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Model-independent predictions for decays of double-heavy hadrons into pairs of heavy hadrons

High Energy Physics - Phenomenology · Submitted 9 Aug 2024

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim From these constraints, we derive model-independent selection rules for decays of double-heavy hadrons into pairs of heavy hadrons.

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arXiv ID2408.05150 (version 2)
Pith ID5DYZW662, Pith's permanent record of this paper and its review
CitationR. Bruschini. "Model-independent predictions for decays of double-heavy hadrons into pairs of heavy hadrons." arXiv:2408.05150 (2024). https://pith.science/paper/5DYZW662
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What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.35 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.05 · mentions code or data availability 0.02.

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arXiv listing abstract v2. Results and the main claim are underlined; .

Double-heavy hadrons can decay into pairs of heavy hadrons through transitions from confining Born-Oppenheimer potentials to heavy-hadron-pair potentials with the same Born-Oppenheimer quantum numbers. The states of the double-heavy hadron are constrained by a Born-Oppenheimer exclusion principle from the identical heavy quarks. The states of a pair of identical heavy hadrons are constrained by exclusion principles from identical particles. The transitions are also constrained by conservation of angular momentum and parity. From these constraints, we derive model-independent selection rules for decays of double-heavy hadrons into pairs of heavy hadrons. The coupling potentials are expressed as sums of products of Born-Oppenheimer transition amplitudes and angular-momentum coefficients. If there is a single dominant Born-Oppenheimer transition amplitude, it factors out of the coupling potentials between double-heavy hadrons in the same Born-Oppenheimer multiplet and pairs of heavy hadrons in specific heavy-quark-spin-symmetry multiplets and out of the corresponding partial decay rates. As examples, we discuss the Born-Oppenheimer potentials and multiplets for conventional double-heavy baryons and for double-heavy tetraquark mesons. We also discuss the relative partial decay rates for conventional double-heavy baryons into pairs of heavy hadrons.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Double-heavy hadrons can decay into pairs of heavy hadrons through transitions from confining Born-Oppenheimer potentials to heavy-hadron-pair potentials with the same Born-Oppenheimer quantum numbers. background 0.87 0.15 0.14 asserted 0.63
s1 The states of the double-heavy hadron are constrained by a Born-Oppenheimer exclusion principle from the identical heavy quarks. background 0.72 0.15 0.05 asserted 1.00
s2 The states of a pair of identical heavy hadrons are constrained by exclusion principles from identical particles. background 0.84 0.09 0.04 asserted 1.00
s3 The transitions are also constrained by conservation of angular momentum and parity. background 0.57 0.16 0.04 asserted 1.00
s4 From these constraints, we derive model-independent selection rules for decays of double-heavy hadrons into pairs of heavy hadrons. result 0.52 0.95 0.78 asserted 1.00
s5 The coupling potentials are expressed as sums of products of Born-Oppenheimer transition amplitudes and angular-momentum coefficients. method 0.86 0.81 0.06 asserted 1.00
s6 If there is a single dominant Born-Oppenheimer transition amplitude, it factors out of the coupling potentials between double-heavy hadrons in the same Born-Oppenheimer multiplet and pairs of heavy hadrons in specific heavy-quark-spin-symmetry multiplets and out of the corresponding partial decay rates. result 0.88 0.82 0.23 asserted 0.76
s7 As examples, we discuss the Born-Oppenheimer potentials and multiplets for conventional double-heavy baryons and for double-heavy tetraquark mesons. contribution 0.98 0.84 0.04 asserted 0.84
s8 We also discuss the relative partial decay rates for conventional double-heavy baryons into pairs of heavy hadrons. contribution 0.81 0.87 0.06 asserted 0.57

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The paper
Original abstract

Double-heavy hadrons can decay into pairs of heavy hadrons through transitions from confining Born-Oppenheimer potentials to heavy-hadron-pair potentials with the same Born-Oppenheimer quantum numbers. The states of the double-heavy hadron are constrained by a Born-Oppenheimer exclusion principle from the identical heavy quarks. The states of a pair of identical heavy hadrons are constrained by exclusion principles from identical particles. The transitions are also constrained by conservation of angular momentum and parity. From these constraints, we derive model-independent selection rules for decays of double-heavy hadrons into pairs of heavy hadrons. The coupling potentials are expressed as sums of products of Born-Oppenheimer transition amplitudes and angular-momentum coefficients. If there is a single dominant Born-Oppenheimer transition amplitude, it factors out of the coupling potentials between double-heavy hadrons in the same Born-Oppenheimer multiplet and pairs of heavy hadrons in specific heavy-quark-spin-symmetry multiplets and out of the corresponding partial decay rates. As examples, we discuss the Born-Oppenheimer potentials and multiplets for conventional double-heavy baryons and for double-heavy tetraquark mesons. We also discuss the relative partial decay rates for conventional double-heavy baryons into pairs of heavy hadrons.

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