Performance of Molecular Mechanics Force Fields for RNA Simulations: Stability of UUCG and GNRA Hairpins.
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Michal Otyepka | Modesto Orozco | Thomas E. Cheatham | Petr Jurečka | Marie Zgarbová | Pavel Banáš | Jiří Šponer | Daniel Hollas | J. Šponer | M. Orozco | T. Cheatham | M. Otyepka | P. Banáš | P. Jurečka | Marie Zgarbová | D. Hollas
[1] P. Moore,et al. The sarcin/ricin loop, a modular RNA. , 1995, Journal of molecular biology.
[2] Joachim Frank,et al. Dynamics of the base of ribosomal A-site finger revealed by molecular dynamics simulations and Cryo-EM , 2009, Nucleic acids research.
[3] H. Heus,et al. A network of heterogeneous hydrogen bonds in GNRA tetraloops. , 1996, Journal of molecular biology.
[4] E. Westhof,et al. Analysis of RNA motifs. , 2003, Current opinion in structural biology.
[5] H. Berendsen,et al. Molecular dynamics with coupling to an external bath , 1984 .
[6] J. Šponer,et al. Single Stranded Loops of Quadruplex DNA As Key Benchmark for Testing Nucleic Acids Force Fields. , 2009, Journal of chemical theory and computation.
[7] Hirotaka Ode,et al. Force field parameters for rotation around χ torsion axis in nucleic acids , 2008, J. Comput. Chem..
[8] Seema Chauhan,et al. Tertiary interactions determine the accuracy of RNA folding. , 2008, Journal of the American Chemical Society.
[9] M. Bansal,et al. A self-consistent formulation for analysis and generation of non-uniform DNA structures. , 1989, Journal of biomolecular structure & dynamics.
[10] J. Feigon,et al. Site-directed spin labeling studies reveal solution conformational changes in a GAAA tetraloop receptor upon Mg(2+)-dependent docking of a GAAA tetraloop. , 2005, Journal of molecular biology.
[11] B. Brooks,et al. Constant pressure molecular dynamics simulation: The Langevin piston method , 1995 .
[12] Harry A. Stern,et al. Reparameterization of RNA χ Torsion Parameters for the AMBER Force Field and Comparison to NMR Spectra for Cytidine and Uridine , 2010, Journal of chemical theory and computation.
[13] T. Cheatham,et al. Determination of Alkali and Halide Monovalent Ion Parameters for Use in Explicitly Solvated Biomolecular Simulations , 2008, The journal of physical chemistry. B.
[14] Jaroslav Koča,et al. Conformations of Flanking Bases in HIV-1 RNA DIS Kissing Complexes Studied by Molecular Dynamics , 2007, Biophysical journal.
[15] D. Crothers,et al. Bent helix formation between RNA hairpins with complementary loops. , 1995, Science.
[16] Jiří Šponer,et al. Molecular dynamics simulations of sarcin–ricin rRNA motif , 2006, Nucleic acids research.
[17] P. Kollman,et al. How well does a restrained electrostatic potential (RESP) model perform in calculating conformational energies of organic and biological molecules? , 2000 .
[18] Pavel Hobza,et al. Stabilization and structure calculations for noncovalent interactions in extended molecular systems based on wave function and density functional theories. , 2010, Chemical reviews.
[19] T. Xia,et al. Direct revelation of multiple conformations in RNA by femtosecond dynamics. , 2007, Journal of the American Chemical Society.
[20] W. L. Jorgensen,et al. Comparison of simple potential functions for simulating liquid water , 1983 .
[21] T. Steitz,et al. Crystal structure of the ribosomal RNA domain essential for binding elongation factors. , 1998, Proceedings of the National Academy of Sciences of the United States of America.
[22] M. Klein,et al. Constant pressure molecular dynamics algorithms , 1994 .
[23] T. Xia. Taking femtosecond snapshots of RNA conformational dynamics and complexity. , 2008, Current opinion in chemical biology.
[24] Eric J. Sorin,et al. Equilibrium conformational dynamics in an RNA tetraloop from massively parallel molecular dynamics , 2010, Nucleic acids research.
[25] K. Hall,et al. Thermodynamics of 2'-ribose substitutions in UUCG tetraloops. , 2001, RNA.
[26] J. Šponer,et al. Different intrastrand and interstrand contributions to stacking account for roll variations at the alternating purine-pyrimidine sequences in A-DNA and A-RNA. , 1991, Journal of molecular biology.
[27] Philip C. Bevilacqua,et al. Contribution of the closing base pair to exceptional stability in RNA tetraloops: roles for molecular mimicry and electrostatic factors. , 2009, Journal of the American Chemical Society.
[28] K. Hall,et al. Unrestrained stochastic dynamics simulations of the UUCG tetraloop using an implicit solvation model. , 1999, Biophysical journal.
[29] C R Woese,et al. Architecture of ribosomal RNA: constraints on the sequence of "tetra-loops". , 1990, Proceedings of the National Academy of Sciences of the United States of America.
[30] A. Garcia,et al. Simulation of the pressure and temperature folding/unfolding equilibrium of a small RNA hairpin. , 2008, Journal of the American Chemical Society.
[31] P. Kollman,et al. A Second Generation Force Field for the Simulation of Proteins, Nucleic Acids, and Organic Molecules , 1995 .
[32] T. Steitz,et al. The kink‐turn: a new RNA secondary structure motif , 2001, The EMBO journal.
[33] A. Klug,et al. The crystal structure of an AII-RNAhammerhead ribozyme: A proposed mechanism for RNA catalytic cleavage , 1995, Cell.
[34] Takeshi Sakata,et al. Studies on the structure and stabilizing factor of the CUUCGG hairpin RNA using chemically synthesized oligonucleotides , 1990, Nucleic Acids Res..
[35] E Westhof,et al. Involvement of a GNRA tetraloop in long-range RNA tertiary interactions. , 1994, Journal of molecular biology.
[36] Daniel Herschlag,et al. RNA simulations: probing hairpin unfolding and the dynamics of a GNRA tetraloop. , 2002, Journal of molecular biology.
[37] F. Javier Luque,et al. Towards a molecular dynamics consensus view of B-DNA flexibility , 2008, Nucleic acids research.
[38] G. Varani. Exceptionally stable nucleic acid hairpins. , 1995, Annual review of biophysics and biomolecular structure.
[39] P A Kollman,et al. Theoretical studies of an exceptionally stable RNA tetraloop: observation of convergence from an incorrect NMR structure to the correct one using unrestrained molecular dynamics. , 1997, Journal of molecular biology.
[40] Y. Chan,et al. The common and the distinctive features of the bulged-G motif based on a 1.04 A resolution RNA structure. , 2003, Nucleic acids research.
[41] Leonidas J. Guibas,et al. Structural Insight into RNA Hairpin Folding Intermediates , 2008, Journal of the American Chemical Society.
[42] Alexander D. MacKerell,et al. All‐atom empirical force field for nucleic acids: II. Application to molecular dynamics simulations of DNA and RNA in solution , 2000 .
[43] M. Karplus,et al. CHARMM: A program for macromolecular energy, minimization, and dynamics calculations , 1983 .
[44] T. Straatsma,et al. THE MISSING TERM IN EFFECTIVE PAIR POTENTIALS , 1987 .
[45] C. Ehresmann,et al. Detailed analysis of RNA-protein interactions within the ribosomal protein S8-rRNA complex from the archaeon Methanococcus jannaschii. , 2001, Journal of molecular biology.
[46] G. Stock,et al. Molecular dynamics simulation of the structure, dynamics, and thermostability of the RNA hairpins uCACGg and cUUCGg. , 2008, The journal of physical chemistry. B.
[47] P. Bevilacqua,et al. Structures, kinetics, thermodynamics, and biological functions of RNA hairpins. , 2008, Annual review of physical chemistry.
[48] C. G. Hoogstraten,et al. Extensive backbone dynamics in the GCAA RNA tetraloop analyzed using 13C NMR spin relaxation and specific isotope labeling. , 2008, Journal of the American Chemical Society.
[49] K. Réblová,et al. Conformational transitions of flanking purines in HIV‐1 RNA dimerization initiation site kissing complexes studied by CHARMM explicit solvent molecular dynamics , 2008, Biopolymers.
[50] T. Darden,et al. A smooth particle mesh Ewald method , 1995 .
[51] G. Varani,et al. Structure of the P1 helix from group I self-splicing introns. , 1995, Journal of molecular biology.
[52] A. Serganov,et al. The crystal structure of UUCG tetraloop. , 2000, Journal of molecular biology.
[53] T. Darden,et al. Particle mesh Ewald: An N⋅log(N) method for Ewald sums in large systems , 1993 .
[54] J. Šponer,et al. Theoretical studies of RNA catalysis: hybrid QM/MM methods and their comparison with MD and QM. , 2009, Methods.
[55] Piotr Cieplak,et al. Free energy profile of RNA hairpins: a molecular dynamics simulation study. , 2010, Biophysical journal.
[56] K. Réblová,et al. Extensive molecular dynamics simulations showing that canonical G8 and protonated A38H+ forms are most consistent with crystal structures of hairpin ribozyme. , 2010, The journal of physical chemistry. B.
[57] H. Heus,et al. Structural features that give rise to the unusual stability of RNA hairpins containing GNRA loops. , 1991, Science.
[58] F. Eckstein,et al. Dynamics of the RNA hairpin GNRA tetraloop. , 2000, Biochemistry.
[59] Wei Wang,et al. Folding of a small RNA hairpin based on simulation with replica exchange molecular dynamics. , 2010, The journal of physical chemistry. B.
[60] David H Mathews,et al. Prediction of RNA secondary structure by free energy minimization. , 2006, Current opinion in structural biology.
[61] Laxmikant V. Kalé,et al. Scalable molecular dynamics with NAMD , 2005, J. Comput. Chem..
[62] A. Tannenbaum,et al. Single nucleotide RNA choreography , 2006, Nucleic acids research.
[63] Gerhard Stock,et al. Free-energy landscape of RNA hairpins constructed via dihedral angle principal component analysis. , 2009, The journal of physical chemistry. B.
[64] V. Ramakrishnan,et al. Functional insights from the structure of the 30S ribosomal subunit and its interactions with antibiotics , 2000, Nature.