K) with a critical temperature of 10 K in the bulk, together with

142 eld-tunable superconductivity with a maximum critical temperature of 2.1 kelvin.

143 ting the same (within experimental accuracy) critical temperature of 3.8+/-0.1 K and practically iden

144 egrees twisted bilayer WSe(2) with a maximum critical temperature of 426 mK.

145 n-based superconductor--without reducing its critical temperature of 50 K.

146 ed compound MgCNi3 is superconducting with a critical temperature of 8 K.

147 ectric response engineering may increase the critical temperature of a composite superconductor-diele

148 The relatively high critical temperature of A15 vanadium silicide is an appe

149 t from a temperature of 0.5 kelvin through a critical temperature of about 90 kelvin, with no change

150 Moreover, there exists a critical temperature of approximately 150 degrees C, abo

151 take place at least 15 K below the observed critical temperature of approximately 245 K.

152 Here we report superconductivity with a critical temperature of around 250 kelvin within the [Fo

153 The superconducting critical temperature of H(3)S ranks among the highest me

154 ttern of the Swc5 segments can influence the critical temperature of LLPS.

155 han 40 tesla, a considerable scale given its critical temperature of only 2 K.

156 pproach with its reaction temperature at the critical temperature of S activation (180 degrees C) use

157 lectron-phonon coupling parameter lambda and critical temperature of several K.

158 Molecular weight, critical pressure, and critical temperature of solvents along with pressure and

159 itution) that yield superconductivity with a critical temperature of T(c) = 3.5 K.

160 Here, we observed power-law behavior of the critical temperature of the coupled nematic/structural p

161 onic strength of the solution and the pseudo-critical temperature of the gas mixture decreases the so

162 mal avalanche component is identified at the critical temperature of the material.

163 An increase of the critical temperature of the order of DeltaT ~ 0.15 K com

164 referred to as pup flow, is predicted at the critical temperature of the phase transition, consistent

165 at temperatures substantially lower than the critical temperature of the superconducting transition.

166 esponsive to ultrafast excitations above the critical temperature of the superconductor and in the me

167 Below the critical temperature of the superconductor, ultrafast ex

168 rimentally observed relationship between the critical temperature of the thermal transition, T(1/2),

169 The critical temperature of the transition increases from 6

170 mechanism for enhancing the supercurrent and critical temperature of two-dimensional superconductors.

171 etallic helium to be a superconductor with a critical temperature of ~ 20 K just above its metallizat

172 ensional kagome superconducting state with a critical temperature of ~5.4 K is intertwined with the b

173 Examples are the high critical temperatures of the cuprate superconductors and

174 axation rate that can be identified with the critical temperatures of the predicted phase transitions

175 erate pressure and at temperatures above the critical temperatures of the respective gases.

176 nu ~ -2, superconductivity is observed below critical temperatures of up to 3 kelvin.

177 ity with weak electron-phonon coupling below critical temperatures of up to 7 K.

178 verges smoothly without any indication for a critical temperature or critical velocity of a supersoli

179 ge excitations across the Mott gap in a high-critical temperature parent cuprate (Ca(2)CuO(2)Cl(2)),

180 plastic deformation of the lithosphere in a critical temperature range, leading to long-term weakeni

181 nsional covalent system with superconducting critical temperature reaching its maximum of 10 K.

182 her displacement field and features a higher critical temperature, reaching up to 0.5 K.

183 unveiling Puf6-mediated rRNA compaction as a critical temperature-regulated rescue mechanism that cou

184 in which the incubation temperature during a critical temperature sensitive period (TSP) determines s

185 solvates by 540 meV at 350 K, and below the critical temperature, solvation decreases to 200 meV at

186 e is observed only below the superconducting critical temperature, suggesting an inherent correlation

187 generated by quantized vortices in the high critical temperature superconductor Bi2Sr2CaCu2O8+delta.

188 In this context, the iron-based high critical temperature superconductors are a promising pla

189 of dopant atom distributions in cuprate high-critical temperature superconductors has long been suspe

190 echanisms of single-photon detection in high-critical-temperature superconductors.

191 r strongly correlated materials such as high-critical-temperature superconductors.

192 goes a sharp superconducting transition at a critical temperature T (c) 1.5 K, while TiSi(2) is a nor

193 sity of states (DOS) and the superconducting critical temperature T c .

194 nd a linear scaling with the superconducting critical temperature T c is observed under pressure.

195 n to phase-separate, as characterized by the critical temperature T( *)cr, is related to the protein'

196 he favorable SCO properties in acetonitrile [critical temperature T(1/2) = 322(2) K], (ii) saturates

197 narrow window of density and with a maximum critical temperature T(c )~ 30 mK.

198 atures T much lower than its superconducting critical temperature T(c) = 2.1 K, the heavy fermion sup

199 .05)Ba(2)Cu(3)O(7-delta) single crystal with critical temperature T(c) = 85.2 K (at P = 0) was invest

200 e pressure dependence of the superconducting critical temperature T(c) below 150 gigapascals, is expl

201 ed as a second order phase transition with a critical temperature T(c) of 204 K.

202 stantial increase in the observed domain and critical temperature T(c) of superconducting states(12-1

203 Below a critical temperature T(c), a small amount of MoS(2) give

204 Upon cooling below the critical temperature T(c), the red phase with increased

205 a characteristic lambda-like feature at the critical temperature T(c)/T(F) = 0.167(13).

206 he discovery of superconducting H(3)S with a critical temperature T(c)~200 K opened a door to room te

207 The increasing critical temperatures T(c), with increasing S could not

208 uperconducting (SC) K(1.9)Fe(4.2)Se(5) has a critical temperature (T (c)) of ~31 K with a varying sup

209 l of H-dominated compounds to possess a high critical temperature (T(c) ).

210 discovery of superconductivity with maximum critical temperature (T(c)) above 210 K in calcium super

211 essed, and superconductivity arises with the critical temperature (T(c)) increasing to 5.5 K.

212 This large shifting of the critical temperature (T(c)) is attributed to the very la

213 a Cooper pair in superconductors with a high critical temperature (T(c)) is being actively pursued in

214 mergence of superconductivity with a maximum critical temperature (T(c)) of around 30 K at 69.0 GPa.

215 The critical temperature (T(c)) of the phase transition scal

216 mising candidate as the pairing glue of high critical temperature (T(c)) superconductivity in cuprate

217 strated a sensitivity of the superconducting critical temperature (T(c)) to parallel (P) and antipara

218 doping with a dome-like dependence of their critical temperature (T(c)).

219 iron selenide can significantly increase the critical temperature (T(c)).

220 (J(c)=2.1 x 10(4) A(.)cm(-2), 77 K) and high critical temperature (T(c)= 88-89.5 K).

221 Coefficients from these models, i.e. critical temperature (T(crit) ) and the initial response

222 egella was separated into two domains at the critical temperature (T(critical) = 4 degrees C).

223 Cuprate superconductors have the highest critical temperatures (T(c)) at ambient pressure, yet a

224 6), YH(9), and LaH(10)) with superconducting critical temperatures (T(c)) well above 200 K has opened

225 nanoparticles causes drastic modulations to critical temperatures (T(c)), hysteresis widths, and the

226 r high pressure, and considering that record critical temperatures (T(c)s) across various systems hav

227 ain the strong variations in superconducting critical temperature, T(c), among cuprates that have ide

228 tates at the Fermi level and superconducting critical temperature, T(c), can be tuned by changing the

229 n, which induces an important enhancement in critical temperature, T(c), of the material.

230 re, T(TRSB), is generally found to match the critical temperature, T(c), within resolution.

231 temperatures well above the superconducting critical temperature, T(c).

232 above 50 GPa with a maximum superconducting critical temperature, T(c)of 17 K at 91 GPa.

233 In this paper, the critical temperatures, T(c) and pressures, P(c), have be

234 ictide superconductor BaFe2(As0.7P0.3)2 with critical temperature Tc = 30 K.

235 ort phonon-mediated superconductivity with a critical temperature Tc = 6.8-8.1 K, in good agreement w

236 The critical temperature Tc and the critical current density

237 arth element) is the family with the highest critical temperature Tc but also with a large anisotropy

238 Eliashberg function and the superconducting critical temperature Tc from the spectral function.

239 of achieving this goal, such as tripling the critical temperature TC in Al-Al2O3 epsilon near zero (E

240 onducting transition appears at 8 GPa with a critical temperature TC of 5.3 K.

241 In the quest to increase the critical temperature Tc of cuprate superconductors, it i

242 (X = N, P, As, Sb) and find superconducting critical temperature TC of MnP sharply increases near th

243 Superconducting critical temperature Tc(x) in ZrTe3-xSex (0 </= x </= 0.

244 octet phenomenology at the superconductor's critical temperature Tc, and it survives up to at least

245 ts a charge density wave (CDW) transition at critical temperature TC=232+/-5 K, which is higher than

246 ctivity in In2 Se3 occurs at 41.3 GPa with a critical temperature (Tc ) of 3.7 K, peaking at 47.1 GPa

247 In cuprate bilayers, the critical temperature (Tc) can be significantly enhanced

248 tures include pi-junctions, triplet pairing, critical temperature (Tc) control in FM/S/FM superconduc

249 ma-membrane-derived vesicles by lowering the critical temperature (Tc) for phase separation.

250 igh-temperature superconductivity (HTS), the critical temperature (Tc) has a dome-shaped doping depen

251 A superconducting critical temperature (Tc) is found ranging from 9 to 16

252 erconductivity in boron-doped diamond with a critical temperature (TC) near 4 K, great interest has b

253 We show that anesthetics depress the critical temperature (Tc) of these GPMVs without strongl

254 The complex phase diagram of high-critical temperature (Tc) superconductors can be deduced

255 be used as a means to reach superconducting critical temperatures (Tc) of up to 80 K.

256 recent observation of superconductivity with critical temperatures (Tc) up to 55 K in the pnictide RF

257 Their superconducting critical temperatures (Tc) were computed as 70 and 76 K,

258 sion of superconducting order just below the critical temperature, Tc.

259 r understanding the doping dependence of the critical temperature Tc0.

260 an interlayer exchange field leads to higher critical temperature than that of either CrI(3) or CrCl(

261 form fibrils at temperatures greater than a critical temperature that decreases with peptide concent

262 This is, to our knowledge, the highest critical temperature that has been confirmed so far in a

263 after hydrothermal aging at 900 degrees C, a critical temperature that the current commercial Cu-SSZ-

264 1(M), which order antiferromagnetically with critical temperatures that depend on M.

265 Far below the superfluid critical temperature, the impurities formed well-defined

266 In line with the high critical temperature, the new MOF exhibits magnetic hyst

267 We show that, near the critical temperature, the single-particle spectral funct

268 Close to the BEC critical temperature, the spectral width exceeded the im

269 However, above the critical temperature, there was no coexistence of 2D pha

270 When these vesicles are heated above a critical temperature, they transform into long, flexible

271 arly in recent decades, and models predict a critical temperature threshold beyond which the current

272 lands there was a variable yield response to critical temperature threshold exceedance, specifically

273 The primary readout was change in critical temperature thresholds (CTT).

274 We analyzed the effects of treatments on critical temperature thresholds (CTTs) and critical stim

275 The results highlight the critical temperature thresholds at which buckling is mos

276 Do crop critical temperature thresholds during TSP exist in real

277 rfluidity nevertheless emerges at a non-zero critical temperature through the infinite-order Berezins

278 The critical temperature to form active sites is 800 degrees

279 For ultra-thin membranes, however, the critical temperature to initiate crystallization is abou

280 onally weak response of the superconductor's critical temperature to pressure.

281 A change in pH from 7 to 6 shifted the critical temperature towards higher values and resulted

282 stance, an isotope effect, and a decrease in critical temperature under an external magnetic field, w

283 y-antibody interactions in the form of T(c) (critical temperature) under the different solution condi

284 is determined by the unfolding step below a critical temperature up to the point, where the proteins

285 Ni2B2C family of superconductors, which have critical temperatures up to 16 K.

286 resulting metal-organic ferrimagnets feature critical temperatures up to 242 degrees C and a 7500-oer

287 precise, empirically measured thresholds and critical temperatures used to describe damage in the fie

288 which AGMT began to consistently exceed that critical temperature was 1988.

289 ermoregulation was about 8.0 C and the upper critical temperature was about 28 C.

290 A critical temperature was identified below which the mono

291 h explains why such a large reduction of the critical temperature was never reported before, neither

292 dependence of these distributions above the critical temperature, we extract an independent critical

293 Our analysis explains why high critical temperatures were only predicted for second or

294 At a critical temperature, where the ferromagnet transitions

295 e rest mass of Kane fermions changes sign at critical temperature, whereas their velocity remains con

296 These assemble into fibrils above a critical temperature which decreases with concentration

297 ide a basis for the trend of superconducting critical temperature with increasing pressure.

298 sal exponent that governs the scaling of the critical temperature with the applied field, in excellen

299 nct magnetic phase transitions with separate critical temperatures within a moire supercell of small-

300 e has demonstrated a 10% increase in nominal critical temperature without noticeable variation in the