0000000000697670

AUTHOR

M. Pavon Valderrama

showing 4 related works from this author

Decay widths of the spin-2 partners of the X (3872)

2015

We consider the $X(3872)$ resonance as a $J^{PC}=1^{++}$ $D\bar D^*$ hadronic molecule. According to heavy quark spin symmetry, there will exist a partner with quantum numbers $2^{++}$, $X_{2}$, which would be a $D^*\bar D^*$ loosely bound state. The $X_{2}$ is expected to decay dominantly into $D\bar D$, $D\bar D^*$ and $\bar D D^*$ in $d$-wave. In this work, we calculate the decay widths of the $X_{2}$ resonance into the above channels, as well as those of its bottom partner, $X_{b2}$, the mass of which comes from assuming heavy flavor symmetry for the contact terms. We find partial widths of the $X_{2}$ and $X_{b2}$ of the order of a few MeV. Finally, we also study the radiative $X_2\to …

PhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyHadronFOS: Physical sciencesFísicaOrder (ring theory)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Quantum numberHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Bound stateHigh Energy Physics::ExperimentEngineering (miscellaneous)X(3872)Bar (unit)Spin-½European Physical Journal C
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Heavy Quark Symmetries: Molecular Partners of the X(3872) and $Z_{b}(10610)/Z_{b}'(10650)$

2013

In this work, we have used an Effective Field Theory (EFT) framework based on Heavy Quark Spin (HQSS), Heavy Flavour (HFS) and Heavy Antiquark-Diquark symmetries (HADS). Using a standard lagrangian for the heavy meson-heavy antimeson system, we fit the counter-terms of the model to predict some promising experimental data that can be interpreted as heavy meson-heavy antimeson molecules, that is, the X(3872) and the $Z_{b}(10610)/Z'_{b}(10650)$. Next, and, taking advantage of HADS, we use the same lagrangian to explore the consequences for heavy meson-doubly heavy baryon molecules, which can also be interpreted as triply heavy pentaquarks.

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesBaryonsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spacesymbolsEffective field theoryHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentLagrangianSpin-½X(3872)
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Inverse amplitude method in pi pi scattering in chiral perturbation theory to two loops

2002

The inverse amplitude method is used to unitarize the two loop $\pi\pi$ scattering amplitudes of SU(2) Chiral Perturbation Theory in the $I=0,J=0$, $I=1,J=1$ and $I=2,J=0$ channels. An error analysis in terms of the low energy one-loop parameters $\bar l_{1,2,3,4,}$ and existing experimental data is undertaken. A comparison to standard resonance saturation values for the two loop coefficients $\bar b_{1,2,3,4,5,6} $ is also carried out. Crossing violations are quantified and the convergence of the expansion is discussed.

PhysicsScattering amplitudeNuclear and High Energy PhysicsHigh Energy Physics - PhenomenologyChiral perturbation theoryAmplitudeScatteringQuantum mechanicsPartial wave analysisSaturation (graph theory)InverseFísicaResonance (particle physics)
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Heavy meson-antimeson molecules in effective field theory: The role of one pion exchange and heavy quark spin symmetry

2012

In this contribution we study heavy meson-antimeson molecules from the effective field theory perspective. In particular, we are concerned with the role of the one pion exchange interaction and heavy quark spin symmetry in the description of molecular states. As we will show, one pion exchange is in general a perturbative effect. This means that at lowest order we can describe the molecular states in terms of contact interactions only, a remarkable simplification. The application of heavy quark spin symmetry will be very interesting, as we will be able to predict new heavy meson-antimeson bound states from known ones. For instance, if we assume that the X(3872) is in fact a JPC = 1++ DD/DD …

PhysicsQuarkParticle physicsMesonHigh Energy Physics::PhenomenologyExchange interactionOrder (ring theory)Nuclear physicsPionBound stateEffective field theoryMoleculeHigh Energy Physics::ExperimentNuclear Experiment
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