Abstract
The NA62 experiment at CERN aims at the very challenging task of measuring with 10% relative error the Branching Ratio of the ultra-rare decay of the K<sup>+</sup> into π<sup>+</sup> ν¯ν which is expected to occur only in about 8 out of 10<sup>11</sup> Kaon decays. This will be achieved by means of an intense hadron beam, an accurate kinematical reconstruction and a redundant veto system for identifying and suppressing all spurious events. Good resolution on the missing mass in the decay is achieved using a high-resolution beam tracker to measure the kaon momentum and with a spectrometer equipped with straw tubes operating in vacuum. Hermetic veto (up to 50 mrad) of the photon from π<sup>0</sup> decays is achieved with a combination of large angle veto (with a creative reuse of the old OPAL lead glass blocks), the NA48 liquid Krypton calorimeter and two small angle calorimeters to cover the angle down to zero. The identification of the muons and the consequent veto is performed by a fast hodoscope plane (used in the first level of the trigger to reduce the rate) and by a 17 meter, neon-filled RICH counter which is able to separate pions and muons in the momentum interval between 15 and 35 GeV. Particle identification in the beam (K<sup>+</sup> separation) is achieved with an H2 differential Cherenkov counter. The trigger for the experiment is based on a multilevel structure with a first level implemented in the readout boards and with the subsequent level done in the software. The aim is to reduce the 10MHz level zero rate to a few kHz sent to the CERN computing centre. Studies are underway to use GPU boards in some key point of the trigger system to improve the performance.<p> </p>
Highlights
Among the many flavour-changing neutral current rare K and B decays, the decays K → πνν play a key role in the search for new physics
The experiment will be housed in the CERN North Area High Intensity Facility (NAHIF) where the NA48 [3] was located, and it will use the same Super Proton Synchrotron (SPS) extraction line and target of NA48 to produce a 75 GeV/c (±1 %) positive hadron beam Two-body and three-body decay modes will be reduced by a factor of 104 by cutting on the missing mass of reconstructed candidates
Further rejection of Kμ 2,3,4 and Ke 2,3,4 background will be obtained with a ring-imaging Cherenkov counter (RICH), used to efficiently and non-destructively identify daughter pions and disentangle them from muons and electrons
Summary
Among the many flavour-changing neutral current rare K and B decays, the decays K → πνν play a key role in the search for new physics. The Standard Model (SM) branching ratio can be computed to an exceptionally high degree of precision: the theoretical comes mainly from the uncertainty on the CKM matrix elements, while the irreducible theoretical uncertainty amounts to less than 2.5 % for the neutral mode and 3.7 % for the charged one, and the latter could be further reduced by lattice calculation [1]. The only existing measurement of K+ → π+νν based on seven signal events collected by BNLAGS-E787(E949), which estimated a branching ratio of (1.73+−11..1055) · 1010 [2]. Only a measurement of the branching ratio with at least 10 % accuracy can be a significant test of new physics
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