Abstract:An efficient combination of the Wang-Landau and transition matrix Monte Carlo methods for protein and peptide simulations is described. At the initial stage of simulation the algorithm behaves like the Wang-Landau algorithm, allowing to sample the entire interval of energies, and at the later stages, it behaves like transition matrix Monte Carlo method and has significantly lower statistical errors. This combination allows to achieve fast convergence to the correct values of density of states. We propose that … Show more
“…There has already been a considerable effort devoted to numerical simulation of the densities of states for complex systems, especially in the context of biomolecules, 29,30 supercooled liquids and glassy systems, [26][27][28][31][32][33][34] as well as in spin systems. 35,36 The recent progress in developing "flat histogram" methods 29,32,33,35,36 has been responsible for much of this success.…”
Section: The Statistical Thermodynamics Of the Potential Energy Lmentioning
confidence: 99%
“…35,36 The recent progress in developing "flat histogram" methods 29,32,33,35,36 has been responsible for much of this success. However, the computational simplicity of this energy-landscape route to the configurational entropy seems to offer some advantages when compared to the effort required by a number of other methods.…”
Section: The Statistical Thermodynamics Of the Potential Energy Lmentioning
In principle, all of the dynamical complexities of many-body systems are encapsulated in the potential energy landscapes on which the atoms move -an observation that suggests that the essentials of the dynamics ought to be determined by the geometry of those landscapes. But what are the principal geometric features that control the long-time dynamics? We suggest that the key lies not in the local minima and saddles of the landscape, but in a more global property of the surface: its accessible pathways. In order to make this notion more precise we introduce two ideas: (1) a switch to a new ensemble that removes the concept of potential barriers from the problem, and (2) a way of finding optimum pathways within this new ensemble. The potential energy landscape ensemble, which we describe in the current paper, regards the maximum accessible potential energy, rather than the temperature, as a control variable.We show here that while this approach is thermodynamically equivalent to the canonical ensemble, it not only sidesteps the idea of barriers, it allows us to be quantitative about the connectivity of a landscape. We illustrate these ideas with calculations on a simple atomic liquid and on the Kob-Andersen model of a glass-forming liquid, showing, in the process, that the landscape of the Kob-Anderson model appears to have a connectivity transition at the landscape energy associated with its mode-coupling transition. We turn to the problem of finding the most efficient pathways through potential energy landscapes in our companion paper.3
“…There has already been a considerable effort devoted to numerical simulation of the densities of states for complex systems, especially in the context of biomolecules, 29,30 supercooled liquids and glassy systems, [26][27][28][31][32][33][34] as well as in spin systems. 35,36 The recent progress in developing "flat histogram" methods 29,32,33,35,36 has been responsible for much of this success.…”
Section: The Statistical Thermodynamics Of the Potential Energy Lmentioning
confidence: 99%
“…35,36 The recent progress in developing "flat histogram" methods 29,32,33,35,36 has been responsible for much of this success. However, the computational simplicity of this energy-landscape route to the configurational entropy seems to offer some advantages when compared to the effort required by a number of other methods.…”
Section: The Statistical Thermodynamics Of the Potential Energy Lmentioning
In principle, all of the dynamical complexities of many-body systems are encapsulated in the potential energy landscapes on which the atoms move -an observation that suggests that the essentials of the dynamics ought to be determined by the geometry of those landscapes. But what are the principal geometric features that control the long-time dynamics? We suggest that the key lies not in the local minima and saddles of the landscape, but in a more global property of the surface: its accessible pathways. In order to make this notion more precise we introduce two ideas: (1) a switch to a new ensemble that removes the concept of potential barriers from the problem, and (2) a way of finding optimum pathways within this new ensemble. The potential energy landscape ensemble, which we describe in the current paper, regards the maximum accessible potential energy, rather than the temperature, as a control variable.We show here that while this approach is thermodynamically equivalent to the canonical ensemble, it not only sidesteps the idea of barriers, it allows us to be quantitative about the connectivity of a landscape. We illustrate these ideas with calculations on a simple atomic liquid and on the Kob-Andersen model of a glass-forming liquid, showing, in the process, that the landscape of the Kob-Anderson model appears to have a connectivity transition at the landscape energy associated with its mode-coupling transition. We turn to the problem of finding the most efficient pathways through potential energy landscapes in our companion paper.3
“…Since the method gives direct access to the density of states of the system, which is independent of the temperature, one can calculate various thermodynamic averages by canonical reweighting at arbitrary nonzero temperature [8]. There has been several improvements and refinements to the WLA by various authors [12][13][14][15][16][17], consequently it has been successfully applied to systems possessing continuous energy spectra also, e.g., liquid crystals, polymers, biomolecules etc. See for example [15], where the authors propose a hybrid algorithm based on the Wang-Landau and transition matrix Monte Carlo methods.…”
Section: Wang-landau Algorithmmentioning
confidence: 99%
“…There has been several improvements and refinements to the WLA by various authors [12][13][14][15][16][17], consequently it has been successfully applied to systems possessing continuous energy spectra also, e.g., liquid crystals, polymers, biomolecules etc. See for example [15], where the authors propose a hybrid algorithm based on the Wang-Landau and transition matrix Monte Carlo methods. In our calculations we implement the t −1 variant [16,17] of WLA which facilitates, in general, a faster convergence rate than the conventional scheme.…”
We propose a method based on the Wang-Landau algorithm to numerically generate the spectral densities of random matrix ensembles. The method employs Dyson's log-gas formalism for random matrix eigenvalues and also enables one to simultaneously investigate the thermodynamic properties. This approach is a powerful alternative to the conventionally used Monte Carlo simulations based on the Boltzmann sampling, and is ideally suited for investigating β-ensembles.
“…The method was tested by Shell et al [12] in two-dimensional Ising model and a Lenard-Jones fluid which suggests that the method is capable of handling both discrete and continuous systems. More recently Ghulghazaryan et al have applied the WLTM method [13] to simulate protein and peptide.…”
Monte Carlo simulation using a combination of Wang-Landau (WL) and Transition Matrix (TM) Monte Carlo algorithms to simulate two lattice spin models with continuous energy is described. One of the models, the one-dimensional Lebwohl-Lasher model has an exact solution and we have used this to test the performance of the mixed algorithm (WLTM). The other system we have worked on is the two-dimensional XY-model. The purpose of the present work is to test the performance of the WLTM algorithm in continuous models and to suggest methods for obtaining best results in such systems using this algorithm.
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