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Dive into the research topics where M. Ghazisaeidi is active.

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Featured researches published by M. Ghazisaeidi.


Applied Physics Letters | 2008

Single impact crater functions for ion bombardment of silicon

N. Kalyanasundaram; M. Ghazisaeidi; Jonathan B. Freund; H. T. Johnson

The average effect of a single 500eV incident argon ion on a silicon surface is studied using molecular dynamics simulations. More than 103 ion impacts at random surface points are averaged for each of seven incidence angles, from 0° to 28° off normal, to determine a local surface height change function, or a crater function. The crater shapes are mostly determined by mass rearrangement; sputtering has a relatively small effect. Analytical fitting functions are provided for several cases, and may serve as input into kinetic Monte Carlo calculations or stability analyses for surfaces subjected to ion bombardment.


Nature Communications | 2018

Magnetically-driven phase transformation strengthening in high entropy alloys

Changning Niu; Carlyn R. LaRosa; Jiashi Miao; M.J. Mills; M. Ghazisaeidi

CrCoNi alloy exhibits a remarkable combination of strength and plastic deformation, even superior to the CrMnFeCoNi high-entropy alloy. We connect the magnetic and mechanical properties of CrCoNi, via a magnetically tunable phase transformation. While both alloys crystallize as single-phase face-centered-cubic (fcc) solid solutions, we find a distinctly lower-energy phase in CrCoNi alloy with a hexagonal close-packed (hcp) structure. Comparing the magnetic configurations of CrCoNi with those of other equiatomic ternary derivatives of CrMnFeCoNi confirms that magnetically frustrated Mn eliminates the fcc-hcp energy difference. This highlights the unique combination of chemistry and magnetic properties in CrCoNi, leading to a fcc-hcp phase transformation that occurs only in this alloy, and is triggered by dislocation slip and interaction with internal boundaries. This phase transformation sets CrCoNi apart from the parent quinary, and its other equiatomic ternary derivatives, and provides a new way for increasing strength without compromising plastic deformation.Medium entropy alloy CoCrNi has better mechanical properties than high entropy alloys such as CrMnFeCoNi, but why that is remains unclear. Here, the authors show that a nanostructured phase at lattice defects in CoCrNi causes its extraordinary properties, while it is magnetically frustrated and suppressed in CrMnFeCoNi.


Physical Review E | 2009

Convergence rate for numerical computation of the lattice Green's function

M. Ghazisaeidi; Dallas R. Trinkle

Flexible boundary-condition methods couple an isolated defect to bulk through the bulk lattice Greens function. Direct computation of the lattice Greens function requires projecting out the singular subspace of uniform displacements and forces for the infinite lattice. We calculate the convergence rates for elastically isotropic and anisotropic cases for three different techniques: relative displacement, elastic Greens function correction, and discontinuity correction. The discontinuity correction has the most rapid convergence for the general case.


Microscopy and Microanalysis | 2015

HAADF/MAADF Observations and Image Simulations of Dislocation Core Structures in a High Entropy Alloy

T.M. Smith; Bryan D. Esser; E.P. George; F. Otto; M. Ghazisaeidi; D.W. McComb; M.J. Mills

High entropy alloys (HEAs) are a new class of multi-component alloys in which the individual elements have similar concentrations. A single-phase solid solution HEA containing 5 elements (Co, Cr, Fe, Mn, and Ni) with equiatomic composition was first discovered by Cantor [1]. Among the surprising characteristics of this fcc HEA are: strong temperature dependence of the yield strength at temperatures around and below room temperature, relatively weak strain-rate dependence over the same temperature range [3]; very large hardening rates [2,3]; and large fracture toughness at room temperature [4]. These features are linked to deformation twinning and dislocation-mediated plasticity, yet presently there is insufficient knowledge of dislocation dissociation, stacking fault energy, or core structures in this alloy. The highly planar deformation involves dislocation arrays on active slip systems (Figure 1a and 1b). This characteristic could imply the presence of short range order, low fault energy, or supplementary displacements in the wake of glide dislocations.


Physical Review B | 2010

Lattice Green’s function for crystals containing a planar interface

M. Ghazisaeidi; Dallas R. Trinkle

Flexible boundary condition methods couple an isolated defect to a harmonically responding medium through the bulk lattice Greens function; in the case of an interface, interfacial lattice Greens functions. We present a method to compute the lattice Greens function for a planar interface with arbitrary atomic interactions suited for the study of line defect/interface interactions. The interface is coupled to two different semi-infinite bulk regions, and the Greens function for interface-interface, bulk-interface, and bulk-bulk interactions are computed individually. The elastic bicrystal Greens function and the bulk lattice Greens function give the interaction between bulk regions. We make use of partial Fourier transforms to treat in-plane periodicity. Direct inversion of the force constant matrix in the partial Fourier space provides the interface terms. The general method makes no assumptions about the atomic interactions or crystal orientations. We simulate a screw dislocation interacting with a


Microscopy and Microanalysis | 2017

STEM Characterization of the Deformation Substructure of a NiCoCr Equiatomic Solid Solution Alloy

J. Miao; C.E. Slone; T.M. Smith; C. Niu; Hongbin Bei; M. Ghazisaeidi; G.M. Pharr; M.J. Mills

(10\overline{1}2)


Microscopy and Microanalysis | 2016

Through-Focal HAADF-STEM Analysis of Dislocation Cores in a High-Entropy Alloy

T.M. Smith; Bryan D. Esser; M.S. Hooshmand; E.P. George; F. Otto; M. Ghazisaeidi; D.W. McComb; M.J. Mills

twin boundary in Ti using flexible boundary conditions and compare with traditional fixed boundary conditions results. Flexible boundary conditions give the correct core structure with significantly less atoms required to relax by energy minimization. This highlights the applicability of flexible boundary conditions methods to modeling defect/interface interactions by ab initio methods.


Journal of Applied Physics | 2008

Statistical characterization of surface defects created by Ar ion bombardment of crystalline silicon

M. Ghazisaeidi; Jonathan B. Freund; H. T. Johnson

High entropy alloys have attracted increasing research interest due to their exceptional mechanical properties such as high tensile strength, ductility, and fracture toughness [1,2]. These alloys normally consist of five or more components to achieve high configurational entropy. Recent study shows that ternary NiCoCr equiatomic solid solution alloy with “medium entropy” actually has superior properties, especially at cryogenic temperature, as compared with 5 component Cantor alloy [3,4]. Previous study shows that deformation twinning plays an important role in the deformation process of Cantor alloy [5]. However, the origin of the exceptional mechanical properties of ternary NiCoCr solid solution alloy is still unclear.


Acta Materialia | 2012

Core structure of a screw dislocation in Ti from density functional theory and classical potentials

M. Ghazisaeidi; Dallas R. Trinkle

High-entropy alloys (HEAs) are a new class of multi-component alloys that exhibit surprising characteristics, [1] including very large strain hardening rates, large fracture toughness at room temperature [2], and a strong temperature dependence of yield strength at or below room temperature. These properties are closely linked to nano-twinning and dislocation-mediated plasticity, yet little experimental work has explored dislocation dissociation, stacking fault energy, or core structures in these alloys [3]. In this study, an HEA, containing 5 elements (Cr, Co, Mn, Fe, and Ni) with equiatomic composition was deformed to a 5% plastic strain at room temperature [4]. Post-mortem 3mm disks were electro-polished using a solution consisting of 21% Perchloric acid and 79% Acetic acid and analyzed using a probe-corrected Titan 80-300kV along a [110] zone axis. Highly planar deformation was first observed by Otto et al. [5] and was active for this study as well. This planar deformation, involving dislocation arrays on {111} slip systems, may imply the existence of short-range order, low stacking fault energy (SFE), and/or supplementary displacements in the wake of dislocations.


Scripta Materialia | 2014

First-principles core structures of edge and screw dislocations in Mg

M. Ghazisaeidi; Louis G. Hector; W.A. Curtin

Ion bombardment of crystalline silicon targets induces pattern formation by the creation of mobile surface species that participate in forming nanometer-scale structures. The formation of these mobile species on a Si(001) surface, caused by sub-keV argon ion bombardment, is investigated through molecular dynamics simulation of Stillinger-Weber [Phys. Rev. B 31, 5262 (1985)] silicon. Specific criteria for identifying and classifying these mobile atoms based on their energy and coordination number are developed. The mobile species are categorized based on these criteria and their average concentrations are calculated.

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W.A. Curtin

École Polytechnique Fédérale de Lausanne

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E.P. George

Ruhr University Bochum

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F. Otto

Ruhr University Bochum

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D. Buey

Ohio State University

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