Search results for "G0"

showing 5 items of 85 documents

"Figure 5" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

2023

$R_{AA}$ vs. $p_T$ for $\phi$ for 30-40% centrality Au+Au and 0-10% centrality Cu+Cu collisions, and $R_{AA}$ vs. $p_T$ for $\phi$ and $\pi^0$ for 40-50% centrality Au+Au and 10-20% centrality Cu+Cu collisions. The global uncertainty of ~ 10% related to the $p$+$p$ reference normalization is not shown.

ppg096Cu Cu --> CHARGED XAu Au --> CHARGED Xmidrapiditytransverse momentum200.0
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"Figure 6a" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

2023

$R_{AA}$ for $\phi$ integrated at $p_T$ > 2.2 GeV/$c$ in Cu+Cu and Au+Au collisions vs. $N_{part}$. The global uncertainty related to the $p$+$p$ reference normalization is shown as a box on the right in the figure from the paper.

ppg096Cu Cu --> CHARGED XAu Au --> CHARGED Xmidrapiditytransverse momentum200.0
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"Figure 7" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

2023

$R_{dA}$ vs. $p_T$ for $\phi$, $\pi^0$, and ($p$+$\bar{p}$) for 0-20% centrality $d$+Au collisions, and $R_{dA}$ vs. $p_T$ for $\phi$, $\pi^0$, and ($p$+$\bar{p}$) for 60-88% peripheral $d$+Au collisions. The global uncertainty of ~ 10% related to the $p$+$p$ reference normalization is not shown.

ppg096midrapiditytransverse momentum200.0$d$ Au --> CHARGED X
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Jeu de Taquin and Diamond Cone for so(2n+1, C)

2020

International audience; The diamond cone is a combinatorial description for a basis of a natural indecomposable n-module, where n is the nilpotent factor of a complex semisimple Lie algebra g. After N. J. Wildberger who introduced this notion, this description was achieved for g = sl(n) , the rank 2 semisimple Lie algebras and g = sp (2n).In this work, we generalize these constructions to the Lie algebra g = so(2n + 1). The orthogonal semistandard Young tableaux were defined by M. Kashiwara and T. Nakashima, they index a basis for the shape algebra of so(2n + 1). Defining the notion of orthogonal quasistandard Young tableaux, we prove that these tableaux describe a basis for a quotient of t…

quasistandard Young tableauMathematics::Quantum AlgebraShape algebrajeu de taquinMSC: 20G05 05A15 17B10[MATH] Mathematics [math][MATH]Mathematics [math]Mathematics::Representation Theorysemistandard Young tableau
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Acoustic wave guides as infinite-dimensional dynamical systems

2015

We prove the unique solvability, passivity/conservativity and some regularity results of two mathematical models for acoustic wave propagation in curved, variable diameter tubular structures of finite length. The first of the models is the generalised Webster's model that includes dissipation and curvature of the 1D waveguide. The second model is the scattering passive, boundary controlled wave equation on 3D waveguides. The two models are treated in an unified fashion so that the results on the wave equation reduce to the corresponding results of approximating Webster's model at the limit of vanishing waveguide intersection.

regularityControl and OptimizationDynamical systems theoryWave propagationwave propagationDynamical Systems (math.DS)Curvaturelaw.inventionMathematics - Analysis of PDEslawWebster’s horn modelFOS: MathematicspassivityMathematics - Dynamical SystemsMathematicstubular domainMathematical modelta111Mathematical analysisAcoustic waveDissipationWave equationPrimary 35L05 secondary 35L20 93C20 47N70Computational MathematicsControl and Systems Engineering: Mathematics [G03] [Physical chemical mathematical & earth Sciences]wave equation: Mathématiques [G03] [Physique chimie mathématiques & sciences de la terre]WaveguideAnalysis of PDEs (math.AP)ESAIM: Control, Optimisation and Calculus of Variations
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