S. Agaev

collaborators

15 papers

hep-ph2026

Fully-beauty tensor tetraquark

S. S. Agaev, K. Azizi, H. Sundu

Parameters of the fully-beauty tensor tetraquark $T = bb b b$ are computed using QCD sum rule method. The mass $m$ and coupling $I^$ of this state are evaluated…

hep-ph2026

Tensor states $I^¥ B_{c}^{-}$ and $J / I ¨ B_{c}^{+}$

S. S. Agaev, K. Azizi, H. Sundu

Tensor states $M_{T}^{b} = I^¥ B_{c}^{*-}$ and $M_{T}^{c} = J / I ¨ B_{c}^{*+}$ are explored using techniques of QCD sum rule…

hep-ph2026

Tensor molecule $J / I ¨ J / I ¨ $ : A candidate to the resonance $X (6200)$

S. S. Agaev, K. Azizi, H. Sundu

The hadronic tensor molecule $M = J / I ¨ J / I ¨ $ is investigated in the framework of QCD sum rule method. We evaluate its mass and current coupling using the two-point SR approa…

hep-ph2026

Scalar molecules $I^\cdot_{b} B_{c}^{-}$ and $I^\cdot_{c} B_{c}^{+}$ with asymmetric quark contents

S. S. Agaev, K. Azizi, H. Sundu

The hadronic scalar molecules $M_{b}$ and $M_{c}$ with asymmetric quark contents $bb b c$ and $cc c b$ are explored b…

hep-ph2026

Molecular states $J / I ¨ B_{c}^{+}$ and $I^\cdot_{c} B_{c}^{*+}$

S. S. Agaev, K. Azizi, H. Sundu

Hadronic molecules $M = J / I ¨ B_{c}^{+}$ and $M = I^\cdot_{c} B_{c}^{*+}$ are investigated in the framework of QCD sum rule method. These particles wit…

hep-ph2026

Resonance $X (6600)$

S. S. Agaev, K. Azizi, H. Sundu

The resonance $X (6600)$ is explored as the all-charm tetraquark structure with spin-parities $J^{PC} = 2^{++}$ . It is considered in the diquark-antidiquark picture and model…

Fully-beauty tensor tetraquark

Tensor states I^¥Bc∗−​ and J/I¨Bc∗+​

Tensor molecule J/I¨J/I¨: A candidate to the resonance X(6200)

Scalar molecules I^⋅b​Bc−​ and I^⋅c​Bc+​ with asymmetric quark contents

Molecular states J/I¨Bc+​ and I^⋅c​Bc∗+​

Resonance X(6600)

Tensor states $I^¥ B_{c}^{-}$ and $J / I ¨ B_{c}^{+}$

Tensor molecule $J / I ¨ J / I ¨ $ : A candidate to the resonance $X (6200)$

Scalar molecules $I^\cdot_{b} B_{c}^{-}$ and $I^\cdot_{c} B_{c}^{+}$ with asymmetric quark contents

Molecular states $J / I ¨ B_{c}^{+}$ and $I^\cdot_{c} B_{c}^{*+}$

Resonance $X (6600)$