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1 layer that is already stable above the bulk melting temperature).
2 10-30 mus for complete dissociation near the melting temperature.
3 They are strongest near the charge-stripe melting temperature.
4 r, as indicated by a 9 degrees C increase in melting temperature.
5 from an extrapolation of our results to the melting temperature.
6 of the duplex, linearly correlating with the melting temperature.
7 same temperature difference with the model's melting temperature.
8 s convert to the WZ lattice above a critical melting temperature.
9 ompromised for long strands, except near the melting temperature.
10 terms of the reduction in binding energy and melting temperature.
11 ut 17 kcal/mol in enthalpy or 6 degrees C in melting temperature.
12 elting occurs at temperatures much below the melting temperature.
13 ding was found to increase notably the ds-ON 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 ture that is 22 degrees C lower than the DNA melting temperature.
19 d abnormal electrophoretic migration and low melting temperature.
20 ization temperature but keeping it below the melting temperature.
21 lifiable target length, the sequence, or the melting temperature.
22 and one of the highest cohesive energies and melting temperatures.
23 scence-based measurement of the "on-surface" melting temperatures.
24 adiogenic heat production to achieve crustal melting temperatures.
25 econdary structures like hairpins and higher melting temperatures.
26 ng of the energy landscape at the respective melting temperatures.
27 t an unusual confluence of exceptionally low melting temperature (175 degrees C) and inhibited crysta
28 20 carbons providing the maximal increase in melting temperature (~20 degrees C) while completely abo
30 conductivity, (2) greatly increases the ice melting temperature(7-13) to several thousand kelvin, an
32 ed of ternary mixtures of a lipid with a low melting temperature, a lipid with a high melting tempera
33 though different solvents modify the protein melting temperature, a unique dynamical regime is attain
34 ode made from a refractory metal which has a melting temperature above the melting point of boron.
35 tle silicates and core metal have comparable melting temperatures above 500 to 700 gigapascals, which
36 up to a 14 degrees C decrease in the protein melting temperature after toremifene binding, while ibup
37 e, double-nested PCR approach allowed robust melting temperature analysis with enhanced limits of det
38 A-conjoined copolymers were characterized by melting temperature analysis, circular dichroism spectro
39 e duplex structures were characterized by UV melting temperature analysis, fluorescence spectroscopy,
41 the duplex part possess the highest value of melting temperature and a 2-fold higher anticoagulant ef
42 moduli, Vickers hardness, Debye temperature, melting temperature and a possible superconductivity of
45 The survey reveals a correlation between melting temperature and downhill folding previously obse
47 n, the Hp53 and Dmp53 proteins had a similar melting temperature and generally showed a similar energ
48 aracterized with dTm/dP < 0, where Tm is the melting temperature and P is pressure, above a high thre
49 Cl) crystals, a well-studied sample with low melting temperature and quantum super-shells of clusters
50 able predictions of water properties such as melting temperature and temperature of maximum density.
53 rolactone), affording independent control of melting temperature and Young's modulus by concurrently
54 y are highly stable structures with enhanced melting temperatures and cooperative melting behavior.
55 formation resulted in solids with different melting temperatures and crystallinities, photochemical
56 tion of type I amylose-lipid complexes, with melting temperatures and enthalpies ranging from 82 to 1
58 decreasing differences between the polyester melting temperatures and the experimental temperatures,
59 ween predicted and experimentally determined melting temperatures and unfolding denaturant concentrat
61 slope of the correlation, coincides with the melting temperature, and duplex unfolding occurs at that
62 tabilization may be responsible for the high melting temperature, and hints at residual structure or
63 oil reduced the crystallisation temperature, melting temperature, and melting enthalpy of tristearin.
64 are identified by differences in the duplex melting temperature, and the use of short hybridization
65 sociation constant of 140 muM and raised its melting temperature, and we have determined the binding
66 oil-loaded particles shifted to lower onset melting temperatures, and major polymorphic form transfo
68 he structural transitions that occur at each melting temperature, are used to propose that the relati
70 previous experiments showed nearly constant melting temperature as a function of pressure, in large
72 fluence of small molecular species on, e.g., melting temperature, as well as routes to induce order i
73 Sodium exhibits a pronounced minimum of the melting temperature at approximately 118 gigapascals and
74 l explains this correlation and predicts the melting temperature at which downhill folding becomes po
77 f the folding transition, dispersions in the melting temperatures at the residue level, and timescale
78 is, at temperatures below their equilibrium melting temperatures, before eventually crystallizing.
79 Ionic liquids form a class of solvents with melting temperatures below 100 degrees C and, due to ver
83 d they not only bind when cooled below their melting temperature, but also rearrange so that aggregat
84 that insertion mutations lower mt-tRNA(Ser) melting temperature by 6-9 degrees C and increase the fo
87 y of both ALR forms: e.g., by decreasing the melting temperature by about 10 degrees C, by increasing
88 forms of the quadruplex structures differ in melting temperatures by approximately 8 degrees C (60 an
89 binds a relatively small hapten, reduce the melting temperature compared with its germ-line precurso
90 indicated by an 8 degrees C increase in the melting temperature compared with unliganded form and pp
99 , and electron microscopy showed that capsid melting temperatures differed by more than 20 degrees C
100 l analysis of c-Met mutants revealed minimal melting temperature differences indicating that the muta
101 emarkable suppression of crystallization and melting temperatures (down to -80 degrees C from 15 degr
102 an that of the unfolded RNA, the increase in melting temperature due to the two components is additiv
103 RNA/RNA, DNA/RNA and provided corrections to melting temperatures due to the presence of sodium.
108 tal temperatures appear to be below the bulk melting temperature for a single protein, but above the
109 perature for a single protein, but above the melting temperature for concentrated protein solutions.
110 curve analysis revealed significantly higher melting temperatures for DNA in the presence of oxidized
111 parameters, to facilitate the calculation of melting temperatures for perfectly matching sequences, m
113 sequences, which exhibit large deviations in melting temperature from predictions made by additive th
116 es C but with a conspicuous twist: While the melting temperature goes down the cold unfolding moves i
118 personic vehicles because of their very high melting temperatures (>4000 K) among other properties.
120 with experimentally measuring high pressure melting temperatures has motivated the use of ab initio
121 torically eluded researchers due to its high melting temperature, high reactivity and unfavorably hig
122 triplexes formed from three G-triads exhibit melting temperatures higher than 37 degrees C, especiall
123 me digital LAMP (dLAMP) with high-resolution melting temperature (HRM) analysis and use this single-m
127 All serogroups were found to display unique melting temperatures, indicating that mutations have acc
128 ing T, and at high-pressure we show that the melting temperature is only 5000 K at 120 GPa, a value l
129 experiments in which pressurized ice at its melting temperature is slid over a water-saturated till
131 ences have identical length, GC content, and melting temperature; (iv) the identity of each standard
132 lipid bilayers composed of a high and a low melting temperature lipid and cholesterol represent a mo
133 ayers composed of a ternary mixture of a low-melting temperature lipid, a high-melting temperature li
135 ion by eliminating spilling because its high melting temperature means it is solid at room temperatur
136 approximately 0.3 kcal/mol) calculated from melting temperature measurements comparing matched vs. m
137 A combination of chemical ON synthesis, melting temperature measurements, cyclic voltammetry (CV
138 na (like surface melting, size dependence of melting temperature, melting of few nm-size particles an
139 (Ni, Pt, Pd), when dissolved in inactive low-melting temperature metals (In, Ga, Sn, Pb), produce sta
140 on in beta-Sn, unlike grain rotation in high melting temperature metals which undergo displacive defo
141 tool ensures consistent oligomer overlapping melting temperatures, minimizes the likelihood of misann
142 304 bp amplicon, which compared well to the melting temperature obtained using a conventional PCR sy
147 rated using IR heating, and this indicated a melting temperature of 85 degrees C for the 304 bp ampli
148 icles into superstructures, we show that the melting temperature of a 10-base DNA sequence is depende
150 When the agarose-GUVs are heated above the melting temperature of agarose for 2 h before use, vesic
152 terpreted as melting, it would be the lowest melting temperature of any material at these high pressu
160 arth rely critically on the knowledge of the melting temperature of iron at the pressure conditions o
163 pG methylation on the basis of the increased melting temperature of methylated DNA, termed denaturati
166 es below unacetylated fibrils, and below the melting temperature of native Cu2,Zn2-SOD1 (e.g., fibril
171 , the same backbone heterogeneity lowers the melting temperature of RNA duplexes that would otherwise
172 nprecedented conditions and showing that the melting temperature of SiO2 rises to 8300 K at a pressur
173 Tpm3.1 dimers, show that ATM-3507 shifts the melting temperature of the C-terminus and the overlap ju
175 n step, the solution can be heated above the melting temperature of the capture sequence to release t
178 These additional interactions increase the melting temperature of the DBD by up to 2 degrees C and
179 temperatures between 0.5 and 0.64 times the melting temperature of the matrix (1,356 kelvin) under a
180 ture stabilizers, BMVC and BMVC4, raises the melting temperature of the oligonucleotide formed by the
181 the more stable, while being lower than the melting temperature of the original orange, or final yel
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
190 thalate (PET) which has glass transition and melting temperatures of 76 and 250 degrees C, respective
193 ncorporated into the probes to normalize the melting temperatures of all target miRNA hybrids allowin
194 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 of these interactions is reflected in higher melting temperatures of the protein-ligand complexes.
201 that of the t.C mismatched hybrid, while the melting temperatures of the tL-A, tL.G and tL.T hybrids
203 due to easily discernable differences in the melting temperatures of the two species along this mini
205 nd subsequent cooling to a point between the melting temperatures of unnicked substrate and nicked pr
206 We provide evidence that the wide-ranging melting temperatures of zeolitic MOFs are related to the
207 Stabilization, measured as an increase in melting temperature, of approximately 20 degrees C and a
208 to maximize population coverage, matching of melting temperatures, optimizing de novo sequence length
209 itive specimens with an atypical PCR result (melting temperature outside of the expected range) by se
210 show this inference is incorrect for the low melting temperature phosphatidylcholines abundant in mam
211 hickness and the corresponding variations in melting temperature, polymer crystals allow for self-see
213 erall structure but displayed differences in melting temperatures possibly arising from C-terminal co
214 ue biomarker probe pairs with characteristic melting temperatures; post-amplification melting curve a
215 ty of PCR primers is further evaluated using melting temperature, primer dimer, hairpin structure and
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
230 region (RRDR) of the rpoB gene by the use of melting temperature (T(m) ) information from 4 rpoB prob
231 is results in a tunable wavelength-dependent melting temperature (T(m) ) window (4.5-15 degrees C) an
233 urves show that the double mutant exhibits a melting temperature (T(m)) 16 degrees C lower than that
235 rimination is the relationship between probe melting temperature (T(m)) and the temperature at which
236 he protein stability of EftM is tuned with a melting temperature (T(m)) around 37 degrees C such that
237 MSP amplicon, and measures the difference in melting temperature (T(m)) between the two probes (Delta
238 cRNH) share similar structures but differ in melting temperature (T(m)) by 20 degrees C. ttRNH's grea
239 allows us to decouple the distinct gas phase melting temperature (T(m)) from the temperature at which
240 le, monomeric, and remarkably stable, with a melting temperature (T(m)) of 82.6 degrees C, which is a
241 ulfonamide modification caused a decrease in melting temperature (T(m)) of both hybrids, it was lower
243 the DeltaG degrees (37), DeltaH degrees and melting temperature (T(m)) of duplexes containing these
244 an increase of more than 11 degrees C in the melting temperature (T(m)) of the antigen-binding fragme
245 ly stable closed-loop structure, raising the melting temperature (T(m)) of the hybrid by >30 degrees
247 The moderately thermophilic protein has a melting temperature (T(m)) similar to that of the mesoph
249 ds provides a characteristic set of amplicon melting temperature (T(m)) values that identify which sp
250 lted in about a 30 degrees C increase in the melting temperature (T(m)), as compared to that obtained
253 containing U(2'F(ara)) have slightly higher melting temperatures (T(m)) than those containing U(2'F(
256 porcine dermis materials exhibiting a higher melting temperature than their non-crosslinked counterpa
257 relative measure based on apparent simulated melting temperatures that is independent of simulation l
258 -methylamino phosphorodiamidate linkages had melting temperatures that were either comparable or redu
259 concentration tested, formed gel phases with melting temperatures that were equal to, or slightly hig
265 e at pH 8 but a ca. 50 degrees C drop in the melting temperature (Tm ) was observed at pH 2.5: DeltaD
269 -Gly-Lys(Dnp)- Ser-(Gly-Pro-Hyp)4-NH2] had a melting temperature (Tm) of 36.2 degrees C and was hydro
270 Leishmania spp., followed by analysis of the melting temperature (Tm) of the amplicons on qPCR platfo
271 mplate walking mechanism using a pair of low-melting temperature (Tm) solid-surface homopolymer prime
272 a significant negative shift in NBD1 thermal melting temperature (Tm), pointing to direct VX-809 inte
275 different temperatures, we obtained relative melting temperatures (Tm) for RNA structures in over 400
278 ed significant changes on beta-lactoglobulin melting temperature, unfolded conformation and subsequen
279 temperature of solid will not rise above the melting temperature unless all solid is molten, thus nan
280 rationally engineered antagonists exhibited melting temperatures up to approximately 64 degrees C, a
281 useful and very flexible tool for predicting melting temperatures using approximative formulae or Nea
286 hibited superheating, the enhancement of the melting temperature was far smaller than the depression
289 in were also generated, and the experimental melting temperature was not significantly different from
291 rmal stability (up to 29 degrees C increased melting temperature) when compared to that of the linear
292 tability of the duplex (as measured from the melting temperature), where a greater noise in the measu
294 kers are uniformly distributed above the DNA melting temperature, while visibly accumulating at the i
295 mino modified PMO was found to have a higher melting temperature with either complementary DNA or RNA
296 on properties by using accurate estimates of melting temperature with mismatches, computed based on t
297 ordered layer that forms well above the bulk melting temperature with thickness that increases on app
298 fected both the gelling rate and the network melting temperature, with the beta-glucan itself giving
299 eriments reveal that DAP substitution raises melting temperatures without diminishing sequence-depend
300 both states of RC(L), increasing their half-melting temperature, without affecting enthalpy changes.