REVIEW
The X(3872) boson: Molecule or charmonium
High Energy Physics - Phenomenology · Submitted 24 Aug 2005 · 35 references
Pith's verdict: The delta-function argument in Section II.A is the real contribution; the production-rate argument is order-of-magnitude and depends on a regulator set at its minimum, so the abstract's 'incompatible' is stronger than the calculation supports.
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Referee report
The paper
The paper claims
X(3872) is more likely the 2 3P1 charmonium mixed with a D-D* component than a deuteron-like D-D* molecule, since one-pion exchange gives no long-range binding and a loose molecule would be produced one to two orders of magnitude too rarely.
The reading
Extended reading notes
Core claim
X(3872) is more likely the 2 3P1 charmonium, mixed with a D-D* component of up to roughly one third, than a loosely bound D0 anti-D*0 molecule, because (i) one-pion exchange between D and D* reduces to a delta function and supplies no long-range binding (Section II.A, Eq. 5), and (ii) the observed production rates in B to K X and pp to X are one to two orders of magnitude larger than a loose molecule's |Psi(0)|^2 allows (Eqs. 24 and 28).
Load-bearing premise
The quantitative backbone of the 'incompatible with the molecule' claim is the regularized wavefunction of Eq. (14) with regulator M roughly 3 kappa chosen by hand, combined with the factor 0.5 in Eq. (23) for the amplitude ratio A(B to K + DD*) / A(B to K + cc). Neither number is derived. Changing M or the counting factor shifts the predicted branching fraction by factors that could close the gap with the experimental lower bound of Eq. (20), so the production argument is only as strong as these two hand choices.
Original abstract
It has been argued that the mystery boson X(3872) is a molecule state consisting of primarily D0-D0*bar + D0bar-D*0. In contrast, apparent puzzles and potential difficulties have been pointed out for the charmonium assignment of X(3872). We examine several aspects of these alternatives by semiquantitative methods since quantitatively accurate results are often hard to reach on them. We find that some of the observed properties of X(3872), in particualr, the binding and the production rates are incompatible with the molecule interpretation. Despite puzzles and obstacles, X(3872) may fit more likely to the excited triplet P_1 charmonium than to the molecule after mixing of cc-bar with DD*-bar +Dbar-D* is taken into account. One simple experimental test is pointed out for distinguishing between a charmonium and an isospin-mixed molecule in the neutral B decay.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
It has been argued that the mystery boson X(3872) is a molecule state consisting of primarily D0-D0*bar + D0bar-D*0. In contrast, apparent puzzles and potential difficulties have been pointed out for the charmonium assignment of X(3872). We examine several aspects of these alternatives by semiquantitative methods since quantitatively accurate results are often hard to reach on them. We find that some of the observed properties of X(3872), in particualr, the binding and the production rates are incompatible with the molecule interpretation. Despite puzzles and obstacles, X(3872) may fit more likely to the excited triplet P_1 charmonium than to the molecule after mixing of cc-bar with DD*-bar +Dbar-D* is taken into account. One simple experimental test is pointed out for distinguishing between a charmonium and an isospin-mixed molecule in the neutral B decay.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It has been argued that the mystery boson X(3872) is a molecule state consisting of primarily D0-D0*bar + D0bar-D*0. | background 1.00 | 0.04 | 0.03 | hedged possibility 0.40 |
| s1 | In contrast, apparent puzzles and potential difficulties have been pointed out for the charmonium assignment of X(3872). | background 0.98 | 0.05 | 0.02 | asserted 0.64 |
| s2 | We examine several aspects of these alternatives by semiquantitative methods since quantitatively accurate results are often hard to reach on them. | method 0.85 | 0.66 | 0.02 | asserted 0.91 |
| s3 | We find that some of the observed properties of X(3872), in particualr, the binding and the production rates are incompatible with the molecule interpretation. | result 1.00 | 0.94 | 0.15 | asserted 1.00 |
| s4 | Despite puzzles and obstacles, X(3872) may fit more likely to the excited triplet P_1 charmonium than to the molecule after mixing of cc-bar with DD*-bar +Dbar-D* is taken into account. | interpretation 0.70 | 0.76 | 0.90 | hedged possibility 1.00 |
| s5 | One simple experimental test is pointed out for distinguishing between a charmonium and an isospin-mixed molecule in the neutral B decay. | future work 0.91 | 0.78 | 0.04 | asserted 0.83 |
What was examined, and what was not
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Figures
Showing 4 of the paper's 6 figures. See all figures in the PDF ↗ Figures reproduced from arXiv:hep-ph/0508258 by the authors.
References
How the literature uses it
54 arXiv papers cite this in 71 sentences
Papers citing it · 48 sentences without a confident label
Cites it as support 2 papers
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These considerations imply a kinematic suppression of the amplitude for $X(3872)ω$ decays relative to the $ρ$ channel by a factor of about $∼$4, in which case the near equality of the $ρ$ and $ω$ decay rates implies that an $I=0$ assignment is favored [ref] , but a sizable isovector component in the X(3872) wavefunction is still allowed.
Non-Standard Heavy Mesons and Baryons, an Experimental Review · $X(3872)$ · 0.97
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Actually, the above difficulties indicate that there should exist a significant $cc̅$ component in the wave function of the $X(3872)$ [ref] .
The $X(3872)\rightarrow J/\psi \pi \gamma$ and $X(3872)\rightarrow J/\psi \pi\pi \gamma$ decays · Introduction · 0.98
Cites it as background 19 papers
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The $X(3872)$ [ref] , also known as $χ_c1(3872)$, and the $Z_c(3900)$ [ref] have been proposed as candidates of isoscalar and isovector $DD̅^*$ hadronic molecules, respectively, since long [ref] .
Establishing the heavy quark spin and light flavor molecular multiplets of the $X(3872)$, $Z_c(3900)$ and $X(3960)$ · Introduction · 0.89
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The $X(3872)$ became the first candidate for exotic charmoniumlike states, and many hypotheses have been put forward about its nature; see Refs. [ref] and references herein.
Toward an estimate of the amplitude $X(3872)\to\pi^0\chi_{c1}(1P)$ · Introduction · 0.98
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Besides, based on the $DD̅^*$ molecular picture of $X(3872)$, the isospin breaking effects of the $X(3872) →J/ψρ^0$ and $X(3872) →J/ψω$ decays were investigated in Refs. [ref] .
Theoretical study on the contributions of $\omega$ meson to the $X(3872) \to J/\psi\pi^+\pi^-$ and $J/\psi\pi^+\pi^-\pi^0$ decays · Introduction · 0.93
Discussion
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