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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 ing of the membranes below their miscibility phase transition temperature.
5 lators with lower ferrimagnetic-paramagnetic phase transition temperature.
6  material and often a high nematic-isotropic phase transition temperature.
7  only at temperatures below a characteristic phase transition temperature.
8 mal around 37-40 degrees C, close to the LPS phase transition temperature.
9 hange conformation above and below the lipid phase transition temperature.
10  from 0.070 to 0.059 upon heating across the phase transition temperature.
11 electrical and thermal conductivities at the phase transition temperature.
12  T* as a crossover temperature rather than a phase transition temperature.
13 sing a membrane mixture near its miscibility phase transition temperature.
14 verges at the fluid-gel (L(alpha) - L(beta)) phase-transition temperature.
15 t is a facile method for determining polymer phase transition temperatures.
16 properties and lipid vesicles with different phase transition temperatures.
17  enables the predictable tuning of mesophase phase transition temperatures.
18 r diester phosphatidylcholines at their main phase transition temperatures.
19 were hydrated above their gel-liquid crystal phase transition temperatures.
20 e pronounced effects on observables, such as phase-transition temperatures.
21  materials, particularly in the case of high phase-transition temperatures.
22 l dichalcogenide semimetal 1T-TiSe2 Near the phase-transition temperature (190 kelvin), the energy of
23 t to the general belief that below the lipid phase-transition temperature (30 degrees C) LDL are quas
24   During the heating cycles and close to the phase transition temperature, a surprising behavior is o
25      But below the gel-to-liquid crystalline phase transition temperature, an additional emission pea
26 er (Tg > 110 degreesC), does not depress the phase transition temperature and affects only slightly t
27 d by considering their size, zeta-potential, phase transition temperature and fluidity.
28       The sudden decrease of mobility around phase transition temperature and the presence of hystere
29 ane fluidity above, but not below, the lipid phase-transition temperature and did not alter the tempe
30                Here, we demonstrate that the phase-transition temperature and hysteresis can be tuned
31 ied out at 305 K, above the membrane thermal phase transition temperature, and at pH 7.0.
32 re, washed using solvent also held above the phase transition temperature, and then analyzed by reduc
33 esses large-scale phase separation below the phase transition temperature, and, on the other hand, pr
34  from the lowering of the gel-liquid-crystal phase transition temperature as monitored from temperatu
35 in films which results in an increase in the phase transition temperature as thickness is reduced.
36 ced the fluid lamellar-to-inverted hexagonal phase transition temperature at very low concentrations
37 e of dissipation monitoring to determine the phase transition temperature based on the temperature-in
38 rized N-isopropylacrylamide (ppNIPAM) show a phase transition temperature below which the polymer sur
39 m, the phase state deviates from the nominal phase transition temperature by tens of degrees.
40 ition of a second CH CH moiety decreased the phase-transition temperature by approximately 19 degrees
41                  A double bond decreased the phase-transition temperature by approximately 40 degrees
42 th variable thicknesses demonstrate that the phase transition temperature decreases with reducing mic
43 ngle-crystalline VO(2) nanostructures with a phase-transition temperature depressed to as low as 32 d
44              Furthermore, the higher surface-phase-transition temperature driven by surface stabiliza
45 icated that incorporation of BPL reduced the phase transition temperature, enthalpy, and average bila
46 sozyme surface dominated the process and the phase transition temperature followed an inverse Hofmeis
47 e AsF(6)(-) content decreases the reversible-phase-transition temperature gradually down to 99 degree
48 of either antioxidant increased the liposome phase transition temperature (>50 degrees C).
49  experiments identified domains of different phase transition temperatures in the mixed membranes.
50 ambient conditions as well as an increase in phase transition temperatures in the solid state.
51 erature to > 433 K (amorphous-to-crystalline phase transition temperature) in just 0.37 ns with a low
52                                          The phase transition temperature increases slightly dependin
53                            Most (82%) of the phase-transition temperatures measured for Md were above
54                                    Above the phase transition temperature of -74 degrees C, the ring
55 sed the fluid lamellar to inverted hexagonal phase transition temperature of 1,2-dipalmitoleoyl-phosp
56  increase the lamellar to inverted hexagonal phase transition temperature of both PE model lipid syst
57 15am, increases the lamellar-to-hexagonal II phase transition temperature of dioleoylphosphatidyletha
58  (DMPM) vesicles are most prominent near the phase transition temperature of DMPM.
59 tion-induced gel lamellar --> fluid lamellar phase transition temperature of either dipalmitoylphosph
60  chain-length-dependent increase in the main phase transition temperature of equimolar PSM/Cer bilaye
61 egreesC), a very effective depressant of the phase transition temperature of freeze-dried DPPC, marke
62                The liquid crystalline-to-gel phase transition temperature of supported phospholipid b
63  molecules into the bulk solution caused the phase transition temperature of the bilayer to increase.
64                                     Near the phase transition temperature of the DPPC/POPG lipid mixt
65 rs of magnitude lower than the ferromagnetic phase transition temperature of the films.
66 affected by either the gel-to-liquid-crystal phase transition temperature of the lipid or the tempera
67 ture that is stable for weeks just above the phase transition temperature of the lipid.
68  the AFP to the bilayer, which increases the phase transition temperature of the membranes and alters
69  the crystal above the characteristic volume phase transition temperature of the microgel particles r
70 he solution temperature traverses the volume phase transition temperature of the particles.
71 s on cooling below the liquid-crystal to gel phase transition temperature of the pure phospholipid.
72                                          The phase transition temperature of the saturated derivative
73 simple way to determine the true mesomorphic phase transition temperatures of other lipid and lyotrop
74 d to determine the gel-to-liquid crystalline phase transition temperatures of the bolalipids (C32BAS
75 33 of 185 picocoulombs per newton and a high phase-transition temperature of 406 kelvin (K) (16 K abo
76 aining the influence of the compounds on the phase-transition temperature of DPPA liposomes, while th
77                         The influence on the phase-transition temperature of liposomes of dipalmitoyl
78                           Measurement of the phase-transition temperature of peptide-DiPoPE dispersio
79 ain show significant sensitivity to the main phase-transition temperature of the lipid, consistent wi
80   Cholesterol ester had little effect on the phase-transition temperature of the waxes.
81 ed study of the dependence of phase type and phase transition temperatures on several key structural
82 uction of the lamellar-to-inverted hexagonal phase transition temperature, suggesting that Cer-1-P in
83 n of increasing temperature toward the lipid-phase transition temperature (T(C)), for coronene-labele
84 pacings on either side of the L(alpha)/H(II) phase transition temperature (T(h)) depends significantl
85 s (WALP14-17) lowered the inverted hexagonal phase transition temperature (T(H)) of DEPE, with an eff
86 eability of liposomes near the gel-to-liquid phase transition temperature (T(m)) to deliver reagents
87 e thermal stability of the bilayer below the phase-transition temperature (T(m)) as compared to the g
88  cycled repeatedly across the L(alpha)/H(II) phase transition temperature, T(H), or when the H(II) ph
89 ss-forming sugars to affect the gel-to-fluid phase transition temperature, T(m), of several phosphati
90          The main gel-to-liquid-crystal (LC) phase transition temperature, T(m), of the distal lipid
91 egrees C/hr, and the rate-dependent apparent phase transition temperatures, T(A)(r) were determined f
92            Phenolic compounds also increased phase transition temperature (Tc) of nanoliposomes (2.01
93 sition arises because of the lowering of the phase transition temperature that occurs due to the perd
94 esters of mycolic acids were found to have a phase transition temperature that was linearly related t
95              Surprisingly, we found that the phase transition temperature (Tm) of F-DPPC occurs near
96   The biphasic effect of ethanol on the main phase transition temperature (Tm) of identical-chain pho
97 atalytic rate of PLA2 peaks around the lipid phase transition temperature (Tm) when Tm is not too far
98 phospholipid membranes displaying a range of phase transition temperatures (Tm).
99 )PE can affect the gel-to-liquid crystalline phase transition temperature, Tm, of the lipid bilayer i
100 (M6) conducting to a greater increase in the phase transition temperatures up to 4.14 degrees C, whil
101                                          The phase-transition temperature was significantly higher (4
102 LDI probe surface at a temperature above the phase transition temperature, washed using solvent also
103 iding more physiological lipids with a lower phase transition temperature, we achieved efficient fusi
104 iffering shell thicknesses display identical phase transition temperatures when PCS is used to monito
105  an abrupt behavior near the superconducting phase transition temperature where phase coherence sets
106  of the latency period was greatest near the phase transition temperature where the latency was short
107  both above and below the liquid crystalline phase transition temperature, whereas DOPC displays only
108  alpha,alpha-galacto-trehalose depressed the phase transition temperature, whereas the introduction o

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