R. Molina

activity

20082023

most citedElliptic flow of charged particles in Pb-Pb collisions at 2.76 TeV

876 citations · 3.1k across the 52 of their papers we have counts for

collaborators

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16 papers · 1 filter

hep-ph2021★ 14 cited

$Z_{cs}$ states from the $D_{s}^{} D ˉ^{}$ and $J / ψ K^{*}$ coupled channels: Signal in $B^{+} \to J / ψ ϕ K^{+}$ decay

Natsumi Ikeno, Raquel Molina, Eulogio Oset

We study the $D_{s}^{*} D ˉ^{*}$ system in connection with the $J / ψ K^{*}$ in coupled channels and observe that, within reasonable values of the cut-off used to regularize the loops, t…

hep-ph2020★ 44 cited

The $Z_{cs} (3985)$ as a threshold effect from the $D ˉ_{s}^{} D + D ˉ_{s} D^{}$ interaction

Natsumi Ikeno, Raquel Molina, Eulogio Oset

We study the $e^{+} e^{-} \to K^{+} (D_{s}^{*-} D^{0} + D_{s}^{-} D^{* 0})$ reaction recently measured at BESIII, from where a new $Z_{cs}$ state has been reported. We study the interaction of $…

hep-ph2020★ 88 cited

Molecular picture for the $X_{0} (2866)$ as a $D^{} K ˉ^{}$ $J^{P} = 0^{+}$ state and related $1^{+}, 2^{+}$ states

R. Molina, E. Oset

We recall the predictions made ten years ago about a bound state of $J^{P} = 0^{+}$ in $I = 0$ of the $D^{*} K ˉ^{*}$ system, which is manifestly exotic, and we associate it to the $X_0(2…

hep-ph2020★ 24 cited

Triangle singularity in $B^{-} \to K^{-} X (3872); X \to π^{0} π^{+} π^{-}$ and the X(3872) mass

Raquel Molina, Eulogio Oset

We evaluate the contribution to the $X (3872)$ width from a triangle mechanism in which the $X$ decays into $D^{* 0} D ˉ^{0} - cc$ , then the $D^{* 0} (D ˉ^{* 0})$ decays into $D^0…

hep-ph2019★ 48 cited

Theoretical interpretation of the $D_{s}^{+} \to π^{+} π^{0} η$ decay and the nature of $a_{0} (980)$

Raquel Molina, Ju-Jun Xie, Wei-Hong Liang +2

In a recent paper \cite{Ablikim:2019pit}, the BESIII collaboration reported the so-called first observation of pure $W$ -annihilation decays $D_{s}^{+} \to a_{0}^{+} (980) π^{0}$ and $D_s^+ \t…

hep-ph2016★ 9 cited

Determination of the compositeness of resonances from decays: the case of the $B_{s}^{0} \to J / ψ f_{1} (1285)$

R. Molina, M. Döring, E. Oset

We develop a method to measure the amount of compositeness of a resonance, mostly made as a bound state of two hadrons, by simultaneously measuring the rate of production of the re…

hep-ph2016★ 143 cited

Weak decays of heavy hadrons into dynamically generated resonances

Eulogio Oset, Wei-Hong Liang, Melahat Bayar +24

In this review we give a perspective of the theoretical work done recently on the interpretation of results from $B$ , $D$ , $Λ_{b}$ , $Λ_{c}$ weak decays into final states that contain i…

hep-ph2015

Strategies for an accurate determination of the X(3872) energy from QCD lattice simulations

E. J. Garzon, R. Molina, A. Hosaka +1

We develop a method to determine accurately the binding energy of the X(3872) from lattice data for the DD* interaction. We show that, because of the small difference between the n…

hep-ph2010★ 2 cited

The $f_{0} (1370)$ , $f_{0} (1710)$ , $f_{2} (1270)$ , $f_{2}^{'} (1525)$ , and $K_{2}^{*} (1430)$ as dynamically generated states from vector meson - vector meson interaction

L. S. Geng, E. Oset, R. Molina +5

We report on some recent developments in understanding the nature of the low-lying mesonic resonances $f_{0} (1370)$ , $f_{0} (1710)$ , $f_{2} (1270)$ , $f_{2}^{'} (1525)$ , and $K_{2}^{*} (1430)$ . In par…

hep-ph2010★ 34 cited

Radiative decays of the Y(3940), Z(3930) and the X(4160) as dynamically generated resonances

Tanja Branz, Raquel Molina, Eulogio Oset

We study the radiative decay properties of the charmonium-like X, Y and Z mesons generated dynamically from vector meson-vector meson interaction in the framework of a unitarized h…

hep-ph2010

Scalar, axial-vector and tensor resonances from the $ρ D^{}$ , $ω D^{}$ interaction in the hidden gauge formalism

R. Molina, H. Nagahiro, A. Hosaka +1

We apply a unitary approach together with a set of hidden-gauge Lagrangians to study the vector-vector interaction. We study the case of the $ρ$ ( $ω$ ) $D^{*}$ interaction within the mo…

hep-ph2010★ 7 cited

The Y(3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction

R. Molina, E. Oset

We study the vector-vector interaction within the framework of the hidden gauge formalism for the sector with quantum numbers charm C=0 and strangeness S=0 in the region around 400…

hep-ph2009

Strange and charm mesons at FAIR

L. Tolos, D. Cabrera, D. Gamermann +5

We study the properties of strange and charm mesons in hot and dense matter within a self-consistent coupled-channel approach for the experimental conditions of density and tempera…

hep-ph2009★ 157 cited

The Y(3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction

R. Molina, E. Oset

We study the vector-vector interaction within the framework of the hidden gauge formalism for the channels with quantum numbers Charm C=0 and Strangeness S=0 in the energy region a…

hep-ph2009

Dynamically generated resonances from vector meson-vector meson interaction based on a hidden-gauge unitary approach

L. S. Geng, E. Oset, R. Molina +1

We present a recent study of vector meson-vector meson interaction using a unitary approach based on the hidden-gauge Lagrangians. We find that 11 states get dynamically generated,…

hep-ph2008★ 1 cited

Strangeness and charm at FAIR

Laura Tolos, Daniel Cabrera, Daniel Gamermann +4

We study the properties of strange and charm mesons in hot and dense matter within a self-consistent coupled-channel approach for the experimental conditions of density and tempera…

Zcs​ states from the Ds∗​Dˉ∗ and J/ψK∗ coupled channels: Signal in B+→J/ψϕK+ decay

The Zcs​(3985) as a threshold effect from the Dˉs∗​D+Dˉs​D∗ interaction

Molecular picture for the X0​(2866) as a D∗Kˉ∗ JP=0+ state and related 1+,2+ states

Triangle singularity in B−→K−X(3872);X→π0π+π− and the X(3872) mass

Theoretical interpretation of the Ds+​→π+π0η decay and the nature of a0​(980)

Determination of the compositeness of resonances from decays: the case of the Bs0​→J/ψf1​(1285)

Weak decays of heavy hadrons into dynamically generated resonances

Strategies for an accurate determination of the X(3872) energy from QCD lattice simulations

The f0​(1370), f0​(1710), f2​(1270), f2′​(1525), and K2∗​(1430) as dynamically generated states from vector meson - vector meson interaction

Radiative decays of the Y(3940), Z(3930) and the X(4160) as dynamically generated resonances

Scalar, axial-vector and tensor resonances from the ρD∗, ωD∗ interaction in the hidden gauge formalism

The Y(3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction

Strange and charm mesons at FAIR

The Y(3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction

Dynamically generated resonances from vector meson-vector meson interaction based on a hidden-gauge unitary approach

Strangeness and charm at FAIR

$Z_{cs}$ states from the $D_{s}^{} D ˉ^{}$ and $J / ψ K^{*}$ coupled channels: Signal in $B^{+} \to J / ψ ϕ K^{+}$ decay

The $Z_{cs} (3985)$ as a threshold effect from the $D ˉ_{s}^{} D + D ˉ_{s} D^{}$ interaction

Molecular picture for the $X_{0} (2866)$ as a $D^{} K ˉ^{}$ $J^{P} = 0^{+}$ state and related $1^{+}, 2^{+}$ states

Triangle singularity in $B^{-} \to K^{-} X (3872); X \to π^{0} π^{+} π^{-}$ and the X(3872) mass

Theoretical interpretation of the $D_{s}^{+} \to π^{+} π^{0} η$ decay and the nature of $a_{0} (980)$

Determination of the compositeness of resonances from decays: the case of the $B_{s}^{0} \to J / ψ f_{1} (1285)$

The $f_{0} (1370)$ , $f_{0} (1710)$ , $f_{2} (1270)$ , $f_{2}^{'} (1525)$ , and $K_{2}^{*} (1430)$ as dynamically generated states from vector meson - vector meson interaction

Scalar, axial-vector and tensor resonances from the $ρ D^{}$ , $ω D^{}$ interaction in the hidden gauge formalism