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| Format: | Preprint |
| Veröffentlicht: |
2023
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| Online-Zugang: | https://arxiv.org/abs/2312.13383 |
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| _version_ | 1866914754885320704 |
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| author | Mutuk, Halil |
| author_facet | Mutuk, Halil |
| contents | We present mass spectrum and magnetic moments of the $\bar{n}\bar{n}QQ$ states, where $n=u,d,s$ and $Q=c,b$. We solve four-body Schrödinger equation with a quark potential model by using diffusion Monte Carlo (DMC) method. The quark potential is based on the Coulomb, confinement and spin-spin interaction terms. We find mass and magnetic moment of the $T_{cc}^+$ state as $M_{T_{cc}^+}=3892 ~\text{MeV}$ and $μ=0.28 μ_N$, respectively. We also find the mass and magnetic moment of $T_{bb}^-$ as $M_{T_{bb}^-}=10338 ~\text{MeV}$ and $μ=-0.32 μ_N$, respectively. We find some bound state candidates of doubly heavy tetraquark systems with $I(J^P)=0(1)^+$ $nn \bar b \bar b$, $I(J^P)=0(0)^+$ $nn \bar c \bar b$, $I(J^P)=0(1)^+$ $nn \bar c \bar b$, and $I(J^P)=1/2(1)^+$ $ns \bar b \bar b$. We compare our results with other approaches in the literature. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2312_13383 |
| institution | arXiv |
| publishDate | 2023 |
| record_format | arxiv |
| spellingShingle | Masses and Magnetic Moments of Doubly Heavy Tetraquarks via Diffusion Monte Carlo Method Mutuk, Halil High Energy Physics - Phenomenology High Energy Physics - Experiment We present mass spectrum and magnetic moments of the $\bar{n}\bar{n}QQ$ states, where $n=u,d,s$ and $Q=c,b$. We solve four-body Schrödinger equation with a quark potential model by using diffusion Monte Carlo (DMC) method. The quark potential is based on the Coulomb, confinement and spin-spin interaction terms. We find mass and magnetic moment of the $T_{cc}^+$ state as $M_{T_{cc}^+}=3892 ~\text{MeV}$ and $μ=0.28 μ_N$, respectively. We also find the mass and magnetic moment of $T_{bb}^-$ as $M_{T_{bb}^-}=10338 ~\text{MeV}$ and $μ=-0.32 μ_N$, respectively. We find some bound state candidates of doubly heavy tetraquark systems with $I(J^P)=0(1)^+$ $nn \bar b \bar b$, $I(J^P)=0(0)^+$ $nn \bar c \bar b$, $I(J^P)=0(1)^+$ $nn \bar c \bar b$, and $I(J^P)=1/2(1)^+$ $ns \bar b \bar b$. We compare our results with other approaches in the literature. |
| title | Masses and Magnetic Moments of Doubly Heavy Tetraquarks via Diffusion Monte Carlo Method |
| topic | High Energy Physics - Phenomenology High Energy Physics - Experiment |
| url | https://arxiv.org/abs/2312.13383 |