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Wang, B.; Abudinen, F.; Ackermann, K.; Ahlburg, P.; Albalawi, M.; Alonso, O.; Andricek, L.; Ayad, R.; Babu, V.; Baur, A.; Bernlochner, F.; Bilka, T.; Bolz, A.; Bozek, A.; Camien, C.; Caldwell, A.; Cao, L.; Chekelian, V.; Dieguez, A.; Dingfelder, J.; Dolezal, Z.; Fras, M.; Frey, A.; Gabriel, M.; Gadow, K.; Gessler, T.; Giakoustidis, G.; Gioi, L.; Greenwald, D.; Heck, M.; Hensel, M.; Hoek, M.; Huber, S.; Kandra, J.; Kapusta, P.; Karl, R.; Kehl, J.; Kiesling, C.; Kisielewski, B.; Kittlinger, D.; Klose, D.; Kodys, P.; Koffmane, C.; Konorov, I.; Krivokuca, S.; Kuhr, T.; Kurz, S.; Kvasnicka, P.; Lange, J. S.; Lautenbach, K.; Leis, U.; Leitl, P.; Levit, D.; Liemann, G.; Liu, Q.; Liu, Z.; Lueck, T.; Marinas, C.; Mccarney, S.; Moser, H. G.; Moya, D.; Mueller, F. J.; Mueller, F.; Niebuhr, C.; Ninkovic, J.; Paschen, B.; Paul, S.; Peric, I.; Pitzl, D.; Rabusov, A.; Reif, M.; Reiter, S. P.; Richter, R.; Ritter, M.; Ritzert, M.; Sanchez, J. G.; Scavino, B.; Schaller, G.; Schmitz, J.; Schnecke, M.; Schopper, F.; Schreeck, H.; Schwenker, B.; Schwickardi, M.; Sedlmeyer, R.; Sfienti, C.; Simon, F.; Skambraks, S.; Skorupa, J.; Soloviev, Y.; Spruck, B.; Stefkova, S.; Stever, R.; Tafelmayer, E.; Takahashi, M.; Vila, I.; Virto, A. L.; Vogt, S.; Wang, C.; Wieduwilt, P.; Windel, H.; Ye, H.; Zhao, J. and Zlebcik, R. (2022): Operational experience of the Belle II pixel detector. In: Nuclear Instruments & Methods in Physics Research Section A-Accelerators Spectrometers Detectors and Associated Equipment, Vol. 1032, 166631

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The Belle II experiment at the SuperKEKB accelerator has started its physics data taking with the full detector setup in March 2019. It aims to collect 40 times more e+e- collision data compared with its predecessor Belle experiment. The Belle II pixel detector (PXD) is based on the Depleted P-channel Field Effect Transistor (DEPFET) technology. The PXD plays an important role in the tracking and vertexing of the Belle II detector. Its two layers are arranged at radii of 14 mm and 22 mm around the interaction point. The sensors are thinned down to 75 mu m to minimize multiple scattering, and each module has interconnects and ASICs integrated on the sensor with silicon frames for mechanical support. PXD showed good performance during data taking. It also faces several operational challenges due to the high background level from the SuperKEKB accelerator, such as the damage from beam loss events, the drift in the HV working point due to radiation effect, and the impact of the high background.

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