1. [PDF] Length orthospectrum of convex bodies on flat tori - Matthieu Léautaud
19 jul 2022 · In analogy with the study of Pollicott-Ruelle resonances on nega- tively curved manifolds, we define anisotropic Sobolev spaces that.
2. Tori Matthieu - KenTamplinVocalAcademy.com
Bevat niet: measurements | Resultaten tonen met:measurements
“Ken Tamplin has done more for my voice than I could have ever imagined. He has transformed my pitch, range, style power and tone. I can’t say enough good things about Ken Tamplin Vocal Academy.”
3. [PDF] stabilization of the wave equation on larger-dimension tori with rough ...
Abstract. This paper deals with uniform stabilization of the damped wave equation. When the manifold is compact and the damping is continuous, the geometric ...
4. ISMIR 2023
Homepage of the International Society for Music Information Retrieval.
Homepage of the International Society for Music Information Retrieval
5. [PDF] Length orthospectrum and the correlation function on flat tori
Length orthospectrum and the correlation function on flat tori. Nguyen Viet Dang. Matthieu Léautaud. Gabriel Rivi`ere. Abstract. This note presents some of the ...
6. REPORT on job creation – the just transition and impact investments
6 nov 2023 · ... and impact investments (2022/2170(INI)) Committee on Employment and Social Affairs Rapporteur: Sara Matthieu.
REPORT on job creation - the just transition and impact investments (2022/2170(INI)) Committee on Employment and Social Affairs Rapporteur: Sara Matthieu
7. Mathieu Willard, Author at Agricultural and Rural Convention - ARC2020
After five years of studying agronomy, it was time for Mathieu to get on his bike and discover the idyllic landscapes of rural France and Spain.
Mathieu Willard
8. Andrey Karchevsky - Google Scholar
Coautori ; Estimation of stresses and deformation properties of rock masses which is based on the solution of an inverse problem from the measurement data of the ...
Sobolev Institute of Mathematics SB RAS - 1.205 citazioni - numerical methods for ill-posed and inverse problems
9. Matthieu Léautaud
Indiana Univ. Math. J., to appear. Length orthospectrum of convex bodies on flat tori (with Nguyen Viet Dang and Gabriel Rivière)
10. Measurements of the branching fractions of $\Lambda_{c}^{+} ... - HAL
... Matthieu Marinangeli , Pietro Marino , Jörg Marks , Giuseppe Martellotti ... Toriello , Rafael Tourinho Jadallah Aoude , Edwige Tournefier (4) , Murdo ...
The ratios of the branching fractions of the decays Λ$_{c}^{+}$ → pπ$^{−}$π$^{+}$, Λ$_{c}^{+}$ → pK$^{−}$K$^{+}$, and Λ$_{c}^{+}$ → pπ$^{−}$K$^{+}$ with respect to the Cabibbo-favoured Λ$_{c}^{+}$ → pK$^{−}$π$^{+}$ decay are measured using proton-proton collision data collected with the LHCb experiment at a 7 TeV centre-of-mass energy and corresponding to an integrated luminosity of 1.0 fb$^{−1}$: $ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{\pi}^{+}\right)}{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right)}=\left(7.44\pm 0.08\pm 0.18\right)\%,\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{K}^{+}\right)}{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right)}=\left(1.70\pm 0.03\pm 0.03\right)\%\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{K}^{+}\right)}{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right)}=\left(0.165\pm 0.015\pm 0.005\right)\%,\hfill \end{array} $ where the uncertainties are statistical and systematic, respectively. These results are the most precise measurements of these quantities to date. When multiplied by the world-average value for $ \mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right) $ , the corresponding branching fractions are $ \begin{array}{l}\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{\pi}^{+}\right)=\left(4.72\pm 0.05\pm 0.11\pm 0.25\right)\times {10}...
11. CaliFormer: Leveraging Unlabeled Measurements to Calibrate Sensors ...
8 okt 2023 · Matthieu Puigt, Farouk Yahaya, Gilles Delmaire, Gilles Roussel, 2021. ... Author Picture Monica Tentori. (CICESE, Mexico). ,; Author Picture ...
research-article
12. Smooth stabilizers for measures on the torus
Matthieu Porte. Linear response for Dirac ... Katok, Measure rigidity beyond uniform hyperbolicity: Invariant measures for Cartan actions on tori, J.
For a dissipative Anosov diffeomorphism $f$ of the 2-torus, we give examples of $f$-invariant measures $\mu$ such that the group of $\mu$-preserving diffeomorphisms is virtually cyclic.
13. Katalea - Facebook
- In low speed (Punching : 1500-time/min.) 1,300/min. Square drive dimension (mm) 12.7 mm ... Tori Matthieu ... · · · Igor Bačík▻Katalea. 5 Απρ 2024.
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14. Updated branching fraction measurements of $B^0_{(s)} \to K_ ...
7 jul 2017 · ) ; Kecke, Matthieu (Heidelberg U.) ; Kelsey, Matthew (Syracuse U ... ) ; Toriello, Francis (Syracuse U.) ; Tourinho Jadallah Aoude ...
The charmless three-body decays B$_{(s}_{)}^{0}$ → K$_{S}^{0}$ h$^{+}$ h$^{′ −}$ (where h$^{(′)}$ = π, K) are analysed using a sample of pp collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 3 fb$^{−1}$. The branching fractions are measured relative to that of the B$^{0}$ → K$_{S}^{0}$ π$^{+}$ π$^{−}$ decay, and are determined to be: $ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{\pi}^{-}\right)}=0.123\pm 0.009\left(\mathrm{stat}\right)\pm 0.015\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.549\pm 0.018\left(\mathrm{stat}\right)\pm 0.033\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.191\pm 0.027\left(\mathrm{stat}\right)\pm 0.031\left(\mathrm{syst}\right)\pm 0.011\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=1.70\pm 0.07\left(\mathrm{stat}\right)\pm 0.11\left(\mathrm{syst}\right)\pm 0.10\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathca...
15. Library - cooperation works - Interact
Interact is an EU programme, funded by ERDF, focused on service delivery to support cooperation programmes (Interreg, Interreg IPA-CBC and ENI CBC).
16. Data Archive - SEPM
... Measurements. March 2015, no. 3,. Chemical fingerprinting, a precise and ... Matthieu J.B. Cartigny, Joris T. Eggenhuisen, Ernst W.M. Hansen, and George ...
Click on the journal year to access the 2018 Supplemental Data or search by year, title, author below to access data by volume and issue of publication. If any materials are not listed, please contact the editorial office (jsedres@gmail.com) and we will be happy to send them.
17. [PDF] Programme des Journées de Dynamique
(Joint work with Matthieu Astorg and Anna Miriam Benini). Jeudi 29 ... kered tori in a sea of maximal ones. The work is still in progress, and some ...
18. Relations - Measurements of delays of gas-phase compounds in a wide ...
28 jun 2019 · Machesky, Tori Hass-Mitchell, Cong Cao, Junqi Wang, Francesca ... Matthieu Riva, Pekka Rantala, Jordan E. Krechmer, Otso Peräkylä ...
Abstract. Losses of gas-phase compounds or delays on their transfer through tubing are important for atmospheric measurements and also provide a method to characterize and quantify gas–surface interactions. Here we expand recent results by comparing different types of Teflon and other polymer tubing, as well as glass, uncoated and coated stainless steel and aluminum, and other tubing materials by measuring the response to step increases and decreases in organic compound concentrations. All polymeric tubings showed absorptive partitioning behavior with no dependence on humidity or concentration, with PFA Teflon tubing performing best in our tests. Glass and uncoated and coated metal tubing showed very different phenomenology due to adsorptive partitioning to a finite number of surface sites. Strong dependencies on compound concentration, mixture composition, functional groups, humidity, and memory effects were observed for glass and uncoated and coated metals, which (except for Silonite-coated stainless steel) also always caused longer delays than Teflon for the compounds and concentrations tested. Delays for glass and uncoated and coated metal tubing were exacerbated at low relative humidity but reduced for RH >20 %. We find that conductive PFA and Silonite tubing perform best among the materials tested for gas-plus-particle sampling lines, combining reduced gas-phase delays with good particle transmission.
19. Wigner measures and observability for the Schrödinger equation on the disk
3 jun 2014 · They are obtained by performing a finer localization in phase space around each of these tori ... From: Matthieu Léautaud [view email] [v1] ...
We analyse the structure of semiclassical and microlocal Wigner measures for solutions to the linear Schrödinger equation on the disk, with Dirichlet boundary conditions. Our approach links the propagation of singularities beyond geometric optics with the completely integrable nature of the billiard in the disk. We prove a "structure theorem", expressing the restriction of the Wigner measures on each invariant torus in terms of {\em second-microlocal measures}. They are obtained by performing a finer localization in phase space around each of these tori, at the limit of the uncertainty principle, and are shown to propagate according to Heisenberg equations on the circle. Our construction yields as corollaries (a) that the disintegration of the Wigner measures is absolutely continuous in the angular variable, which is an expression of the dispersive properties of the equation; (b) an observability inequality, saying that the $L^2$-norm of a solution on any open subset intersecting the boundary (resp. the $L^2$-norm of the Neumann trace on any nonempty open set of the boundary) controls its full $L^2$-norm (resp. $H^1$-norm). These results show in particular that the energy of solutions cannot concentrate on periodic trajectories of the billiard flow other than the boundary.
