Nanoscale size effects in α-FAPbI<sub>3</sub> evinced by large-scale ab initio simulations. [PDF]
Carnevali V +5 more
europepmc +1 more source
Phase Field Failure Modeling: Brittle‐Ductile Dual‐Phase Microstructures under Compressive Loading
The approach by Amor and the approach by Miehe and Zhang for asymmetric damage behavior in the phase field method for fracture are compared regarding their fitness for microcrack‐based failure modeling. The comparison is performed for the case of a dual‐phase microstructure with a brittle and a ductile constituent.
Jakob Huber, Jan Torgersen, Ewald Werner
wiley +1 more source
Atomistic-Based Fatigue Property Normalization Through Maximum A Posteriori Optimization in Additive Manufacturing. [PDF]
Awd M, Saeed L, Walther F.
europepmc +1 more source
Assessment of the exchange-hole dipole moment dispersion correction for the energy ranking stage of the seventh crystal structure prediction blind test. [PDF]
Mayo RA +3 more
europepmc +1 more source
A Linear-Scaling Integral-Direct Explicitly Correlated Second-Order Møller-Plesset Approach. [PDF]
Kállay M +3 more
europepmc +1 more source
Adaptive Restraints to Accelerate Geometry Optimizations of Large Biomolecular Systems. [PDF]
Hix MA, Walker AR.
europepmc +1 more source
DyeDactic workflow to predict halochromism of biosynthetic colourants. [PDF]
Karlov DS +3 more
europepmc +1 more source
Local Time, Excursions, and Additive Functionals
Semi-martingale local time, Tanaka’s formula, space-time regularity, occupation measure and density, extended Ito formula, regenerative sets and processes, excursion law, excursion local time and Poisson process, approximations of local time, inverse local time as a subordinator, Brownian excursion, Ray–Knight theorem, continuous additive functionals ...
Olav Kallenberg, Kallenberg Olav
exaly +5 more sources
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Jiang, Yiwen, Liu, Luqin
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Any continuous Brownian additive functional locally of zero energy can be represented via a convolution type transform of Brownian local time in one-dimensional case. The Fourier transform of local time plays an essential role in the proof of the representation.
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