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9.9. References 271<br />

• There are three possible causes of CP Violation in kaon decays: The first one<br />

is in the K1 and K2 mixing (mass mixing):<br />

KL = K2 + ɛK1<br />

�<br />

1+ | ɛ | 2 , KS = K1 − ɛK2<br />

� ,, (9.91)<br />

1+ | ɛ | 2<br />

where ɛ is a measure of the CP-violation. It is the KL and KS which have definite<br />

lifetimes. Experimentally, it is found that<br />

ɛ =(2.284 ± 0.014) × 10 −3 . (9.92)<br />

The second possibile cause of CP Violation is in the decay matrix element itself.<br />

A third one is an interference beween these two causes. The CP violation in the<br />

decay matrix element, measured by a parameter called ɛ ′ , occurs due to an admixture<br />

of isospin 2 to isospin 0 (or change of isospin by 3/2 vs. 1/2 in the decay), see<br />

Problem 9.46. The ratio of ɛ ′ to ɛ is of the order of 10 −3 . •<br />

9.9 References<br />

General references concerning invariance properties are given in Section 7.7.<br />

Discontinuous transformations and unitary and antiunitary operators are treated<br />

in detail in Messiah, Vol. II, Chapter XV. Some of the theoretical aspects of parity<br />

and time reversal are discussed in E. M. Henley, “Parity and Time Reversal Invariance<br />

in Nuclear <strong>Physics</strong>,” Annu. Rev. Nucl. Sci. 19, 367 (1969), and in Symetries<br />

and Fundamental Interactions in Nuclei, ed. W.C. Haxton and E.M. Henley, World<br />

Sci., Singapore, 1995. A detailed treatise is Robert G. Sachs, The <strong>Physics</strong> of Time<br />

Reversal Invariance, University of Chicago Press, Chicago, 1987. The theory and<br />

status of these symmetries are discussed in a number of reviews: E.N. Fortson and<br />

L.L. Lewis, “Atomic Parity Nonconservation Experiments,” Phys. Rep. 113, 289<br />

(1984); E.G. Adelberger and W. Haxton, “Parity Violation in the Nucleon–Nucleon<br />

Interaction,” Annu. Rev. Nucl. Part. Sci. 35, 501 (1985); E.M. Henley, “Status of<br />

Some Symmetries”, Prog. Part. Nucl. Phys., (A. Faessler, ed.) 20, 387 (1987); and<br />

Tests of Time Reversal Invariance, (N.R. Roberson, C.R. Gould, and J.D. Bowman,<br />

eds.) World Scientific, Teaneck, NJ, 1988.<br />

A popular account of CP and T violation is given by N. Fortson, P. Sandars,<br />

and S. Barr, Phys. Tod. 56, 33 (June 2003); see also R. G. Sachs, Science 176, 587<br />

(1972). CP violation in the K and B meson systems can be found on R. Kleinknecht,<br />

Experimental Clarification in the Neutral K Meson and B Meson Systems, Springer,<br />

NY, 2003; and in P. Bloch and L. Tauscher, Annu. Rev. Nucl. Part. Sci. 53, 123<br />

(2003); see also CP Violation in Particle, Nuclear and Astrophysics, ed.M.Beyer,<br />

Springer, New York, 2002; and I.I. Bigi and A.I. Sanda, CP Violation in Nature—A<br />

Status Report, Comm. Nucl. Part. Phys. 14, 149 (1985); I.B. Khriplovich, S.K.<br />

Lamoreaux, CP violation without strangeness: electric dipole moments of particles,<br />

atoms, and molecules, Berlin ; New York : Springer-Verlag, 1997.

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