- Zwalinski, L;
- Zou, W;
- Zormpa, O;
- Zorbas, TG;
- Zoch, K;
- Zoccoli, A;
- Živković, L;
- Ziolkowski, M;
- Zinsser, J;
- Zimine, NI;
- Zhulanov, V;
- Zhukov, K;
- Zhuang, X;
- Zhu, Y;
- Zhu, Y;
- Zhu, J;
- Zhu, CG;
- Zhou, Y;
- Zhou, N;
- Zhou, H;
- Zhou, B;
- Zhong, D;
- Zheng, Z;
- Zheng, X;
- Zheng, K;
- Zheng, J;
- Zhemchugov, A;
- Zhao, Z;
- Zhao, Y;
- Zhao, T;
- Zhao, H;
- Zhang, Z;
- Zhang, Z;
- Zhang, Y;
- Zhang, Y;
- Zhang, Y;
- Zhang, X;
- Zhang, X;
- Zhang, T;
- Zhang, S;
- Zhang, S;
- Zhang, R;
- Zhang, P;
- Zhang, L;
- Zhang, K;
- Zhang, J;
- Zhang, J;
- Zhang, DF;
- Zhang, B;
- Zhai, M;
- Zerwas, D;
- Zerradi, S;
- Zenz, S;
- Ženiš, T;
- Zenin, O;
- Zenger, DT;
- Zeng, JC;
- Zeng, H;
- Zeitnitz, C;
- Zaplatilek, O;
- Zanzi, D;
- Zang, J;
- Saa, JAZ;
- Zambito, S;
- Zakharchuk, N;
- Zakareishvili, T;
- Zak, ZK;
- Zaid, E;
- Zabinski, B;
- Zaazoua, M;
- Yue, L;
- Yuan, R;
- Yuan, M;
- Yu, Y;
- Yu, C;
- Young, C;
- Young, CJS;
- Younas, S;
- Yorita, K;
- Yin, P;
- Yexley, MR;
- Yeo, BK;
- Yeletskikh, I;
- Yeh, Y;
- Ye, X;
- Ye, S;
- Ye, J;
- Ye, H;
- Ye, H;
- Yap, YC;
- Yao, WM;
- Yang, Z;
- Yang, Y;
- Yang, Y;
- Yang, X;
- Yang, X;
- Yang, T;
- Yang, S;
- Yang, HT;
- Yang, HJ
Clusters of topologically connected calorimeter cells around cells with large absolute signal-to-noise ratio (topo-clusters) are the basis for calorimeter signal reconstruction in the ATLAS experiment. Topological cell clustering has proven performant in LHC Runs 1 and 2. It is, however, susceptible to out-of-time pile-up of signals from soft collisions outside the 25 ns proton-bunch-crossing window associated with the event’s hard collision. To reduce this effect, a calorimeter-cell timing criterion was added to the signal-to-noise ratio requirement in the clustering algorithm. Multiple versions of this criterion were tested by reconstructing hadronic signals in simulated events and Run 2 ATLAS data. The preferred version is found to reduce the out-of-time pile-up jet multiplicity by ∼50% for jet pT∼20 GeV and by ∼80% for jet pT≳50 GeV, while not disrupting the reconstruction of hadronic signals of interest, and improving the jet energy resolution by up to 5% for 20