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Okun, Sov. J. Nucl. Phys. 1, 670 (1965) 21 3. T. D. Lee, L. Wolfenstein, Phys. Rev. B 138, 1490 (1965) 21 26 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. 18. 19. 20. 21. 22. 23. 24. 25. 4 Models of CP Violation J. Bernstein, G. Feinberg, T. D. Lee, Phys. Rev. B 139, 1650 (1965) 22 S. Barshay, Phys. Lett. 17, 78 (1965) 22 F. Salzman, G. Salzman, Phys. Lett. 15, 91 (1965) 22 B. Arbuzov, A. T. Filipov, Phys. Lett. 20, 537; Phys. Lett. 21, 771 (1965) 22 L. Wolfenstein, Nuovo Cimento 42, 17 (1966) 22 W.

In the third chamber, only the horizontal and vertical planes were instrumented. 2%. The space point resolution was ≈95 µm. 009% × p, where the momentum p is in GeV/c. 5 MeV. The magnetic spectrometer was followed by a scintillator hodoscope, composed of two planes segmented into horizontal and vertical strips. Fast logic combine the strip signals (arranged in four quadrants) for use in the first level of the π + π − trigger, with a time resolution of 200 ps. A liquid-krypton (LKr) calorimeter was used to reconstruct K → 2π 0 decays.

B 565, 3 (2000) 25 M. Ciuchini and G. Martinelli, Nucl. Phys. Proc. Suppl. 99B, 27 (2001) 25 S. Bertolini, M. O. Eeg, Phys. D 63, 056009 (2001) 25 E. Pallante, A. Pich, I. Scimemi, Nucl. Phys. 2) 0 − q|K0 where KL is the heavier state (h), from experiment. The lifetimes of the two eigenstates are very different. e. 600 times larger. This is due to the fact that the dominant CP-conserving decays are KS → 2π and KL → 3π, πeν, πµν, with a much smaller phasespace for the three-body decays. 2) can also be written |KS = |KL = 1 (|K1 + ε|K2 ) , 1 + |ε|2 1 (|K2 + ε|K1 ) .

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