- The H1 collaboration;
- Andreev, V;
- Arratia, M;
- Baghdasaryan, A;
- Baty, A;
- Begzsuren, K;
- Bolz, A;
- Boudry, V;
- Brandt, G;
- Britzger, D;
- Buniatyan, A;
- Bystritskaya, L;
- Campbell, AJ;
- Avila, KB Cantun;
- Cerny, K;
- Chekelian, V;
- Chen, Z;
- Contreras, JG;
- Cvach, J;
- Dainton, JB;
- Daum, K;
- Deshpande, A;
- Diaconu, C;
- Drees, A;
- Eckerlin, G;
- Egli, S;
- Elsen, E;
- Favart, L;
- Fedotov, A;
- Feltesse, J;
- Fleischer, M;
- Fomenko, A;
- Gal, C;
- Gayler, J;
- Goerlich, L;
- Gogitidze, N;
- Gouzevitch, M;
- Grab, C;
- Greenshaw, T;
- Grindhammer, G;
- Haidt, D;
- Henderson, RCW;
- Hessler, J;
- Hladký, J;
- Hoffmann, D;
- Horisberger, R;
- Hreus, T;
- Huber, F;
- Jacobs, PM;
- Jacquet, M;
- Janssen, T;
- Jung, AW;
- Katzy, J;
- Kiesling, C;
- Klein, M;
- Kleinwort, C;
- Klest, HT;
- Kogler, R;
- Kostka, P;
- Kretzschmar, J;
- Krücker, D;
- Krüger, K;
- Landon, MPJ;
- Lange, W;
- Laycock, P;
- Lee, SH;
- Levonian, S;
- Li, W;
- Lin, J;
- Lipka, K;
- List, B;
- List, J;
- Lobodzinski, B;
- Long, OR;
- Malinovski, E;
- Martyn, H-U;
- Maxfield, SJ;
- Mehta, A;
- Meyer, AB;
- Meyer, J;
- Mikocki, S;
- Mikuni, VM;
- Mondal, MM;
- Müller, K;
- Nachman, B;
- Naumann, Th;
- Newman, PR;
- Niebuhr, C;
- Nowak, G;
- Olsson, JE;
- Ozerov, D;
- Park, S;
- Pascaud, C;
- Patel, GD;
- Perez, E;
- Petrukhin, A;
- Picuric, I;
- Pitzl, D;
- Polifka, R;
- Preins, S;
- Radescu, V;
- Raicevic, N;
- Ravdandorj, T;
- Reimer, P;
- Rizvi, E;
- Robmann, P;
- Roosen, R;
- Rostovtsev, A;
- Rotaru, M;
- Sankey, DPC;
- Sauter, M;
- Sauvan, E;
- Schmitt, S;
- Schmookler, BA;
- Schnell, G;
- Schoeffel, L;
- Schöning, A;
- Sefkow, F;
- Shushkevich, S;
- Soloviev, Y;
- Sopicki, P;
- South, D;
- Specka, A;
- Steder, M;
- Stella, B;
- Straumann, U;
- Sun, C;
- Sykora, T;
- Thompson, PD;
- Acosta, F Torales;
- Traynor, D;
- Tseepeldorj, B;
- Tu, Z;
- Tustin, G;
- Valkárová, A;
- Vallée, C;
- Van Mechelen, P;
- Wegener, D;
- Wünsch, E;
- Žáček, J;
- Zhang, J;
- Zhang, Z;
- Žlebčík, R;
- Zohrabyan, H;
- Zomer, F
The radiation pattern within high energy quark- and gluon-initiated jets (jet
substructure) is used extensively as a precision probe of the strong force as
well as an environment for optimizing event generators with numerous
applications in high energy particle and nuclear physics. Looking at
electron-proton collisions is of particular interest as many of the
complications present at hadron colliders are absent. A detailed study of
modern jet substructure observables, jet angularities, in electron-proton
collisions is presented using data recorded using the H1 detector at HERA. The
measurement is unbinned and multi-dimensional, using machine learning to
correct for detector effects. All of the available reconstructed object
information of the respective jets is interpreted by a graph neural network,
achieving superior precision on a selected set of jet angularities. Training
these networks was enabled by the use of a large number of GPUs in the
Perlmutter supercomputer at Berkeley Lab. The particle jets are reconstructed
in the laboratory frame, using the $k_{\mathrm{T}}$ jet clustering algorithm.
Results are reported at high transverse momentum transfer $Q^2>150$ GeV${}^2$,
and inelasticity $0.2 < y < 0.7$. The analysis is also performed in sub-regions
of $Q^2$, thus probing scale dependencies of the substructure variables. The
data are compared with a variety of predictions and point towards possible
improvements of such models.