Physics:CP violation
Beyond the Standard Model 

Standard Model 
In particle physics, CP violation is a violation of CPsymmetry (or charge conjugation parity symmetry): the combination of Csymmetry (charge symmetry) and Psymmetry (parity symmetry). CPsymmetry states that the laws of physics should be the same if a particle is interchanged with its antiparticle (C symmetry) while its spatial coordinates are inverted ("mirror" or P symmetry). The discovery of CP violation in 1964 in the decays of neutral kaons resulted in the Nobel Prize in Physics in 1980 for its discoverers James Cronin and Val Fitch.
It plays an important role both in the attempts of cosmology to explain the dominance of matter over antimatter in the present universe, and in the study of weak interactions in particle physics.
Overview
Until the 1950s, parity conservation was believed to be one of the fundamental geometric conservation laws (along with conservation of energy and conservation of momentum). After the discovery of parity violation in 1956, CPsymmetry was proposed to restore order. However, while the strong interaction and electromagnetic interaction seem to be invariant under the combined CP transformation operation, further experiments showed that this symmetry is slightly violated during certain types of weak decay.
Only a weaker version of the symmetry could be preserved by physical phenomena, which was CPT symmetry. Besides C and P, there is a third operation, time reversal T, which corresponds to reversal of motion. Invariance under time reversal implies that whenever a motion is allowed by the laws of physics, the reversed motion is also an allowed one and occurs at the same rate forwards and backwards.
The combination of CPT is thought to constitute an exact symmetry of all types of fundamental interactions. Because of the CPT symmetry, a violation of the CPsymmetry is equivalent to a violation of the T symmetry. CP violation implied nonconservation of T, provided that the longheld CPT theorem was valid. In this theorem, regarded as one of the basic principles of quantum field theory, charge conjugation, parity, and time reversal are applied together. Direct observation of the time reversal symmetry violation without any assumption of CPT theorem was done in 1998 by two groups, CPLEAR and KTeV collaborations, at CERN and Fermilab, respectively.^{[1]} Already in 1970 Klaus Schubert observed T violation independent of assuming CPT symmetry by using the BellSteinberger unitarity relation.^{[2]}
History
Psymmetry
The idea behind parity symmetry was that the equations of particle physics are invariant under mirror inversion. This led to the prediction that the mirror image of a reaction (such as a chemical reaction or radioactive decay) occurs at the same rate as the original reaction. However, in 1956 a careful critical review of the existing experimental data by theoretical physicists TsungDao Lee and ChenNing Yang revealed that while parity conservation had been verified in decays by the strong or electromagnetic interactions, it was untested in the weak interaction.^{[3]} They proposed several possible direct experimental tests.
The first test based on beta decay of cobalt60 nuclei was carried out in 1956 by a group led by ChienShiung Wu, and demonstrated conclusively that weak interactions violate the P symmetry or, as the analogy goes, some reactions did not occur as often as their mirror image.^{[4]} However, parity symmetry still appears to be valid for all reactions involving electromagnetism and strong interactions.
CPsymmetry
Overall, the symmetry of a quantum mechanical system can be restored if another approximate symmetry S can be found such that the combined symmetry PS remains unbroken. This rather subtle point about the structure of Hilbert space was realized shortly after the discovery of P violation, and it was proposed that charge conjugation, C, which transforms a particle into its antiparticle, was the suitable symmetry to restore order.
In 1956 Reinhard Oehme in a letter to Yang and shortly after, Ioffe, Okun and Rudik showed that the parity violation meant that charge conjugation invariance must also be violated in weak decays.^{[5]}
Charge violation was confirmed in the Wu experiment and in experiments performed by Valentine Telegdi and Jerome Friedman and Garwin and Lederman who observed parity nonconservation in pion and muon decay and found that C is also violated. Charge violation was more explicitly shown in experiments done by John Riley Holt at the University of Liverpool.^{[6]}^{[7]}^{[8]}
Oehme then wrote up a paper with Lee and Yang in which they discussed the interplay of noninvariance under P, C and T. The same result was also independently obtained by B.L. Ioffe, Okun and A.P. Rudik. Both groups also discussed possible CP violations in neutral kaon decays.^{[5]}^{[9]}
Lev Landau proposed in 1957 CPsymmetry,^{[10]} often called just CP as the true symmetry between matter and antimatter. CPsymmetry is the product of two transformations: C for charge conjugation and P for parity. In other words, a process in which all particles are exchanged with their antiparticles was assumed to be equivalent to the mirror image of the original proces and so the combined CP symmetry would be conserved in the weak interaction.
In 1962, a group of experimentalists at Dubna, on Okun's insistence, unsuccessfully searched for CPviolating kaon decay.^{[11]}
Experimental status
Indirect CP violation
In 1964, James Cronin, Val Fitch and coworkers provided clear evidence from kaon decay that CPsymmetry could be broken.^{[12]} This work^{[13]} won them the 1980 Nobel Prize. This discovery showed that weak interactions violate not only the chargeconjugation symmetry C between particles and antiparticles and the P or parity, but also their combination. The discovery shocked particle physics and opened the door to questions still at the core of particle physics and of cosmology today. The lack of an exact CPsymmetry, but also the fact that it is so close to a symmetry, introduced a great puzzle.
The kind of CP violation discovered in 1964 was linked to the fact that neutral kaons can transform into their antiparticles (in which each quark is replaced with the other's antiquark) and vice versa, but such transformation does not occur with exactly the same probability in both directions; this is called indirect CP violation.
Direct CP violation
Despite many searches, no other manifestation of CP violation was discovered until the 1990s, when the NA31 experiment at CERN suggested evidence for CP violation in the decay process of the very same neutral kaons (direct CP violation). The observation was somewhat controversial, and final proof for it came in 1999 from the KTeV experiment at Fermilab^{[14]} and the NA48 experiment at CERN.^{[15]}
Starting in 2001, a new generation of experiments, including the BaBar experiment at the Stanford Linear Accelerator Center (SLAC)^{[16]} and the Belle Experiment at the High Energy Accelerator Research Organisation (KEK)^{[17]} in Japan, observed direct CP violation in a different system, namely in decays of the B mesons.^{[18]} A large number of CP violation processes in B meson decays have now been discovered. Before these "Bfactory" experiments, there was a logical possibility that all CP violation was confined to kaon physics. However, this raised the question of why CP violation did not extend to the strong force, and furthermore, why this was not predicted by the unextended Standard Model, despite the model's accuracy for "normal" phenomena.
In 2011, a hint of CP violation in decays of neutral D mesons was reported by the LHCb experiment at CERN using 0.6 fb^{−1} of Run 1 data.^{[19]} However, the same measurement using the full 3.0 fb^{−1} Run 1 sample was consistent with CP symmetry.^{[20]}
In 2013 LHCb announced discovery of CP violation in strange B meson decays.^{[21]}
In March 2019, LHCb announced discovery of CP violation in charmed [math]\displaystyle{ D^{0} }[/math] decays with a deviation from zero of 5.3 standard deviations.^{[22]}
In 2020, the T2K Collaboration reported some indications of CP violation in leptons for the first time.^{[23]} In this experiment, beams of muon neutrinos (_{}ν_{μ}) and muon antineutrinos (_{}ν_{μ}) were alternately produced by an accelerator. By the time they got to the detector, a significantly higher proportion of electron neutrinos (_{}ν_{e}) were detected from the _{}ν_{μ} beams, than electron antineutrinos (_{}ν_{e}) were from the _{}ν_{μ} beams. The results were not yet precise enough to determine the size of the CP violation, relative to that seen in quarks. In addition, another similar experiment, NOvA sees no evidence of CP violation in neutrino oscillations^{[24]} and is in slight tension with T2K.^{[25]}^{[26]}
CP violation in the Standard Model
"Direct" CP violation is allowed in the Standard Model if a complex phase appears in the CKM matrix describing quark mixing, or the PMNS matrix describing neutrino mixing. A necessary condition for the appearance of the complex phase is the presence of at least three generations of quarks. If fewer generations are present, the complex phase parameter can be absorbed into redefinitions of the quark fields. A popular rephasing invariant whose vanishing signals absence of CP violation and occurs in most CP violating amplitudes is the Jarlskog invariant,
 [math]\displaystyle{ \, J = c_{12}c_{13}^2 c_{23}s_{12}s_{13}s_{23}\sin \delta \approx 3 \times 10^{5}\,. }[/math]
The reason why such a complex phase causes CP violation is not immediately obvious, but can be seen as follows. Consider any given particles (or sets of particles) [math]\displaystyle{ a }[/math] and [math]\displaystyle{ b }[/math], and their antiparticles [math]\displaystyle{ \bar{a} }[/math] and [math]\displaystyle{ \bar{b} }[/math]. Now consider the processes [math]\displaystyle{ a \rightarrow b }[/math] and the corresponding antiparticle process [math]\displaystyle{ \bar{a} \rightarrow \bar{b} }[/math], and denote their amplitudes [math]\displaystyle{ M }[/math] and [math]\displaystyle{ \bar{M} }[/math] respectively. Before CP violation, these terms must be the same complex number. We can separate the magnitude and phase by writing [math]\displaystyle{ M=Me^{i\theta} }[/math]. If a phase term is introduced from (e.g.) the CKM matrix, denote it [math]\displaystyle{ e^{i\phi} }[/math]. Note that [math]\displaystyle{ \bar{M} }[/math] contains the conjugate matrix to [math]\displaystyle{ M }[/math], so it picks up a phase term [math]\displaystyle{ e^{i\phi} }[/math].
Now the formula becomes:
 [math]\displaystyle{ M=Me^{i\theta}e^{i\phi} }[/math]
 [math]\displaystyle{ \bar{M}=Me^{i\theta}e^{i\phi} }[/math]
Physically measurable reaction rates are proportional to [math]\displaystyle{ M^{2} }[/math], thus so far nothing is different. However, consider that there are two different routes: [math]\displaystyle{ a \overset{1}{\longrightarrow} b }[/math] and [math]\displaystyle{ a \overset{2}{\longrightarrow} b }[/math] or equivalently, two unrelated intermediate states: [math]\displaystyle{ a \rightarrow 1\rightarrow b }[/math] and [math]\displaystyle{ a \rightarrow 2\rightarrow b }[/math]. Now we have:
 [math]\displaystyle{ M = M_{1} e^{i\theta_{1}} e^{i\phi_{1}} + M_{2} e^{i\theta_{2}} e^{i\phi_{2}} }[/math]
 [math]\displaystyle{ \bar{M} = M_{1} e^{i\theta_{1}} e^{i\phi_{1}} + M_{2} e^{i\theta_{2}} e^{i\phi_{2}} }[/math]
Some further calculation gives:
 [math]\displaystyle{ M^{2}  \bar{M}^{2} = 4 M_{1} M_{2} \sin(\theta_{1}  \theta_{2})\sin(\phi_{1}  \phi_{2}) }[/math]
Thus, we see that a complex phase gives rise to processes that proceed at different rates for particles and antiparticles, and CP is violated.
From the theoretical end, the CKM matrix is defined as V_{CKM} = U_{u}. U﹢d, where U_{u} and U_{d} are unitary transformation matrices which diagonalize the fermion mass matrices M_{u} and M_{d}, respectively.
Thus, there are two necessary conditions for getting a complex CKM matrix:
 At least one of U_{u} and U_{d} is complex, or the CKM matrix will be purely real.
 If both of them are complex, U_{u} and U_{d} mustn’t be the same, i.e., U_{u} ≠ U_{d}, or CKM matrix will be an identity matrix which is also purely real.
Strong CP problem
Unsolved problem in physics: Why is the strong nuclear interaction force CPinvariant? (more unsolved problems in physics)

There is no experimentally known violation of the CPsymmetry in quantum chromodynamics. As there is no known reason for it to be conserved in QCD specifically, this is a "fine tuning" problem known as the strong CP problem.
QCD does not violate the CPsymmetry as easily as the electroweak theory; unlike the electroweak theory in which the gauge fields couple to chiral currents constructed from the fermionic fields, the gluons couple to vector currents. Experiments do not indicate any CP violation in the QCD sector. For example, a generic CP violation in the strongly interacting sector would create the electric dipole moment of the neutron which would be comparable to 10^{−18} e·m while the experimental upper bound is roughly one trillionth that size.
This is a problem because at the end, there are natural terms in the QCD Lagrangian that are able to break the CPsymmetry.
 [math]\displaystyle{ {\mathcal L} = \frac{1}{4} F_{\mu\nu}F^{\mu\nu}\frac{n_f g^2\theta}{32\pi^2} F_{\mu\nu}\tilde F^{\mu\nu}+\bar \psi(i\gamma^\mu D_\mu  m e^{i\theta'\gamma_5})\psi }[/math]
For a nonzero choice of the θ angle and the chiral phase of the quark mass θ′ one expects the CPsymmetry to be violated. One usually assumes that the chiral quark mass phase can be converted to a contribution to the total effective [math]\displaystyle{ \scriptstyle{\tilde\theta} }[/math] angle, but it remains to be explained why this angle is extremely small instead of being of order one; the particular value of the θ angle that must be very close to zero (in this case) is an example of a finetuning problem in physics, and is typically solved by physics beyond the Standard Model.
There are several proposed solutions to solve the strong CP problem. The most wellknown is Peccei–Quinn theory, involving new scalar particles called axions. A newer, more radical approach not requiring the axion is a theory involving two time dimensions first proposed in 1998 by Bars, Deliduman, and Andreev.^{[27]}
Matter–antimatter imbalance
Unsolved problem in physics: Why does the universe have so much more matter than antimatter? (more unsolved problems in physics)

The universe is made chiefly of matter, rather than consisting of equal parts of matter and antimatter as might be expected. It can be demonstrated that, to create an imbalance in matter and antimatter from an initial condition of balance, the Sakharov conditions must be satisfied, one of which is the existence of CP violation during the extreme conditions of the first seconds after the Big Bang. Explanations which do not involve CP violation are less plausible, since they rely on the assumption that the matter–antimatter imbalance was present at the beginning, or on other admittedly exotic assumptions.
The Big Bang should have produced equal amounts of matter and antimatter if CPsymmetry was preserved; as such, there should have been total cancellation of both—protons should have cancelled with antiprotons, electrons with positrons, neutrons with antineutrons, and so on. This would have resulted in a sea of radiation in the universe with no matter. Since this is not the case, after the Big Bang, physical laws must have acted differently for matter and antimatter, i.e. violating CPsymmetry.
The Standard Model contains at least three sources of CP violation. The first of these, involving the Cabibbo–Kobayashi–Maskawa matrix in the quark sector, has been observed experimentally and can only account for a small portion of the CP violation required to explain the matterantimatter asymmetry. The strong interaction should also violate CP, in principle, but the failure to observe the electric dipole moment of the neutron in experiments suggests that any CP violation in the strong sector is also too small to account for the necessary CP violation in the early universe. The third source of CP violation is the Pontecorvo–Maki–Nakagawa–Sakata matrix in the lepton sector. The current longbaseline neutrino oscillation experiments, T2K and NOνA, may be able to find evidence of CP violation over a small fraction of possible values of the CP violating Dirac phase while the proposed nextgeneration experiments, HyperKamiokande and DUNE, will be sensitive enough to definitively observe CP violation over a relatively large fraction of possible values of the Dirac phase. Further into the future, a neutrino factory could be sensitive to nearly all possible values of the CP violating Dirac phase. If neutrinos are Majorana fermions, the PMNS matrix could have two additional CP violating Majorana phases, leading to a fourth source of CP violation within the Standard Model. The experimental evidence for Majorana neutrinos would be the observation of neutrinoless doublebeta decay. The best limits come from the GERDA experiment. CP violation in the lepton sector generates a matterantimatter asymmetry through a process called leptogenesis. This could become the preferred explanation in the Standard Model for the matterantimatter asymmetry of the universe once CP violation is experimentally confirmed in the lepton sector.
If CP violation in the lepton sector is experimentally determined to be too small to account for matterantimatter asymmetry, some new physics beyond the Standard Model would be required to explain additional sources of CP violation. Adding new particles and/or interactions to the Standard Model generally introduces new sources of CP violation since CP is not a symmetry of nature.
Sakharov proposed a way to restore CPsymmetry using Tsymmetry, extending spacetime before the Big Bang. He described complete CPT reflections of events on each side of what he called the "initial singularity". Because of this, phenomena with an opposite arrow of time at t < 0 would undergo an opposite CP violation, so the CPsymmetry would be preserved as a whole. The anomalous excess of matter over antimatter after the Big Bang in the orthochronous (or positive) sector, becomes an excess of antimatter before the Big Bang (antichronous or negative sector) as both charge conjugation, parity and arrow of time are reversed due to CPT reflections of all phenomena occurring over the initial singularity:
We can visualize that neutral spinless maximons (or photons) are produced at t < 0 from contracting matter having an excess of antiquarks, that they pass "one through the other" at the instant t = 0 when the density is infinite, and decay with an excess of quarks when t > 0, realizing total CPT symmetry of the universe. All the phenomena at t < 0 are assumed in this hypothesis to be CPT reflections of the phenomena at t > 0.
See also
 Bfactory
 Parity (physics) § Parity violation
 Charge conjugation
 Tsymmetry
 CPT symmetry
 BTeV experiment
 Cabibbo–Kobayashi–Maskawa matrix
 LHCb
 Penguin diagram
 Neutral particle oscillation
 Electron electric dipole moment
References
 ↑ Schwarzschild, Bertram (1999). "Two Experiments Observe Explicit Violation of Time‐Reversal Symmetry". Physics Today 52 (2): 19–20. doi:10.1063/1.882519. Bibcode: 1999PhT....52b..19S.
 ↑ Schubert, K.R. (2015). "T violation and CPT tests in neutralmeson systems". Progress in Particle and Nuclear Physics 81: 1–38. doi:10.1016/j.ppnp.2014.12.001. Bibcode: 2015PrPNP..81....1S.
 ↑ Lee, T. D.; Yang, C. N. (1956). "Question of Parity Conservation in Weak Interactions". Physical Review 104 (1): 254–258. doi:10.1103/PhysRev.104.254. Bibcode: 1956PhRv..104..254L.
 ↑ Wu, C. S.; Ambler, E.; Hayward, R. W.; Hoppes, D. D.; Hudson, R. P. (1957). "Experimental Test of Parity Conservation in Beta Decay". Physical Review 105 (4): 1413–1415. doi:10.1103/PhysRev.105.1413. Bibcode: 1957PhRv..105.1413W.
 ↑ ^{5.0} ^{5.1} Ioffe, B. L.; Okun, L. B.; Rudik, A. P. (1957). "The Problem of Parity Nonconservation in Weak Interactions". Journal of Experimental and Theoretical Physics 32: 328–330. http://www.jetp.ac.ru/cgibin/dn/e_005_02_0328.pdf.
 ↑ Friedman, J. I.; Telegdi, V. L. (1957). "Nuclear Emulsion Evidence for Parity Nonconservation in the Decay Chain π^{+}→μ^{+}→e^{+}". Physical Review 106 (6): 1290–1293. doi:10.1103/PhysRev.106.1290. Bibcode: 1957PhRv..106.1290F.
 ↑ Garwin, R. L.; Lederman, L. M.; Weinrich, M. (1957). "Observations of the Failure of Conservation of Parity and Charge Conjugation in Meson Decays: The Magnetic Moment of the Free Muon". Physical Review 105 (4): 1415–1417. doi:10.1103/PhysRev.105.1415. Bibcode: 1957PhRv..105.1415G.
 ↑ Culligan, G.; Frank, S. G. F.; Holt, J. R. (1959). "Longitudinal polarization of the electrons from the decay of unpolarized Positive and Negative Muons". Proceedings of the Physical Society 73 (2): 169. doi:10.1088/03701328/73/2/303. Bibcode: 1959PPS....73..169C.
 ↑ Lee, T. D.; Oehme, R.; Yang, C. N. (1957). "Remarks on Possible Noninvariance under Time Reversal and Charge Conjugation". Physical Review 106 (2): 340–345. doi:10.1103/PhysRev.106.340. Bibcode: 1957PhRv..106..340L. http://www.slac.stanford.edu/spires/find/hep/www?j=PHRVA,106,340.
 ↑ Landau, L. (1957). "On the conservation laws for weak interactions". Nuclear Physics 3 (1): 127–131. doi:10.1016/00295582(57)900615. Bibcode: 1957NucPh...3..127L.
 ↑ Anikina, M. Kh.; Neagu, D. V.; Okonov, E. O.; Petrov, N. I.; Rozanova, A. M.; Rusakov, V. A.. "An experimental investigation of some consequences of CPinvariance in K02 meson decays". Soviet Physics JETP 15 (1): 93–96. http://jetp.ac.ru/cgibin/dn/e_015_01_0093.pdf.
 ↑ The FitchCronin Experiment
 ↑ Christenson, J. H.; Cronin, J. W.; Fitch, V. L.; Turlay, R. (1964). "Evidence for the 2π Decay of the K02 Meson System". Physical Review Letters 13 (4): 138. doi:10.1103/PhysRevLett.13.138. Bibcode: 1964PhRvL..13..138C.
 ↑ AlaviHarati, A. (1999). "Observation of Direct CP Violation in K_{S,L}→ππ Decays". Physical Review Letters 83 (1): 22–27. doi:10.1103/PhysRevLett.83.22. Bibcode: 1999PhRvL..83...22A.
 ↑ Fanti, V. (1999). "A new measurement of direct CP violation in two pion decays of the neutral kaon". Physics Letters B 465 (1–4): 335–348. doi:10.1016/S03702693(99)010308. Bibcode: 1999PhLB..465..335F.
 ↑ Aubert, B (2001). "Measurement of CPViolating Asymmetries in B^{0} Decays to CP Eigenstates". Physical Review Letters 86 (12): 2515–22. doi:10.1103/PhysRevLett.86.2515. PMID 11289970. Bibcode: 2001PhRvL..86.2515A.
 ↑ Abe K (2001). "Observation of Large CP Violation in the Neutral B Meson System". Physical Review Letters 87 (9): 091802. doi:10.1103/PhysRevLett.87.091802. PMID 11531561. Bibcode: 2001PhRvL..87i1802A.
 ↑ Rodgers, Peter (August 2001). "Where did all the antimatter go?". Physics World. p. 11. http://physicsworld.com/cws/article/print/2001/aug/01/wheredidalltheantimattergo.
 ↑ Carbone, A. (2012). "A search for timeintegrated CP violation in D^{0}→h^{−}h^{+} decays". arXiv:1210.8257 [hepex].
 ↑ LHCb Collaboration (2014). "Measurement of CP asymmetry in D^{0}→K^{+}K^{−} and D^{0}→π^{+}π^{−} decays". Journal of High Energy Physics 2014 (7): 41. doi:10.1007/JHEP07(2014)041. Bibcode: 2014JHEP...07..041A.
 ↑ Aaij, R. (30 May 2013). "First Observation of CP Violation in the Decays of B^{0}_{s} Mesons". Physical Review Letters 110 (22): 221601. doi:10.1103/PhysRevLett.110.221601. PMID 23767711. Bibcode: 2013PhRvL.110v1601A.
 ↑ R. Aaij (2019). "Observation of CP Violation in Charm Decays". Physical Review Letters 122 (21): 211803. doi:10.1103/PhysRevLett.122.211803. PMID 31283320. Bibcode: 2019PhRvL.122u1803A. https://iris.unica.it/bitstream/11584/270374/2/PhysRevLett.122.211803.pdf.
 ↑ Abe, K. et al. (16 April 2020). "Constraint on the matterantimatter symmetryviolating phase in neutrino oscillations". Nature 580 (7803): 339–344. doi:10.1038/s4158602021770. PMID 32296192. Bibcode: 2020Natur.580..339T.
 ↑ Himmel, Alex (2 July 2020). "New Oscillation Results from the NOvA Experiment". doi:10.5281/zenodo.3959581. https://indico.fnal.gov/event/43209/timetable/#194newoscillationresultsfr.
 ↑ Kelly, Kevin J.; Machado, Pedro A.N.; Parke, Stephen J.; PerezGonzalez, Yuber F.; Funchal, Renata Zukanovich (2021). "Neutrino mass ordering in light of recent data". Physical Review D 103 (1): 013004. doi:10.1103/PhysRevD.103.013004. Bibcode: 2021PhRvD.103a3004K.
 ↑ Denton, Peter B.; Gehrlein, Julia; Pestes, Rebekah (2021). "CPViolating Neutrino NonStandard Interactions in LongBaselineAccelerator Data". Physical Review Letters 126 (5): 051801. doi:10.1103/PhysRevLett.126.051801. PMID 33605742. Bibcode: 2021PhRvL.126e1801D.
 ↑ I. Bars; C. Deliduman; O. Andreev (1998). "Gauged Duality, Conformal Symmetry, and Spacetime with Two Times". Physical Review D 58 (6): 066004. doi:10.1103/PhysRevD.58.066004. Bibcode: 1998PhRvD..58f6004B.
Further reading
 Sozzi, M.S. (2008). Discrete symmetries and CP violation. Oxford University Press. ISBN 9780199296668.
 G. C. Branco; L. Lavoura; J. P. Silva (1999). CP violation. Clarendon Press. ISBN 9780198503996.
 I. Bigi; A. Sanda (1999). CP violation. Cambridge University Press. ISBN 9780521443494.
 Michael Beyer, ed (2002). CP Violation in Particle, Nuclear and Astrophysics. Springer. ISBN 9783540437055. (A collection of essays introducing the subject, with an emphasis on experimental results.)
 L. Wolfenstein (1989). CP violation. North–Holland Publishing. ISBN 9780444880819. (A compilation of reprints of numerous important papers on the topic, including papers by T.D. Lee, Cronin, Fitch, Kobayashi and Maskawa, and many others.)
 David J. Griffiths (1987). Introduction to Elementary Particles. John Wiley & Sons. ISBN 9780471603863.
 Bigi, I. (1998). "CP Violation – An Essential Mystery in Nature's Grand Design". Surveys of High Energy Physics 12 (1–4): 269–336. doi:10.1080/01422419808228861. Bibcode: 1998SHEP...12..269B.
 Mark Trodden (1999). "Electroweak Baryogenesis". Reviews of Modern Physics 71 (5): 1463–1500. doi:10.1103/RevModPhys.71.1463. Bibcode: 1999RvMP...71.1463T.
 Davide Castelvecchi. "What is direct CPviolation?". SLAC. http://www2.slac.stanford.edu/tip/special/cp.htm.
 An elementary discussion of parity violation and CP violation is given in chapter 15 of this student level textbook [1]
External links
Original source: https://en.wikipedia.org/wiki/CP violation.
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