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Featured researches published by K. Kleinknecht.


Physics Letters B | 1990

Observation of the decay K(L) ---> pi0 gamma gamma

G. Barr; David Coward; D. Fournier; H. Wahl; L. Iconomidou-Fayard; L. Gatignon; D. Cundy; H.G. Sander; P. Calafiura; G. Zech; R. Heinz; H. Burkhardt; H. N. Nelson; M. Rost; W. Weihs; M. Calvetti; N. Doble; H. Rohrer; A. Nappi; G. Kesseler; A.C. Schaffer; D.J. Candlin; G. Quast; B. Panzer; R. Carosi; I. Mannelli; H. Blümer; K. Kleinknecht; P. Grafström; L. Bertanza

Abstract The decay mode K L → π 0 γγ has been observed with a signal of 21 events and an expected background of 1.5±0.9 events. A branching ratio for decays with invariant γγ masses above 280 MeV of (2.1±0.6)×10 −6 is calculated. This result is compared with the values estimated from theoretical models and has implications for the CP conserving contribution to K L → π 0 e + e − decay.


Physics Letters B | 1969

Interference between KL → π+π- and KS → π+π- behind a copper regenerator

H. Faissner; H. Foeth; A. Staude; K. Tittel; P. Darriulat; K. Kleinknecht; C. Rubbia; J. Sandweiss; M.I. Ferrero; C. Grosso

Abstract The interference between K L → π + π - and K S → π + π - behind a copper regenerator has been observed in a high statistics experiment. The modulus and the argument of the complex ratio ϱ ( p )/ η +- , where ϱ ( p ) is the regeneration amplitude and η +- = A ( K L → π + π - )/ A (K S → π + π - ) has been measured over the momentum interval from 2.0 GeV/ c to 6.0 GeV/ c . The phase of η +- as deduced from this measurement and from the optical model value of arg [ ϱ ( p )] is 49.3° ± 6.8°. The K L K S mass difference has been found to be Δm/ h = (0.555 ± 0.020) × 10 10 sec −1 .


Physics Letters B | 1968

On KL - KS regeneration in copper

A. Böhm; P. Darriulat; C. Grosso; V. Kaftanov; K. Kleinknecht; H.L. Lynch; C. Rubbia; H. Ticho; K. Tittel

Abstract The transmission regeneration amplitude after a thick copper block has been measured. The quantity ∣ƒ(0)− ƒ (0)∣ k varies from 20.0 ± 1.4 mb at 2.75 GeV/ c to 13.6 ± 1.2 mb at 7.25 GeV/ c . Results are in agreement with optical model calculations in which real and imaginary parts of the amplitudes for single nucleon scattering are determined from forward dispersion relations and total cross-sections.


Physics Letters B | 1970

A precision determination of the KL - KS mass difference

M. Cullen; P. Darriulat; J. Deutsch; H. Foeth; C. Grosso; M. Holder; K. Kleinknecht; E. Radermacher; C. Rubbia; D. Shambroom; M. Scire; A. Staude; K. Tittel

Abstract The K L - L S mass difference has been measured to be δm = (0.542 ± 0.006) × 10 10 sec −1 . Combined with K L - L S interference experiments in the π + π − decay channel, the experiment gives an improved value for arg (K L → π + π − /K S → π + π − ).


Physics Letters B | 1969

Pomeranchuk theorem and KL-KS regeneration

K. Kleinknecht

Abstract A sensitive test of the Pomeranchuk theorem can be performed by measuring the interference effects between KS → π+π− and KL → π+π− behind a regenerator at 20–60 GeV/c. This method gives not only the total cross-section differences between K0 and K 0 on nucleus, but also the difference of the real parts of the K0, K 0 forward scattering amplitudes.


Physics Letters B | 1970

Angular dependence of KLKS regenerative scattering for copper and lead nuclei at high energies

H. Foeth; M. Holder; E. Radermacher; A. Staude; P. Darriulat; J. Deutsch; K. Kleinknecht; C. Rubbia; K. Tittel; M.I. Ferrero; C. Grosso

Abstract Elastic and inelastic K L  S regenerative scattering on copper and lead nuclei have been observed up to a momentum transfer of 0.17 GeV/ c . The elastic differential cross-section is of a ”diffractive” type. It can be described successfully in terms of an optical model only assuming an appreciable neutron excess in the vicinity of the nuclear surface.


Physics Letters B | 1968

Observation of time-dependent KS and KL interference in the π+π− decay channel from an initial K0 state

A. Böhm; P. Darriulat; C. Grosso; V. Kaftanov; K. Kleinknecht; H.L. Lynch; C. Rubbia; H. Ticho; K. Tittel

Abstract The phase ϕ +− between the amplitudes K L → π + π − and K S → π + π − has been measured. The result is 46 0 ± ± 15 0 for a K L - K S mass difference Δm/ h = (0.526±0.20) × 10 10 s −1 , in good agreement with the “superweak model” of Wolfenstein which predicts ϕ +− SW = 42.6 0 ± 1.0 0 .


Physics Letters B | 1969

Search for coherent regeneration from electrons the K0 charge radius

H. Foeth; M. Holder; E. Radermacher; A. Staude; P. Darriulat; J. Deutsch; K. Kleinknecht; C. Rubbia; K. Tittel; M.I. Ferrero; A. Germak; C. Grosso

Abstract We have searched for coherent interactions of a long-lived neutral kaon with the electrons of lead and copper plates. Results are compatible with the absence of such effects. In terms of the kaon r.m.s. charge radius we find 〈 R 2 〉 = 0.22 − 0.22 + 0.20 fm .


Nuclear Physics | 1969

The phase difference between KL → π+π− and KS → π+π− decay amplitudes

A. Böhm; P. Darriulat; C. Grosso; V. Kaftanov; K. Kleinknecht; H.L. Lynch; C. Rubbia; H. Ticho; K. Tittel

The phase difference between the KL → π+π− and KS → π+π− decay amplitudes has been measured by observing the time dependence of the π+π− decay intensity from an initial K° (strangeness = +1) state. The phase difference φ/+− is found to be 41° ± 12° for a KL − KS mass difference Δm/h = 0.526 × 1010sec−. The error includes statistical and systematic uncertainties. The phase φ+− is strongly correlated to the value adopted for Δm/h. The present uncertainty on Δm/h increases our error on φ+− from 12° to 15°. The result is in agreement with the prediction of the ‘superweak model’ of CP violation.


Physics Letters B | 1968

The ΔS = ΔQ rule in the decay Ko → e± + ν + π

S. Bennett; David R. Nygren; Harry Saal; J. Sunderland; J. Steinberger; K. Kleinknecht

Abstract The magnitude of the charge asymmetry in Ke3 decay following a regenerator is analysed with the help of auxiliary experiments which determine the magnitude of the regeneration amplitude. It is found that (1 − |x| 2 ) |1 + x | 2 = (1.06±0.06) , where x is the ΔS − ΔQ violating amplitude relative to the ΔS = ΔQ conserving amplitude. The test is more sensitive than previous tests of ΔS ± ΔQ conservation, and in agreement with no violation.

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