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TPC track distortions IV: post tenebras lux

We present a comprehensive discussion and summary of static and dynamic track distortions in the HARP TPC in terms of physical origin, mathematical modelling and correction algorithms. `Static' distortions are constant with time, while `dynamic' distortions are distortions that occur only...

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Detalles Bibliográficos
Autores principales: Ammosov, V, Bolshakova, A, Boyko, I, Chelkov, G, Dedovitch, D, Dydak, F, Elagin, A, Gostkin, M, Guskov, A, Koreshev, V, Krumshtein, Z, Nefedov, Y, Nikolaev, K, Wotschack, J, Zhemchugov, A
Lenguaje:eng
Publicado: 2007
Materias:
Acceso en línea:http://cds.cern.ch/record/1143067
Descripción
Sumario:We present a comprehensive discussion and summary of static and dynamic track distortions in the HARP TPC in terms of physical origin, mathematical modelling and correction algorithms. `Static' distortions are constant with time, while `dynamic' distortions are distortions that occur only during the 400 ms long accelerator spill. The measurement of dynamic distortions, their mathematical modelling and the correction algorithms build on our understanding of static distortions. In the course of corroborating the validity of our static distortion corrections, their reliability and precision was further improved. Dynamic TPC distortions originate dominantly from the `stalactite' effect: a column of positive-ion charge starts growing at the begin of the accelerator spill, and continues growing with nearly constant velocity out from the sense-wire plane into the active TPC volume. However, the `stalactite' effect is not able to describe the distortions that are present already at the start of the spill and which have a sign opposite to the one of `stalactite' distortions. The 'margaritka' effect accounts for this: the radially outward oriented electric field generated by a deposit of positive ions on the insulating inner ring of the TPC readout chamber.