Pith. sign in

REVIEW 7 cited by

New anomaly observed in $^{12}$C supports the existence and the vector character of the hypothetical X17 boson

Not yet reviewed by Pith; the record is open.

This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.

SPECIMEN: schema-true, not a live event

T0 review · schema-true

One-sentence machine reading of the paper's core claim.

pith:XXXXXXXX · record.json · timestamp

arxiv 2209.10795 v2 pith:SQ7ZH5Z2 submitted 2022-09-22 nucl-ex hep-ex

classification nucl-exhep-ex
keywords circparticleobservedanglesangularanomalycreationderived
verification ladder T0 review T1 audit T2 compute T3 formal
0 comments
abstract

Employing the $^{11}$B(p,$\gamma$)$^{12}$C nuclear reaction, the angular correlation of $e^+e^-$ pairs was investigated in the angular range of $40^\circ\Theta\leq 175^\circ$ for five different proton energies between E$_p$ = 1.50 - 2.50 MeV. At small angles ($\Theta\leq 120^\circ$), the results can be well interpreted by the internal pair creation process of electromagnetic radiations with E1 and M1 multipolarities and by the external pair creation in the target backing. However, at angles greater than $120^\circ$, additional count excess and anomalies were observed, which could be well accounted for by the existence of the previously suggested hypotetical X17 particle. Our results show that the X17 particle was generated mainly in E1 radiation. The derived mass of the particle is $m_\mathrm{X}c^2$=17.03$\pm 0.11 (stat) \pm 0.20 (syst)$ MeV. According to the mass, and to the derived branching ratio ($B_x=3.6(3)\times10^{-6}$), this is likely the same X17 particle, which we recently suggested for describing the anomaly observed in the decay of $^8$Be and $^4$He.

Discussion (0). Sign in to comment.

Forward citations

Cited by 7 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Possible Evidence for Neutral Color-Singlet $q\bar q$ Quark Matter from High-Energy Pb-Emulsion Collisions

    hep-ph 2026-04 unverdicted novelty 7.0 of 10

    The complex e+e- invariant mass spectrum below 50 MeV is attributed to thermal annihilation and bound states of QED-deconfined and confined neutral q bar q quark matter.

  2. Updated E141 constraints on a long-lived $X_{17}$ vector boson

    hep-ph 2026-07 conditional novelty 6.0 of 10

    A refined simulation of SLAC E141 shows the experiment's old exclusion region does not cover the 16.9 MeV X17, leaving a window at ε_e between 6.5e-5 and 1.1e-4.

  3. Flavor specific chiral $U(1)_X$ framework for explaining the ATOMKI anomaly

    hep-ph 2026-04 unverdicted novelty 6.0 of 10

    A gauged, flavor-specific U(1)_X two-Higgs-doublet model can realize the axial-vector Z' couplings needed to explain the ATOMKI 8Be and 4He anomalies while evading current bounds.

  4. The X17 with Chiral Couplings

    hep-ph 2026-02 conditional novelty 6.0 of 10

    A spin-1 X17 with chiral couplings fits the ATOMKI nuclear anomalies at 99% CL only in a parameter region that atomic parity violation and KLOE-2/NA64 exclude, driven mainly by the 12C(17.23) transition.

  5. Probing the ATOMKI X17 vector boson using Dalitz decays $V\to Pe^+e^-$

    hep-ph 2025-06 conditional novelty 6.0 of 10

    In a quark-model calculation, X17 contributions to D*, B*, and J/psi Dalitz decays are too small to explain the BESIII D*0 e+e- excess unless quark couplings are far outside ATOMKI-favored ranges.

  6. Potential for the discovery of the protophobic boson at the STCF

    hep-ph 2025-12 conditional novelty 5.0 of 10

    Detector-level simulations indicate the proposed STCF drift chamber could discover the 17 MeV protophobic X17 boson through displaced electron-positron vertices if Standard Model backgrounds stay below about 10^4 even...

  7. Where to find $X(17)$?

    hep-ph 2026-01 reject novelty 4.0 of 10

    Combining existing bounds with a new parity-violating Møller asymmetry constraint, the paper's body claims no surviving parameter space for scalar, pseudoscalar, vector, axial-vector, or V±A X(17)-electron couplings.

Pith tools