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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
27 and catalyst is semicrystalline with a T(m) (melting temperature) = 87 degrees C.
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,
37 me PCR assays followed by electrophoresis or melting temperature analysis, respectively.
38 moduli, Vickers hardness, Debye temperature, melting temperature and a possible superconductivity of
39        In particular, the sudden drop of the melting temperature and appearance of the dip at N = 56
40 plementary pairs above the oligonucleotides' melting temperature and attaching new bioreceptors.
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.
45                                          The melting temperature and the heat flow reflect the type a
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
50                                          The melting temperatures and latent heat of CPCMs are in the
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
54 low melting temperature, a lipid with a high melting temperature, and cholesterol.
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
62                                 Our computed melting temperatures are consistent with existing diamon
63 he structural transitions that occur at each melting temperature, are used to propose that the relati
64                           We obtain the same melting temperature (around 45 degrees C) using the bulk
65  previous experiments showed nearly constant melting temperature as a function of pressure, in large
66          These proteins have probe-dependent melting temperatures as high as 80 degrees C and exhibit
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
70 useful tool for designing primers at various melting temperatures at good target coverage.
71                              A dispersion of melting temperatures at pH5.3 for individual residues of
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
76                    The shared ancestor has a melting temperature between those of ttRNH and ecRNH; th
77                                      2), The melting temperature, both in the bulk and at surfaces, d
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
80 -carbon increases the peptide's triple helix melting temperature by 8.6 degrees C.
81 axially compressed solid state, reducing the melting temperature by 80% or 4,000 K.
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
86       The interruptions had little effect on melting temperature, consistent with the high thermal st
87                                          The melting temperatures decrease linearly as the concentrat
88 the temperature of maximum stability and the melting temperature decreased on encapsulation.
89  while UV melting studies revealed shifts in melting temperature (DeltaT(m)) as large as 10 degrees C
90 indicated by the substantial decrease in its melting temperature (DeltaTm = -22.9 degrees C).
91 ative hybridization but have distinguishable melting temperatures depending on their positions.
92                          However, transition melting temperatures derived from the differential scann
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
96 RNA/RNA, DNA/RNA and provided corrections to melting temperatures due to the presence of sodium.
97 ucleic acid probes by recording nucleic acid melting temperature during ISH.
98  must be added to free duplex DNA to achieve melting temperatures equivalent to hybridized systems fo
99 ability of target structure in the ensemble, melting temperature, etc.
100                               Furthermore, a melting temperature experiment carried out with an STV-d
101  restricted to temperature ranges around the melting temperature for a pseudoknot.
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
108         Acetylation decreased onset and peak melting temperatures for the insoluble complexes, wherea
109 sequences, which exhibit large deviations in melting temperature from predictions made by additive th
110                                          The melting temperatures from the specific heat profiles are
111                                Probe length, melting temperature, GC content, SNP location in the pro
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 &gt;70 degrees C at 100 muM peptide con
114 an 94% folded at 298 K (97.5% at 280 K) with melting temperatures &gt; 75 degrees C.
115 stability; five of six mutants analyzed have melting temperatures &gt;89 degrees C.
116 personic vehicles because of their very high melting temperatures (&gt;4000 K) among other properties.
117              Computing accurate nucleic acid melting temperatures has become a crucial step for the e
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
122             As this represents ~90% of their melting temperature, if higher-temperature engines are e
123              The power law dependence of the melting temperature increase (DeltaT(m)) on the volume f
124                              The apparent CD melting temperatures indicated that the introduction of
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
127                        It was found that the melting temperature is very similar for KGE and KGD pept
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
130 e of a low-melting temperature lipid, a high-melting temperature lipid, and cholesterol.
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
141  and maintains good thermal stability with a melting temperature of 37 degrees C.
142                           The FSD-1 apparent melting temperature of 41 degrees C may be a reflection
143 e peptide forms a stable triple helix with a melting temperature of 41 degrees C.
144                       However, E2 has a high melting temperature of 84.8 degrees C, which is more aki
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
147            We find that for a given CDK, the melting temperature of a CDK/cyclin/inhibitor complex co
148   When the agarose-GUVs are heated above the melting temperature of agarose for 2 h before use, vesic
149        Phonon density of states, entropy and melting temperature of aluminum were calculated using th
150 terpreted as melting, it would be the lowest melting temperature of any material at these high pressu
151 milar to each other and should not reach the melting temperature of any of the matched hybrids.
152             E3330-amide has no effect on the melting temperature of APE1, suggesting that it does not
153         However, this interaction lowers the melting temperature of APE1, which is consistent with a
154 PPO, isotactic PPO is semicrystalline with a melting temperature of approximately 67 degrees C.
155                      The model describes the melting temperature of DNA as a function of composition
156 f polymerization correlate with the apparent melting temperature of each building block, which is dep
157                                          The melting temperature of ice in the aerosols decreases mon
158 arth rely critically on the knowledge of the melting temperature of iron at the pressure conditions o
159               Here we report new data on the melting temperature of iron in a laser-heated diamond an
160                           Our results show a melting temperature of iron in agreement with most previ
161 pG methylation on the basis of the increased melting temperature of methylated DNA, termed denaturati
162 emperatures more than 30 degrees C above the melting temperature of naked DNA.
163                                          The melting temperature of nanoparticles can be designed to
164 es below unacetylated fibrils, and below the melting temperature of native Cu2,Zn2-SOD1 (e.g., fibril
165 otein that lacks cysteine residues and has a melting temperature of nearly 100 degrees C.
166 are which computes the enthalpy, entropy and melting temperature of nucleic acids.
167  thermal stability, up to more than half the melting temperature of one of the constituents.
168       There is a correlation in the apparent melting temperature of p53 with the body temperature of
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
171                  The ability to increase the melting temperature of tertiary structure by strengtheni
172 reduced upon methionine oxidation, while the melting temperature of the C(H)3 domain was only affecte
173 length and in each case is close to the bulk melting temperature of the capping molecules.
174 n step, the solution can be heated above the melting temperature of the capture sequence to release t
175                                          The melting temperature of the ClU-G mispair is not experime
176  shows dependence on casting temperature and melting temperature of the crystalline segment.
177   These additional interactions increase the melting temperature of the DBD by up to 2 degrees C and
178                                          The melting temperature of the GAAA minihairpin is reduced t
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
182 tween solid and L(o) phases occurs below the melting temperature of the phospholipid (T(m)).
183                         Upon heated over the melting temperature of the polymer, the pores of the nan
184 alamide compound crystallizes just below the melting temperature of the polymer.
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 ion of type II amylose-lipid complexes, with melting temperatures of about 100-120 degrees C.
191                                       First, melting temperatures of all mismatched hybrids should be
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.
194                                              Melting temperatures of duplexes containing cationic or
195                                 The observed melting temperatures of most oligomers correlated roughl
196 orithms were developed to accurately predict melting temperatures of nanoparticles of various composi
197                                          The melting temperatures of slightly hypostoichiometric TaC,
198  currently considerable uncertainty over the melting temperatures of the high-pressure mantle mineral
199                                          The melting temperatures of the hydrates are very similar to
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
204                           By calculating the melting temperatures of the TM strands, our method can a
205                The thermodynamic equilibrium melting temperatures of these phases differ as much as ~
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
214                                  The optimal melting temperatures, positions and concentrations of bl
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
217 hybridize to a siRNA within a user-specified melting temperature range.
218 re assessed; six unfolded cooperatively with melting temperatures ranging from <11 to >50 degrees C.
219 e crystal growth inhibition concomitant with melting temperature reduction.
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
222                                A decrease in melting temperature resulted from the interesterificatio
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,
225                               The calculated melting temperatures showed that the doubly acetylated p
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
228 r, even at temperatures close to the thermal melting temperature T(m).
229                                          The melting temperatures T(m) of the nanoparticles are not a
230                                    While the melting temperature ( T M approximately 59 degrees C) an
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
233 symmetric PCR of the M. tuberculosis RRDR by melting temperature (T(m)) analysis.
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
237                                 We find that melting temperature (T(m)) has the most significant effe
238 le, monomeric, and remarkably stable, with a melting temperature (T(m)) of 82.6 degrees C, which is a
239                                          The melting temperature (T(m)) of DNA is affected not only b
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.
244                    Mutations are detected by melting temperature (T(m)) shifts that occur when the SM
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
248 g times that correspond well with the duplex melting temperature (T(m)).
249 e alpha-helicity (approximately 70%), median melting temperature (T(m)=58 degrees C), enthalpy (Delta
250                      Based on the calculated melting temperatures (T(m) values), however, poly(A)/oli
251  containing U(2'F(ara)) have slightly higher melting temperatures (T(m)) than those containing U(2'F(
252 ntiate the four SNP alleles by four distinct melting temperatures (termed the "4Tm probe").
253 ts, alpha1alpha1alpha2 demonstrated a higher melting temperature than the other two.
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
258                                    Below the melting temperature the threshold for Al44(-) is smaller
259 urs at a temperature that is higher than the melting temperature, the data at 1669 cm (-1) are still
260                When relaxation occurs at the melting temperature, the kinetics at both wavenumbers ar
261                                    Below the melting temperature, the ordered layer initiates crystal
262 s transition temperature Tg, and the crystal melting temperature, TL.
263 d iron (hcp-Fe) at 360 gigapascals up to its melting temperature Tm.
264 e at pH 8 but a ca. 50 degrees C drop in the melting temperature (Tm ) was observed at pH 2.5: DeltaD
265       Both methods have little effect on the melting temperature (Tm) although some differences were
266           Here, we demonstrate that both the melting temperature (Tm) in a subsection of siRNA non-se
267                  We herein report the novel "melting temperature (Tm) mapping method" for rapidly ide
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
270                                          The melting temperature (Tm) of the C(H)2 domain of the huma
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
274 ismatches and the overall sequence-dependent melting temperature (Tm).
275 ng a ssNMR-observed reduction in the lipids' melting temperature (Tm).
276 different temperatures, we obtained relative melting temperatures (Tm) for RNA structures in over 400
277                     Amplifiable beta-globin (melting temperature [Tm], 87.2 degrees C +/- 0.2 degrees
278 lternation in exactly the same manner as the melting temperature, Tm.
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
284 s, allowing genotype discrimination based on melting temperature values.
285                        However, the absolute melting temperatures vary with the selected thermodynami
286  temperature for the Al plane surface and on melting temperature versus particle radius.
287 LEDGF1-326 was 3.3 +/- 0.5 kcal mol(-1), and melting temperature was 44.8 +/- 0.2 degrees C.
288 hibited superheating, the enhancement of the melting temperature was far smaller than the depression
289                                      The DSC melting temperature was lowered by 6 degrees C and the c
290                             This increase in melting temperature was more appreciable for hyperactive
291 in were also generated, and the experimental melting temperature was not significantly different from
292 o undergo an exceptionally steep increase in melting temperature when compressed.
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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