A search for signatures of a dark analog to quantum chromodynamics is performed. The analysis targets long-lived dark mesons that decay into standard-model particles, with a high branching fraction of the dark mesons decaying into muons. The dark mesons are formed by the hadronisation of dark partons, which are produced by a decay of the Higgs boson. The search is performed using a data set corresponding to an integrated luminosity of $41.6~\textrm{fb}^{-1}$, which was collected in proton-proton collisions at $\sqrt{s}=13~\textrm{TeV}$ by the CMS experiment at the CERN LHC in 2018 using non-prompt muon triggers. The search is based on resonant muon pair signatures. Machine-learning techniques are employed in the analysis, utilising boosted decision trees to discriminate between signal and background. No significant excess is observed above the standard model expectation. Upper limits on the branching fraction of the Higgs boson decaying to dark partons are determined to be as low as $10^{-4}$ at 95% confidence level, surpassing and extending the existing limits on models with dark $\tilde{\omega}$ mesons for mean proper decay lengths of less than $500~\textrm{mm}$ and for $\tilde{\omega}$ masses down to $0.3~\textrm{GeV}$. First limits are set for extended dark-shower models with two dark flavours that contain dark photons, probing their masses down to $0.33~\textrm{GeV}$.
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Dimuon invariant mass distributions in mass windows around $0.67~\textrm{GeV}$ in the single-vertex category with $1~\textrm{cm}<l_{xy}<10~\textrm{cm}$ and $\textrm{pointing angle}<0.2$. The background...
Scenario B1 dimuon mass distribution at 1.33 GeV
Figure 7b
10.17182/hepdata.165888.v1/t2
Dimuon invariant mass distributions in mass windows around $1.33~\textrm{GeV}$ in the single-vertex category with $1~\textrm{cm}<l_{xy}<10~\textrm{cm}$ and $\textrm{pointing angle}<0.2$. The background...
Vector portal limits, $m_{\tilde{\omega}}=2$GeV
Figure 8a
10.17182/hepdata.165888.v1/t3
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson $c\tau$ for $m_{\tilde{\omega}}=2~\textrm{GeV}$...
Vector portal limits, $m_{\tilde{\omega}}=5$GeV
Figure 8b
10.17182/hepdata.165888.v1/t4
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson $c\tau$ for $m_{\tilde{\omega}}=5~\textrm{GeV}$...
Vector portal limits, $m_{\tilde{\omega}}=15$GeV
Figure 8c
10.17182/hepdata.165888.v1/t5
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson $c\tau$ for $m_{\tilde{\omega}}=15~\textrm{GeV}$...
Vector portal limits, $m_{\tilde{\omega}}=20$GeV
Figure 8d
10.17182/hepdata.165888.v1/t6
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson $c\tau$ for $m_{\tilde{\omega}}=20~\textrm{GeV}$...
Scenario A limits, $m_{A'}=0.33$ GeV
Figure 9a
10.17182/hepdata.165888.v1/t7
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\textrm{A}'$ $c\tau$ for $m_{\tilde{\pi}_{3}}=1~\textrm{GeV}$ and...
Scenario A limits, $m_{A'}=0.4$ GeV
Figure 9b
10.17182/hepdata.165888.v1/t8
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\textrm{A}'$ $c\tau$ for $m_{\tilde{\pi}_{3}}=4~\textrm{GeV}$ and...
Scenario A limits, $m_{A'}=0.67$ GeV
Figure 9c
10.17182/hepdata.165888.v1/t9
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\textrm{A}'$ $c\tau$ for $m_{\tilde{\pi}_{3}}=2~\textrm{GeV}$ and...
Scenario A limits, $m_{A'}=1.33$ GeV
Figure 9d
10.17182/hepdata.165888.v1/t10
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\textrm{A}'$ $c\tau$ for $m_{\tilde{\pi}_{3}}=4~\textrm{GeV}$ and...
Scenario B1 limits, $m_{A'}=0.33$ GeV
Figure 10a
10.17182/hepdata.165888.v1/t11
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\pi}_{3}$ meson $c\tau$ for $m_{\tilde{\pi}_{3}}=1~\textrm{GeV}$...
Scenario B1 limits, $m_{A'}=0.4$ GeV
Figure 10b
10.17182/hepdata.165888.v1/t12
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\pi}_{3}$ meson $c\tau$ for $m_{\tilde{\pi}_{3}}=2~\textrm{GeV}$...
Scenario B1 limits, $m_{A'}=0.67$ GeV
Figure 10c
10.17182/hepdata.165888.v1/t13
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\pi}_{3}$ meson $c\tau$ for $m_{\tilde{\pi}_{3}}=2~\textrm{GeV}$...
Scenario B1 limits, $m_{A'}=1.33$ GeV
Figure 10d
10.17182/hepdata.165888.v1/t14
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\pi}_{3}$ meson $c\tau$ for $m_{\tilde{\pi}_{3}}=4~\textrm{GeV}$...
Vector portal limits, $c\tau=10$mm
Figure 11a
10.17182/hepdata.165888.v1/t15
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson mass for $c\tau=10~\textrm{mm}$...
Vector portal limits, $c\tau=100$mm
Figure 11b
10.17182/hepdata.165888.v1/t16
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson mass for $c\tau=100~\textrm{mm}$...
Scenario A limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$, $c\tau=10$mm
Figure 12a
10.17182/hepdata.165888.v1/t17
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario A,...
Scenario A limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$, $c\tau=10$mm
Figure 12b
10.17182/hepdata.165888.v1/t18
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario A,...
Scenario A limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$, $c\tau=100$mm
Figure 12c
10.17182/hepdata.165888.v1/t19
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario A,...
Scenario A limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$, $c\tau=100$mm
Figure 12d
10.17182/hepdata.165888.v1/t20
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario A,...
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario B1,...
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario B1,...
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario B1,...
Upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\to\psi\overline{\psi}\right)$ as a function of the $\mathrm{A}'$ mass in Scenario B1,...
Vector portal 2D limits
Figure 14
10.17182/hepdata.165888.v1/t25
Observed upper limits at 95% CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as a function of the $\tilde{\omega}$ meson mass and...
Scenario A 2D limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$
Figure 15a
10.17182/hepdata.165888.v1/t26
Observed upper limits at $95\%$ CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as functions of the $\textrm{A}'$ mass and $c\tau$ for...
Scenario A 2D limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$
Figure 15b
10.17182/hepdata.165888.v1/t27
Observed upper limits at $95\%$ CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as functions of the $\textrm{A}'$ mass and $c\tau$ for...
Observed upper limits at $95\%$ CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as functions of the $\textrm{A}'$ mass and $c\tau$ for...
Observed upper limits at $95\%$ CL on the branching fraction $\mathcal{B}\left(\textrm{H}\rightarrow\psi\overline{\psi}\right)$ as functions of the $\textrm{A}'$ mass and $c\tau$ for...
Vector portal cutflow efficiencies
Example location
10.17182/hepdata.165888.v1/t30
Cutflow efficiencies for representative signal model points in the vector portal.
Scenario A cutflow efficiencies
Example location
10.17182/hepdata.165888.v1/t31
Cutflow efficiencies for representative signal model points in Scenario A.
Scenario B1 cutflow efficiencies
Example location
10.17182/hepdata.165888.v1/t32
Cutflow efficiencies for representative signal model points in Scenario B1.
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Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV. HEPData (collection).
https://doi.org/10.17182/hepdata.165888
or, if you prefer, a specific version of the
record:
CMS
Collaboration
(2025).
Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV (Version 1). HEPData (collection).
https://doi.org/10.17182/hepdata.165888.v1
You can also cite the 32 data
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CMS
Collaboration
(2025).
“Scenario A dimuon mass distribution at 0.67 GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t1
CMS
Collaboration
(2025).
“Scenario B1 dimuon mass distribution at 1.33 GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t2
CMS
Collaboration
(2025).
“Vector portal limits, $m_{\tilde{\omega}}=2$GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t3
CMS
Collaboration
(2025).
“Vector portal limits, $m_{\tilde{\omega}}=5$GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t4
CMS
Collaboration
(2025).
“Vector portal limits, $m_{\tilde{\omega}}=15$GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t5
CMS
Collaboration
(2025).
“Vector portal limits, $m_{\tilde{\omega}}=20$GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t6
CMS
Collaboration
(2025).
“Scenario A limits, $m_{A'}=0.33$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t7
CMS
Collaboration
(2025).
“Scenario A limits, $m_{A'}=0.4$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t8
CMS
Collaboration
(2025).
“Scenario A limits, $m_{A'}=0.67$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t9
CMS
Collaboration
(2025).
“Scenario A limits, $m_{A'}=1.33$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t10
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{A'}=0.33$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t11
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{A'}=0.4$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t12
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{A'}=0.67$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t13
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{A'}=1.33$ GeV” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t14
CMS
Collaboration
(2025).
“Vector portal limits, $c\tau=10$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t15
CMS
Collaboration
(2025).
“Vector portal limits, $c\tau=100$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t16
CMS
Collaboration
(2025).
“Scenario A limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$, $c\tau=10$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t17
CMS
Collaboration
(2025).
“Scenario A limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$, $c\tau=10$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t18
CMS
Collaboration
(2025).
“Scenario A limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$, $c\tau=100$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t19
CMS
Collaboration
(2025).
“Scenario A limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$, $c\tau=100$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t20
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$, $c\tau=10$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t21
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$, $c\tau=10$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t22
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$,$c\tau=100$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t23
CMS
Collaboration
(2025).
“Scenario B1 limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$,$c\tau=100$mm” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t24
CMS
Collaboration
(2025).
“Vector portal 2D limits” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t25
CMS
Collaboration
(2025).
“Scenario A 2D limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t26
CMS
Collaboration
(2025).
“Scenario A 2D limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t27
CMS
Collaboration
(2025).
“Scenario B1 2D limits, $m_{\tilde{\pi}_{3}}=10m_{A'}$” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t28
CMS
Collaboration
(2025).
“Scenario B1 2D limits, $m_{\tilde{\pi}_{3}}=3m_{A'}$” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t29
CMS
Collaboration
(2025).
“Vector portal cutflow efficiencies” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t30
CMS
Collaboration
(2025).
“Scenario A cutflow efficiencies” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t31
CMS
Collaboration
(2025).
“Scenario B1 cutflow efficiencies” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.165888.v1/t32
Additional resources
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CMS
Collaboration
(2025).
“pythia_cards.tar.gz” of “Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV” (Version 1). HEPData (other).
https://doi.org/10.17182/hepdata.165888.v1/r1
When using this data, please cite the original publication:
CMS
Collaboration
(2025).
Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $\sqrt{s}$ = 13 TeV. CMS-EXO-24-008.
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