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Structure, stoichiometry, and charge transfer in cocrystals of perylene with TCNQ-F<sub>x</sub>

Semiconductor charge transfer (CT) cocrystals are an emerging class of molecular materials which combines the characteristics of the constituent molecules in order to tune physical properties. Cocrystals can exhibit...

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Structure, stoichiometry, and charge transfer in cocrystals of perylene with TCNQ-F<sub>x</sub>

Semiconductor charge transfer (CT) cocrystals are an emerging class of molecular materials which combines the characteristics of the constituent molecules in order to tune physical properties. Cocrystals can exhibit...

Published by:
Synthesis and characterization of fluorinated β-ketoiminate zinc precursors and their utility in the AP-MOCVD growth of ZnO
A novel family of zinc bis beta-ketoiminate complexes 2b-2h have been synthesized by reaction of the isolated free ligands (1a-h) with dimethylzinc. The isolated zinc complexes were characterized by elemental analysis, NMR...
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Synthesis and characterization of fluorinated β-ketoiminate zinc precursors and their utility in the AP-MOCVD growth of ZnO
A novel family of zinc bis beta-ketoiminate complexes 2b-2h have been synthesized by reaction of the isolated free ligands (1a-h) with dimethylzinc. The isolated zinc complexes were characterized by elemental analysis, NMR...
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f-scLVM
Single-cell RNA-sequencing (scRNA-seq) allows studying heterogeneity in gene expression in large cell populations. Such heterogeneity can arise due to technical or biological factors, making decomposing sources of variation...
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3D Characterisation of Dry Powder Inhaler Formulations
Carrier-based dry powder inhaler (DPI) formulations need to be accurately characterised for their particle size distributions, surface roughnesses, fines contents and flow properties. Understanding the micro-structure of the...
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Criteria for Dynamical Timescale Mass Transfer of Metal-poor Intermediate-mass Stars
Abstract The stability criteria of rapid mass transfer and common-envelope evolution are fundamental in binary star evolution. They determine the mass, mass ratio, and orbital...
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Structural diversity and electronic properties of Cu(2)SnX(3) (X = S, Se)
The ternary semiconductors Cu(2)SnX(3) (X = S, Se) are found frequently as secondary phases in synthesized Cu(2)ZnSnS(4) and Cu(2)ZnSnSe(4) samples, but previous reports on their crystal structures and electronic band gaps are...
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Structural diversity and electronic properties of Cu(2)SnX(3) (X = S, Se)
The ternary semiconductors Cu(2)SnX(3) (X = S, Se) are found frequently as secondary phases in synthesized Cu(2)ZnSnS(4) and Cu(2)ZnSnSe(4) samples, but previous reports on their crystal structures and electronic band gaps are...
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Resonant Raman scattering of ZnS<sub>x</sub>Se<sub>1-x</sub> solid solutions
A comprehensive Raman resonance scattering study of ZnSxSe1-x (ZnSSe) solid solutions over the whole compositional range (0 ≤ x ≤ 1) has been made using 325 and 455 nm excitation wavelengths. The Raman scattering intensities of...
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Nonsense-mediated decay targets have multiple sequence-related features that can inhibit translation
Nonsense-mediated mRNA decay (NMD) is a surveillance system that eliminates transcripts with premature termination codons. In this study, we show that mRNAs targeted by NMD are also suppressed at the translational level. The low...
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Resonant Raman scattering of ZnS<sub>x</sub>Se<sub>1-x</sub> solid solutions
A comprehensive Raman resonance scattering study of ZnSxSe1-x (ZnSSe) solid solutions over the whole compositional range (0 ≤ x ≤ 1) has been made using 325 and 455 nm excitation wavelengths. The Raman scattering intensities of...
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Searching for axion-like particles with X-ray polarimeters
F Day, S Krippendorf
Sep 18, 2018
X-ray telescopes are an exceptional tool for searching for new fundamental physics. In particular, X-ray observations have already placed world-leading bounds on the interaction between photons and axion-like particles (ALPs)....
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Importance of a measurement of F(L)(X,Q**2) at HERA.
Robert S Thorne
Jan 26, 2010
I investigate what a direct measurement of the longitudinal structure function FL(x,Q2) could teach us about the structure of the proton and the best way in which to use perturbative QCD for structure functions. I assume HERA...
Increase in Tau Pathology in P290S Mapt Knock-In Mice Crossed with App NL-G-F Mice.
Alzheimer's Disease (AD) is characterized by the pathologic assembly of amyloid β (Aβ) peptide, which deposits into extracellular plaques, and tau, which accumulates in intraneuronal inclusions. To investigate the link between...
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Nonsense-mediated decay targets have multiple sequence-related features that can inhibit translation
Nonsense-mediated mRNA decay (NMD) is a surveillance system that eliminates transcripts with premature termination codons. In this study, we show that mRNAs targeted by NMD are also suppressed at the translational level. The low...
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The role of F-L(x, Q(2)) in parton analyses
We investigate the effect of the structure function FL in global parton analyses of deep inelastic and related hard scattering data. We perform NLO and NNLO analyses which include the reduced cross section HERA data at high y...
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Homer F. Swift, 1920
Homer F. Swift, M.D. Trench Fever Lecture delivered January 10th, 1920
Published by: J.B. Lippincott Company
Geometric ergodicity in a weighted sobolev space
A Devraj, I Kontoyiannis, S Meyn
Jul 31, 2019
For a discrete-time Markov chain $\{X(t)\}$ evolving on $\Re^\ell$ with transition kernel $P$, natural, general conditions are developed under which the following are established: 1. The transition kernel $P$ has a purely...
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Existence, uniqueness and structure of second order absolute minimisers
Let Ω⊆Rn be a bounded open C1,1 set. In this paper we prove the existence of a unique second order absolute minimiser u∞ of the functional
E∞(u,O):=∥F(⋅,Δu)∥L∞(O),O⊆Ωmeasurable,
with prescribed boundary conditions for u...
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Existence, uniqueness and structure of second order absolute minimisers
Let Ω⊆Rn be a bounded open C1,1 set. In this paper we prove the existence of a unique second order absolute minimiser u∞ of the functional
E∞(u,O):=∥F(⋅,Δu)∥L∞(O),O⊆Ωmeasurable,
with prescribed boundary conditions for u...
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