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1 tion of diffusion coefficients, close to the thermal transition.
2 kinetic parameters for the first step of the thermal transition.
3 ing, the papain fragments exhibited a single thermal transition.
4 ramolecular polymers as evidenced by a lower thermal transition.
5 king tendency to face directions with strong thermal transitions.
6  the activation of acute responses to sudden thermal transitions.
7  DSC showed carrier-dependent differences in thermal transitions.
8 n stiffness leads to low solubility and high thermal transitions.
9 esters is triglyceride-rich, does not have a thermal transition above 0 degrees C, and exhibits impai
10                                              Thermal transition analysis of snap-to-it probes with co
11 ut lack the ability to undergo a cooperative thermal transition and are substantially less resistant
12                         The midpoints of the thermal transition and chemical denaturing curves (repre
13 elution time, and refractive indices), bulk (thermal transitions), and film (thermomechanical and rhe
14 polypeptides and the relation to the inverse thermal transition are discussed.
15                                              Thermal transitions are continuous, with a strong compos
16               The MCM protein shows a single thermal transition at 67 degrees C.
17                                          The thermal transition at pH 6.8 leads to a protein state th
18           Electron microscopy shows that the thermal transition at pH 6.8 results in fibril formation
19 lues show that the protein has a distinctive thermal transition at pH 6.8.
20 lization from the neutral pH value, with two thermal transitions at 24 and 27 degrees C.
21        The RAD52(1--192) mutant had only two thermal transitions at 47.6 and 100.9 degrees C (labeled
22 BS sample was found to undergo a cooperative thermal transition between 70 and 75 degrees C, consiste
23                        The results display a thermal transition between different backbone conformati
24 n cooling, these barriers reduce the rate of thermal transitions between the potential wells so much
25 al stability, decreasing the midpoint of the thermal transition by almost 40 degrees C.
26 an provide spatially resolved information on thermal transitions by applying a novel algorithm to ima
27 C, fully hydrated C16:0-LacCer shows complex thermal transitions characteristic of polymorphic behavi
28 hermore, we demonstrate structure-controlled thermal transitions, conjugation to human lysozyme throu
29 ignificant difference in the midpoint of the thermal transition curves (DeltaTm of 21.8 degrees C) an
30  A three-state thermodynamic analysis of the thermal transition curves gives a total DeltaH(0) of unf
31  denaturation: melting temperature, width of thermal transition, deltaG, deltaH, deltaS, and deltaCp.
32 eak as a function of temperature gives sharp thermal transitions for both peptides, similar to those
33                             Furthermore, the thermal transitions for Ca(2+)- and Mg(2+)-regenerated b
34                                          The thermal transitions for the holo form follow the same pa
35 ifferential scanning calorimetry revealed no thermal transitions for these proteins in the range 15-1
36                                          The thermal transitions for these two domains are superimpos
37 cholesteryl ester-rich core that undergoes a thermal transition from a liquid crystalline to an isotr
38 rod and tropomyosin, for which non-two-state thermal transitions have been observed.
39                                              Thermal transitions identified at (150 +/- 10) degrees C
40 pectra of complex polymer systems undergoing thermal transitions, illustrated by application to sever
41 ake at ambient temperature are overcome by a thermal transition in the apo-protein structure.
42                  Using a host polymer with a thermal transition in the regime of interest, we demonst
43 This review focuses on the nature of the non-thermal transitions in semiconductors under femtosecond
44 ecular pieces of evidence on the coupling of thermal transitions in the channels.
45                                    The three thermal transitions in this model were assigned as follo
46 ments show that heat invokes robust, complex thermal transitions in TRPV1 that include both channel o
47 non-Fermi liquid which undergoes first-order thermal transition into a nematic insulator or continuou
48 ition into a nematic insulator or continuous thermal transition into a nematic metal phase, separated
49 V-vis spectra, and XRD all indicate that the thermal transition is due to a crystal-crystal phase tra
50                          This worm-to-sphere thermal transition is essentially irreversible on heatin
51 TPgammaS and AMP-PNP, however, only a single thermal transition is observed at temperatures slightly
52 d where almost complete reversibility of the thermal transitions is attained.
53                                        Three thermal transitions (labeled A, B, and C) were observed
54                                         From thermal transition measurements in the presence of low-m
55                             The irreversible thermal transition (melting), monitored by the appearanc
56                                              Thermal, transition metal-catalysed, and also two differ
57 m-Phe led to a 7.5 degrees C increase in the thermal transition midpoint (T(m)) for denaturation, the
58 e is 12.4 +/- 0.3 kJ mol(-1) (pH 5), and the thermal transition midpoint is 59 +/- 1 degrees C (pH 7)
59  of the Scl2 protein all showed a very sharp thermal transition near 36 degrees C, indicating a highl
60        Furthermore, the unique nature of the thermal transition observed for this system offers up co
61                                  The loss of thermal transition observed in DPC confirms that the pro
62 alorimetry (DSC) showed that an irreversible thermal transition occurred at approximately 39 degrees
63 nteractions are also shown by a calorimetric thermal transition of low cooperativity, and the extende
64 nt of this model, it is found that the major thermal transition of SA in 1% SDS is reversible.
65                                          The thermal transition of the beta2 subunit below 60 degrees
66                                          The thermal transitions of fibrillar collagen are investigat
67 t fiber fortification did not interfere with thermal transitions of surimi myosin and actin.
68 o deionized bacteriorhodopsin (dI-bR) on the thermal transitions of the protein secondary structure h
69                                          The thermal transitions of the TTTT, TTTC, and AAAA octamers
70                                          The thermal transitions of the two derivatives at neutral pH
71 ild-type channels possess a single concerted thermal transition peak, the chimera, in which strong te
72 on by Ferguson analysis and by observing its thermal transition profile; the two molecules behave vir
73                                              Thermal transition profiles suggest a premelting transit
74                                 The observed thermal transition represents the unfolding of the four-
75 allowed the previously reported 75 degrees C thermal transition seen in the excess heat capacity func
76 ith high fidelity, confirmed by native PAGE, thermal transition study, and Ferguson analysis.
77 ship between the critical temperature of the thermal transition, T(1/2), and the highest temperature
78 oreover, RuBisCo proteins exhibited a single thermal transition temperature (~66 degrees C) whereas e
79  decreased whereas fatty acids increased the thermal transition temperature of firefly luciferase.
80                                          The thermal transition temperature of swim bladder ASC (35.0
81                                          The thermal transition temperatures measured by circular dic
82 and bovine fibrinogen as model proteins, the thermal transition temperatures of proteins in dilute an
83 lar morphologies, their domain spacings, and thermal transition temperatures of such materials can be
84 xes with the C-C mismatch cross-link have UV thermal transition temperatures that are 25 degrees C hi
85 culation of a broad distribution of midpoint thermal-transition temperatures measured by the nuclear
86 gesting that virion surface proteins undergo thermal transitions that expose cysteine residues to mod
87 d arenarone broadened the native-to-unfolded thermal transition (Tm), quite different to the large in
88 hodopsin, the primary photoproduct K makes a thermal transition to the L intermediate, which prepares
89            In contrast, BHBmon shows a broad thermal transition, typical of multistate unfolding for
90 ally altered with the appearance of a second thermal transition up to 10 degrees C higher in the pres
91                                          The thermal transitions were asymmetric, and the temperature
92                          Only noncooperative thermal transitions were observed for the PHF samples in
93 were asymmetric, and the temperatures of the thermal transitions were scan rate dependent.
94 ion parameters obtained from the fits to the thermal transitions were used to assess the kinetic stab
95 reversible, endothermic, and very asymmetric thermal transition with a concentration-dependent transi