Kevin Ingles

activity

20182020

X (3872)

at High Multiplicity

43 citations · 69 across the 2 of their papers we have counts for

collaborators

8 papers

hep-ph2020★ 43 cited

Production of $X (3872)$ at High Multiplicity

Eric Braaten, Li-Ping He, Kevin Ingles +1

The dependence of the production of the $X (3872)$ meson on the hadron multiplicity in $pp$ collisions has been used as evidence against $X$ being a charm-meson molecule. The argume…

hep-ph2020★ 26 cited

Charm-meson Triangle Singularity in $e^{+} e^{-}$ Annihilation into $D^{* 0} D ˉ^{0} + γ$

Eric Braaten, Li-Ping He, Kevin Ingles +1

We calculate the cross section for $e^{+} e^{-}$ annihilation into $D^{* 0} D ˉ^{0} + γ$ at center-of-mass energies near the $D^{* 0} D ˉ^{* 0}$ threshold under the assumption that $X(…

hep-ph2019

Production of $X (3872)$ and a Photon in $e^{+} e^{-}$ Annihilation

Eric Braaten, Li-Ping He, Kevin Ingles

If the $X (3872)$ is a weakly bound charm-meson molecule, it can be produced in $e^{+} e^{-}$ annihilation by the creation of $D^{* 0} D ˉ^{* 0}$ from a virtual photon followed by the…

hep-ph2019

Branching Fractions of the $X (3872)$

Eric Braaten, Li-Ping He, Kevin Ingles

The recoil momentum spectrum from the decay $B^{+} \to K^{+} + anything$ has recently been measured by the BaBar collaboration. The spectrum has a peak with invariant mass near…

hep-ph2019

Triangle Singularity in the Production of $X (3872)$ and a Photon in $e^{+} e^{-}$ Annihilation

Eric Braaten, Li-Ping He, Kevin Ingles

If the $X (3872)$ is a weakly bound charm-meson molecule, it can be produced in $e^{+} e^{-}$ annihilation by the creation of $D^{* 0} D ˉ^{* 0}$ from a virtual photon followed by the…

hep-ph2019

Production of $X (3872)$ Accompanied by a Soft Pion at Hadron Colliders

Eric Braaten, Li-Ping He, Kevin Ingles

If the $X (3872)$ is a weakly bound charm-meson molecule, it can be produced by the creation of $D^{* 0} D ˉ^{0}$ or $D^{0} D ˉ^{* 0}$ at short distances followed by the formati…

Production of X(3872) at High Multiplicity

Charm-meson Triangle Singularity in e+e− Annihilation into D∗0Dˉ0+γ

Production of X(3872) and a Photon in e+e− Annihilation

Branching Fractions of the X(3872)

Triangle Singularity in the Production of X(3872) and a Photon in e+e− Annihilation

Production of X(3872) Accompanied by a Soft Pion at Hadron Colliders

Production of $X (3872)$ at High Multiplicity

Charm-meson Triangle Singularity in $e^{+} e^{-}$ Annihilation into $D^{* 0} D ˉ^{0} + γ$

Production of $X (3872)$ and a Photon in $e^{+} e^{-}$ Annihilation

Branching Fractions of the $X (3872)$

Triangle Singularity in the Production of $X (3872)$ and a Photon in $e^{+} e^{-}$ Annihilation

Production of $X (3872)$ Accompanied by a Soft Pion at Hadron Colliders