ライフサイエンスコーパス: phase transition temperature

1 oth having similar gel to liquid-crystalline phase transition temperatures).

2 ermal conductivity, thermal diffusivity, and phase transition temperatures).

3 /- 2.1%) above the gel to liquid crystalline phase transition temperature.

4 ns studied here, when sufficiently above the phase transition temperature.

5 f heat through FeRh locally heated above the phase transition temperature.

6 ways reveal what will beneficially shift the phase transition temperature.

7 ing of the membranes below their miscibility phase transition temperature.

8 lators with lower ferrimagnetic-paramagnetic phase transition temperature.

9 material and often a high nematic-isotropic phase transition temperature.

10 only at temperatures below a characteristic phase transition temperature.

11 mal around 37-40 degrees C, close to the LPS phase transition temperature.

12 hange conformation above and below the lipid phase transition temperature.

13 from 0.070 to 0.059 upon heating across the phase transition temperature.

14 electrical and thermal conductivities at the phase transition temperature.

15 low its structural antiferrodistortive (AFD) phase transition temperature.

16 T* as a crossover temperature rather than a phase transition temperature.

17 red thermally by taking the crystal over the phase transition temperature.

18 sing a membrane mixture near its miscibility phase transition temperature.

19 verges at the fluid-gel (L(alpha) - L(beta)) phase-transition temperature.

20 were hydrated above their gel-liquid crystal phase transition temperatures.

21 utectoid behavior for the melting points and phase transition temperatures.

22 properties and lipid vesicles with different phase transition temperatures.

23 t is a facile method for determining polymer phase transition temperatures.

24 enables the predictable tuning of mesophase phase transition temperatures.

25 r diester phosphatidylcholines at their main phase transition temperatures.

26 e pronounced effects on observables, such as phase-transition temperatures.

27 materials, particularly in the case of high phase-transition temperatures.

28 l dichalcogenide semimetal 1T-TiSe2 Near the phase-transition temperature (190 kelvin), the energy of

29 t to the general belief that below the lipid phase-transition temperature (30 degrees C) LDL are quas

30 During the heating cycles and close to the phase transition temperature, a surprising behavior is o

31 perturbation of the BIP molecules to the LC phase transition temperature, allowing analytical modeli

32 But below the gel-to-liquid crystalline phase transition temperature, an additional emission pea

33 er (Tg > 110 degreesC), does not depress the phase transition temperature and affects only slightly t

34 d by considering their size, zeta-potential, phase transition temperature and fluidity.

35 The sudden decrease of mobility around phase transition temperature and the presence of hystere

36 ane fluidity above, but not below, the lipid phase-transition temperature and did not alter the tempe

37 Here, we demonstrate that the phase-transition temperature and hysteresis can be tuned

38 ied out at 305 K, above the membrane thermal phase transition temperature, and at pH 7.0.

39 re, washed using solvent also held above the phase transition temperature, and then analyzed by reduc

40 al properties of NLCE (liquid crystallinity, phase transition temperature, and viscoelastic propertie

41 esses large-scale phase separation below the phase transition temperature, and, on the other hand, pr

42 Modelling the esterase phase transition temperature as a measure of structural

43 from the lowering of the gel-liquid-crystal phase transition temperature as monitored from temperatu

44 in films which results in an increase in the phase transition temperature as thickness is reduced.

45 Here we demonstrate a model for the phase transition temperatures associated with these stru

46 Raw TMC exhibited a first-order phase transition temperature at 58.15 +/- 0.38 degrees C

47 ced the fluid lamellar-to-inverted hexagonal phase transition temperature at very low concentrations

48 e of dissipation monitoring to determine the phase transition temperature based on the temperature-in

49 e crystal lattice spacing of 3.5 nm and of a phase transition temperature below 43 degrees C, we attr

50 rized N-isopropylacrylamide (ppNIPAM) show a phase transition temperature below which the polymer sur

51 m, the phase state deviates from the nominal phase transition temperature by tens of degrees.

52 ned by Raman measurement and as derived from phase transition temperatures by microthermometry experi

53 ition of a second CH CH moiety decreased the phase-transition temperature by approximately 19 degrees

54 A double bond decreased the phase-transition temperature by approximately 40 degrees

55 th variable thicknesses demonstrate that the phase transition temperature decreases with reducing mic

56 ngle-crystalline VO(2) nanostructures with a phase-transition temperature depressed to as low as 32 d

57 Furthermore, the higher surface-phase-transition temperature driven by surface stabiliza

58 icated that incorporation of BPL reduced the phase transition temperature, enthalpy, and average bila

59 sozyme surface dominated the process and the phase transition temperature followed an inverse Hofmeis

60 d liquid (HD-SCL) phase with a liquid-liquid phase transition temperature ([Formula: see text]) ~35 K

61 e AsF(6)(-) content decreases the reversible-phase-transition temperature gradually down to 99 degree

62 of either antioxidant increased the liposome phase transition temperature (>50 degrees C).

63 hysicochemical properties-including elevated phase transition temperature, improved toughness, and re

64 experiments identified domains of different phase transition temperatures in the mixed membranes.

65 ambient conditions as well as an increase in phase transition temperatures in the solid state.

66 erature to > 433 K (amorphous-to-crystalline phase transition temperature) in just 0.37 ns with a low

67 The phase transition temperature increases slightly dependin

68 Most (82%) of the phase-transition temperatures measured for Md were above

69 Phase transition temperature measurements were correlate

70 Above the phase transition temperature of -74 degrees C, the ring

71 sed the fluid lamellar to inverted hexagonal phase transition temperature of 1,2-dipalmitoleoyl-phosp

72 n different ratios, we continuously tune the phase transition temperature of 2D perovskites from appr

73 ipoTherm sized around 100 nm and exhibited a phase transition temperature of 43 degrees C.

74 increase the lamellar to inverted hexagonal phase transition temperature of both PE model lipid syst

75 15am, increases the lamellar-to-hexagonal II phase transition temperature of dioleoylphosphatidyletha

76 2 to 45 degrees C, covering the Lbeta-Lalpha phase transition temperature of dipalmitoylphosphatidylc

77 (DMPM) vesicles are most prominent near the phase transition temperature of DMPM.

78 tion-induced gel lamellar --> fluid lamellar phase transition temperature of either dipalmitoylphosph

79 chain-length-dependent increase in the main phase transition temperature of equimolar PSM/Cer bilaye

80 The phase transition temperature of FP20 was determined by u

81 egreesC), a very effective depressant of the phase transition temperature of freeze-dried DPPC, marke

82 induced by aqueous salt solutions lowers the phase transition temperature of poly(N-isopropylacrylami

83 We demonstrate control over the phase transition temperature of Ruddlesden-Popper two-di

84 The liquid crystalline-to-gel phase transition temperature of supported phospholipid b

85 molecules into the bulk solution caused the phase transition temperature of the bilayer to increase.

86 Near the phase transition temperature of the DPPC/POPG lipid mixt

87 percooled critical point may correspond to a phase transition temperature of the dynamic polymer stru

88 rs of magnitude lower than the ferromagnetic phase transition temperature of the films.

89 affected by either the gel-to-liquid-crystal phase transition temperature of the lipid or the tempera

90 ture that is stable for weeks just above the phase transition temperature of the lipid.

91 the AFP to the bilayer, which increases the phase transition temperature of the membranes and alters

92 the crystal above the characteristic volume phase transition temperature of the microgel particles r

93 he solution temperature traverses the volume phase transition temperature of the particles.

94 s on cooling below the liquid-crystal to gel phase transition temperature of the pure phospholipid.

95 The phase transition temperature of the saturated derivative

96 simple way to determine the true mesomorphic phase transition temperatures of other lipid and lyotrop

97 Phase transition temperatures of pure water and aqueous

98 d to determine the gel-to-liquid crystalline phase transition temperatures of the bolalipids (C32BAS

99 In this study, the structure and phase transition temperatures of the organic-inorganic m

100 33 of 185 picocoulombs per newton and a high phase-transition temperature of 406 kelvin (K) (16 K abo

101 aining the influence of the compounds on the phase-transition temperature of DPPA liposomes, while th

102 The influence on the phase-transition temperature of liposomes of dipalmitoyl

103 Measurement of the phase-transition temperature of peptide-DiPoPE dispersio

104 ain show significant sensitivity to the main phase-transition temperature of the lipid, consistent wi

105 Cholesterol ester had little effect on the phase-transition temperature of the waxes.

106 ed study of the dependence of phase type and phase transition temperatures on several key structural

107 ve impulse propagation by lowering the lipid phase transition temperature, or 3) modulate the lateral

108 The well-known halide perovskite cubic phase transition temperature shifts near room temperatur

109 Furthermore, the LCST phase transition temperature showed 100 x more unbinding

110 incorporates chemical composition, magnetic phase transition temperatures, structural details, and m

111 uction of the lamellar-to-inverted hexagonal phase transition temperature, suggesting that Cer-1-P in

112 size at temperatures below the lipid's main phase transition temperature T(m) and, based on these re

113 e to a simultaneous drastic reduction of the phase transition temperature T(MIT) from 68.8 degrees C

114 the (13)C and (207)Pb nuclei varied near the phase transition temperature (T(C) = 236 K), indicating

115 n of increasing temperature toward the lipid-phase transition temperature (T(C)), for coronene-labele

116 pacings on either side of the L(alpha)/H(II) phase transition temperature (T(h)) depends significantl

117 s (WALP14-17) lowered the inverted hexagonal phase transition temperature (T(H)) of DEPE, with an eff

118 eability of liposomes near the gel-to-liquid phase transition temperature (T(m)) to deliver reagents

119 domains in a fluid-like bilayer close to the phase transition temperature (T(m)).

120 The phase transition temperatures (T(C); 268K for Cl and 272

121 e thermal stability of the bilayer below the phase-transition temperature (T(m)) as compared to the g

122 The gel-to-liquid-crystalline phase-transition temperature (T(m)) of DMPC:DMPG (7:3 w/

123 cycled repeatedly across the L(alpha)/H(II) phase transition temperature, T(H), or when the H(II) ph

124 ss-forming sugars to affect the gel-to-fluid phase transition temperature, T(m), of several phosphati

125 The main gel-to-liquid-crystal (LC) phase transition temperature, T(m), of the distal lipid

126 egrees C/hr, and the rate-dependent apparent phase transition temperatures, T(A)(r) were determined f

127 Phenolic compounds also increased phase transition temperature (Tc) of nanoliposomes (2.01

128 sition arises because of the lowering of the phase transition temperature that occurs due to the perd

129 esters of mycolic acids were found to have a phase transition temperature that was linearly related t

130 Surprisingly, we found that the phase transition temperature (Tm) of F-DPPC occurs near

131 The biphasic effect of ethanol on the main phase transition temperature (Tm) of identical-chain pho

132 atalytic rate of PLA2 peaks around the lipid phase transition temperature (Tm) when Tm is not too far

133 phospholipid membranes displaying a range of phase transition temperatures (Tm).

134 )PE can affect the gel-to-liquid crystalline phase transition temperature, Tm, of the lipid bilayer i

135 etic field, to exactly suppress a continuous phase transition temperature to the absolute zero.

136 (M6) conducting to a greater increase in the phase transition temperatures up to 4.14 degrees C, whil

137 etermine viscoelastic properties and sol-gel phase transition temperatures using rheological methods.

138 elling of the PNM ball [temperature > volume phase transition temperature (VPTT) of the hydrogel], an

139 The phase-transition temperature was significantly higher (4

140 LDI probe surface at a temperature above the phase transition temperature, washed using solvent also

141 iding more physiological lipids with a lower phase transition temperature, we achieved efficient fusi

142 iffering shell thicknesses display identical phase transition temperatures when PCS is used to monito

143 an abrupt behavior near the superconducting phase transition temperature where phase coherence sets

144 of the latency period was greatest near the phase transition temperature where the latency was short

145 both above and below the liquid crystalline phase transition temperature, whereas DOPC displays only

146 alpha,alpha-galacto-trehalose depressed the phase transition temperature, whereas the introduction o

147 Control over defined phase transition temperature with rapid reconfiguration