318 research outputs found
Theoretical correction to the neutral meson asymmetry
Certain types of asymmetries in neutral meson physics have not been treated
properly, ignoring the difference of normalization factors with an assumption
of the equality of total decay width. Since the corrected asymmetries in
meson are different from known asymmetries by a shift in the first order of CP-
and CPT-violation parameters, experimental data should be analyzed with the
consideration of this effect as in meson physics.Comment: 7 page
Improved Methods for Observing CP Violation in B+/- --> K+/- D0 and Measuring the CKM Phase gamma
Various methods are discussed for obtaining the CKM angle gamma through the
interference of the charged B-meson decay channels B- -> K- D0 and B- -> K-
D0-bar where the D0 and D0-bar decay to common final states. It is found that
choosing final states which are not CP eigenstates can lead to large direct CP
violation which can give significant bounds on gamma without any theoretical
assumptions. If two or more modes are studied, gamma may be extracted with a
precision on the order of +/-15 degrees given about 10^8 B-mesons. We also
discuss the case of three body decays of the D0 where additional information
may be obtained from the distribution of the D0 decay products and consider the
impact of D-D-bar oscillations.Comment: 51 pages 8 figures, typo in equation 33 correcte
CP violation and CKM phases from angular distributions for decays into admixtures of CP eigenstates
We investigate the time-evolutions of angular distributions for decays
into final states that are admixtures of CP-even and CP-odd configurations. A
sizable lifetime difference between the mass eigenstates allows a probe
of CP violation in time-dependent untagged angular distributions. Interference
effects between different final state configurations of , determine the Wolfenstein parameter from
untagged data samples, or -- if one uses as an additional
input -- the notoriously difficult to measure CKM angle . Another
determination of is possible by using isospin symmetry of strong
interactions to relate untagged data samples of
and . We note that the untagged angular
distribution for provides interesting information about
electroweak penguins.Comment: 19 pages, LaTeX, no figure
Bose-Einstein Correlations for Mixed Neutral Mesons
Correlations are shown to arise in nonidentical mixed-particle pairs like
when observed in identical decay modes like in
multiparticle final states containing many partial waves. No enhancement is
found in any single partial wave and all partial wave analyses of the s-wave
threshold resonance and should give the same results for all decay
modes. In CP violation experiments where pairs are inclusively
produced and correlated decays into and leptonic modes are observed,
the CP-violating lepton asymmetry is enhanced by a factor of two in the
kinematic region where Bose enhancement occurs.Comment: 11 page
Framework for Identification of Neutral B Mesons
We introduce a method for the study of CP-violating asymmetries in tagged
states of neutral mesons with arbitrary coherence properties. A set of
time-dependent measurements is identified which completely specifies the
density matrix of the initial state in a two-component space with basis vectors
and , and permits a determination of phases in the
Cabibbo-Kobayashi-Maskawa matrix. For a given tagging configuration, the
measurement of decays both to flavor eigenstates and to CP eigenstates provides
the necessary information.Comment: Submitted to Phys. Rev. Letters. 8 pages, LaTeX, Technion-PH-93-31 /
EFI 93-3
Penguins, Trees and Final State Interactions in B Decays in Broken SU3
The availability of data on decays to strange quasi-two-body final
states, either with or without charmonium opens new possibilities for
understanding different contributions of weak diagrams and in particular the
relative contributions of tree and penguin diagrams. Corresponding and
decays to charge conjugate final states are equal in the SU(3) symmetry
limit and the dominant SU(3) breaking mechanism is given by ratios of CKM
matrix elements. Final State Interactions effects should be small, because
strong interactions conserve and should tend to cancel in ratios between
charge conjugate states. Particularly interesting implications of decays into
final states containing and are discussed.Comment: special macro - phyzz
Angular distributions and lifetime differences in decays
The strange meson and its charge-conjugate are expected to mix with one another in such a way that
the mass eigenstates (``heavy'') and (``light'') may have a
perceptible lifetime difference of up to 40\%, with the CP-even eigenstate
being shorter-lived. A simple transversity analysis permits one to separate the
CP-even and CP-odd components of , and thus to determine
the lifetime difference. The utility of a similar analysis for is noted.Comment: 10 pages, latex, no figure
Determining the Quark Mixing Matrix From CP-Violating Asymmetries
If the Standard Model explanation of CP violation is correct, then
measurements of CP-violating asymmetries in meson decays can in principle
determine the entire quark mixing matrix.Comment: 8 pages (plain TeX), 1 figure (postscript file appended), DAPNIA/SPP
94-06, NSF-PT-94-2, UdeM-LPN-TH-94-18
One-particle inclusive CP asymmetries
One-particle inclusive CP asymmetries in the decays of the type B -> D(*) X
are considered in the framework of a QCD based method to calculate the rates
for one-particle inclusive decays.Comment: Latex, 13 pages, 6 figures (eps). Analytical and numerical results
unchanged, extended discussion of model assumptions and systematic
uncertainties. Version to be published in Phys. Rev. D 62, 0960xx. Additional
transparencies are available via the WWW at
http://www-ttp.physik.uni-karlsruhe.de/Slides
CP Violation and Lifetime Differences of Neutral B Mesons from Correlated B^0-B^0bar Pairs
We present a technique to determine the CP violating phases, as well as, the
lifetime differences of the mass eigenstates for both and , by
considering correlated pairs produced at the resonances.
We do not require a detailed time dependent study, but only partial time
integrated rates, with the tag time, either preceding or following the decay of
the other meson to a final state f. f may be a CP eigenstate or a non-CP
eigenstate.Comment: 11 Pages Revte
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