arXiv subjects

E. Akturk

Publications and source records attributed to E. Akturk.

12 recordsLinked to original sources

arXiv2009

High-capacity hydrogen storage by metallized graphene

First-principles plane wave calculations predict that Li can be adsorbed on graphene forming a uniform and stable coverage on both sides. A significant part of the electronic charge of the Li-$2s$ orbital is donated to graphene and is accommodated by its distorted $π^*$-bands. As a result, semimetallic graphene and semiconducting graphene ribbons change into good metals. It is even more remarkable that Li covered graphene can serve as a high-capacity hydrogen storage medium with each adsorbed Li absorbing up to four H$_2$ molecules amounting to a gravimetric density of 12.8 wt%.

cond-mat.mes-hall↗

arXiv2009

Hydrogen storage of calcium atoms adsorbed on graphene: First-principles plane wave calculations

Based on the first-principles plane wave calculations, we showed that Ca adsorbed on graphene can serve as a high-capacity hydrogen storage medium, which can be recycled by operations at room temperature. Ca is chemisorbed by donating part of its 4s-charge to the empty $π^*$-band of graphene. At the end adsorbed Ca atom becomes positively charged and the semi-metallic graphene change into a metallic state. While each of adsorbed Ca atoms forming the (4x4) pattern on the graphene can absorb up to five H_2 molecules, hydrogen storage capacity can be increased to 8.4 wt % by adsorbing Ca to both sides of graphene and by increasing the coverage to form the (2x2) pattern. Clustering of Ca atoms is hindered by the repulsive Coulomb interaction between charged Ca atoms.

cond-mat.mes-hall↗

arXiv2008

Two and One-dimensional Honeycomb Structure of Boron Nitride

This paper presents a systematic study of two and one dimensional honeycomb structure of boron nitride (BN) using first-principles plane wave method. Two-dimensional (2D) graphene like BN is a wide band gap semiconductor with ionic bonding. Phonon dispersion curves demonstrate the stability of 2D BN flakes. Quasi 1D armchair BN nanoribbon are nonmagnetic semiconductors with edge states. Upon passivation of B and N with hydrogen atoms these edge states disappear and band gap increases. Bare zigzag BN nanoribbons are metallic, but become a ferromagnetic semiconductor when their both edges are passivated with hydrogen. However, their magnetic ground state, electronic band structure and band gap are found to be strongly dependent on whether B- or N-edge of the ribbon is saturated with hydrogen. Vacancy defects in armchair and zigzag nanoribbons affects also magnetic state and electronic structure. In order to reveal dimensionality effects these properties are contrasted with those of various 3D BN crystals and 1D BN atomic chain.

cond-mat.mes-hall↗

arXiv2008

Monitoring of band gap and magnetic state of graphene nanoribbons through vacancies

Using first-principles plane wave calculations we predict that electronic and magnetic properties of graphene nanoribbons can be affected by defect-induced itinerant states. The band gaps of armchair nanoribbons can be modified by hydrogen saturated holes. Defects due to periodically repeating vacancy or divacancies induce metallization, as well as magnetization in non-magnetic semiconducting nanoribbons due to the spin-polarization of local defect states. Antiferromagnetic ground state of semiconducting zigzag ribbons can change to ferrimagnetic state upon creation of vacancy defects, which reconstruct and interact with edge states. Even more remarkable is that all these effects of vacancy defects are found to depend on their geometry and position relative to edges. It is shown that these effects can, in fact, be realized without really creating defects.

cond-mat.mes-hall↗

arXiv2007

Nonextensive Statistical Mechanics Application to Vibrational Dynamics of Protein Folding

The vibrational dynamics of protein folding is analyzed in the framework of Tsallis thermostatistics. The generalized partition functions, internal energies, free energies and temperature factor (or Debye-Waller factor) are calculated. It has also been observed that the temperature factor is dependent on the non-extensive parameter q which behaves like a scale parameter in the harmonic oscillator model. As $q\to 1$, we also show that these approximations agree with the result of Gaussian network model.

cond-mat.stat-mech↗

arXiv2007

Infrared Spectrum and STM images of Cyclohexene-2-Ethanamine: First Principle Investigation

We have investigated the structure of cyclohexene-2-ethanamine molecule both theoretically and experimantally. Theoretical investigation is based on a first principle technique Density Functional Theory (DFT) using plane wave basis sets and ultrasoft pseudo-potentials while the experimental technique is infrared (IR) spectroscopy. Exchange-correlation potential of DFT was approximated in the frame of both local density approximation (LDA) and generalized gradient approximation (GGA) schemes. Vibrational properties of this molecule are given by the assignments in the range for wavenumber 4000-400 $cm^{-1}$. Stable equilibrium structure of the molecule was also obtained by using LDA and GGA. Obtained optimized geometrical structure was used to calculate vibrational properties and STM images. A remarkable agreement was obtained between theory and experiment, especially in the symmetric and asymmetric vibrations of NH groups.

cond-mat.mtrl-sci↗

arXiv2007

Time Dependent Entropy of Constant Force Motion

Time dependent entropy of constant force motion is investigated. Their joint entropy so called Leipnik's entropy is obtained. The main purpose of this work is to calculate Leipnik's entropy by using time dependent wave function which is obtained by the Feynman path integral method. It is found that, in this case, the Leipnik's entropy increase with time and this result has same behavior free particle case.

quant-ph↗

arXiv2007

Joint Entropy of the Harmonic Oscillator with Time Dependent Mass and Frequency

Time dependent entropy of harmonic oscillator with time dependent mass and frequency are investigated. The joint entropy so called Leipnik's entropy is calculated by using time dependent wave function obtained by the Feynman path integral method. It is shown that, Leipnik's entropy fluctuates with time. However in constant mass and time dependent frequency case, entropy increases monotonically with time.

quant-ph↗

arXiv2007

Time dependence of joint entropy of oscillating quantum systems

The time dependent entropy (or Leipnik's entropy) of harmonic and damped harmonic oscillators is extensively investigated by using time dependent wave function obtained by the Feynman path integral method. Our results for simple harmonic oscillator are in agrement with the literature. However, the joint entropy of damped harmonic oscillator shows remarkable discontinuity with time for certain values of damping factor. According to the results, the envelop of the joint entropy curve increases with time monotonically. This results is the general properties of the envelop of the joint entropy curve for quantum systems.

quant-ph↗

arXiv2007

The structure of the free energy surface of coarse-grained off-lattice protein models

We have performed multicanonical simulations of hydrophobic-hydrophilic heteropolymers with a simple effective, coarse-grained off-lattice model to study the structure and the topology of the energy surface. The multicanonical method samples the whole rugged energy landscape, in particular the low-energy part, and enables one to better understand the critical behaviors and visualize the folding pathways of the considered protein model.

cond-mat.soft↗

arXiv2007

Solvation Effects on Free Energy Surface of Polyalanine

We have simulated 10-residue polyalanine chain by multicanonical method to visualize the 3D topographic picture of the free energy landscape over the whole range of temperatures, hence to show the funnel along the folding pathway exhaustively. We have simulated and compared the system in vacuo and in solvent, and examined the changes in the free energy landscape due to the solvent effects, which are taken into account by commonly used model Accessible Surface Area.

cond-mat.soft↗

arXiv2007

Is Sharma-Mittal entropy really a step beyond Tsallis and Renyi entropies?

We studied the Sharma-Mittal relative entropy and showed that its physical meaning is the free energy difference between the off-equilibrium and equilibrium distributions. Unfortunately, Sharma-Mittal relative entropy may acquire this physical interpretation only in the limiting case when both parameters approach to 1 in which case it approaches Kullback-Leibler entropy. We also note that this is exactly how Rényi relative entropy behaves in the thermostatistical framework thereby suggesting that Sharma-Mittal entropy must be thought to be a step beyond not both Tsallis and Rényi entropies but rather only as a generalization of Rényi entropy from a thermostatistical point of view. Lastly, we note that neither of them conforms to the Shore-Johnson theorem which is satisfied by Kullback-Leibler entropy and one of the Tsallis relative entropies.

cond-mat.stat-mech↗