Core Concepts
The triangular singularity mechanism can be used to predict the existence of new hadronic molecular states that exist above the threshold of their constituent particles, challenging the traditional view that these states only exist below the threshold.
Abstract
Bibliographic Information:
Huang, Y., & Chen, X. (2024). Predicting New Above-Threshold Molecular States Via Triangular Singularities. arXiv preprint arXiv:2411.03119v1.
Research Objective:
This research paper aims to propose a new approach for predicting and identifying hadronic molecular states, particularly those that exist above the threshold of their constituent particles, using the triangular singularity mechanism.
Methodology:
The authors utilize the theoretical framework of triangular singularities (TS), applying the Landau equation and Coleman-Norton theorem to analyze the kinematic conditions required for TS formation in hadronic decays. They leverage existing experimental data on confirmed and candidate molecular states, focusing on those with masses exceeding their constituent thresholds. By selecting appropriate initial and final state particles, along with intermediate particles fulfilling TS requirements, they predict the masses of potential new molecular states.
Key Findings:
The study predicts the existence of 16 new heavy quark molecular states, including potential partner states of already observed particles like X(3872), Y(4320), Z(4430), and Υ(11020). These predictions challenge the conventional understanding that molecular states primarily exist below the threshold and provide specific decay channels and mass ranges for experimental verification.
Main Conclusions:
The authors argue that the triangular singularity mechanism offers a robust and experimentally testable method for discovering new hadronic molecular states, particularly those above the threshold. They emphasize that confirming the existence of these predicted states would provide strong support for heavy quark symmetry and significantly enhance our understanding of hadronic dynamics and molecular state formation.
Significance:
This research has significant implications for the field of hadron physics. It proposes a novel approach to identifying new particles, potentially resolving the discrepancy between theoretically predicted and experimentally observed molecular states. The confirmation of these predictions would validate heavy quark symmetry and deepen our understanding of the strong force.
Limitations and Future Research:
The study relies on specific interpretations of existing experimental data and theoretical models. Further experimental investigation is crucial to confirm the existence and properties of the predicted molecular states. Future research could explore the production mechanisms and decay properties of these states in more detail, refining theoretical models and guiding experimental searches.
Stats
The mass of T++c¯s0(2900) exceeds the threshold of its molecular components by approximately 20 MeV.
The mass of X(3872) is mC = 3871.69 MeV.
The masses of D∗0 and D0 are 2006.85 MeV and 1864.84 MeV, respectively.
δ(D∗±D0π±, D∗0D0π0) = (5.85, 7.03) MeV.
The mass of the molecular state A with a ¯cc¯qq quark component is in the range of M = 4017.11 −4017.33 MeV for δ(D∗±D0π±) and M = 4013.70 −4013.96 MeV for δ(D∗0D0π0).
δ(D∗0D0γ) ≈ 142.0 MeV.
The mass range for A is M = 4013.7 −4016.4 MeV.
The mass of Y(4320) is M = 4298 ± 12 ± 26 MeV and a width of Γ = 127 ± 17 ± 10 MeV.
δ(D1(2420)±D∗±π0) = 280.86 MeV.
The mass of A lies in the range 4436.36 −4453.76 MeV.
δ(D1(2420)0D∗0π0) = 280.27 MeV.
The initial state mass allowing for a triangle singularity is within 4428.95 − 4446.33 MeV.
δ(D1(2420)0D∗±π∓) = 272.27 MeV.
The mass range is 4432.36 −4449.26 MeV.
δ(D1(2420)0D∗±π∓) = 279.68 MeV.
The mass range is 4432.95 −4450.54 MeV.
δ(Ds1(2536)+D∗+K0) = 27.24 MeV.
The mass of Zcs is predicted to lie within M = 4545.37 −4548.43 MeV.
δ(Ξ′+c Ξ+c γ) = 110.51 MeV.
The mass of the Ξ′c ¯D state is M = 4447.86 −4448.9 MeV.
δ(Ξ∗+c Ξ+c π0) = 42.42 MeV.
The mass of the Ξ∗c ¯D state is M = 4514.76 −4515.87 MeV.
δ(D1(2420)+D∗+π0) = 280.86 MeV.
The mass of the D+1 K∗+ molecular state is M = 3313.77 −3323.89 MeV.
The mass of the B∗+ ¯B∗− molecular state is M = 10655.5 −10655.6 MeV.
The mass of A lies within M = 11005.4 −11011.8 MeV.
The mass of Υ(11020) is M = 11000±4 MeV.
The lower mass limit for B1(5721) is M = 5723.3 MeV.
The mass of the B1(5721) ¯B molecular state is expected to have a mass of M = 11002.7 −11009.0 MeV.
The mass of the B1(5721) ¯B∗ molecular state is M = 11051.7 − 11058.1 MeV.
The mass of the Bs1(5828)0 ¯B∗0 molecular state is M = 11154.4 −11154.9 MeV.
δ(ψ(3770) ¯D0D0) = 44.02 MeV.
The mass of the tetraquark state Xcc¯c is in the range M = 5783.96 −5799.42 MeV.
Quotes
"The discovery of molecular states has prompted theoretical predictions of numerous additional states, particularly in the context of heavy quarks. However, the lack of experimental confirmation for these anticipated states casts doubt on the validity of various theoretical frameworks."
"Our main point is that the molecular states theoretically predicted to probe HQS do indeed exist; however, their experimental detection is challenging primarily because these molecular states exist above the threshold, rather than below it as typically anticipated."
"In contrast to the ambiguous mechanisms underlying the enhancements observed in resonant states, the production mechanism of TS peaks is well-characterized."
"Consequently, when particles 1 and 3 are interpreted as molecular components of hadron C, the re-scattering event leading to the formation of C, the TS signal provides direct experimental evidence for the molecular structure of C."
"Upon successful experimental validation of these states, they can serve as a robust framework for testing heavy quark symmetry."