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Relevant bibliographies by topics / Quark mixing

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Academic literature on the topic 'Quark mixing'

Author: Grafiati

Published: 4 June 2021

Last updated: 9 February 2022

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Journal articles on the topic "Quark mixing"

1

Abbas, Gauhar, Mehran Zahiri Abyaneh, Aritra Biswas, Saurabh Gupta, Monalisa Patra, G. Rajasekaran, and Rahul Srivastava. "High scale mixing relations as a natural explanation for large neutrino mixing." International Journal of Modern Physics A 31, no. 17 (June 20, 2016): 1650095. http://dx.doi.org/10.1142/s0217751x16500950.

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The origin of small mixing among the quarks and a large mixing among the neutrinos has been an open question in particle physics. In order to answer this question, we postulate general relations among the quarks and the leptonic mixing angles at a high scale, which could be the scale of Grand Unified Theories. The central idea of these relations is that the quark and the leptonic mixing angles can be unified at some high scale either due to some quark–lepton symmetry or some other underlying mechanism and as a consequence, the mixing angles of the leptonic sector are proportional to that of the quark sector. We investigate the phenomenology of the possible relations where the leptonic mixing angles are proportional to the quark mixing angles at the unification scale by taking into account the latest experimental constraints from the neutrino sector. These relations are able to explain the pattern of leptonic mixing at the low scale and thereby hint that these relations could be possible signatures of a quark–lepton symmetry or some other underlying quark–lepton mixing unification mechanism at some high scale linked to Grand Unified Theories.

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Xing, Zhi-Zhong. "Quark mass hierarchy and flavor mixing puzzles." International Journal of Modern Physics A 29, no. 30 (December 8, 2014): 1430067. http://dx.doi.org/10.1142/s0217751x14300671.

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The fact that quarks of the same electric charge possess a mass hierarchy is a big puzzle in particle physics, and it must be highly correlated with the hierarchy of quark flavor mixing. This chapter is intended to provide a brief description of some important issues regarding quark masses, flavor mixing and CP-violation. A comparison between the salient features of quark and lepton flavor mixing structures is also made.

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Kagawa, Ai, Masatoshi Morimoto, Yasuhiko Tsue, João da Providência, Constança Providência, and Masatoshi Yamamura. "Nonzero tensor condensates in cold quark matter within the three-flavor Nambu–Jona–Lasinio model with the Kobayashi–Maskawa–’t Hooft interaction." International Journal of Modern Physics E 29, no. 06 (June 2020): 2050036. http://dx.doi.org/10.1142/s0218301320500366.

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The possible formation of tensor condensates originated from a tensor-type interaction between quarks is investigated in the three-flavor Nambu–Jona–Lasinio model including the Kobayashi–Maskawa–’t Hooft interaction, which leads to flavor mixing. It is shown that independent two tensor condensates appear and a tensor condensate related to the strange quark easily occurs by the effect of the flavor mixing compared with one related to light quarks. Also, it is shown that the tensor condensate related to the strange quark appears at a slightly smaller chemical potential if the Kobayashi–Maskawa–’t Hooft interaction is included, due to the flavor mixing effect. It is also shown that the two kinds of tensor condensates may coexist in a certain quark chemical potential due to the flavor mixing.

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FUKUYAMA, TAKESHI, and HIROYUKI NISHIURA. "UNIVERSALITY OF QUARK–LEPTON MASS MATRIX." Modern Physics Letters A 28, no. 08 (March 12, 2013): 1350017. http://dx.doi.org/10.1142/s021773231350017x.

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The recently observed lepton mixing angle θ13 of the MNS mixing matrix is well incorporated in a universal mixing hypothesis between quark and lepton sectors. This hypothesis asserts that, in the charged lepton diagonal base, all other mass matrices for up- and down-type quarks and light neutrinos are diagonalized by the same unitary matrix except for the phase elements. It is expressed as V CKM = U MNS (δ′)†PU MNS (δ) for quark mixing matrix V CKM and lepton mixing matrix U MNS (δ) in the phenomenological level. Here P is a diagonal phase mass matrix. δ′ is a slightly different phase parameter from the Dirac CP-violating phase δ = 1.1π (best fit) in the MNS lepton mixing matrix.

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NISHIURA, HIROYUKI, and TAKESHI FUKUYAMA. "UNIVERSAL MASS MATRIX AND LEPTONIC θ13 ANGLE." Modern Physics Letters A 26, no. 09 (March 21, 2011): 661–67. http://dx.doi.org/10.1142/s0217732311035158.

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We propose a universal mixing hypothesis between quark and lepton sectors at high energy scale (probably GUT scale) where quark–lepton universality holds. Namely in the charged lepton diagonal base, all the other mass matrices for up and down quarks and neutrinos are diagonalized by the same unitary matrix except for the phase elements. Thanks to this hypothesis, the observed values of the Cabibbo–Kobayashi–Maskawa (CKM) quark mixing matrix and the mixing angles θ12 and θ23 in the Maki–Nakagawa–Sakata (MNS) lepton mixing matrix can predict the unknown magnitudes of the mixing angle θ13 and of the CP violating Dirac phase δ in the MNS matrix. Their allowed regions are rather narrow, 0.036 < sin θ13 < 0.048 and 6° < δ < 12°.

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EVANS, P. W., and B. A. ROBSON. "COMPARISON OF QUARK MIXING IN THE STANDARD AND GENERATION MODELS." International Journal of Modern Physics E 15, no. 03 (April 2006): 617–25. http://dx.doi.org/10.1142/s0218301306004077.

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The different interpretations of quark mixing involved in weak interaction processes in the Standard Model and the Generation Model are discussed with a view to obtaining a physical understanding of the Cabibbo angle and related quantities. It is proposed that hadrons are composed of mixed-quark states, with the quark mixing parameters being determined by the Cabibbo-Kobayashi-Maskawa matrix elements. In this model, protons and neutrons contain a contribution of about 5% and 10%, respectively, of strange valency quarks.

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NISHIURA, HIROYUKI, KOICHI MATSUDA, and TAKESHI FUKUYAMA. "QUARK MIXING FROM MASS MATRIX MODEL WITH FLAVOR 2 ↔ 3 SYMMETRY." International Journal of Modern Physics A 23, no. 27n28 (November 10, 2008): 4557–68. http://dx.doi.org/10.1142/s0217751x08041463.

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We consider a universal mass matrix model which has a seesaw-invariant structure with the most general texture based on flavor 2 ↔ 3 symmetry common to all quarks and leptons. The CKM quark mixing matrix of the model is analyzed. It is shown that the model is consistent with all the experimental data of quark mixings by tuning free parameters of the model. We also show that the values of parameters of the present model consistent with the experimental data are not far from the ones of the mass matrix model with a vanishing (1, 1) element.

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KITAZAWA, NORIAKI. "QUARK MASS HIERARCHY IN THE SUPERSYMMETRIC COMPOSITE MODEL." International Journal of Modern Physics A 14, no. 27 (October 30, 1999): 4237–57. http://dx.doi.org/10.1142/s0217751x99001998.

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A mechanism to have the quark mass hierarchy in the supersymmetric composite model is proposed. The source of the hierarchy is the kinetic-term mixing between composite quarks. Such mixing can be expected, if quarks are composite particles. A model in which the mechanism works is constructed, although it is not perfectly realistic because of some assumptions and unnaturalness.

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9

Gupta, Suraj N., and James M. Johnson. "Quark mixing andCPviolation." Physical Review D 44, no. 7 (October 1, 1991): 2110–13. http://dx.doi.org/10.1103/physrevd.44.2110.

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TERAZAWA, HIDEZUMI. "HOW TO SOLVE THE CKM QUARK MIXING MATRIX." Modern Physics Letters A 07, no. 36 (November 30, 1992): 3373–77. http://dx.doi.org/10.1142/s0217732392002767.

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It was pointed out that given the us element of the CKM quark mixing matrix, all the other elements can be successfully explained or predicted by using the five relations derived in a composite model of quarks (and leptons).

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Dissertations / Theses on the topic "Quark mixing"

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Ogasahara, Atsushi. "Discrete flavor symmetry for lepton mixing and quark mixing." 京都大学 (Kyoto University), 2014. http://hdl.handle.net/2433/189340.

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Hazelton, William Donald. "Configuration mixing of quark states in nucleons and other baryons in the MIT bag model /." Thesis, Connect to this title online; UW restricted, 1997. http://hdl.handle.net/1773/9770.

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Menzel, Andreas. "Constraints on the Fourth-Generation Quark Mixing Matrix from Precision Flavour Observables." Doctoral thesis, Humboldt-Universität zu Berlin, Mathematisch-Naturwissenschaftliche Fakultät, 2017. http://dx.doi.org/10.18452/17711.

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Das Standardmodell einer zusätzlichen sequentiellen Fermiongeneration (SM4) war 2012 auf Basis eines Fits an elektroschwache Präzisionsobservable und die Higgs-Signalstärken mit einer Signifikanz von 5.3 sigma ausgeschlossen worden. Komplementär dazu wurden in der vorliegenden Arbeit Fits des SM4 an eine Kombination eines typischen Satzes von Flavour-Observablen mit den Ergebnissen des zuvor durchgeführten Elektroschwachen Präzisionsfits durchgeführt. Im SM3-Kontext extrahierte Größen wurden gemäß ihrer Bedeutung im SM4 reinterpretiert und die angepassten theoretischen Ausdrücke angegeben. Die resultierenden Einschränkungen der CKM-Matrix des SM4, ihrer potentiell CP-verletzenden Phasen sowie der Masse des up-type-Quarks der 4. Generation t'' werden angegeben. Zum Vergleich des SM4 mit dem SM3 werden die erreichten chi^2-Werte genutzt. chi^2=15.53 im SM4 und 9.56 im SM3 passen fast vollkommen zu einer gleich guten Beschreibung der Experimente durch beide Modelle, wobei das SM3 aber sechs Freiheitsgrade mehr besitzt. Außerdem wurden die Vorhersagen des SM3 und des SM4 für die Dimyon-Ladungsasymmetrie ASL mit experimentellen Werten verglichen. Die Vorhersage des SM3 ist ca. 2 sigma vom experimentellen Wert entfernt, die des SM4 ca. 3 sigma.\par Die Ergebnisse deuten nicht darauf hin, dass die Signifikanz des 2012 erreichten Ausschlusses des SM4 durch die Hinzunahme von Flavour-Observablen zu den damals verwendeten elektroschwachen Präzisionsobservablen und Higgs-Querschnitten bedeutend verringert würde.\par Es konnte jedoch keine genaue quantitative Aussage über die Auswirkungen der Flavourobservablen auf diese Signifikanz getroffen werden, weil das Programm CKMfitter likelihood-ratio-Berechnung nur durchführen kann, wenn sich eines der untersuchten Modelle durch Fixierung von Parametern aus dem anderen ergibt (nested models), was hier nicht der Fall ist.
The Standard Model extended by an additional sequential generation of Dirac fermions (SM4) was excluded with a significance of 5.3 sigma in 2012. This was achieved in a combined fit of the SM4 to Electroweak Precision Observables and signal strengths of the Higgs boson. This thesis complements this excludion by a fit of the SM4 to a typical set of Flavour physics observables and the results of the previously performed Electroweak Precision fit. Quantities extracted in an SM3 framework are reinterpreted in SM4 terms and the adapted theoretical expressions are given. The resultant constraints on the SM4''s CKM matrix, its potentially CP-violating phases and the mass of the new up-type quark t'' are given. To compare the relative performance of the SM4 and the SM3, this work uses the chi^2 values achieved in the fit. The values of 15.53 for the SM4 and 9.56 for the SM4 are almost perfectly consistent with both models describing the experimental data equally well with the SM3 having six degrees of freedom more. The dimuon charge asymmetry ASL was not used as a fit input because the interpretation of its measurement was subject to debate at the time when the fits were produced, but its prediction in the fit was used as an additional test of the SM4. The SM3''s prediction differs from the experimental values by about 2 sigma, and the SM4''s prediction by about 3 sigma. \par In summary, these results do not suggest that any significant reduction of the 5.3 sigma exclusion could be achieved by combining the Electroweak Precision Observables and Higgs inputs with Flavour physics data. However, the exact effect of the Flavour physics input on the significance of the SM4''s exclusion cannot be given at this point because the CKMfitter software is currently not able to perform a statistically stringent likelihood comparison of non-nested models.

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Ohlsson, Tommy. "Properties of baryons in the chiral quark model." Licentiate thesis, KTH, Fysik, 1997. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-756.

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In this thesis, several properties of baryons are studied using the chiral quark model. The chiral quark model is a theory which can be used to describe low energy phenomena of baryons. In Paper 1, the chiral quark model is studied using wave functions with configuration mixing. This study is motivated by the fact that the chiral quark model cannot otherwise break the Coleman–Glashow sum-rule for the magnetic moments of the octet baryons, which is xperimentally broken by about ten standard deviations. Configuration mixing with quark-diquark components is also able to reproduce the octet baryon magnetic moments very accurately. In Paper 2, the chiral quark model is used to calculate the decuplet baryon magnetic moments. The values for the magnetic moments of the ++and− are in good agreement with the experimental results. The total quark spin polarizations are also calculated and are found to be significantly smaller than the non-relativistic quark model results. In Paper 3, the weak form factors for semileptonic octet baryon decays are studied in the chiral quark model. The “weak magnetism” form factors are found to be consistent with the conserved vector current (CVC) results and the induced pseudotensor form factors, which seem to be model independent, are small. The results obtained are in general agreement with experiments and are also compared with other model calculations.
QC 20100618

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Villa, Andrea. "Measurement of y_CP with D^0 mesons from semileptonic B-meson decays at LHCb." Master's thesis, Alma Mater Studiorum - Università di Bologna, 2020. http://amslaurea.unibo.it/21249/.

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This thesis reports a measurement of the charm-mixing observable yCP using D^0->K^+K^−, D^0->pi^+pi^−, and D^0->K^−pi^+ decays, where the D^0 meson originates from semileptonic B-meson decays. The analysis is performed on the full Run 2 dataset collected by LHCb with pp collisions at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.57 fb^−1 . The dataset is divided into 18 exclusive D^0 decay-time bins, in which an invariant mass fit is performed to extract the signal yield for each decay channel. The ratios of KK/Kpi and pipi/Kpi yields in each bin, corrected for the efficiency as function of the decay-time estimated from a Monte Carlo sample, are then fitted to extract the difference between the decay widths of KK (pipi) and Kpi channels, ∆Γ^{KK} (∆Γ^{pipi}). Finally, y_CP is computed as ∆Γt(D^0), where t(D^0) is the precisely known D^0 lifetime. The values obtained from the two decay channels with preliminary systematic uncertainties are y_CP^{KK} = (75.98 ± 0.07 (stat) ± 0.06 (syst))%, y_CP^{pipi} = (76.29 ± 0.14 (stat) ± 0.05 (syst))%, which are consistent with each other (the central values are blind), and when combined yield a result of y_CP = (76.08 ± 0.06 (stat) ± 0.04 (syst))%. The analysis aims at updating the previous LHCb measurement with a larger data sample size, and is expected to improve the precision by a factor two with respect to the current world average y_CP = (0.715 ± 0.111)%.

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Nguyen, Phuc Bao-Uyen. "Quark mass generation and mixing; and the next-to-leading order QCD calculation for hadron-hadron elastic collisions." Thesis, McGill University, 1993. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=41226.

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This thesis is arranged in two distinct parts. The first part involves the construction of a novel dynamical scheme which is capable of generating the masses of the quarks and the elements of the Kobayashi-Maskawa matrix, and which does not rely upon the Higgs mechanism. The up quarks acquire their masses by coupling to a new heavy fermion via emission and reabsorption of a new scalar boson. The down quarks, on the other hand, obtain their masses via a correction to the up mass matrix as a result of an anomalous flavour changing interaction of the $W sp pm$. Extensions of the mass generation model are proposed and discussed. The second part involves the leading-log s study of hadron-hadron elastic scattering to order $ alpha sb{s} sp3$. By introducing wave functions, it is found that there are three types of form factor for the proton, and two for the pion. These form factors turn out to cancel the infrared divergence which occurs in quark-quark scattering. To this order in $ alpha sb{s}$, the amplitude of such elastic scattering is shown to have the form $ sim$(1 + log(s)($ alpha sb{o}$ + $ alpha sp prime t$ + $O(t sp2))$ for the imaginary part and a constant $ sim alpha sb{odd}$ for the real part, where s and t are the usual Mandelstam variables, and the $ alpha$'s are constants.

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Menzel, Andreas [Verfasser], Heiko [Gutachter] Lacker, Peter [Gutachter] Uwer, and Thorsten [Gutachter] Feldmann. "Constraints on the Fourth-Generation Quark Mixing Matrix from Precision Flavour Observables / Andreas Menzel ; Gutachter: Heiko Lacker, Peter Uwer, Thorsten Feldmann." Berlin : Mathematisch-Naturwissenschaftliche Fakultät, 2017. http://d-nb.info/1127108956/34.

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Di, Pierro Massimo. "B physics from lattice simulations." Thesis, University of Southampton, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.297379.

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Ohlsson, Tommy. "Dynamics of quarks and leptons : theoretical Studies of Baryons and Neutrinos." Doctoral thesis, KTH, Fysik, 2000. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-2991.

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The Standard Model of Elementary Particle Physics (SM) is the present theoryfor the elementary particles and their interactions and is a well-established theorywithin the physics community. The SM is a combination of Quantum Chromodynamics(QCD) and the Glashow{Weinberg{Salam (GWS) electroweak model. QCDis a theory for the strong force, whereas the GWS electroweak model is a theoryfor the weak and electromagnetic forces. This means that the SM describes allfundamental forces in Nature, except for the gravitational force. However, the SMis not a nal theory and some of its problems will be discussed in this thesis.In the rst part of this thesis, several properties of baryons are studied suchas spin structure, spin polarizations, magnetic moments, weak form factors, andnucleon quark sea isospin asymmetries, using the chiral quark model (QM). TheQM is an eective chiral eld theory developed to describe low energy phenomena of baryons, since perturbative QCD is not applicable at low energies. The resultsof the QM are in good agreement with experimental data.The second part of the thesis is devoted to the concept of quantum mechanicalneutrino oscillations. Neutrino oscillations can, however, not occur within the GWSelectroweak model. Thus, this model has to be extended in some way. All studiesincluding neutrino oscillation are done within three avor neutrino oscillationmodels. Both vacuum and matter neutrino oscillations are considered. Especially,global ts to all data of candidates for neutrino oscillations are presented and alsoan analytical formalism for matter enhanced three avor neutrino oscillations usingtime evolution operators is derived. Furthermore, investigations of matter eectswhen neutrinos traverse the Earth are included.The thesis begins with an introductory review of the QM and neutrino oscillationsand ends with the research results, which are given in the nine accompanyingscientic articles.
QC 20100616

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Volk, Alexei. "Measurement of the Partial Branching Fraction for Inclusive Semileptonic B Meson Decays to Light Hadrons B->Xu l nu and an Improved Determination of the Quark-Mixing Matrix Element |V_ub|." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2009. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-24169.

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This thesis presents an analysis of inclusive semileptonic $B \to X_u e \nu$ decays using approximately 454 million $\Upsilon(4S) \to B \bar{B}$ decays collected during the years 1999 to 2008 with the BABAR detector. The electron energy, $E_e$, and the invariant mass squared of the electron-neutrino pair,$ q^2$, are reconstructed, where the neutrino kinematics is deduced from the decay products of both B mesons. The final hadronic state,$ X_u$, consists of a sum of many hadronic channels, each of which contains at least one $u$ quark. The variables $q^2$ and $E_e$ are then combined to compute the maximum kinematically allowed invariant mass squared of the hadronic system, $s_h^{max}$. Using these kinematic quantities, the partial branching fraction, $\Delta BR(B \to X_u e \nu)$, unfolded for detector effects, is measured to be $\Delta BR(E_e>2.0 GeV, s_h^{max}<3.52 GeV^2) = (3.33 \pm 0.18 \pm 0.21) \times 10^{-4} in the $\Upsilon(4S)$ and \Delta \tilde{\BR}(\tilde E_e>1.9 GeV, \tilde {s}^{max}_{h} < 3.5 GeV^2) = (4.57 \pm 0.24 \pm 0.32) \times 10^{-4} in the $B$ meson rest frames. The quoted errors are statistical and systematic, respectively. The CKM matrix element $|V_{ub}|$ is determined from the measured $\Delta \tilde{\BR}$ using theoretical calculation based on Heavy Quark Expansion. The result is $|V_{ub}| = (4.19 \pm 0.18{}^{+0.26}_{-0.20} {}^{+0.26}_{-0.25}) \times 10^{-3}, where the errors represent experimental uncertainties, uncertainties from HQE parameters and theoretical uncertainties, respectively.

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Books on the topic "Quark mixing"

1

Bordes, J. Features of quark and lepton mixing from differential geometry of curves on surfaces. Chilton: Rutherford Appleton Laboratory, 1998.

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1942-, Koide Y., ed. International Workshop on Masses and Mixings of Quarks and Leptons: Shizuoka, Japan, 19-21 March 1997. Singapore: World Scientific, 1998.

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Thackray, Nicholas James. A measurement of mixing in the B0B0 system and extraction of the Z0 coupling to b quarks using prompt leptons at OPAL. Birmingham: University of Birmingham, 1993.

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Vigdor, Steven E. Trinity. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198814825.003.0003.

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Chapter 3 explains evidence for three generations of quarks and leptons, as needed to provide natural means for standard model CP violation. It describes the cross-generational mixing of quarks and of neutrinos of different flavor, and the matrices that characterize the mixing. CP violation from quark mixing is well measured but insufficient to explain the universe’s matter–antimatter imbalance, while CP violation in neutrino mixing is the subject of ongoing searches. Discoveries revealing and quantifying flavor oscillations among neutrinos from the sun and the atmosphere are reviewed. In describing attempts to understand the lightness and nature of neutrinos—whether they are Majorana neutrinos that are their own antiparticles—the chapter introduces the concept of chirality and searches for neutrinoless double beta decay. It also notes the strong CP problem, wherein nature maintains CP symmetry in interactions among the three quark colors even though quantum chromodynamics allows for sizable violations.

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Kagan, Alexander L. Radiative quark mass and mixing hierarchies from supersymmetric models with a fourth mirror family. 1989.

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Koide, Yoshio. International Workshop on Masses and Mixings of Quarks and Leptons: Shizuoka, Japan, 19-21 March 1997. World Scientific Publishing Company, 1998.

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Book chapters on the topic "Quark mixing"

1

Aleksan, R. "Quark Mixing and CP Violation." In Techniques and Concepts of High Energy Physics X, 487–595. Dordrecht: Springer Netherlands, 1999. http://dx.doi.org/10.1007/978-94-011-4689-0_12.

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2

Kleinknecht, K. "Quark and lepton mixing in weak interactions." In Springer Tracts in Modern Physics, 149–64. Berlin, Heidelberg: Springer Berlin Heidelberg, 1986. http://dx.doi.org/10.1007/bfb0041271.

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Jarlskog, C. "The Quark Mixing Matrix and Cp Violation." In Techniques and Concepts of High-Energy Physics VII, 55–100. Boston, MA: Springer US, 1994. http://dx.doi.org/10.1007/978-1-4615-2419-9_2.

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Kleinknecht, Konrad. "Weak Quark Mixing and the CKM Matrix." In Springer Tracts in Modern Physics, 123–38. Berlin, Heidelberg: Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/978-3-540-44916-4_7.

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Kleinknecht, Konrad. "10.7 Weak quark mixing and the CKM matrix." In Theory and Experiments, 473–81. Berlin, Heidelberg: Springer Berlin Heidelberg, 2008. http://dx.doi.org/10.1007/978-3-540-74203-6_16.

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Suekane, Fumihiko. "Quark Mass, Cabibbo Angle and CKM Mixing Matrix." In Quantum Oscillations, 79–94. Cham: Springer International Publishing, 2021. http://dx.doi.org/10.1007/978-3-030-70527-5_8.

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de Rafael, Eduardo. "Lectures on Quark Flavor Mixing in the Standard Model." In Springer Proceedings in Physics, 344–439. Berlin, Heidelberg: Springer Berlin Heidelberg, 1985. http://dx.doi.org/10.1007/978-3-642-93289-2_13.

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Hanhart, C. "Aspects of a 0 0 -f0 mixing in the reaction pn → dX." In Refereed and selected contributions from International Conference on Quark Nuclear Physics, 359–61. Berlin, Heidelberg: Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/978-3-662-09712-0_53.

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Nachtmann, Otto. "Decay Processes in the Standard Model and the Determination of the Quark Mixing Angles in the Charged Current." In Elementary Particle Physics, 372–94. Berlin, Heidelberg: Springer Berlin Heidelberg, 1990. http://dx.doi.org/10.1007/978-3-642-61281-7_23.

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Stech, Berthold. "Charged Current Mixing and CP-Violation." In Quarks, Leptons, and Beyond, 81–93. Boston, MA: Springer US, 1985. http://dx.doi.org/10.1007/978-1-4899-2254-0_2.

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Conference papers on the topic "Quark mixing"

1

Barr, S. M., and Heng-Yu Chen. "Relating quark mixing neutrino mixing and δlep." In WORKSHOP ON DARK MATTER, UNIFICATION AND NEUTRINO PHYSICS: CETUP∗ 2012. AIP, 2013. http://dx.doi.org/10.1063/1.4807362.

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Schäfer, Marion. "Update on B0-B̄0 mixing." In Internatinal symposium on heavy quark physics. AIP, 1989. http://dx.doi.org/10.1063/1.38913.

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DONOGHUE, JOHN F. "LIGHT QUARK MASSES AND MIXING ANGLES." In Proceedings of the 1993 Theoretical Advanced Study Institute in Elementary Particle Physics. WORLD SCIENTIFIC, 1994. http://dx.doi.org/10.1142/9789814503785_0003.

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Gupta, V., G. Sánchez-Colón, and S. Chaturvedi. "Quark flavor mixing and mass matrices." In PARTICLES AND FIELDS. ASCE, 2009. http://dx.doi.org/10.1063/1.3131542.

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5

Soto, Joan. "The mixing of hybrids with quarkonia." In XIII Quark Confinement and the Hadron Spectrum. Trieste, Italy: Sissa Medialab, 2019. http://dx.doi.org/10.22323/1.336.0130.

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Blaylock, Guy. "Heavy Quark Lifetimes, Mixing, and CP Violation." In Proceedings of the XIX International Symposium. WORLD SCIENTIFIC, 2000. http://dx.doi.org/10.1142/9789812793942_0007.

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NIERSTE, ULRICH. "QUARK MIXING AND CP VIOLATION — THE CKM MATRIX." In Proceedings of the XXII International Symposium. WORLD SCIENTIFIC, 2006. http://dx.doi.org/10.1142/9789812704023_0014.

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Blossier, Benoit, Damir Becirevic, Ph Boucaud, A. Le-Yaouanc, J. P. Leroy, and Olivier Pene. "Bs-Bsbar mixing with chiral light quark action." In XXIIIrd International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2005. http://dx.doi.org/10.22323/1.020.0218.

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Fritzsch, H. "Flavor Mixing, Quark Masses, Neutrino Masses and Neutrino Oscillations." In Proceedings of the Workshop in Honor of the 60th Birthday of Misha Shifman. WORLD SCIENTIFIC, 2010. http://dx.doi.org/10.1142/9789814304030_0035.

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Chaturvedi, S. "Parametrization of the Quark Mixing Matrix Involving its Eigenvalues." In PARTICLES AND FIELDS: Tenth Mexican School on Particles and Fields. AIP, 2003. http://dx.doi.org/10.1063/1.1594321.

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Reports on the topic "Quark mixing"

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Yu, Zhaoou. Bottom quark anti-quark production and mixing in proton anti-proton collisions. Office of Scientific and Technical Information (OSTI), March 2003. http://dx.doi.org/10.2172/1374854.

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Roberts, C. D., K. L. Mitchell, P. C. Tandy, and R. T. Cahill. {rho}-{omega} mixing self-energy and model quark-gluon dynamics. Office of Scientific and Technical Information (OSTI), August 1995. http://dx.doi.org/10.2172/166440.

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Schietinger, Thomas. Using kaon regeneration to probe the quark mixing parameter cos(2 beta) in B -> psi K decays. Office of Scientific and Technical Information (OSTI), July 2001. http://dx.doi.org/10.2172/787175.

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Lavoura, L., and J. P. Silva. Bounds on the mixing of the down-type quarks with vector-like singlet quarks. Office of Scientific and Technical Information (OSTI), September 1992. http://dx.doi.org/10.2172/10188401.

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Lavoura, L., and J. P. Silva. Bounds on the mixing of the down-type quarks with vector-like singlet quarks. Office of Scientific and Technical Information (OSTI), September 1992. http://dx.doi.org/10.2172/6949791.

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