NA62 experiment

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The NA62 experiment (known as P-326 at the stage of proposal) is a particle physics experiment in the North Area of the SPS accelerator at CERN. The experiment was approved in February 2007. Data taking began in 2015, and the experiment is expected to become the first in the world to probe the decays of the charged kaon with probabilities down to 10−12. The experiment's spokesperson is Augusto Ceccucci. The collaboration involves 333 individuals from 30 institutions and 13 countries around the world.[1]

Goals[edit]

The experiment is designed to conduct precision tests of the Standard Model by studying rare decays of charged kaons. The principal goal, for which the design has been optimized, is the measurement of the rate of the ultra-rare decay K+ → π+ + ν + ν with a precision of 10%, by detecting about 100 decay candidates with a low background in two years of data taking. This will lead to the determination of the CKM matrix element |Vtd| with a precision better than 10%.[2] This element relates very accurately the likelihood that top quarks decay to down quarks. The Particle Data Group's 2008 Review of Particle Physics lists |Vtd| = 0.00874+0.00026
−0.00037
.[3]

Experimental Apparatus[edit]

In order to achieve the desired precision, the NA62 experiment requires a certain level of background rejection with respect to signal strength. Namely, high-resolution timing (to support a high-rate environment), kinematic rejection (involving the cutting on the square of the missing mass of the observed particles in the decay with respect to the incident kaon vector), particle identification, hermetic vetoing of photons out to large angles and of muons within the acceptance, and redundancy of information.[4]

Due to these necessities, the NA62 experiment has constructed a detector which is approximately 270 m in length. The components of the experiment are explained below.

Beam Line[edit]

The foundation of the NA62 experiment is observing the decays of kaons. In order to do this, the experiment receives two beams from the SPS,

The Primary Beam, called P42, is used for the production of the K+ beam. The 400 GeV/c proton beam is split into three branches and strikes three targets (T2, T4, and T6). This produces beams of secondary particles which are directed through the underground target tunnel (TCC2). At the exit of T4, the beam of transmitted protons passes through apertures in two vertically-motorized beam-dump/collimator modules, TAX 1 and TAX 2 for P42, in which holes of different apertures define the angular acceptance of the beam and hence allow the flux of protons to be selected over a wide range. In order to protect the components of the apparatus, a computer surveillance program allows the currents in the principle magnets along the P42 beam line to be monitored and to close Tax 2 in case of error.

A secondary beam line, K12HIKA+, is kaon beam line. This beam is designed to come from a high flux of 400GeV/c protons in the North Area High Intensity Facility. The target/beam tunnel, TCC8, and the cavern, ECN3, where the detectors of experiment NA48 have been installed, have a combined length of 270m. It is planned to reuse the existing target station, T10, (located 15m from the beginning of TCC8), and to install the secondary beam along the existing (straight) K12 beam line, of length 102m to the exit of the final collimator, which marks the beginning of the decay fiducial region and points to the NA48 detectors (notably the liquid krypton electro-magnetic calorimeter, LKR).

These beams lead to 4.5 MHz of kaon decays in the fiducial region with a ration of ~6% for K+ decays per Hadron Flux.[5]

GigaTracker (GTK)[edit]

Placed immediately before the decay region of the kaons, the GTK is designed to measure the time, direction, and momentum of all the beam tracks. The GTK is a spectrometer and can provide the measurement from the incoming 75 GeV/c kaon beam. The measurements of the GTK are used for decay selections and for background reduction.

The GTK is composed of three different stations labeled GTK1, GTK2, and GTK3 based on the order in which they are found relative to the beam path. They are mounted around four achromat magnets (which are used to deflect the beam). The entire system is placed along the beam line and is inside the vacuum tank.[6]

Straw Tracker[edit]

Once the kaons beam has gone through the decay region, the straw tracker will track the decay elements. The system measures the direction and the momentum of secondary charged particles which come from the decay region. This spectrometer is made with four chambers intersected with a high aperture dipole magnet. Each of the chambers consists of multiple straw tubes positioned to offer four views to give four coordinates. Out of 7168 straws in the whole system, only one was flawed. The leaking straw was sealed and the detector operated normally during the 2015 run.[7]

Data[edit]

The experiment has run multiple tests to ensure that the new detector components were working properly. The first physics run with a nearly complete detector took place in 2015. The data collected is being analysed and results are still preliminary. NA62 will begin data taking for the 2016 run in April.

As part of the experiment, several papers have been, and are in the process of being created. A list of published papers for the NA62 experiment can be found in the "See Also" section of this article.

See also[edit]

References[edit]

  1. ^ "Experiment's detail". greybook.cern.ch. Retrieved 2016-04-06. 
  2. ^ "Proposal to Measure the Rare Decay K+ → π +νν¯ at the CERN SPS" (PDF). 
  3. ^ C. Amsler; et al. (2008). "Review of Particles Physics" (PDF). Physics Letters B. 667: 1–1340. Bibcode:2008PhLB..667....1A. doi:10.1016/j.physletb.2008.07.018. 
  4. ^ "CERN-PH-NA62". na62.web.cern.ch. Retrieved 2016-04-06. 
  5. ^ "The K+ Beam Line" (PDF). CERN. 
  6. ^ "Gigatracker (GTK)". CERN
  7. ^ "2015 NA62 Status Report to the CERN SPSC". CERN

Further reading[edit]

External links[edit]