ライフサイエンスコーパス: critical temperature

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

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

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

4 CuO4 at temperatures significantly above the critical temperature.

5 temperature of the environment falls below a critical temperature.

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

7 he superconductor, eventually depressing its critical temperature.

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

9 rring at temperatures notably below the bulk critical temperature.

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

11 mall fermion pairs for superfluidity at high critical temperatures.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

33 Above a critical temperature associated with a structural phase

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

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

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

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

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

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

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

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

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

43 High-critical temperature cuprate superconductors set the pre

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

45 Here we report a critical temperature dependence on magnetic configuratio

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

89 Below the critical temperature of the superconductor, ultrafast ex

90 The critical temperature of the transition increases from 6

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

118 The critical temperature Tc and the critical current density

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

150 Do crop critical temperature thresholds during TSP exist in real

151 The critical temperature to form active sites is 800 degrees

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

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

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

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

156 A critical temperature was identified below which the mono

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

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

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

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