Shandong University

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19962026

most citedObservation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC

10.9k citations

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415 papers · 1 filter

hep-ph2026

$T_{c s ˉ 0}^{a} (2900)$ , $T_{cs 0}^{*} (2900)^{0}$ , and other singly heavy tetraquark states

Zi-Long Man, Yu-Nan Liu, Yan-Rui Liu

We systematically study the mass spectra of $S$ -wave singly heavy tetraquark states $Qq q ˉ q ˉ$ ( $Q = c, b$ ; $q = u, d, s$ ) in a mass splitting model. We adopt the assumption that…

hep-ph2026

Higgs boson decay to massive bottom quarks at order $α_{s}^{4}$ induced by top-quark Yukawa couplings

Jian Wang, Xing Wang, Yefan Wang

The Higgs boson decay to massive bottom quarks has the largest branching ratio. The decay is mainly induced by the bottom-quark Yukawa coupling with the decay rate calculated up to…

hep-ph2026★ 2 cited

Two nearby states in the $X (3872)$ region: Resolving the radiative-decay ratio tension with $η_{c 2}$

Satoshi X. Nakamura

Recently, LHCb reported the radiative-decay ratio $R^{ψ γ} \equiv B [X (3872) \to ψ^{'} γ] / B [X (3872) \to J / ψ γ] = 1.67 \pm 0.25$ extracted from $B^{+} \to K^{+} (J / ψ γ, ψ^{'} γ)$ . This…

hep-ph2026

Fully differential Higgs boson pair production at N $^{3}$ LO with top quark mass effects

Xuan Chen, Yuesheng Dai, Hai Tao Li +3

Higgs-boson pair production is of fundamental importance for probing the Higgs potential. At hadron colliders, the dominant production channel proceeds via gluon-gluon fusion (ggF)…

hep-ph2026

Constraining the Higgs potential using multi-Higgs production

Jia-Le Ding, Zach Gillis, Ulrich Haisch +10

The Higgs self-couplings remain only weakly constrained by current Large Hadron Collider (LHC) measurements, leaving ample room for physics beyond the Standard Model that could mod…

hep-ph2026

The Hadronization Impact on $J / ψ$ Energy Correlators: A Pythia8 Study from Partonic to Hadronic Observables

Jin-peng Zhang, Qian Yang, Wen-Chao Zhang +1

A comprehensive study of the $J / ψ$ energy correlator as a probe of non-perturbative hadronization in color-octet $c c ˉ$ production is performed. The energy correlator measures…

Tcsˉ0a​(2900), Tcs0∗​(2900)0, and other singly heavy tetraquark states

Higgs boson decay to massive bottom quarks at order αs4​ induced by top-quark Yukawa couplings

Two nearby states in the X(3872) region: Resolving the radiative-decay ratio tension with ηc2​

Fully differential Higgs boson pair production at N3LO with top quark mass effects

Constraining the Higgs potential using multi-Higgs production

The Hadronization Impact on J/ψ Energy Correlators: A Pythia8 Study from Partonic to Hadronic Observables

$T_{c s ˉ 0}^{a} (2900)$ , $T_{cs 0}^{*} (2900)^{0}$ , and other singly heavy tetraquark states

Higgs boson decay to massive bottom quarks at order $α_{s}^{4}$ induced by top-quark Yukawa couplings

Two nearby states in the $X (3872)$ region: Resolving the radiative-decay ratio tension with $η_{c 2}$

Fully differential Higgs boson pair production at N $^{3}$ LO with top quark mass effects

The Hadronization Impact on $J / ψ$ Energy Correlators: A Pythia8 Study from Partonic to Hadronic Observables