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1 bel-free single-molecule analysis of DNA and RNA folding.
2 nstead, they are governed by the kinetics of RNA folding.
3 property of transcription that can influence RNA folding.
4 nents: primary ligand binding and subsequent RNA folding.
5 section of the roles of DEAD box proteins in RNA folding.
6 roup I intron, to address basic questions in RNA folding.
7 osome, and an interesting paradigm for large RNA folding.
8 inants in the energetic balance that governs RNA folding.
9 he energetic contribution of these forces in RNA folding.
10 at nature has not completely optimized P4-P6 RNA folding.
11 acromolecules via comparisons of protein and RNA folding.
12 e-resolved infrared spectroscopy in studying RNA folding.
13 rucial to a detailed understanding of global RNA folding.
14 nactive structures that are kinetic traps in RNA folding.
15 ose continued presence is not required after RNA folding.
16 teractions from the intrinsic free energy of RNA folding.
17 ll picture of the energetics of Mg2+-induced RNA folding.
18 al utility of pyrene fluorescence to monitor RNA folding.
19 tly for the rapid collapse observed early in RNA folding.
20 lows us to extract the elusive prefactor for RNA folding.
21 e generalized to understand protein-assisted RNA folding.
22 hat is not anticipated by current models for RNA folding.
23 lar mechanism of transcriptional pausing and RNA folding.
24 volved in catalysis from those important for RNA folding.
25 ly formed prior to the rate-limiting step in RNA folding.
26 o resolve nonnative structures formed during RNA folding.
27 by demonstrating functional reversibility in RNA folding.
28 sms driving these early compaction events in RNA folding.
29 y, as well as allow genome-scale analyses of RNA folding.
30 pecific RNases and thermodynamic modeling of RNA folding.
31 -loop-helix motifs, serves as a paradigm for RNA folding.
32 interactions as essential driving forces for RNA folding.
33 r for the use of human-guided simulations to RNA folding.
34 ze topological constraints as a key force in RNA folding.
35 act order model will not suffice to describe RNA folding.
36 argely ignored the effects of nonequilibrium RNA folding.
37 synergy between ligand- and Mg(2+)-mediated RNA folding.
38 ia a rugged energy landscape, reminiscent of RNA folding.
39 anging from simple ligand binding to complex RNA folding.
40 sition with regulatory factor binding and/or RNA folding, a direct causal link between pausing and ch
43 n is an original extension of the underlying RNA folding algorithm to account for the likely existenc
44 Based on our experimental results and an RNA folding algorithm, we predict that RepE binding to t
46 extensive RNA structure was predicted using RNA folding algorithms and confirmed by selective 2'-hyd
47 oximately 150 nt 3'-adjacent to the UGA, and RNA folding algorithms revealed the potential for a phyl
48 vity data that can be used as constraints in RNA folding algorithms to predict structures on par with
49 singly apparent over the last several years: RNA folding algorithms underlie numerous applications in
54 r results indicate substantial modularity in RNA folding and assembly and suggest that these processe
55 understanding of the roles of metal ions in RNA folding and catalysis and have applications in struc
56 us cofactor for nucleic acids, with roles in RNA folding and catalysis as well as in processing of nu
60 s is important for high-precision studies of RNA folding and catalytic behavior, but photodamage accr
61 f the physical origins of the DeltaC(P)s for RNA folding and consider their impact on biological func
62 eight specific pRNA sites without perturbing RNA folding and dimer formation, and a total of 17 inter
70 ors, recent advances in our understanding of RNA folding and functions have motivated the use of RNA
71 Our results highlight multiple pathways in RNA folding and illustrate how kinetic competitions betw
73 hese findings provide a global assessment of RNA folding and its significant regulatory effects in a
76 ing to an understanding of the principles of RNA folding and of the molecular interactions that under
77 landscape, with sequential and hierarchical RNA folding and protein binding events finally convergin
78 d mutation assay, we show that strengthening RNA folding and reducing R-loop formation by synonymous
79 for quantitative, time-resolved analysis of RNA folding and ribonucleoprotein (RNP) assembly mechani
80 A collapsed states play fundamental roles in RNA folding and ribonucleoprotein assembly processes, th
85 bility, uncover rG4-dependent differences in RNA folding and show evolutionarily conserved enrichment
87 e native state is not a universal feature of RNA folding and that there is an alternative paradigm in
88 between the early conformational changes in RNA folding and the "burst phase" changes and molten glo
89 abilizing transient RNA conformations, while RNA folding and the early stages of protein binding are
91 These findings provide a new paradigm for RNA folding and they underscore the diversity of RNA bio
92 alized conformational events contributing to RNA folding and unfolding that could not be observed by
94 to investigate the biophysical mechanisms of RNA folding and unfolding, its interactions with ligands
95 d connectivity are important determinants of RNA folding, and demonstrates the potential of coarse-gr
97 red to be a dedicated regulator of ribosomal RNA folding, and has been shown to prevent Rho-dependent
98 ng been recognized as a key factor governing RNA folding, and is crucial for many diverse functions o
100 ess: specific binding by a few copies of CP, RNA folding, and then cooperative binding of CP to the "
101 RS3D is widely applicable to a variety of RNA folding architectures currently present in the struc
104 deal system for investigating this aspect of RNA folding as ligand-dependent termination is obligator
105 lead to a superior fluorescence signal upon RNA folding, as demonstrated by equilibrium titrations w
106 lly active RNA structure is still limited by RNA folding, as visualized directly using time-resolved
108 ghlight the importance of chain stiffness to RNA folding; at 10 mM Mg2 +, a stiff hinge limits the ra
109 tive framework for describing key aspects of RNA folding behavior and also provide the first evidence
113 , is not designed for applications involving RNA folding but rather offers a stable RNA structure for
114 tead we propose that higher [Mg(2+)] can aid RNA folding by decreasing the entropic penalty of counte
115 stigated the mechanism of chaperone-mediated RNA folding by following the time-resolved dimerization
118 strated that the local free-energy minima of RNA folding can be used to detect the positions of the s
121 perimental results for the thermodynamics of RNA folding cannot be explained by simple pairwise hydro
122 ses, sequentially acquiring capabilities for RNA folding, catalysis, subunit association, correlated
123 m whereby metabolite-dependent alteration of RNA folding controls splicing and alternative 3' end pro
124 oss protein-coding transcripts that indicate RNA folding demarcates regions of protein translation an
125 ructure determines the speed and accuracy of RNA folding, docking of a tetraloop with its receptor in
126 s and was greatly facilitated by a conserved RNA folding domain (1,470 to 1,877 nucleotides upstream)
128 We explore the temperature dependence of RNA folding due to the ubiquitous GAAA tetraloop-recepto
135 extracted from the data correlate well with RNA folding energies obtained from cotranscriptional fol
137 active folds occurs unexpectedly high on the RNA folding energy landscape, resulting in partially irr
138 aled two sequential steps of protein-induced RNA folding, establishing a hierarchical RNP assembly me
141 resistance that we used with mutagenesis and RNA folding experiments to show that Xrn1-resistant RNAs
142 energetic linkage between Mg(2+) binding and RNA folding for both of these systems without requiring
146 in the eventual quantitative description of RNA folding from its secondary and tertiary structural e
148 the experimental study of cotranscriptional RNA folding has been limited by the lack of easily appro
150 insights into electrostatic contributions to RNA folding; however, it can be challenging to isolate t
152 free grammars, that emulates the kinetics of RNA folding in a simplified way, in combination with a m
154 ms, yet the thermodynamic forces which drive RNA folding in vitro may not be sufficient to predict st
155 and II introns are prone to kinetic traps in RNA folding in vivo and that the splicing of both types
158 The data support a mechanistic model of RNA folding in which the element is comprised of both ca
159 ifs carry out a wide variety of functions in RNA folding, in RNA-RNA and RNA-protein interactions.
160 ulated data obtained from a kinetic model of RNA folding, in which the dynamics consists of jumping b
162 he opportunity to determine the structure of RNA folding intermediates and conformational trajectorie
165 iological processes, including initiation of RNA folding into complex tertiary shapes, promotion of d
166 ch backbone heterogeneity is compatible with RNA folding into defined three-dimensional structures th
167 s suggest that the protein cofactor-assisted RNA folding involves sequential non-specific and specifi
184 key issues in the theoretical prediction of RNA folding is the prediction of loop structure from the
186 counting for this phenomenon of Mg2+-induced RNA folding, it is necessary to independently determine
188 the rugged energy landscapes and multistate RNA folding kinetics even for small RNA systems such as
189 a general computational approach to simulate RNA folding kinetics that can be used to extract populat
193 an unprecedented view of the topology of an RNA folding landscape and the RNA structural features th
194 identify the same biases in a computational RNA-folding landscape as well as regulatory sequence bin
195 oximating the set of local minima in partial RNA folding landscapes associated with a bounded-distanc
196 esults show that RNA chaperones can simplify RNA folding landscapes by weakening intramolecular inter
197 e data demonstrate that severe ruggedness of RNA folding landscapes extends into conformational space
201 motions have the greater potential to govern RNA folding, ligand recognition, and ribonucleoprotein a
202 quitous nature of misfolded intermediates in RNA folding, little is known about their physical proper
203 oped thermodynamic scanning method predicted RNA folding mapping precisely to regions of SSSV and at
204 he perspective that a generalizable model of RNA folding may be developed from understanding of the f
205 he weak capacity of Tris-borate to stabilize RNA folding may reflect relatively unfavorable interacti
206 d with temperature-dependent single-molecule RNA folding measurements, which identify that crowding e
207 ous thermodynamics-based models of a general RNA folding mechanism, our observations indicate that st
208 on in bacterial cells, putrescine2+, and how RNA folding might be influenced by the three ions in com
209 ly developed "Vfold" model (a coarse-grained RNA folding model) provides an effective method to gener
213 tion (GAIT)-elements relies on the conserved RNA folding motifs rather than the conserved sequence mo
217 biophysical factors, such as the kinetics of RNA folding; no current implementation considers both ev
218 er the potential for intramolecular rod-like RNA folding nor the presence of the delta protein confer
223 rder of protein binding, suggesting that the RNA folding pathway forms the basis for early steps of r
225 RET methods to address the thermodynamics of RNA folding pathways by probing the intramolecular docki
228 lysis, m-values (change in DeltaG degrees of RNA folding per molal concentration of osmolyte) have be
230 econdary structures of the HIV-2 RRE and two RNA folding precursors have been identified using the SH
232 ates that successful designs for the inverse RNA folding problem does not necessarily have to rely on
235 raction with a combinatorial approach to the RNA folding problem in order to compute all possible non
243 complex energy landscapes often observed for RNA folding processes and lays the groundwork for a sign
246 Sequence alignment software, thermodynamic RNA folding programs, and classical comparative phylogen
247 ion is not predicted by available predictive RNA folding programs, is the major conformer at physiolo
249 s to promote only the final few angstroms of RNA folding rather than mediate global conformational re
252 nding the linkage between Mg(2+) binding and RNA folding requires a proper theoretical model describi
253 oteins to DNA and RNA, DNA condensation, and RNA folding, requires an understanding of the ion atmosp
255 h that used mechanistic modeling and kinetic RNA folding simulations to engineer RNA-regulated geneti
256 eveloped an open software for coarse-grained RNA folding simulations, guided by human intuition.
261 -pair resolution while also allowing for the RNA folding statistics of smaller RNA sequences to be co
262 V is involved in a critical Mg(2+)-dependent RNA folding step in group II introns and demonstrate the
263 ndicate that cellular factors delay specific RNA folding steps to ensure the quality of assembly.
267 biophysical effects that are known to affect RNA folding such as chemical nucleotide modifications an
268 es about the cellular environment effects in RNA folding, such as molecular crowding and cotranscript
269 kinetic and thermodynamic profiles for this RNA folding system when stabilized by potassium versus m
270 We describe a protocol developed to study RNA folding that can be readily tailored to particular a
271 s a new and important level of complexity in RNA folding that could be relevant to the biological fun
273 opose a new regulatory mechanism mediated by RNA folding that may also explain the dual properties of
274 undational for a predictive understanding of RNA folding that will allow manipulation of RNA folding
275 nce information as well as simple aspects of RNA folding that would be occurring during the RNA/capsi
276 e of their frequent transcription and strong RNA folding, the latter also improves translational fide
277 rary to the expectation that Mg2+ stabilizes RNA folding, the mtRNAMet D-domain structure was unfolde
278 ugh DEAD-box proteins play multiple roles in RNA folding, the physiological function of Mss116p in aI
280 hypothesis inspired by this modularity-that RNA folding thermodynamics and kinetics can be quantitat
283 -molecular-weight polyethylene glycol on the RNA folding thermodynamics is dramatic, with up to Delta
286 lecular processes, spanning from protein and RNA folding to functional transitions in molecular machi
288 roblems, from fibril structure prediction to RNA folding to the design of new protein interfaces, to
290 extension (SHAPE)-directed ensemble for the RNA folding under different conditions, and we project t
292 s permit crowding effects on the kinetics of RNA folding/unfolding to be explored for the first time
293 though we have illustrated the complexity of RNA folding using hTR as a case study, general arguments
295 o study the role of sequence and topology in RNA folding, we determined the kinetic folding pathways
296 ne the role of topology and contact order in RNA folding, we screened for circular permutants of the
297 the massively parallel genetic algorithm for RNA folding, we show that the core region of the 3'-untr
298 iversal mechanism for monovalent facilitated RNA folding, whereby an increasing monovalent concentrat
299 turn provides an excellent, simple model for RNA folding, which can be dissected at the atomic level.
300 Synchronization of factor binding and/or RNA folding with the RNA polymerase position is a major
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