Results 191 to 200 of about 681,896 (307)
Residential energy expenditures in Germany: intertemporal evolution and determinants
Katrin Rehdanz, Carsten Schröder
openalex +1 more source
Energy expenditure in the control of biochemical systems by covalent modification.
Albert Goldbeter, Daniel E. Koshland
openalex +1 more source
Theory‐Guided Design of Non‐Precious Single‐Atom Catalyst for Electrocatalytic Chlorine Evolution
To overcome the reliance on noble metals for the chlorine evolution reaction (CER), we designed a non‐precious single‐atom catalyst (SAC), NiN3O–O. It achieves a low overpotential of 75 mV, 95.8% Cl2 selectivity, and outperforms commercial dimensionally stable anodes (DSAs).
Kai Ma +9 more
wiley +1 more source
Differences in Total Daily Energy Expenditure Across Field Sports: A Narrative Review. [PDF]
Skalitzky B +4 more
europepmc +1 more source
A Re-evaluation of Energy Expenditure During Parenteral Nutrition
Edward J. Quebbeman +2 more
openalex +2 more sources
Permanent magnets derive their extraordinary strength from deep, universal electronic‐structure principles that control magnetization, anisotropy, and intrinsic performance. This work uncovers those governing rules, examines modern modeling and AI‐driven discovery methods, identifies critical bottlenecks, and reveals electronic fingerprints shared ...
Prashant Singh
wiley +1 more source
Mapping Nanoscale Buckling in Atomically Thin Cr2Ge2Te6
Atomic‐resolution STEM is used to resolve nanoscale buckling in monolayer Cr2Ge2Te₆. A noise‐robust image analysis reconstructs three‐dimensional lattice distortions from single plan‐view images, revealing pronounced defect‐driven nm‐scale out‐of‐plane buckling.
Amy Carl +20 more
wiley +1 more source
One-set resistance training elevates energy expenditure for 72 h similar to three sets
Timothy D. Heden +4 more
openalex +2 more sources
Human Resting Energy Expenditure Varies with Circadian Phase [PDF]
Kirsi‐Marja Zitting +9 more
openalex +1 more source
AgCrP2S6 reveals a momentum‐indirect band edge (≈1.35 eV) and chain‐locked linear dichroism: the first direct transitions emerge at 1.6–1.8 eV for E||a. Resonant Raman and photoemission corroborate this assignment. In ACPS/graphene heterostructures, photocurrent turns on above ≈1.5 eV and follows the same polarization selection rules (anisotropy ≈0.53),
Oleksandr Volochanskyi +9 more
wiley +1 more source

