2019
DOI: 10.1016/j.jnoncrysol.2019.01.021
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Structural studies on fluid sulfur at high temperatures and high pressures: II. Molecular structure obtained by ab initio molecular dynamics simulations

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Cited by 5 publications
(6 citation statements)
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“…In a system of N particles in volume V and at temperature T , the correlation function g ( r ) can be written as Equation (). [ 101,102 ] normalg(n)(r1,rn)=VnN!Nnfalse(Nnfalse)!·1ZNekTUNdrn+1drN…”
Section: Density Functional Theorymentioning
confidence: 99%
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“…In a system of N particles in volume V and at temperature T , the correlation function g ( r ) can be written as Equation (). [ 101,102 ] normalg(n)(r1,rn)=VnN!Nnfalse(Nnfalse)!·1ZNekTUNdrn+1drN…”
Section: Density Functional Theorymentioning
confidence: 99%
“…Munejiri et al [ 102 ] investigated the structure of expanded fluid sulfur by AIMD simulations. As shown in Figure a, they found that with decreasing chain length at 1323 K, the bond length at the chain end decreased, whereas the bond length at the inside of the chain increased.…”
Section: Aimd Simulationsmentioning
confidence: 99%
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“…They also carried out experiments at high temperatures and pressures up to the liquid-vapour critical point to elucidate the dynamics of the chain length evolution of sulphur. On the basis of the above experimental data [31] and XRD results [32] at high pressures and temperatures, Munejiri et al [33] carried out an ab initio molecular dynamics simulation to investigate the time evolution of the chain structure. They found differences in bond length in the chains and at the chain ends.…”
Section: Introductionmentioning
confidence: 99%
“…Density functional theory (DFT) and other theoretical approaches have been used previously to elucidate the conformational and thermodynamic properties of S 8 rings. , Ab initio molecular dynamics simulations have also been carried out to study the S 8 -ring opening at elevated temperatures and pressures, as well as upon electronic excitation. However, in these early pioneering studies, the states involved in the excited-state dynamics were prepared by simply placing an electron taken from the highest occupied molecular orbital (HOMO) into the lowest unoccupied molecular orbital (LUMO). , Thus, in spite of many previous efforts, a comprehensive description of the electronic structure and photodegradation pathways of S 8 rings, in particular with respect to the formation of triplet states, remains elusive. Here, to better characterize the nature of the excited electronic states and the possible ring-to-chain relaxation pathways upon photoexcitation, we combine time-dependent (TD)-DFT and highly correlated wave function STEOM-CCSD calculations to evaluate the ground-state and excited-state electronic and geometric structures of the S 8 molecular materials.…”
mentioning
confidence: 99%