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1 layer that is already stable above the bulk melting temperature).
2 They are strongest near the charge-stripe melting temperature.
3 from an extrapolation of our results to the melting temperature.
4 of the duplex, linearly correlating with the melting temperature.
5 same temperature difference with the model's melting temperature.
6 s convert to the WZ lattice above a critical melting temperature.
7 ompromised for long strands, except near the melting temperature.
8 terms of the reduction in binding energy and melting temperature.
9 ut 17 kcal/mol in enthalpy or 6 degrees C in melting temperature.
10 ture that is 22 degrees C lower than the DNA melting temperature.
11 elting occurs at temperatures much below the melting temperature.
12 ding was found to increase notably the ds-ON melting temperature.
13 d abnormal electrophoretic migration and low melting temperature.
14 previous studies that were performed at the melting temperature.
15 e from nanorod-based complexes below the DNA melting temperature.
16 ient solution temperature well below the DNA melting temperature.
17 8)-fold increase in the reaction rate at the melting temperature.
18 ization temperature but keeping it below the melting temperature.
19 lifiable target length, the sequence, or the melting temperature.
20 10-30 mus for complete dissociation near the melting temperature.
21 scence-based measurement of the "on-surface" melting temperatures.
22 ng of the energy landscape at the respective melting temperatures.
23 adiogenic heat production to achieve crustal melting temperatures.
24 econdary structures like hairpins and higher melting temperatures.
25 and one of the highest cohesive energies and melting temperatures.
26 und six transient denaturing events near the melting temperature (323 and 330 K) and an additional re
28 ed of ternary mixtures of a lipid with a low melting temperature, a lipid with a high melting tempera
29 though different solvents modify the protein melting temperature, a unique dynamical regime is attain
30 ode made from a refractory metal which has a melting temperature above the melting point of boron.
31 tle silicates and core metal have comparable melting temperatures above 500 to 700 gigapascals, which
32 up to a 14 degrees C decrease in the protein melting temperature after toremifene binding, while ibup
33 or some, but not all, sequence compositions, melting temperature analyses have revealed that both ena
34 e, double-nested PCR approach allowed robust melting temperature analysis with enhanced limits of det
35 A-conjoined copolymers were characterized by melting temperature analysis, circular dichroism spectro
36 e duplex structures were characterized by UV melting temperature analysis, fluorescence spectroscopy,
38 moduli, Vickers hardness, Debye temperature, melting temperature and a possible superconductivity of
41 The survey reveals a correlation between melting temperature and downhill folding previously obse
42 n, the Hp53 and Dmp53 proteins had a similar melting temperature and generally showed a similar energ
43 aracterized with dTm/dP < 0, where Tm is the melting temperature and P is pressure, above a high thre
44 able predictions of water properties such as melting temperature and temperature of maximum density.
46 y are highly stable structures with enhanced melting temperatures and cooperative melting behavior.
47 mol/cm2), and as a result, exhibit increased melting temperatures and cooperative melting properties.
48 formation resulted in solids with different melting temperatures and crystallinities, photochemical
49 tion of type I amylose-lipid complexes, with melting temperatures and enthalpies ranging from 82 to 1
51 decreasing differences between the polyester melting temperatures and the experimental temperatures,
52 ween predicted and experimentally determined melting temperatures and unfolding denaturant concentrat
53 We find that the experimentally measured melting temperatures and unzipping forces are approximat
55 slope of the correlation, coincides with the melting temperature, and duplex unfolding occurs at that
56 tabilization may be responsible for the high melting temperature, and hints at residual structure or
57 oil reduced the crystallisation temperature, melting temperature, and melting enthalpy of tristearin.
58 are identified by differences in the duplex melting temperature, and the use of short hybridization
59 emperature is lowered sufficiently below the melting temperature, and then at even lower temperatures
60 sociation constant of 140 muM and raised its melting temperature, and we have determined the binding
61 oil-loaded particles shifted to lower onset melting temperatures, and major polymorphic form transfo
63 he structural transitions that occur at each melting temperature, are used to propose that the relati
65 previous experiments showed nearly constant melting temperature as a function of pressure, in large
67 fluence of small molecular species on, e.g., melting temperature, as well as routes to induce order i
68 Sodium exhibits a pronounced minimum of the melting temperature at approximately 118 gigapascals and
69 l explains this correlation and predicts the melting temperature at which downhill folding becomes po
72 f the folding transition, dispersions in the melting temperatures at the residue level, and timescale
73 m(Phi) - T m, where T m(Phi) and T m are the melting temperatures at volume fraction Phi of the osmol
74 is, at temperatures below their equilibrium melting temperatures, before eventually crystallizing.
75 Ionic liquids form a class of solvents with melting temperatures below 100 degrees C and, due to ver
78 d they not only bind when cooled below their melting temperature, but also rearrange so that aggregat
79 that insertion mutations lower mt-tRNA(Ser) melting temperature by 6-9 degrees C and increase the fo
82 y of both ALR forms: e.g., by decreasing the melting temperature by about 10 degrees C, by increasing
83 forms of the quadruplex structures differ in melting temperatures by approximately 8 degrees C (60 an
84 binds a relatively small hapten, reduce the melting temperature compared with its germ-line precurso
85 indicated by an 8 degrees C increase in the melting temperature compared with unliganded form and pp
89 while UV melting studies revealed shifts in melting temperature (DeltaT(m)) as large as 10 degrees C
93 , and electron microscopy showed that capsid melting temperatures differed by more than 20 degrees C
94 l analysis of c-Met mutants revealed minimal melting temperature differences indicating that the muta
95 an that of the unfolded RNA, the increase in melting temperature due to the two components is additiv
98 must be added to free duplex DNA to achieve melting temperatures equivalent to hybridized systems fo
102 tal temperatures appear to be below the bulk melting temperature for a single protein, but above the
103 perature for a single protein, but above the melting temperature for concentrated protein solutions.
104 Thermal melting data illustrate that the melting temperature for CYP231A2 increases nearly 10 deg
105 improves the predication of free energy and melting temperature for duplexes closed by wobble base p
106 curve analysis revealed significantly higher melting temperatures for DNA in the presence of oxidized
107 parameters, to facilitate the calculation of melting temperatures for perfectly matching sequences, m
109 sequences, which exhibit large deviations in melting temperature from predictions made by additive th
112 es C but with a conspicuous twist: While the melting temperature goes down the cold unfolding moves i
113 thermal unfolding of MW is reversible with a melting temperature >70 degrees C at 100 muM peptide con
116 personic vehicles because of their very high melting temperatures (>4000 K) among other properties.
118 with experimentally measuring high pressure melting temperatures has motivated the use of ab initio
119 folding (no barrier), the WW domain average melting temperatures have to be >/=50 degrees C for inci
120 torically eluded researchers due to its high melting temperature, high reactivity and unfavorably hig
121 triplexes formed from three G-triads exhibit melting temperatures higher than 37 degrees C, especiall
125 All serogroups were found to display unique melting temperatures, indicating that mutations have acc
126 ing T, and at high-pressure we show that the melting temperature is only 5000 K at 120 GPa, a value l
128 ences have identical length, GC content, and melting temperature; (iv) the identity of each standard
129 ayers composed of a ternary mixture of a low-melting temperature lipid, a high-melting temperature li
131 chain-melting temperature lipids, low chain-melting temperature lipids, and cholesterol undergo late
132 de variety of ternary mixtures of high chain-melting temperature lipids, low chain-melting temperatur
133 ion by eliminating spilling because its high melting temperature means it is solid at room temperatur
134 approximately 0.3 kcal/mol) calculated from melting temperature measurements comparing matched vs. m
135 A combination of chemical ON synthesis, melting temperature measurements, cyclic voltammetry (CV
136 na (like surface melting, size dependence of melting temperature, melting of few nm-size particles an
137 (Ni, Pt, Pd), when dissolved in inactive low-melting temperature metals (In, Ga, Sn, Pb), produce sta
138 on in beta-Sn, unlike grain rotation in high melting temperature metals which undergo displacive defo
139 tool ensures consistent oligomer overlapping melting temperatures, minimizes the likelihood of misann
140 304 bp amplicon, which compared well to the melting temperature obtained using a conventional PCR sy
145 rated using IR heating, and this indicated a melting temperature of 85 degrees C for the 304 bp ampli
146 icles into superstructures, we show that the melting temperature of a 10-base DNA sequence is depende
148 When the agarose-GUVs are heated above the melting temperature of agarose for 2 h before use, vesic
150 terpreted as melting, it would be the lowest melting temperature of any material at these high pressu
156 f polymerization correlate with the apparent melting temperature of each building block, which is dep
158 arth rely critically on the knowledge of the melting temperature of iron at the pressure conditions o
161 pG methylation on the basis of the increased melting temperature of methylated DNA, termed denaturati
164 es below unacetylated fibrils, and below the melting temperature of native Cu2,Zn2-SOD1 (e.g., fibril
169 , the same backbone heterogeneity lowers the melting temperature of RNA duplexes that would otherwise
170 nprecedented conditions and showing that the melting temperature of SiO2 rises to 8300 K at a pressur
172 reduced upon methionine oxidation, while the melting temperature of the C(H)3 domain was only affecte
174 n step, the solution can be heated above the melting temperature of the capture sequence to release t
177 These additional interactions increase the melting temperature of the DBD by up to 2 degrees C and
179 two-phase approach is used to determine the melting temperature of the ice-VII phase in the range of
180 temperatures between 0.5 and 0.64 times the melting temperature of the matrix (1,356 kelvin) under a
181 ture stabilizers, BMVC and BMVC4, raises the melting temperature of the oligonucleotide formed by the
185 ntary-DNA-modified nanoparticles through the melting temperature of the system gives the thermodynami
186 iscriminatory power comes from the decreased melting temperature of the tL.C mismatched hybrid as com
187 e, cooperative unfolding transition having a melting temperature of Tm = 71 +/- 2 degrees C, in agree
188 om temperature, a temperature well below the melting temperature of type I collagen, by collagenase d
189 energies per basepair with the experimental melting temperatures of 60 oligonucleotides, yielding a
192 ncorporated into the probes to normalize the melting temperatures of all target miRNA hybrids allowin
193 lexed with actinomycin D are stabilized with melting temperatures of approximately 79 degrees C.
196 orithms were developed to accurately predict melting temperatures of nanoparticles of various composi
198 currently considerable uncertainty over the melting temperatures of the high-pressure mantle mineral
200 mixtures is dominated by the intrinsic chain melting temperatures of the lipid components, rather tha
201 m) = 324 K), which is notably lower than the melting temperatures of the other four peptides (T(m) ap
202 of these interactions is reflected in higher melting temperatures of the protein-ligand complexes.
203 that of the t.C mismatched hybrid, while the melting temperatures of the tL-A, tL.G and tL.T hybrids
206 nd subsequent cooling to a point between the melting temperatures of unnicked substrate and nicked pr
207 We provide evidence that the wide-ranging melting temperatures of zeolitic MOFs are related to the
208 Stabilization, measured as an increase in melting temperature, of approximately 20 degrees C and a
209 to maximize population coverage, matching of melting temperatures, optimizing de novo sequence length
210 itive specimens with an atypical PCR result (melting temperature outside of the expected range) by se
211 niqueness, probe length, uniformity of probe melting temperature, overlap with SNPs and common repeat
212 show this inference is incorrect for the low melting temperature phosphatidylcholines abundant in mam
213 hickness and the corresponding variations in melting temperature, polymer crystals allow for self-see
215 erall structure but displayed differences in melting temperatures possibly arising from C-terminal co
216 linked copolymer networks exhibiting a broad melting temperature range (DeltaT(m)) are presented, whi
218 re assessed; six unfolded cooperatively with melting temperatures ranging from <11 to >50 degrees C.
220 hylene polymers possess essentially the same melting temperature, regardless of the size of the branc
221 in frozen medium at a temperature below the melting temperature; relaxation is monitored by periodic
223 ntrinsic lack of strength, ductility and low melting temperature severely restricts practical applica
224 idize, as evidenced by an unusually large MB melting temperature shift observed on bridge formation,
226 ed 24-fold mutant to be stably folded with a melting temperature similar to that of the wild-type pro
227 -BG505 SOSIP.664 complex displayed increased melting temperature stability and reduced V3 recognition
231 the doubly acetylated peptide has the lowest melting temperature (T(m) = 324 K), which is notably low
232 urves show that the double mutant exhibits a melting temperature (T(m)) 16 degrees C lower than that
234 rimination is the relationship between probe melting temperature (T(m)) and the temperature at which
235 cRNH) share similar structures but differ in melting temperature (T(m)) by 20 degrees C. ttRNH's grea
236 allows us to decouple the distinct gas phase melting temperature (T(m)) from the temperature at which
238 le, monomeric, and remarkably stable, with a melting temperature (T(m)) of 82.6 degrees C, which is a
240 the DeltaG degrees (37), DeltaH degrees and melting temperature (T(m)) of duplexes containing these
241 an increase of more than 11 degrees C in the melting temperature (T(m)) of the antigen-binding fragme
242 ly stable closed-loop structure, raising the melting temperature (T(m)) of the hybrid by >30 degrees
243 n rates, even at temperatures well below the melting temperature (T(m)) of the hybridized duplex.
245 The moderately thermophilic protein has a melting temperature (T(m)) similar to that of the mesoph
246 ds provides a characteristic set of amplicon melting temperature (T(m)) values that identify which sp
247 lted in about a 30 degrees C increase in the melting temperature (T(m)), as compared to that obtained
249 e alpha-helicity (approximately 70%), median melting temperature (T(m)=58 degrees C), enthalpy (Delta
251 containing U(2'F(ara)) have slightly higher melting temperatures (T(m)) than those containing U(2'F(
254 porcine dermis materials exhibiting a higher melting temperature than their non-crosslinked counterpa
255 relative measure based on apparent simulated melting temperatures that is independent of simulation l
256 -methylamino phosphorodiamidate linkages had melting temperatures that were either comparable or redu
257 concentration tested, formed gel phases with melting temperatures that were equal to, or slightly hig
259 urs at a temperature that is higher than the melting temperature, the data at 1669 cm (-1) are still
264 e at pH 8 but a ca. 50 degrees C drop in the melting temperature (Tm ) was observed at pH 2.5: DeltaD
268 -Gly-Lys(Dnp)- Ser-(Gly-Pro-Hyp)4-NH2] had a melting temperature (Tm) of 36.2 degrees C and was hydro
269 Leishmania spp., followed by analysis of the melting temperature (Tm) of the amplicons on qPCR platfo
271 affinity can be measured as a change in the melting temperature (Tm) of the DNA-modified Au NP aggre
272 mplate walking mechanism using a pair of low-melting temperature (Tm) solid-surface homopolymer prime
273 a significant negative shift in NBD1 thermal melting temperature (Tm), pointing to direct VX-809 inte
276 different temperatures, we obtained relative melting temperatures (Tm) for RNA structures in over 400
279 trafast unfolding and folding protein at its melting temperature to observe, on an atom-by-atom basis
280 rection function was developed that predicts melting temperatures, transition enthalpies, entropies,
281 temperature of solid will not rise above the melting temperature unless all solid is molten, thus nan
282 rationally engineered antagonists exhibited melting temperatures up to approximately 64 degrees C, a
283 useful and very flexible tool for predicting melting temperatures using approximative formulae or Nea
288 hibited superheating, the enhancement of the melting temperature was far smaller than the depression
291 in were also generated, and the experimental melting temperature was not significantly different from
293 tability of the duplex (as measured from the melting temperature), where a greater noise in the measu
294 be approximately 0.44 micros at the thermal melting temperature, which makes it one of the fastest f
295 kers are uniformly distributed above the DNA melting temperature, while visibly accumulating at the i
296 mino modified PMO was found to have a higher melting temperature with either complementary DNA or RNA
297 on properties by using accurate estimates of melting temperature with mismatches, computed based on t
298 ordered layer that forms well above the bulk melting temperature with thickness that increases on app
299 fected both the gelling rate and the network melting temperature, with the beta-glucan itself giving
300 both states of RC(L), increasing their half-melting temperature, without affecting enthalpy changes.
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