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Measurement of the Two-photon Decay of the K [superscript Degree, Subscript L] Meson

Measurement of the Two-photon Decay of the K [superscript Degree, Subscript L] Meson PDF Author: John Andrew Todoroff
Publisher:
ISBN:
Category :
Languages : en
Pages : 298

Book Description


Measurement of the Two-photon Decay of the K [superscript Degree, Subscript L] Meson

Measurement of the Two-photon Decay of the K [superscript Degree, Subscript L] Meson PDF Author: John Andrew Todoroff
Publisher:
ISBN:
Category :
Languages : en
Pages : 298

Book Description


MEASUREMENT OF THE TWO-PHOTON DECAY OF THE K/sub L/$sup 0$ MESON.

MEASUREMENT OF THE TWO-PHOTON DECAY OF THE K/sub L/$sup 0$ MESON. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description


Measurement of the Two-Photon Decay of the Neutral K(l) Meson

Measurement of the Two-Photon Decay of the Neutral K(l) Meson PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description


MEASUREMENT OF THE TWO PHOTON DECAY OF THE K/sub L/° MESON.

MEASUREMENT OF THE TWO PHOTON DECAY OF THE K/sub L/° MESON. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description


Measurement of the Two Photon Decay of the [symbol for the Neutral K Meson].

Measurement of the Two Photon Decay of the [symbol for the Neutral K Meson]. PDF Author: James Eugene Enstrom
Publisher:
ISBN:
Category :
Languages : en
Pages : 256

Book Description


A Measurement of the K[MUsubscript 3] Decay Spectrum of the K[superscript O][subscript 2] Meson

A Measurement of the K[MUsubscript 3] Decay Spectrum of the K[superscript O][subscript 2] Meson PDF Author: Dwight William Carpenter
Publisher:
ISBN:
Category : Mesons
Languages : en
Pages : 154

Book Description


Observation of the Two-photon Decay of the Neutral-k2 Meson

Observation of the Two-photon Decay of the Neutral-k2 Meson PDF Author: L. Criegee
Publisher:
ISBN:
Category :
Languages : en
Pages : 10

Book Description
An arrangement of spark chambers and scintillation shower detectors was used to investigate the two-photon decay mode of the neutral K2 meson. Twenty-nine candidates were found for this decay mode. However, 12 plus or minus 7 of these events can originate from the neutral-K2 to 3 neutral-pion mode and the CP-violating neutral-K to 2 neutral-pion decay. Monte Carlo simulations indicate that 5 plus or minus of the 12 events are likely to originate from the 3 neutral-pion decays, leaving 7 plus or minus events which may be ascribed to 2 neutral-pion decays. The corresponding branching ratios are: Rate (neutral-K2 to gamma) (neutral-K to all modes) = (1.3 plus or minus 0.6) x 0.0001; Rate 9neutral-K2 to 2 neutral pion)/Rate (Neutral-K2 to all modes) = (1.2 + 1.5 or -1.2) x 0.001.

An Experimental Study of the Two-photon Decays of the Neutral K Mesons

An Experimental Study of the Two-photon Decays of the Neutral K Mesons PDF Author: Melvyn Jay Shochet
Publisher:
ISBN:
Category : Mesons
Languages : en
Pages :

Book Description


Measurement of the Branching Ratio for Eta-meson Decay Into a Neutral Pion and Two Photons

Measurement of the Branching Ratio for Eta-meson Decay Into a Neutral Pion and Two Photons PDF Author: Jason William Brudvik
Publisher:
ISBN: 9780549130093
Category :
Languages : en
Pages : 240

Book Description
This dissertation presents the results of a measurement of the branching ratio for the rare decay eta → pi0gammagamma. The experiment was carried out in the A2 hall of the Mainz Microtron facility at the Institut fur Kernphysik, on the campus of Johannes Gutenberg Universitat Mainz, in Mainz, Germany. The experiment used the Glasgow-Mainz Tagger, which is a recoil-electron spectrometer, to determine the energy of the incident photons. The principal detector is the Crystal Ball, a highly segmented multiphoton spectrometer covering nearly 4pi steradians surrounding the experimental target. There is also a forward detector, TAPS, which is a multiphoton spectrometer arranged as a downstream wall of detectors. Furthermore, our setup includes an instrument used to differentiate between charged and neutral particles called the Particle Identification Detector, and a liquid hydrogen target. The kinematic-fit technique was used to select the eta → pi 0gammagamma events. The major backgrounds, namely eta → 3pi0 and eta → gammagamma decay and 2pi 0 production were measured simultaneously. The result for the branching ratio is BR(eta → pi0gammagamma) = (2.0+/-0.7) x 10-4. This corresponds to a partial width of Gamma (eta → pi0gammagamma) = 0.26 +/- 0.10 eV. This result is somewhat smaller than the result of recent experiments, it is consistent with theoretical calculations based on Chiral Perturbation Theory.

Measurement of the B/s0 Lifetime in B/s0 --] K+ K- Decays

Measurement of the B/s0 Lifetime in B/s0 --] K+ K- Decays PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 218

Book Description
A method is presented to simultaneously separate the contributions to a sample of B{sub (s)}° 2!hh{sup {prime}-} decays, where h = [pi] or K, and measure the B meson lifetimes in the sample while correcting for the bias in the lifetime distributions due to the hadronic trigger at the CDF experiment. Using 1 fb−1 of data collected at CDF the B° lifetime is measured as [tau]{sub B°} = 1.558{sub -0.047}{sup +0.050}{sub stat} ± 0.028{sub syst} ps, in agreement with the world average measurement. The B{sub s}° lifetime in the B{sub s}° 2!KK− decay is measured as [tau]{sub B{sub s}° 2!K+K−} = 1.51{sub -0.11}{sup +0.13}{sub stat} ± 0.04{sub syst} ps. No difference is observed between the lifetime and other measurements of the average B{sub s}° lifetime or the lifetime of the light B{sub s}° mass eigenstate determined from B{sub s}° 2!J/[psi][phi] decays. With the assumptions that B{sub s}° 2!K+K− is 100% CP-even and that [tau]{sub B{sub s}°} = [tau]{sub B°} the width difference in the B{sub s}{sup 0} system is determined as [Delta][Lambda]{sup CP}/[Lambda] = 0.03{sub -0.15}{sup +0.17}{sub stat} ± 0.05{sub syst} using the current world average B{sup 0} lifetime. This is consistent with zero and with the current world average measurement.