Results 111 to 120 of about 61,413 (290)

Clinical Impact of Concordant and Discordant Physiology Parameters Post‐Percutaneous Coronary Intervention in the EASY‐PREDICT Study

open access: yesCatheterization and Cardiovascular Interventions, Volume 106, Issue 7, Page 3867-3875, December 1, 2025.
ABSTRACT Background In the EASY‐PREDICT Study, patients were randomized to angiography‐guidance or post‐percutaneous coronary intervention (PCI) physiology‐guidance. Discordance between resting and hyperemic physiology post‐PCI might have a different relationship with clinical outcomes.
Paola Ulacia Flores   +13 more
wiley   +1 more source

The boundedness and upper semicontinuity of the pullback attractors for a 2D micropolar fluid flows with delay

open access: yesElectronic Research Archive, 2020
In this paper, two properties of the pullback attractor for a 2D non-autonomous micropolar fluid flows with delay on unbounded domains are investigated. First, we establish the \begin{document}$ H^1 $\end{document} -boundedness of the pullback attractor.
Wenlong Sun
semanticscholar   +1 more source

Financialization of Commodity Markets Co‐Movement Behind‐the‐Scenes

open access: yesJournal of Futures Markets, Volume 45, Issue 12, Page 2457-2475, December 2025.
ABSTRACT In the early 2000s, institutional investors entered the commodity futures markets en masse with passive, long only, index‐type positions in sharp contrast with those typically assumed by traditional expert participants. A heated public debate soon erupted over the perceived consequences of the phenomenon—commonly referred to as ...
Devraj Basu, Olivier Bauthéac
wiley   +1 more source

Upper Semicontinuity of Pullback Attractors for the 3D Nonautonomous Benjamin-Bona-Mahony Equations

open access: yesThe Scientific World Journal, 2014
We will study the upper semicontinuity of pullback attractors for the 3D nonautonomouss Benjamin-Bona-Mahony equations with external force perturbation terms. Under some regular assumptions, we can prove the pullback attractors 𝒜ε(t) of equation ut-Δut-
Xinguang Yang   +3 more
doaj   +1 more source

Weak pullback attractors for stochastic Navier-Stokes equations with nonlinear diffusion terms

open access: yesProceedings of the American Mathematical Society, 2018
. This paper is concerned with the asymptotic behavior of the solutions of the two-dimensional stochastic Navier-Stokes equations driven by white noise with nonlinear diffusion terms.
Bixiang Wang
semanticscholar   +1 more source

Pullbacks of the Horrocks-Mumford bundle.

open access: yesJournal für die reine und angewandte Mathematik (Crelles Journal), 1987
The only known indecomposable holomorphic rank 2 vector bundle on \({\mathbb{P}}^ 4\) is the Horrocks-Mumford bundle \({\mathcal F}\) [\textit{G. Horrocks} and \textit{D. Mumford}, Topology 12, 63-81 (1973; Zbl 0255.14017)]. Of course this is not quite true, since we may twist \({\mathcal F}\) by a line bundle or may pull \({\mathcal F}\) back under a ...
Schreyer, F.-O., Decker, W.
openaire   +1 more source

Nontriviality of rings of integral‐valued polynomials

open access: yesMathematische Nachrichten, Volume 298, Issue 12, Page 3974-3994, December 2025.
Abstract Let S$S$ be a subset of Z¯$\overline{\mathbb {Z}}$, the ring of all algebraic integers. A polynomial f∈Q[X]$f \in \mathbb {Q}[X]$ is said to be integral‐valued on S$S$ if f(s)∈Z¯$f(s) \in \overline{\mathbb {Z}}$ for all s∈S$s \in S$. The set IntQ(S,Z¯)${\mathrm{Int}}_{\mathbb{Q}}(S,\bar{\mathbb{Z}})$ of all integral‐valued polynomials on S$S ...
Giulio Peruginelli, Nicholas J. Werner
wiley   +1 more source

A Comparative Study of a Backward Euler and Exponential Update for a Viscoelastic Maxwell Model Within the Material Point Method

open access: yesPAMM, Volume 25, Issue 4, December 2025.
ABSTRACT The material point method (MPM) offers a distinct simulation method compared to conventional techniques such as the finite element method (FEM). In the MPM, physical bodies are represented by a collection of material points while the governing equations are solved on an independent computational mesh. Each simulation step follows a three‐stage
Marvin Koßler   +2 more
wiley   +1 more source

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