76 research outputs found
A Free Energy Model of Boron Carbide
The assessed phase diagram of the boron-carbon system contains a single
non-stoichiometric boron-carbide phase of rhombohedral symmetry with a broad,
thermodynamically improbable, low temperature composition range. We combine
first principles total energy calculations with phenomenological thermodynamic
modeling to propose a revised low temperature phase diagram that contains two
boron-carbide phases of differing symmetries and compositions. One structure
has composition B4C and consists of B11C icosahedra and C-B-C chains, with the
placement of carbon on the icosahedron breaking rhombohedral symmetry. This
phase is destabilized above 600K by the configurational entropy of alternate
carbon substitutions. The other structure, of ideal composition B13C2, has a
broad composition range at high temperature, with rhombohedral symmetry
throughout, as observed experimentally.Comment: 15 pages, 3 figures, submitted to J. Stat. Phys. August 9th, 201
ELSI: A Unified Software Interface for Kohn-Sham Electronic Structure Solvers
Solving the electronic structure from a generalized or standard eigenproblem
is often the bottleneck in large scale calculations based on Kohn-Sham
density-functional theory. This problem must be addressed by essentially all
current electronic structure codes, based on similar matrix expressions, and by
high-performance computation. We here present a unified software interface,
ELSI, to access different strategies that address the Kohn-Sham eigenvalue
problem. Currently supported algorithms include the dense generalized
eigensolver library ELPA, the orbital minimization method implemented in
libOMM, and the pole expansion and selected inversion (PEXSI) approach with
lower computational complexity for semilocal density functionals. The ELSI
interface aims to simplify the implementation and optimal use of the different
strategies, by offering (a) a unified software framework designed for the
electronic structure solvers in Kohn-Sham density-functional theory; (b)
reasonable default parameters for a chosen solver; (c) automatic conversion
between input and internal working matrix formats, and in the future (d)
recommendation of the optimal solver depending on the specific problem.
Comparative benchmarks are shown for system sizes up to 11,520 atoms (172,800
basis functions) on distributed memory supercomputing architectures.Comment: 55 pages, 14 figures, 2 table
ELSI -- An open infrastructure for electronic structure solvers
Routine applications of electronic structure theory to molecules and periodic systems need to compute the electron density from given Hamiltonian and, in case of non-orthogonal basis sets, overlap matrices. System sizes can range from few to thousands or, in some examples, millions of atoms. Different discretization schemes (basis sets) and different system geometries (finite non-periodic vs. infinite periodic boundary conditions) yield matrices with different structures. The ELectronic Structure Infrastructure (ELSI) project provides an open-source software interface to facilitate the implementation and optimal use of high-performance solver libraries covering cubic scaling eigensolvers, linear scaling density-matrix-based algorithms, and other reduced scaling methods in between. In this paper, we present recent improvements and developments inside ELSI, mainly covering (1) new solvers connected to the interface, (2) matrix layout and communication adapted for parallel calculations of periodic and/or spin-polarized systems, (3) routines for density matrix extrapolation in geometry optimization and molecular dynamics calculations, and (4) general utilities such as parallel matrix I/O and JSON output. The ELSI interface has been integrated into four electronic structure code projects (DFTB+, DGDFT, FHI-aims, SIESTA), allowing us to rigorously benchmark the performance of the solvers on an equal footing. Based on results of a systematic set of large-scale benchmarks performed with KohnâSham density-functional theory and density-functional tight-binding theory, we identify factors that strongly affect the efficiency of the solvers, and propose a decision layer that assists with the solver selection process. Finally, we describe a reverse communication interface encoding matrix-free iterative solver strategies that are amenable, e.g., for use with planewave basis sets. Program summary: Program title: ELSI Interface CPC Library link to program files: http://dx.doi.org/10.17632/473mbbznrs.1 Licensing provisions: BSD 3-clause Programming language: Fortran 2003, with interface to C/C++ External routines/libraries: BLACS, BLAS, BSEPACK (optional), EigenExa (optional), ELPA, FortJSON, LAPACK, libOMM, MPI, MAGMA (optional), MUMPS (optional), NTPoly, ParMETIS (optional), PETSc (optional), PEXSI, PT-SCOTCH (optional), ScaLAPACK, SLEPc (optional), SuperLU_DIST Nature of problem: Solving the electronic structure from given Hamiltonian and overlap matrices in electronic structure calculations. Solution method: ELSI provides a unified software interface to facilitate the use of various electronic structure solvers including cubic scaling dense eigensolvers, linear scaling density matrix methods, and other approaches
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Screening of healthcare workers for SARS-CoV-2 highlights the role of asymptomatic carriage in COVID-19 transmission
Funder: Addenbrooke's Charitable Trust, Cambridge University Hospitals; FundRef: http://dx.doi.org/10.13039/501100002927Significant differences exist in the availability of healthcare worker (HCW) SARS-CoV-2 testing between countries, and existing programmes focus on screening symptomatic rather than asymptomatic staff. Over a 3 week period (April 2020), 1032 asymptomatic HCWs were screened for SARS-CoV-2 in a large UK teaching hospital. Symptomatic staff and symptomatic household contacts were additionally tested. Real-time RT-PCR was used to detect viral RNA from a throat+nose self-swab. 3% of HCWs in the asymptomatic screening group tested positive for SARS-CoV-2. 17/30 (57%) were truly asymptomatic/pauci-symptomatic. 12/30 (40%) had experienced symptoms compatible with coronavirus disease 2019 (COVID-19)>7 days prior to testing, most self-isolating, returning well. Clusters of HCW infection were discovered on two independent wards. Viral genome sequencing showed that the majority of HCWs had the dominant lineage Bâ1. Our data demonstrates the utility of comprehensive screening of HCWs with minimal or no symptoms. This approach will be critical for protecting patients and hospital staff
SARS-CoV-2 B.1.617.2 Delta variant replication and immune evasion
Abstract: The B.1.617.2 (Delta) variant of severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2) was first identified in the state of Maharashtra in late 2020 and spread throughout India, outcompeting pre-existing lineages including B.1.617.1 (Kappa) and B.1.1.7 (Alpha)1. In vitro, B.1.617.2 is sixfold less sensitive to serum neutralizing antibodies from recovered individuals, and eightfold less sensitive to vaccine-elicited antibodies, compared with wild-type Wuhan-1 bearing D614G. Serum neutralizing titres against B.1.617.2 were lower in ChAdOx1 vaccinees than in BNT162b2 vaccinees. B.1.617.2 spike pseudotyped viruses exhibited compromised sensitivity to monoclonal antibodies to the receptor-binding domain and the amino-terminal domain. B.1.617.2 demonstrated higher replication efficiency than B.1.1.7 in both airway organoid and human airway epithelial systems, associated with B.1.617.2 spike being in a predominantly cleaved state compared with B.1.1.7 spike. The B.1.617.2 spike protein was able to mediate highly efficient syncytium formation that was less sensitive to inhibition by neutralizing antibody, compared with that of wild-type spike. We also observed that B.1.617.2 had higher replication and spike-mediated entry than B.1.617.1, potentially explaining the B.1.617.2 dominance. In an analysis of more than 130 SARS-CoV-2-infected health care workers across three centres in India during a period of mixed lineage circulation, we observed reduced ChAdOx1 vaccine effectiveness against B.1.617.2 relative to non-B.1.617.2, with the caveat of possible residual confounding. Compromised vaccine efficacy against the highly fit and immune-evasive B.1.617.2 Delta variant warrants continued infection control measures in the post-vaccination era
BaCu<sub>2</sub>Sn(S,Se)<sub>4</sub>: Earth-Abundant Chalcogenides for Thin-Film Photovoltaics
Chalcogenides such
as CdTe, CuÂ(In,Ga)Â(S,Se)<sub>2</sub> (CIGSSe),
and Cu<sub>2</sub>ZnSnÂ(S,Se)<sub>4</sub> (CZTSSe) have enabled remarkable
advances in thin-film photovoltaic performance, but concerns remain
regarding (i) the toxicity (CdTe) and (ii) scarcity (CIGSSe/CdTe)
of the constituent elements and (iii) the unavoidable antisite disordering
that limits further efficiency improvement (CZTSSe). In this work,
we show that a different materials class, the BaCu<sub>2</sub>SnSe<sub><i>x</i></sub>S<sub>4â<i>x</i></sub> (BCTSSe)
system, offers a prospective path to circumvent difficulties (iâiii)
and to target new environmentally friendly and earth-abundant absorbers.
Antisite disordering and associated band tailing are discouraged in
BCTSSe due to the distinct coordination environment of the large Ba<sup>2+</sup> cation. Indeed, an abrupt absorption edge and sharp associated
photoluminescence emission demonstrate a reduced impact of band tailing
in BCTSSe relative to CZTSSe. Our combined experimental and computational
studies of BCTSSe reveal that the compositions 0 ⤠<i>x</i> ⤠4 exhibit a tunable nearly direct or direct bandgap
in the 1.6â2 eV range, spanning relevant values for single-
or multiple-junction photovoltaic applications. For the first time,
a prototype BaCu<sub>2</sub>SnS<sub>4</sub>-based thin-film solar
cell has been successfully demonstrated, yielding a power conversion
efficiency of 1.6% (0.42 cm<sup>2</sup> total area). The systematic
experimental and theoretical investigations, combined with proof-of-principle
device results, suggest promise for BaCu<sub>2</sub>SnSe<sub><i>x</i></sub>S<sub>4â<i>x</i></sub> as a thin-film
solar cell absorber
I<sub>2</sub>âIIâIVâVI<sub>4</sub> (I = Cu, Ag; II = Sr, Ba; IV = Ge, Sn; VI = S, Se): Chalcogenides for Thin-Film Photovoltaics
Recent
work has identified a non-zinc-blende-type quaternary semiconductor,
Cu<sub>2</sub>BaSnS<sub>4â<i>x</i></sub>Se<sub><i>x</i></sub> (CBTSSe), as a promising candidate for thin-film
photovoltaics (PVs). CBTSSe circumvents difficulties of competing
PV materials regarding (i) toxicity (e.g., CdTe), (ii) scarcity of
constituent elements (e.g., CuÂ(In,Ga)Â(S,Se)<sub>2</sub>/CdTe), and
(iii) unavoidable antisite disordering that limits further efficiency
improvement (e.g., in Cu<sub>2</sub>ZnSnS<sub>4â<i>x</i></sub>Se<sub><i>x</i></sub>). In this work, we build on
the CBTSSe paradigm by computationally scanning for further improved,
earth-abundant and environmentally friendly thin-film PV materials
among the 16 quaternary systems I<sub>2</sub>âIIâIVâVI<sub>4</sub> (I = Cu, Ag; II = Sr, Ba; IV = Ge, Sn; VI = S, Se). The band
structures, band gaps, and optical absorption properties are predicted
by hybrid density-functional theory calculations. We find that the
Ag-containing compounds (which belong to space groups <i>I</i>222 or <i>I</i>4Ě
2<i>m</i>) show indirect
band gaps. In contrast, the Cu-containing compounds (which belong
to space group <i>P</i>3<sub>1</sub>/<i>P</i>3<sub>2</sub> and <i>Ama</i>2) show direct or nearly direct band
gaps. In addition to the previously considered Cu<sub>2</sub>BaSnS<sub>4â<i>x</i></sub>Se<sub><i>x</i></sub> system,
two compounds not yet considered for PV applications, Cu<sub>2</sub>BaGeSe<sub>4</sub> (<i>P</i>3<sub>1</sub>) and Cu<sub>2</sub>SrSnSe<sub>4</sub> (<i>Ama</i>2), show predicted quasi-direct/direct
band gaps of 1.60 and 1.46 eV, respectively, and are therefore most
promising with respect to thin-film PV application (both single- and
multijunction). A Cu<sub>2</sub>BaGeSe<sub>4</sub> sample, prepared
by solid-state reaction, exhibits the expected <i>P</i>3<sub>1</sub> structure type. Diffuse reflectance and photoluminescence
spectrometry measurements yield an experimental band gap of 1.91(5)
eV for Cu<sub>2</sub>BaGeSe<sub>4</sub>, a value slightly smaller
than that for Cu<sub>2</sub>BaSnS<sub>4</sub>
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