CRT of the Belle II iTOP detector and search for the rare decay Bs ->Ks π0 in Belle data
by
DrTao LUO
(University of Pittsburgh)
→
Asia/Shanghai
A419 (IHEP)
A419
IHEP
Description
Abstract:
The Belle II experiment is being constructed at the KEK laboratory in Japan
and represents a substantial upgrade to both the Belle detector and the KEKB
accelerator. An important enhancement in the upgrade of the Belle detector is
the particle identification. Due to space constraints imposed on such a barrel
sub-detector update, a novel 8192-channel imaging Time of Propagation (iTOP)
detector is being built. In iTOP passage of hadrons through quartz panels
generates Cerenkov light, which, after multiple reflections, gets collected by
16-channel micro-channel plate photomultipliers (MCP-PMTs). Every
photomultiplier anode wire is inserted in an individual socket of a so-called front
board, which is parallel to the MCP-PMT back surface. The signals are routed to
the pads mounted on the back plane of the front board. Both position and timing
information are used to identify particle species. In order to examine the status
of the optics and the mirrors, the connection of bar-bar joint, and the
performance of the front-end-electronic and MCP-PMT, Cosmic-ray test (CRT) is
very essential. This talk will introduce the structure of the CRT test stand, the
DAQ of the CRT and the iTOP performance obtained from the CRT. Performance of
the more than 8k installed channels will also be presented.
Two-body charmless hadronic decays of B mesons are important not only to
understand the CP-violation and flavor mixing in the Standard Model (SM), but also
to probe the new physics (NP) sceneries beyond the SM. In the second part of this talk,
I will present the search for the rare decay process Bs-> Ks π0 in Belle data. In the SM,
this process proceeds mainly via a b->d “penguin” diagram, and it has not been
observed yet; there is no record of measurement in PDG. Belle is more sensitive to
this decay than LHCb because of the neutral particles in the final states. Discrepancy
of measured branching fractions from the theoretical calculation for this channel will
indicate BSM physics. An important feature of this analysis is that we are using
so-called Neural Network (NN) to select Ks candidates and to suppress the huge
continuum background. This method can increase the signal selection efficiency
greatly.