Abstract
Erratum to: JHEP07(2023)155
ArXiv ePrint: 2211.04172
One correction is noted for the paper [1], which does not affect any of the other results reported. The right vertical axis (gaγγ) of figure 8 was not defined consistently with the description in the caption and was incorrectly lower by a factor of 10.
[Figure provided]
Figure 8. Parameter space of the ALP for c1 = c2 = c3 = 10 (eq. 9.1 of the original publication [1]). The observed and expected lower bounds on the ALP decay constant derived from this analysis are shown in black solid and dashed lines respectively. BABAR bounds on B → Ka derived in ref. [2] are shown in purple; in green the LHC bounds on boosted dijet resonances [3] and in blue the LHC searches for diphoton resonances taken from ref. [4]. The red bounds are derived from Tevatron [5] and LHC [6–8] diphoton cross-section measurements, following the method described in ref. [4]. Weaker constraints covering lower invariant masses are obtained from LHCb diphoton measurements [9] and from LEP searches for Z → γa(jj) [10], in cyan and yellow respectively. On the right, the y-axis shows the ALP-photon coupling gaγγ ≡ αemE/πfa (E = c2 + (5/3)·c1), a standard QCD axion notation.
ArXiv ePrint: 2211.04172
One correction is noted for the paper [1], which does not affect any of the other results reported. The right vertical axis (gaγγ) of figure 8 was not defined consistently with the description in the caption and was incorrectly lower by a factor of 10.
[Figure provided]
Figure 8. Parameter space of the ALP for c1 = c2 = c3 = 10 (eq. 9.1 of the original publication [1]). The observed and expected lower bounds on the ALP decay constant derived from this analysis are shown in black solid and dashed lines respectively. BABAR bounds on B → Ka derived in ref. [2] are shown in purple; in green the LHC bounds on boosted dijet resonances [3] and in blue the LHC searches for diphoton resonances taken from ref. [4]. The red bounds are derived from Tevatron [5] and LHC [6–8] diphoton cross-section measurements, following the method described in ref. [4]. Weaker constraints covering lower invariant masses are obtained from LHCb diphoton measurements [9] and from LEP searches for Z → γa(jj) [10], in cyan and yellow respectively. On the right, the y-axis shows the ALP-photon coupling gaγγ ≡ αemE/πfa (E = c2 + (5/3)·c1), a standard QCD axion notation.
| Original language | English |
|---|---|
| Article number | 143 |
| Number of pages | 22 |
| Journal | JHEP |
| Volume | 2025 |
| Issue number | 12 |
| DOIs |
|
| Publication status | Published - 18 Dec 2025 |
Bibliographical note
Erratum to: The ATLAS collaboration., Aad, G., Abbott, B. et al. Search for boosted diphoton resonances in the 10 to 70 GeV mass range using 138 fb−1 of 13 TeV pp collisions with the ATLAS detector. J. High Energ. Phys. 2023, 155 (2023). https://doi.org/10.1007/JHEP07(2023)155Keywords
- hep-ex
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Search for boosted diphoton resonances in the 10 to 70 GeV mass range using 138 fb−1 of 13 TeV pp collisions with the ATLAS detector
ATLAS Collaboration & Newman, P., 20 Jul 2023, In: JHEP. 2023, 42 p., 155.Research output: Contribution to journal › Article › peer-review
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