22 research outputs found
CLIC simulations from the start of the linac to the interaction point
Simulations for linear colliders are traditionally performed separately for the different sub-systems, like damping ring, bunch compressor, linac, and beam delivery. The beam properties are usually passed from one sub-system to the other via bunch charge, RMS transverse emittances, RMS bunch length, average energy and RMS energy spread. It is implicitly assumed that the detailed 6D correlations in the beam distribution are not relevant for the achievable luminosity. However, it has recently been shown that those correlations can have a strong effect on the beam-beam interaction. We present first results on CLIC simulations that integrate linac, beam delivery, and beam-beam interaction. These integrated simulations also allow a better simulation of time-dependent effects, like ground perturbations and interference between several beam-based feedbacks
HyperCP: A high-rate spectrometer for the study of charged hyperon and kaon decays
The HyperCP experiment (Fermilab E871) was designed to search for rare
phenomena in the decays of charged strange particles, in particular CP
violation in and hyperon decays with a sensitivity of
. Intense charged secondary beams were produced by 800 GeV/c protons
and momentum-selected by a magnetic channel. Decay products were detected in a
large-acceptance, high-rate magnetic spectrometer using multiwire proportional
chambers, trigger hodoscopes, a hadronic calorimeter, and a muon-detection
system. Nearly identical acceptances and efficiencies for hyperons and
antihyperons decaying within an evacuated volume were achieved by reversing the
polarities of the channel and spectrometer magnets. A high-rate
data-acquisition system enabled 231 billion events to be recorded in twelve
months of data-taking.Comment: 107 pages, 45 Postscript figures, 14 tables, Elsevier LaTeX,
submitted to Nucl. Instrum. Meth.
Search for the Lepton-Number-Violating Decay
A sensitive search for the lepton-number-violating decay has been performed using a sample of hyperons
produced in 800 GeV/ -Cu collisions. We obtain at 90% confidence, improving on the best
previous limit by four orders of magnitude.Comment: 9 pages, 5 figures, to be published in Phys. Rev. Let
Evidence for the Decay Sigma+ -> p mu+ mu-
We report the first evidence for the decay Sigma+ -> p mu+ mu- from data
taken by the HyperCP experiment(E871) at Fermilab. Based on three observed
events, the branching ratio is B(Sigma+ -> p,mu+,mu-) = [8.6 +6.6,-5.4(stat)
+/-5.5(syst)] x 10**-8. The narrow range of dimuon masses may indicate that the
decay proceeds via a neutral intermediate state, Sigma+ -> p P0, P0 -> mu+ mu-,
with a P0 mass of 214.3 +/- 0.5 MeV/c**2 and branching ratio B(Sigma+ -> p P0;
P0 -> mu+ mu-) = [3.1 +2.4,-1.(stat) +/-1.5(syst)] x 10**-8.Comment: As published in PR
Measurement of the Alpha Asymmetry Parameter for the Omega- to Lambda K- Decay
We have measured the alpha parameter of the Omega- to Lambda K- decay using
data collected with the HyperCP spectrometer during the 1997 fixed-target run
at Fermilab. Analyzing a sample of 0.96 million Omega- to Lambda K^-, Lambda to
p pi- decays, we obtain alpha_Omega*alpha_Lambda =
[1.33+/-0.33(stat)+/-0.52(syst)] x 10^{-2}. With the accepted value of
alpha_Lambda, alpha_Omega is found to be [2.07+/-0.51(stat)+/-0.81(syst)] x
10^{-2}.Comment: 5 pages, 4 figures, to be appeared as a Rapid Communication in Phys.
Rev.
Measurement of αΩ in Ωâ â ÎÎâ Decays
The HyperCP experiment (E871) at Fermilab has collected the largest sample of hyperon decays in the world. With a data set of over a million Ωâ â ÎÎâ decays we have measured the product of αΩαΠfrom which we have extracted αΩ. This preliminary result indicates that αΩ is small, but nonâzero. Prospects for a test of CP symmetry by comparing the α parameters in Ωâ and ΩÌ+ decays will be discussed. © 2003 American Institute of PhysicsPeer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/87682/2/251_1.pd
CP Violation in Hyperon and Charged Kaon Decays
The primary purpose of the HyperCP experiment at Fermilab is to test CP in hyperon decays by comparing the decay distributions for Îâ (âcascadeâ) decays in the decay sequence: Îâ â Ïâ + Î0, Î0 â Ïâ + p, with those for the antiparticle ÎÌ+. In addition, we can test CP in charged kaon decays by comparing the slopes of the Dalitz plot for Î+ and Îâ decays. We are also looking at rare decay modes of charged kaons and hyperons, particularly those involving muons. In two runs in 1997 and 1999, we collected approx. 500 millon charged kaon decays, 2.5 billion Îâ and ÎÌ+ decays, and 19 million Ωâ and ΩÌ+ decays. This is the largest sample of fully reconstructed particle decays ever collected. © 2002 American Institute of PhysicsPeer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/87464/2/298_1.pd
High Statistics Search for the Theta+(1.54) Pentaquark State
We have searched for Theta+(1.54) -> K0,p decays using data from the 1999 run
of the HyperCP experiment at Fermilab. We see no evidence for a narrow peak in
the K0,p mass distribution near 1.54 GeV/c among 106,000 K0,p candidates, and
obtain an upper limit for the fraction of Theta+(1.54) to K0,p candidates of
<0.3% at 90% confidence.Comment: 4 pages, 4 figure
Search for CP Violation in Charged-Xi and Lambda Hyperon Decays
We have compared the proton and antiproton angular distributions in 117
million Xi-minus -> Lambda + pi-minus -> proton + pi-minus + pi-minus and 41
million anti-Xi-minus -> anti-Lamba + pi-plus -> antiproton + pi-plus + pi-plus
decays using a subset of the data from the HyperCP experiment (E871) at
Fermilab. We find no evidence of CP violation, with the direct-CP-violating
parameter .Comment: 4 pages, 4 figures, to be published in Phys. Rev. Let