Relevant bibliographies by topics / Quark and lepton masses

Academic literature on the topic 'Quark and lepton masses'

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Published: 14 March 2023

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Journal articles on the topic "Quark and lepton masses"

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TERAZAWA, HIDEZUMI. "HOW TO SOLVE THE MASS SPECTRUM OF QUARKS AND LEPTONS." Modern Physics Letters A 07, no. 21 (July 10, 1992): 1879–85. http://dx.doi.org/10.1142/s0217732392001580.

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It is suggested that the existing mass spectrum of quarks and leptons can be explained by solving a set of sum rules for quark and lepton masses. As an illustration, we presented a solution where given the three charged lepton masses, all the six quark masses are correctly derived with the prediction of mt≃131 GeV from the six sum rules including two new empirical ones.
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DECKER, ROGER, and JEAN PESTIEAU. "CANCELLATION OF ULTRAVIOLET DIVERGENCES IN THE SU(2)L×U(1) ELECTROWEAK MODEL." Modern Physics Letters A 04, no. 28 (December 30, 1989): 2733–38. http://dx.doi.org/10.1142/s0217732389003051.

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We assume that, in the SU(2)L×U(1) model, ultraviolet divergences of the charged lepton self-masses are zero. We predict the top and Higgs masses in the vicinity of the Z-boson mass. Our assumption holds only if there are no more than three generations of quarks and leptons and if quarks and leptons, except for the top quark, have negligible masses compared to the W-boson mass.
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ROSEN, GERALD. "IS LEPTON-QUARK MASS PRESET BY A CHARGE-NUMBER RELATION?" Modern Physics Letters A 11, no. 20 (June 28, 1996): 1687–89. http://dx.doi.org/10.1142/s0217732396001673.

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It is shown that a simple expression for m that depends exclusively on the charge-number Q gives experimentally admissible zero mass for the three neutrinos and accurately consistent mass values for the charged leptons and quarks over the five order-of-magnitude range characterized by the ratio mt/me≅3.6×105. Since this charge-number relation is patently predictive, with 12 fermion masses constituting substantial output relative to the postulational input, lepton and quark mass may indeed be preset by this charge-number condition. Hence, lepton-quark mass may actually be primary to the phenomenological standard model Lagrangian.
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Fritzsch, Harald. "Oscillating Neutrinos and Majorana Neutrino Masses." Universe 6, no. 2 (February 6, 2020): 29. http://dx.doi.org/10.3390/universe6020029.

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We discuss the mass matrices with texture zeros for the quarks and leptons. The flavor mixing angles for the quarks are functions of the quark masses and can be calculated. The results agree with the experimental data. The texture zero mass matrices for the leptons and the see-saw mechanism are used to derive relations between the matrix elements of the lepton mixing matrix and the ratios of the neutrino masses. Using the measured neutrino mass differences, the neutrino masses can be calculated. The neutrinoless double beta decay is discussed. The effective Majorana neutrino mass, describing the neutrinoless double beta decay, can be calculated—it is about 4.6 meV. The present experimental limit is at least twenty times larger.
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FUKUYAMA, TAKESHI, and HIROYUKI NISHIURA. "HIERARCHICAL MASSES AND UNIVERSAL MIXING IN QUARK–LEPTON MASS MATRICES." Modern Physics Letters A 28, no. 32 (October 6, 2013): 1350146. http://dx.doi.org/10.1142/s0217732313501460.

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The universality hypothesis for quark and lepton mixing matrices (CKM and MNS) is further developed. This hypothesis explains why the CKM is almost diagonal whereas the MNS is almost maximally mixed. If this hypothesis is true, the Dirac CP violating phase of the MNS mixing matrix is bounded around π or 0. Quark–lepton mass matrices which realize this hypothesis are constructed, showing simple power law relations among mass matrices for up-type, down-type quarks and neutrinos.
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Tanaka, S. "On the Lepton-Quark Masses." Progress of Theoretical Physics 81, no. 4 (April 1, 1989): 743–47. http://dx.doi.org/10.1143/ptp.81.743.

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Ma, Ernest. "Radiative quark and lepton masses." Nuclear Physics B - Proceedings Supplements 13 (February 1990): 603–5. http://dx.doi.org/10.1016/0920-5632(90)90138-k.

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SAWANAKA, HIDEYUKI. "QUARK AND LEPTON MASS MATRICES WITH A4 FAMILY SYMMETRY." International Journal of Modern Physics E 16, no. 05 (June 2007): 1383–93. http://dx.doi.org/10.1142/s0218301307006745.

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Realistic quark masses and mixing angles are obtained applying the successful A4 family symmetry for leptons, motivated by the quark-lepton assignments of SU (5). The A4 symmetry is suitable to give tri-bimaximal neutrino mixing matrix which is consistent with current experimental data. We study new scenario for the quark sector with the A4 symmetry.
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ROSEN, GERALD. "HEURISTIC DEVELOPMENT OF A DIRAC–GOLDHABER MODEL FOR LEPTON AND QUARK STRUCTURE." Modern Physics Letters A 22, no. 04 (February 10, 2007): 283–88. http://dx.doi.org/10.1142/s0217732307022621.

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All three charged lepton pole masses are given to O(10-5) accuracy by [Formula: see text], where θk = 2πk/3 + 2/9 with the generation number k = 1, 2, 3. In the context of a Dirac model, it is shown that this empirical formula for the charged leptons admits a satisfactory S3-parametrized extension for the scale-independent pole masses of quarks and Majorana neutrinos; in particular, the top quark mass emerges as 177.698 GeV. A physical-geometrical interpretation of the mass formula supports Dirac's and Goldhaber's proposals: leptons and quarks of the same generation are identical in size and shape. Specifically, their self-interaction mass appears to be concentrated on spherical surfaces of radii [Formula: see text], in which the Kähler radial complex coordinate zk is a root of the Calabi–Yau condition [Formula: see text] for the envelopment of the particle surfaces and ℓ is a fundamental length constant.
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Antusch, Stefan, and Constantin Sluka. "Testable SUSY spectra from GUTs at a 100 TeV pp collider." International Journal of Modern Physics A 31, no. 33 (November 22, 2016): 1644011. http://dx.doi.org/10.1142/s0217751x16440115.

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Grand Unified Theories (GUTs) are attractive candidates for more fundamental elementary particle theories. They cannot only unify the Standard Model (SM) interactions but also different types of SM fermions, in particular quarks and leptons, in joint representations of the GUT gauge group. We discuss how comparing predictive supersymmetric GUT models with the experimental results for quark and charged lepton masses leads to constraints on the SUSY spectrum. We show an example from a recent analysis where the resulting superpartner masses where found just beyond the reach of LHC Run 1, but fully within the reach of a 100 TeV [Formula: see text] collider.
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Dissertations / Theses on the topic "Quark and lepton masses"

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Malinsky, Michal. "Quark and Lepton Masses and Mixing in Supersymmetric Grand Unified Theories." Doctoral thesis, SISSA, 2005. http://hdl.handle.net/20.500.11767/4198.

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The material is organized as follows: the first chapter is devoted to several remarks on the two basic supersymmetric GUTs - first the minimal SUSY SU(5) is considered and the main shortcomings are pointed-out in brief, and in the second part these issues are addressed concerning a general class of SO(lO) models. This provides a natural motivation to approach and describe shortly the minimal SUSY SO(lO) scheme in the second chapter. The third chapter is dedicated to a detailed study of the correlations among the quark and lepton masses and mixing within the framework with dominant triplet seesaw contribution. An extended framework, a setup with an additional, quasidecoupled Higgs multiplet transforming as 120 of 50(10), is introduced and studied in detail in chapter 4. Chapter 5 is devoted to a class of alternative seesaw schemes emerging in theories with a spinorial 16 in the Higgs sector of SUSY and split-SUSY SO(lO) GUTs. Finally, a set of Appendices is added to coment on technical points in the main text.
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Ferrara, Valentina. "Extraction of the top quark mass from the total top quark pair production cross section in the single lepton channel." Doctoral thesis, Humboldt-Universität zu Berlin, Mathematisch-Naturwissenschaftliche Fakultät I, 2013. http://dx.doi.org/10.18452/16727.

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In dieser Arbeit wird eine Messung des totalen {\ttb} Produktions-Wirkungsquerschnitts im Einzellepton-Kanal vorgestellt. Der Wirkungsquerschnitt wird mittels einer Profile-Likelihood-Anpassung von Templates bestimmt, welche \"uber einen Lieklihood-Klassifikator unter Benutzung von vier kinematischen Variablen konstruiert werden. F\"ur ein Top-Quark der Masse $m_t=172.5$ GeV ergibt sich ein gemessener Wirkungsquerschnitt von $178.9 \pm 12$ pb, welcher innerhalb einer Standardabweichung mit den aktuellsten theoretischen Vorhersagen \"uberein stimmt. Um die Massenabh\"angigkeit des experimentellen Wirkungsquerschnitts zu bestimmen, wird die Messung f\"ur sieben weitere Werte der Top-Quarkmasse im Bereich zwischen 140 GeV und 200 GeV wiederholt. Mittels Vergleich dieser Massenabh\"angigkeit mit theoretischen Vorhersagen h\"oherer Ordnung wird die Top-Quarkmasse ermittelt. Diese Methode erlaubt die Bestimmung von zwei verschiedenen theoretischen Massenparametern: der Top-Quarkmasse im On-Shell-Schema $m_t^{\mathrm{pole}}$ sowie der Masse im $\overline{MS}$-Schema $\overline{m}_t(\overline{m}_t)$. Der Messwert mit der h\"ochsten erhaltenen Genauigkeit liegt bei $m_t^{\mathrm{pole}} = 171.2\pm 4.5$ GeV, und wird durch Verwendung der derzeit pr\"azisesten Berechnungen h\"oherer Ordnung im $\overline{MS}$-Schema erhalten. Dieser Wert stimmt innerhalb einer Standardabweichung mit den derzeitig besten Mittelwert von Messungen der Top-Quarkmasse am Tevatron \"uberein.
A measurement of the total {\ttb} production cross section in the single lepton channel is presented. The cross section is extracted in a profile likelihood fit of templates constructed from a likelihood classifier using four kinematic variables. For a top quark of mass $m_t=172.5$ GeV, the measured cross section is $178.9 \pm 12$ pb. The measurement agrees within one-standard deviation with the latest theoretical predictions. The cross section measurement is repeated for seven other values of the top quark mass ranging from 140 GeV to 200 GeV to obtain the mass dependence of the experimental cross section. By comparing this with the mass dependence of different higher-order predictions, the top quark mass is extracted. This method allows the determination of two different theoretical mass parameters: the top quark mass in the on-shell scheme $m_t^{\mathrm{pole}}$ and in the $\overline{MS}$ scheme $\overline{m}_t(\overline{m}_t)$. The most precise measurement obtained is $m_t^{\mathrm{pole}} = 171.2\pm 4.5$ GeV, obtained when employing the most precise higher-order calculations in the $\overline{MS}$ scheme. This value agrees within one-standard deviation with the latest Tevatron average of the best top quark mass measurements.
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Capelli, Laurent. "Étude des dimuons de la région des masses intermédiaires produits dans les collisions d'ions lourds auprès du SPS du CERN." Lyon 1, 2001. http://www.theses.fr/2001LYO10041.

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Dans cette thèse, nous étudions la production des dimuons dans une région de masse entre les résonances et j/ (région des masses intermédiaires, imr) dans les collisions proton-noyau et noyau-noyau de haute énergie. L'expérience Na50, installée auprès de l'accélérateur SPS du CERN, détecte les paires de muons émises dans ces interactions au moyen d'un spectromètre spécifique. La mesure de la centralité des collisions repose sur trois détecteurs indépendants : un calorimètre électromagnétique, un détecteur de multiplicité et un calorimètre a zéro degré. Les résultats des analyses proton-noyau fournissent une valeur de référence pour l'étude des intéractions noyau-noyau. Les distributions expérimentales, corrigées de l'acceptance et de la résolution par une méthode quadri-dimensionnelle, des dimuons IMR sont correctement reproduites par la superposition des processus conventionnels drell-yan et dd (désintégration des mesons charmes). L'extrapolation linéaire avec le nombre de masse des noyaux des résultats p-a aux collisions s-u et pb-pb, sous-estime systématiquement les spectres mesures dans la région des masses intermédiaires. Cet excès de dimuons imr augmente avec la centralité des collisions. Plusieurs modèles théoriques sont présentés et comparés aux données noyau-noyau. Nous montrons qu'un modèle base sur la diffusion des mesons d et d dans l'état final ne reproduit pas les distributions expérimentales. Finalement, cette étude permet de proposer deux explications possibles de l'excès observe. Les spectres noyau-noyau peuvent être reproduits soit par une augmentation de la production de charme soit par la présence de dimuons thermiques émis par un milieu dense et chaud.
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Wang, Ping. "Studies of lepton and quark interactions." Diss., Virginia Polytechnic Institute and State University, 1985. http://hdl.handle.net/10919/53614.

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Part I Proposed Experimental Tests of the Right-handed Weak Current All possible experiments which test the SU(2)L x U(1)R x U(1)B-L model and SU(2)L x SU(2)R x U(1)B-L model using the LEP e⁺e⁻ collider and HERA e⁻p collider are calculated and the most sensitive experiments are examined. Part II Semi-Phenomenological Theory of (Qq̅) System The (QQ̅) and (Qq̅) mesons are calculated using a QCD motivated potential model. It is discovered that by including a long distance relativistic correction term derived by Grome, the Coulomb + Linear potential works not only for c and b quarks, but s quark as well. The leptonic decay constants of various (Qq̅) mesons together with their masses are predicted. The topponium states are also discussed.
Ph. D.
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Souchlas, Nicholas. "Quark Dynamics and Constituent Masses in Heavy Quark Systems." Kent State University / OhioLINK, 2009. http://rave.ohiolink.edu/etdc/view?acc_num=kent1248013809.

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Kimchi, Itamar. "Quark masses : an environmental impact statement." Thesis, Massachusetts Institute of Technology, 2008. http://hdl.handle.net/1721.1/44761.

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Thesis (S.B.)--Massachusetts Institute of Technology, Dept. of Physics, 2008.
Includes bibliographical references (leaves 63-65).
We investigate how the requirement that organic chemistry be possible constrains the values of the quark masses. Specifically, we choose a slice through the parameter space of the Standard Model in which quark masses vary so that as many as three quarks play a role in the formation of nuclei, while keeping fixed the average mass of the two lightest baryons (in units of the electron mass) and the strength of the low-energy nuclear interaction. We classify universes on that slice as congenial if they contain stable nuclei with electric charge 1 and 6 (thus making organic chemistry possible in principle). Universes that lack one or both such stable nuclei are classified as uncongenial. We reassess the relationship between baryon masses and quark masses, using information in baryon mass differences in our world and the pion-nucleon sigma term [sigma]IIN. We generalize the Weizsacker semi-empirical mass formula through a degenerate Fermi gas model that handles the kinetic energy of new baryonic species as they begin to participate in the nucleus, and derive an expression for the asymmetry energy equivalent in the SU(3) limit through a minimization procedure on the quadratic Casimir operator. We spell out the conditions for decay by weak nucleon emission. Finally, we study the congeniality of various regions in the quark mass space, primarily by direct comparison to analog nuclei in our universe. Considering only two light quarks u and d, we find a band of congeniality roughly 29 MeV wide in mu - md, with our universe living comfortably away from the edge. We find multiple congeniality regions in the three quark mass space. For an important region around the SU(3) limit, we have not determined conclusive results but we have constructed the machinery to aid in its analysis and formulated the relevant problems. We have succeeded in formulating a well defined question about congeniality, and have made concrete progress toward answering it.
by Itamar Kimchi.
S.B.
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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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Antusch, Stefan. "The running of neutrino masses, lepton mixings and CP phases." [S.l. : s.n.], 2003. http://deposit.ddb.de/cgi-bin/dokserv?idn=969430248.

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Rimmer, Steven. "Neutrino masses and lepton flavour violating phenomena in the MSSM." Thesis, Durham University, 2007. http://etheses.dur.ac.uk/2521/.

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The most general supersymmetric model with minimal particle content and an additional discrete Ƶ(_3) symmetry, which allows lepton number violating terms, is considered. In this model, we calculate at the level of one-loop the resulting Majorana neutrino masses and the flavour violating radiative decays of charged leptons, ﺎ→ﺎ’γ. We first study the neutral scalar sector of the model, performing a calculable rotation of the scalar fields to a basis in which the sneutrino vacuum expectation values are zero. Lagrangian parameters are initialised without recourse to assumptions concerning trilinear or bilinear terms, CP-conservation or intergenerational mixing and one-loop corrections to the neutrino masses are analysed. We present scenarios in which the experimental data are reproduced. We find that with bilinear lepton number violating couplings in the superpotential of the order 1MeV the atmospheric mass scale can be reproduced. Certain trilinear superpotential couplings, usually of the order of the electron Yukawa coupling can give rise to either atmospheric or solar mass scales and bilinear supersymmetry breaking terms of the order 0.1 GeV(^2) can set the solar mass scale. Taking parameters which correctly describe the neutrino sector, we consider their repercussions in flavour violating radiative lepton decays. Such decays have not been observed and upper bounds on their branching ratios exist. We note that certain parameter sets, which correctly describe the neutrino sector, will also generate observable branching ratios and suggest four such sets as Benchmarks scenarios. We present as Appendices the full set of Feynman Rules for the general super- symmetric standard model with minimal particle content and details of the loop calculations in the Weyl spinor notation.
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Mes, Alexes K. "Light Quark Masses from QCD Finite Energy Sum Rules." Master's thesis, Faculty of Science, 2019. http://hdl.handle.net/11427/30901.

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Due to quark-gluon confinement in QCD, the quark masses entering the QCD Lagrangian cannot be measured with the same techniques one would use to determine the mass of non-confined particles. They must be determined either numerically from Lattice QCD, or analytically using QCD sum rules. The latter makes use of the complex squared energy plane, and Cauchy’s theorem for the correlator of axial-vector divergences. This procedure relates a QCD expression containing the quark masses, with an hadronic expression in terms of known hadron masses, couplings, and lifetimes/widths. Thus, the quark masses become a function of known hadronic information. In this dissertation, the light quark masses are determined from a QCD finite energy sum rule, using the pseudoscalar correlator to six-loop order in perturbative QCD, with the leading vacuum condensates and higher order quark mass corrections included. The systematic uncertainties stemming from the hadronic resonance sector are reduced, by introducing an integration kernel in the Cauchy integral in the complex squared energy plane. Additionally, the issue of convergence of the perturbative QCD expression for the pseudoscalar correlator is examined. Both the fixed order perturbation theory (FOPT) method and contour improved perturbation theory (CIPT) method are explored. Our results from the latter exhibit good convergence and stability in the window s0 = 3.0 − 5.0 GeV2 for the strange quark and s0 = 1.5 − 4.0 GeV2 for the up and down quarks; where s0 is the radius of the integration contour in the complex s-plane. The results are: ms(2 GeV) = 91.8 ± 9.9 MeV, mu(2 GeV) = 2.6 ± 0.4 MeV, md(2 GeV) = 5.3 ± 0.4 MeV, and the sum mud ≡ (mu + md)/2, is mud(2 GeV) = 3.9 ± 0.3 MeV. They compare favourably to the PDG and FLAG world averages. Further in this dissertation the updated series expansion of the quark mass renormalization group equation (RGE) to five-loop order is derived. The series provides the relation between a light quark mass in the modified minimal subtraction (MS) scheme defined at some given scale, e.g. at the tau-lepton mass scale, and another chosen energy scale, s. This relation explicitly depicts the renormalization scheme dependence of the running quark mass on the scale parameter, s, and is important in accurately determining a light quark mass at a chosen scale. The five-loop QCD β(as) and γ(as) functions are used in this determination.
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Books on the topic "Quark and lepton masses"

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Mohapatra, R. N. Unification and supersymmetry: The frontiersof quark-lepton physics. New York: Springer-Verlag, 1986.

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Mohapatra, R. N. Unification and supersymmetry: The frontiers of quark-lepton physics. 2nd ed. New York: Springer-Verlag, 1992.

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Unification and supersymmetry: The frontiers of quark-lepton physics. 3rd ed. New York: Springer, 2003.

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Mohapatra, Rabindra N. Unification and Supersymmetry: The Frontiers of Quark-Lepton Physics. New York, NY: Springer New York, 1992.

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Unification and supersymmetry: The frontiers of quark-lepton physics. New York: Springer-Verlag, 1986.

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Mohapatra, Rabindra N. Unification and Supersymmetry: The Frontiers of Quark-Lepton Physics. New York, NY: Springer New York, 1986.

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

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

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Marcano, Xabier. Lepton Flavor Violation from Low Scale Seesaw Neutrinos with Masses Reachable at the LHC. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-94604-7.

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Wang, Bigeng. Lattice calculation of the mass difference between the long- and short-lived K mesons for physical quark masses. [New York, N.Y.?]: [publisher not identified], 2021.

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Book chapters on the topic "Quark and lepton masses"

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Fritzsch, Harald. "The Pattern of Lepton and Quark Masses." In New Aspects of High-Energy Proton-Proton Collisions, 377–90. Boston, MA: Springer US, 1988. http://dx.doi.org/10.1007/978-1-4615-9540-3_20.

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Leutwyler, H. "Quark Masses and Chiral Symmetry." In Quarks, Leptons, and Their Constituents, 189–224. Boston, MA: Springer US, 1988. http://dx.doi.org/10.1007/978-1-4613-0889-8_5.

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Nielsen, Holger B., and Yasutaka Takanishi. "Family Replicated Fit of All Quark and Lepton Masses and Mixings." In Particle Physics in the New Millennium, 106–18. Berlin, Heidelberg: Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/3-540-36539-7_8.

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Dominguez, Cesareo A. "Quark Masses." In SpringerBriefs in Physics, 59–67. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-97722-5_9.

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Povh, Bogdan, and Mitja Rosina. "Quasielastische Lepton-Quark-Streuung." In Streuung und Strukturen, 27–44. Berlin, Heidelberg: Springer Berlin Heidelberg, 2002. http://dx.doi.org/10.1007/978-3-642-55962-4_3.

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Neubert, Matthias. "Heavy-Quark Masses." In NATO ASI Series, 115–48. Boston, MA: Springer US, 1997. http://dx.doi.org/10.1007/978-1-4899-0242-9_5.

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Leutwyler, H. "Light-Quark Masses." In NATO ASI Series, 149–64. Boston, MA: Springer US, 1997. http://dx.doi.org/10.1007/978-1-4899-0242-9_6.

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Schmüser, Peter. "Lepton-Quark-Wechselwirkungen, Parton-Modell." In Feynman-Graphen und Eichtheorien für Experimentalphysiker, 105–26. Berlin, Heidelberg: Springer Berlin Heidelberg, 1995. http://dx.doi.org/10.1007/978-3-642-57766-6_7.

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Mohapatra, Rabindra N. "Superstrings and Quark-Lepton Physics." In Unification and Supersymmetry, 342–401. New York, NY: Springer New York, 1992. http://dx.doi.org/10.1007/978-1-4757-4373-9_17.

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Specht, Hans J. "Direct photon and lepton production in high energy collisions." In Quark Matter '84, 221–39. Berlin, Heidelberg: Springer Berlin Heidelberg, 1985. http://dx.doi.org/10.1007/3-540-15183-4_37.

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Conference papers on the topic "Quark and lepton masses"

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ARNOWITT, R., B. DUTTA, and B. HU. "QUARK, LEPTON AND NEUTRINO MASSES IN HORAVA-WITTEN INSPIRED MODELS." In Proceedings of the First International Conference. WORLD SCIENTIFIC, 2003. http://dx.doi.org/10.1142/9789812704917_0013.

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Hung, P. Q. "Rare Κ decays in a model of quark and lepton masses." In COSMOLOGY AND ELEMENTARY PARTICLE PHYSICS: Coral Gables Conference on Cosmology and Elementary Particle Physics. AIP, 2002. http://dx.doi.org/10.1063/1.1492182.

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BARBIERI, RICCARDO. "QUARK MASSES AND WEAK COUPLINGS IN THE SM AND BEYOND." In Proceedings of the XX International Symposium on Lepton and Photon Interactions at High Energies. WORLD SCIENTIFIC, 2002. http://dx.doi.org/10.1142/9789812777881_0011.

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Antusch, Stefan, Pyungwon Ko, and Deog Ki Hong. "SUSY Threshold Effects on Quark and Lepton Masses at the GUT Scale." In SUPERSYMMETRY AND THE UNIFICATION OF FUNDAMENTAL INTERACTIONS. AIP, 2008. http://dx.doi.org/10.1063/1.3051960.

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Koide, Yoshio. "Masses and Mixings of Quarks and Leptons." In International Workshop on Masses and Mixings of Quarks and Leptons. WORLD SCIENTIFIC, 1998. http://dx.doi.org/10.1142/9789814528924.

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Gasser, Jürg. "Quark Masses." In LOW ENERGY ANTIPROTON PHYSICS: Eighth International Conference on Low Energy Antiproton Physics (LEAP '05). AIP, 2005. http://dx.doi.org/10.1063/1.2130131.

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Martinelli, Guido. "Quark Masses." In 8th International Symposium on Heavy Flavour Physics. Trieste, Italy: Sissa Medialab, 1999. http://dx.doi.org/10.22323/1.003.0004.

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Sanfilippo, Francesco. "Quark masses." In The 32nd International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2015. http://dx.doi.org/10.22323/1.214.0014.

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Nakamura, Yoshifumi. "Simulating at realistic quark masses: light quark masses." In XXIVth International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2006. http://dx.doi.org/10.22323/1.032.0160.

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Leutwyler, Heinrich. "Light quark masses." In 6th International Workshop on Chiral Dynamics. Trieste, Italy: Sissa Medialab, 2010. http://dx.doi.org/10.22323/1.086.0005.

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Reports on the topic "Quark and lepton masses"

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Harrington, Robert Duane. Measurement of the top quark mass in lepton+jets events with secondary vertex tagging. Office of Scientific and Technical Information (OSTI), February 2007. http://dx.doi.org/10.2172/918709.

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Fedorko, Wojciech T. Measurement of the Top Quark Mass Simultaneously in Dilepton and Lepton + Jets Decay Channels. Office of Scientific and Technical Information (OSTI), December 2008. http://dx.doi.org/10.2172/938899.

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Brubaker, Erik Matthews. A Measurement of the Mass of the Top Quark in Lepton + Jets Events at CDF. Office of Scientific and Technical Information (OSTI), January 2004. http://dx.doi.org/10.2172/15017205.

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Hare, Matthew Frederick. Measurement of the Top Quark Mass in the Di-lepton Channel using the Dalitz-Goldstein Method. Office of Scientific and Technical Information (OSTI), October 2010. http://dx.doi.org/10.2172/1018349.

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Adelman, Jahred A. Measurement of the Top Quark Mass at CDF Using the Template Method in the Lepton + Jets Channel. Office of Scientific and Technical Information (OSTI), June 2008. http://dx.doi.org/10.2172/947630.

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Tosciri, Cecilia. Approaching the CDF Top Quark Mass Legacy Measurement in the Lepton+Jets channel with the Matrix Element Method. Office of Scientific and Technical Information (OSTI), January 2016. http://dx.doi.org/10.2172/1334264.

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Chan, Kwok Ming. Anomalous Gluon-top Quark-anti-top quark Coupling in Single-lepton Top-anti-topquark Events from Proton-anti-proton Collisions at Center of Mass Energy = 1.8-TeV. Office of Scientific and Technical Information (OSTI), January 2006. http://dx.doi.org/10.2172/1369274.

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Fatakia, Sarosh Noshir. A Measurement of the Mass of the Top Quark in the Di-Lepton Channels Using the DØ Detector at Fermilab. Office of Scientific and Technical Information (OSTI), January 2005. http://dx.doi.org/10.2172/15017181.

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Schieferdecker, Philipp. Measurement of the Top Quark Mass at D0 Run II with the Matrix Element Method in the Lepton+Jets Final State. Office of Scientific and Technical Information (OSTI), August 2005. http://dx.doi.org/10.2172/875532.

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Kubo, Taichi. Measurement of the Top Quark Mass by Dynamical Likelihood Method using the Lepton + Jets Events with the Collider Detector at Fermilab. Office of Scientific and Technical Information (OSTI), February 2008. http://dx.doi.org/10.2172/935478.

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You might also be interested in the extended bibliographies on the topic 'Quark and lepton masses' for particular source types:
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