Adolfo Álvarez

collaborators

4 papers

hep-ex2026

Search for $C P$ violation in $D^{+} \to ϕ π^{+}$ decays

LHCb collaboration, R. Aaij, M. Abdelfatah +1106

A search for charge-parity ( $C P$ ) violation in the Cabibbo-suppressed $D^{+} \to ϕ π^{+}$ decay is presented, using proton-proton collision data corresponding to an integrated luminos…

cond-mat.mtrl-sci2026

Challenging the $p$ -type Paradigm: Intrinsic $n$ -type Mobility in Antiferromagnetic Cr $_{2}$ O $_{3}$

Á. A. Carrasco Álvarez, S. Poncé

Chromium oxide (Cr $_{2}$ O $_{3}$ ) is widely considered a $p$ -type transparent conducting oxide despite ongoing debate regarding its intrinsic transport character. Here, we resolve this…

hep-ex2026

Differential measurement of the branching fraction and $C P$ asymmetry of the decay $B^{\pm} \to π^{\pm} μ^{+} μ^{-}$

LHCb collaboration, R. Aaij, M. Abdelfatah +1121

Differential measurements of the branching fraction and $C P$ asymmetry of the decay $B^{\pm} \to π^{\pm} μ^{+} μ^{-}$ are performed in intervals of the dimuon mass squared, $q^{2}$ , using pro…

hep-ex2025

Search for the lepton-flavour-violating decays $B^{0} \to K^{* 0} τ^{\pm} e^{\mp}$

LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb +1131

A first search for the lepton-flavour-violating decays $B^{0} \to K^{* 0} τ^{\pm} e^{\mp}$ is presented. The analysis is performed using a sample of proton-proton collision data, collected…

Search for CP violation in D+→ϕπ+ decays

Challenging the p-type Paradigm: Intrinsic n-type Mobility in Antiferromagnetic Cr2​O3​

Differential measurement of the branching fraction and CP asymmetry of the decay B±→π±μ+μ−

Search for the lepton-flavour-violating decays B0→K∗0τ±e∓

Search for $C P$ violation in $D^{+} \to ϕ π^{+}$ decays

Challenging the $p$ -type Paradigm: Intrinsic $n$ -type Mobility in Antiferromagnetic Cr $_{2}$ O $_{3}$

Differential measurement of the branching fraction and $C P$ asymmetry of the decay $B^{\pm} \to π^{\pm} μ^{+} μ^{-}$

Search for the lepton-flavour-violating decays $B^{0} \to K^{* 0} τ^{\pm} e^{\mp}$