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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
  
    26 er (Tg > 110 degreesC), does not depress the phase transition temperature and affects only slightly t
  
  
    29 ane fluidity above, but not below, the lipid phase-transition temperature and did not alter the tempe
  
  
    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
  
    40 ition of a second CH CH moiety decreased the phase-transition temperature by approximately 19 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
  
    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
  
    49  experiments identified domains of different phase transition temperatures in the mixed membranes.   
  
    51 erature to > 433 K (amorphous-to-crystalline phase transition temperature) in just 0.37 ns with a low
  
  
  
    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
  
    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
  
    63  molecules into the bulk solution caused the phase transition temperature of the bilayer to increase.
  
  
    66 affected by either the gel-to-liquid-crystal phase transition temperature of the lipid or the tempera
  
    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
  
    71 s on cooling below the liquid-crystal to gel phase transition temperature of the pure phospholipid.  
  
    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
  
  
    79 ain show significant sensitivity to the main phase-transition temperature of the lipid, consistent wi
  
    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
  
    91 egrees C/hr, and the rate-dependent apparent phase transition temperatures, T(A)(r) were determined f
  
    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
  
    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
  
    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
  
   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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