Ludovico Vittorio

activity

20212026

most citedThe last Complex WIMPs standing

64 citations · 158 across the 23 of their papers we have counts for

collaborators

Showing 2023Show all

4 papers · 1 filter

hep-ph2023★ 17 cited

Insights on the current semi-leptonic $B$ -decay discrepancies -- and how $B_{s} \to μ^{+} μ^{-} γ$ can help

Diego Guadagnoli, Camille Normand, Silvano Simula +1

$B_{s} \to μ^{+} μ^{-} γ$ , measured at high $q^{2}$ as a partially reconstructed decay, can probe the origin of the existing discrepancies in semi-leptonic $b \to s$ and $b \to c$ decays.…

hep-ph2023★ 24 cited

Discriminating $B \to D^{*} ℓ ν$ form factors via polarization observables and asymmetries

Marco Fedele, Monika Blanke, Andreas Crivellin +4

Form factors are crucial theory input in order to extract $∣ V_{c b} ∣$ from $B \to D^{(*)} ℓ ν$ decays, to calculate the Standard Model prediction for $R (D^{(*)})$ and to ass…

hep-ph2023

From $D_{s} \to γ$ in lattice QCD to $B_{s} \to μμ γ$ at high $q^{2}$

Diego Guadagnoli, Camille Normand, Silvano Simula +1

We use a recent lattice determination of the vector and axial $D_{s} \to γ$ form factors at high squared momentum transfer $q^{2}$ to infer their $B_{s} \to γ$ counterparts. To this end,…

physics.acc-ph2023

Towards a Muon Collider

Carlotta Accettura, Dean Adams, Rohit Agarwal +294

A muon collider would enable the big jump ahead in energy reach that is needed for a fruitful exploration of fundamental interactions. The challenges of producing muon collisions a…

Insights on the current semi-leptonic B-decay discrepancies -- and how Bs​→μ+μ−γ can help

Discriminating B→D∗ℓν form factors via polarization observables and asymmetries

From Ds​→γ in lattice QCD to Bs​→μμγ at high q2

Towards a Muon Collider

Insights on the current semi-leptonic $B$ -decay discrepancies -- and how $B_{s} \to μ^{+} μ^{-} γ$ can help

Discriminating $B \to D^{*} ℓ ν$ form factors via polarization observables and asymmetries

From $D_{s} \to γ$ in lattice QCD to $B_{s} \to μμ γ$ at high $q^{2}$