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Belle II Pixel Detector Commissioning and Operational Experience

Björn Spruck,Fernando Abudinen, Karlheinz Ackermann,Patrick Ahlburg,Mohammed Albalawi,Oscar Alonso,Laci Andricek,Rachid Ayad,Varghese Babu,Tadeas Bilka,Marca Boronat,Andrzej Bozek,Christian Camien, Allen Christopher Caldwell,Vladimir Chekelian,Bruno Deschamps,Angel Dieguez,Jochen Christian Dingfelder,Zdenek Dolezal,Daniel Esperante,Markus Fras,Ariane Frey,Juan Fuster,Miroslav Gabriel,Karsten Gadow,Uwe Gebauer,Thomas Gessler,Georgios Giakoustidis,Pablo Gomis,Luigi Li Gioi,Daniel Greenwald,Martin Heck,Tomasz Hemperek,Martin Hensel,Matthias Hoek,Stefan Huber,Jakub Kandra,Pjotr Kapusta,Christian Kiesling,Bartlomiej Kisielewski,David Kittlinger,Daniel Klose,Peter Kodys,Christian Koffmane,Igor Konorov,Silvia Krivokuca,Hans Krüger,Thomas Kuhr,Peter Kvasnicka,Carlos Lacasta llacer,Klemens Lautenbach,Jens Sören Lange,Ullrich Leis,Philipp Leitl,Dmytro Levit,Gerhard Liemann,Qingyuan Liu,Zhen’An Liu,Thomas Lück,Florian Lütticke, Lydia Macharski,Carlos Marinas,Sara Mccarney,Hans-Günther Moser,David Moya,Felix Müller,Carsten Niebuhr,Jelena Ninkovic,Botho Paschen,Stephan Paul,Ivan Peric,Frauke Poblotzki,Andrei Rabusov,Simon P. Reiter,Rainer Richter, Martin Ritter,Michael Ritzert, Javier Sanchez,Bianca Scavino,Gerhard Schaller,Martina Schnecke,Florian Schopper,Harrison Schreeck,Benjamin Schwenker,Reinhard Sedlmeyer,Concettina Sfienti,Frank Simon,Sebastian Skambraks,Yuri Soloviev, Slavomira Stefkova,Reimer Stever,Ulf Stolzenberg,Eva Tafelmayer,Maiko Takahashi,Ivan Vila Álvarez,Amparo Lopez Virto,Sven Vogt,Marcel Vos,Chunjie Wang,Norbert Wermes,Christian Wessel,Philipp Wieduwilt,Hendrik Windel,Hua Ye,Jingzhou Zhao

Proceedings of The 28th International Workshop on Vertex Detectors — PoS(Vertex2019)(2020)

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摘要
The Belle II experiment at the Super Flavour Factory SuperKEKB in Tsukuba, Japan, has started regular operation with its final detector setup in spring 2019. The Belle II vertexing system consists of four layers of double sided silicon strips (SVD) and two layers of DEPFET pixel sensors (PXD). These inner most pixel layers are arranged at radii of 14 mm and 22 mm around the beam pipe. The sensors with pixel sizes down to 50 $\mu$m $\times$ 55 $\mu$m are thinned down to 75 $\mu$m thickness to minimize multiple scattering. They are most crucial for reconstructing the secondary decay vertices of short lived B and D mesons with a precision of better than 15 microns. The high luminosity and harsh background conditions impose challenges on the operation of the detector close to the interaction point.
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