A note on comonotonicity and positivity of the control components of decoupled quadratic FBSDE

In this small note we are concerned with the solution of Forward-Backward Stochastic Differential Equations (FBSDE) with drivers that grow quadratically in the control component (quadratic growth FBSDE or qgFBSDE). The main theorem is a comparison result that allows comparing componentwise the signs of the control processes of two different qgFBSDE. As a byproduct one obtains conditions that allow establishing the positivity of the control process.Comment: accepted for publicatio

Event-shape engineering for inclusive spectra and elliptic flow in Pb-Pb collisions at root(NN)-N-S=2.76 TeV

Peer reviewe

The Directional Correlation Of Successive Gamma-rays From Tin-116 And Germanium-72.

PhDNuclear physicsUniversity of Michigan, Horace H. Rackham School of Graduate Studieshttp://deepblue.lib.umich.edu/bitstream/2027.42/181573/2/0012641.pd

Strategic R&D Programme on Technologies for Future Experiments - Annual Report 2024

This report summarises the activities of the CERN/EP strategic R&D programme on technologies for future experiments during the year 2024

Annual Report 2023 and Phase-I Closeout

This report summarises the activities of the CERN strategic R&D programme on technologies for future experiments during the year 2023, and highlights the achievements of the programme during its first phase 2020-2023

Energy dependence of forward-rapidity J/ψ and ψ(2S) production in pp collisions at the LHC

We present results on transverse momentum (pT) and rapidity (y) differential production cross sections, mean transverse momentum and mean transverse momentum square of inclusive J/ψ and ψ(2S) at forward rapidity (2.5 15 GeV/c the non-prompt contribution reaches up to 50% of the total charmonium yield

Production of Σ(1385)±\Sigma(1385)^{\pm} and Ξ(1530)0\Xi(1530)^{0} in p-Pb collisions at sNN=5.02\sqrt{s_{\rm NN}}=5.02 TeV

The transverse momentum distributions of the strange and double-strange hyperon resonances ( $\Sigma (1385)^{\pm }$ , $\Xi (1530)^{0}$ ) produced in p–Pb collisions at $\sqrt{s_{\mathrm{NN}}}= 5.02$ TeV were measured in the rapidity range $-0.5< y_\mathrm {CMS}<0$ for event classes corresponding to different charged-particle multiplicity densities, $\langle$ d $N_{\mathrm{ch}}$ /d $\eta _{\mathrm{lab}}\rangle$ . The mean transverse momentum values are presented as a function of $\langle$ d $N_{\mathrm{ch}}$ /d $\eta _{\mathrm{lab}}\rangle$ , as well as a function of the particle masses and compared with previous results on hyperon production. The integrated yield ratios of excited to ground-state hyperons are constant as a function of $\langle$ d $N_{\mathrm{ch}}$ /d $\eta _{\mathrm{lab}}\rangle$ . The equivalent ratios to pions exhibit an increase with $\langle$ d $N_{\mathrm{ch}}$ /d $\eta _{\mathrm{lab}}\rangle$ , depending on their strangeness content