Results 171 to 180 of about 293,756 (338)
Fast‐Responding O2 Gas Sensor Based on Luminescent Europium Metal‐Organic Frameworks (MOF‐76)
Luminescent MOF‐76 materials based on Eu(III) and mixed Eu(III)/Y(III) show rapid and reversible changes in emission intensity in response to O2 with very short response times. The effect is based on triplet quenching of the linker ligands that act as photosensitizers. Average emission lifetimes of a few milliseconds turn out to be mostly unaffected by
Zhenyu Zhao +5 more
wiley +1 more source
Existence of solutions for elliptic systems with critical Sobolev exponent
We establish conditions for existence and for nonexistence of nontrivial solutions to an elliptic system of partial differential equations. This system is of gradient type and has a nonlinearity with critical growth.
Pablo Amster +2 more
doaj
Computing norms and critical exponents of some operators in $L^{p}$-spaces [PDF]
T. Figiel +2 more
openalex +1 more source
A complementary charge‐trap memristor (CoCTM) featuring a unique current transient with tunable overshoot‐relaxation dynamics is introduced for high‐resolution reservoir computing. By leveraging higher‐order temporal dynamics from engineered trapping layers, the device generates multiple output states from a single input, forming rich, high‐dimensional
Alba Martinez +9 more
wiley +1 more source
Critical Dynamics under Quenched Random Magnetic Fields. II: -- = 6-d Expansion of the Dynamic Critical Exponent -- [PDF]
Fumihiko Tanaka
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Steep‐Switching Memory FET for Noise‐Resistant Reservoir Computing System
We demonstrate the steep‐switching memory FET with CuInP2S6/h‐BN/α‐In2Se3 heterostructure for application in noise‐resistant reservoir computing systems. The proposed device achieves steep switching characteristics (SSPGM = 19 mV/dec and SSERS = 23 mV/dec) through stabilization between CuInP2S6 and h‐BN.
Seongkweon Kang +6 more
wiley +1 more source
Critical exponent for a damped wave system with fractional integral
We shall present the critical exponent $$ F(p, q,\alpha):=\max\big\{\alpha+\frac{(\alpha+1)(p+1)}{pq-1}, \alpha+\frac{(\alpha+1)(q+1)}{pq-1}\big\}-\frac{1}{2} $$ for the Cauchy problem $$\displaylines{ u_{tt}-u_{xx}+u_t=J_{0|t}^{\alpha}(|v|^{p}),
Mijing Wu, Shengjia Li, Liqing Lu
doaj
Critical exponents of small one-dimensional ising magnetic [PDF]
D. V. Spirin, V. N. Udodov
openalex +1 more source
On singular elliptic equation with singular nonlinearities, Hardy-Sobolev critical exponent and weights [PDF]
Mohammed El Mokhtar Ould El Mokhtar +1 more
openalex +1 more source

