1,551 results match your criteria: "and ‡Center for Nanophase Materials Sciences[Affiliation]"
bioRxiv
November 2024
Biosciences Division, Oak Ridge National Laboratory, Oak Ridge, TN, USA 37830.
Nat Commun
November 2024
Department of Mechanical Engineering, University of Michigan, Ann Arbor, MI, USA.
Lithium solid-state batteries offer improved safety and energy density. However, the limited stability of solid electrolytes (SEs), as well as irreversible structural and chemical changes in the cathode active material, can result in inferior electrochemical performance, particularly during high-voltage cycling (>4.3 V vs Li/Li).
View Article and Find Full Text PDFNat Commun
November 2024
Department of Applied Physics, The Hong Kong Polytechnic University, Hung Hom, Kowloon, Hong Kong, China.
Chiral organic-inorganic hybrid perovskites offer a promising platform for developing non-linear chiro-optical applications and chiral-induced spin selectivity. Here, we show that achiral hybrid perovskites that have highly ordered ferroelectric domains with orthogonal polarization exhibit planar chirality, as manifested by second harmonic generation with strong circular dichroism. Interestingly, the handedness of the second harmonic generation circular dichroism response can be alternatingly switched between orthogonally polarized domains and domain walls.
View Article and Find Full Text PDFAdv Sci (Weinh)
January 2025
Chemical Sciences Division, Oak Ridge National Laboratory, Oak Ridge, TN, 37831, USA.
Inorganic fillers play an important role in improving the ionic conductivity of solid composite electrolytes (SCEs) for Li-ion batteries. Among inorganic fillers, perovskite-type lithium lanthanum titanate (LLTO) stands out for its high bulk Li conductivity on the order of 10 S cm at room temperature. According to a literature survey, the optimal LLTO filler should possess the following characteristics: i) a single-crystal structure to minimize grain boundaries; ii) a small particle size to increase the filler/polymer interface area; iii) a 1D morphology for efficient interface channels; and iv) cubic symmetry to facilitate rapid bulk Li diffusion within the filler.
View Article and Find Full Text PDFNat Commun
November 2024
Honda Research Institute USA, Inc., San Jose, CA, 95134, USA.
Nanoribbons (NRs) of atomic layer transition metal dichalcogenides (TMDs) can boost the rapidly emerging field of quantum materials owing to their width-dependent phases and electronic properties. However, the controllable downscaling of width by direct growth and the underlying mechanism remain elusive. Here, we demonstrate the vapor-liquid-solid growth of single crystal of single layer NRs of a series of TMDs (MeX: Me = Mo, W; X = S, Se) under chalcogen vapor atmosphere, seeded by pre-deposited and respective transition metal-alloyed nanoparticles that also control the NR width.
View Article and Find Full Text PDFJ Chem Theory Comput
December 2024
Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United States.
We develop off-lattice simulations of semiflexible polymer chains subjected to applied mechanical forces by using Markov Chain Monte Carlo. Our approach models the polymer as a chain of fixed length bonds, with configurations updated through adaptive nonlocal Monte Carlo moves. This proposed method enables precise calculation of a polymer's response to a wide range of mechanical forces, which traditional on-lattice models cannot achieve.
View Article and Find Full Text PDFMacromolecules
November 2024
School of Polymer Science and Engineering, Center for Optoelectronic Materials and Devices, The University of Southern Mississippi, Hattiesburg, Mississippi 39406, United States.
The conjugated polymer's backbone conformation dictates the delocalization of electrons, ultimately affecting its optoelectronic properties. Most conjugated polymers can be viewed as semirigid rods with their backbone embedded among long alkyl side chains. Thus, it is challenging to experimentally quantify the conformation of a conjugated backbone.
View Article and Find Full Text PDFACS Appl Mater Interfaces
November 2024
Chemical Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37830, United States.
Magnesium oxide (MgO) is a promising sorbent for direct air capture (DAC) of carbon dioxide. Iron (Fe) is a common impurity in naturally occurring MgO and minerals used to produce MgO, yet a molecular-scale understanding of Fe-doping effects on carbonation is lacking. Here, we observed reduced carbonation performance in Fe-doped MgO experimentally.
View Article and Find Full Text PDFAdv Mater
December 2024
Department of Chemical Engineering and SUNCAT Center for Interface Science and Catalysis, Stanford University, 443 via Ortega, Stanford, CA, 94305, USA.
Encapsulation of metal nanoparticles within oxide materials has been shown as an effective strategy to improve activity, selectivity, and stability in several catalytic applications. Several approaches have been proposed to encapsulate nanoparticles, such as forming core-shell structures, growing ordered structures (zeolites or metal-organic frameworks) on nanoparticles, or directly depositing support materials on nanoparticles. Here, a general nanocasting method is demonstrated that can produce diverse encapsulated metal@oxide structures with different compositions (Pt, Pd, Rh) and multiple types of oxides (AlO, AlO-CeO, ZrO, ZnZrO, InO, MnO, TiO) while controlling the size and dispersion of nanoparticles and the porous structure of the oxide.
View Article and Find Full Text PDFJ Am Chem Soc
November 2024
Department of Chemical Engineering, Stanford University, Stanford, California 94305, United States.
Int J Biol Macromol
December 2024
College of Food Science and Technology, Huazhong Agricultural University, Wuhan 430070, China. Electronic address:
Nat Commun
October 2024
Department of Mechanical and Aerospace Engineering, University of Virginia, Charlottesville, VA, 22904, USA.
Nanotechnology
October 2024
School of Physical Sciences, University of Arkansas at Little Rock, 2801 South University Avenue, Little Rock, AR 72204, United States of America.
Adv Mater
January 2025
Materials, Chemistry, and Computational Sciences Directorate, National Renewable Energy Laboratory, Golden, CO, 80401, USA.
Faraday Discuss
October 2024
Department of Physics and Astronomy, University of California, Irvine, 92697, California, USA.
Proc Natl Acad Sci U S A
October 2024
M. N. Miheev Institute of Metal Physics of Ural Branch of Russian Academy of Sciences, Ekaterinburg 620990, Russia.
Adv Mater
November 2024
Department of Materials Science and Engineering, University of California, Los Angeles, CA, 90095, USA.
Nat Commun
October 2024
Chemical Sciences Division, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
Nano Lett
October 2024
Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United States.
Nat Nanotechnol
January 2025
Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
Small Methods
January 2025
Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, 37831, USA.
J Chem Phys
September 2024
Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
ACS Nano
September 2024
Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37830, United States.
Proc Natl Acad Sci U S A
September 2024
University of Tennessee/Oak Ridge National Laboratory Center for Molecular Biophysics, Oak Ridge National Laboratory, Oak Ridge, TN 37831.
Microsc Microanal
September 2024
Institute of Materials Engineering, University of Kassel, Moenchebergstr.3, Kassel 34125, Germany.