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Journal articles on the topic 'Yukawa couplings'

Author: Grafiati

Published: 4 June 2021

Last updated: 17 February 2022

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1

CASAS, J. A., F. GOMEZ, and C. MUÑOZ. "COMPLETE STRUCTURE OF Zn YUKAWA COUPLINGS." International Journal of Modern Physics A 08, no. 03 (January 30, 1993): 455–505. http://dx.doi.org/10.1142/s0217751x93000187.

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We give the complete twisted Yukawa couplings for all the Zn orbifold constructions in the most general case, i.e. when orbifold deformations are considered. This includes a certain number of tasks. Namely, determination of the allowed couplings, calculation of the explicit dependence of the Yukawa couplings values on the moduli expectation values (i.e. the parameters determining the size and shape of the compactified space), etc. The final expressions are completely explicit, which allows a counting of the different Yukawa couplings for each orbifold (with and without deformations). This knowledge is crucial to determine the phenomenological viability of the different schemes, since it is directly related to the fermion mass hierarchy. Other facts concerning the phenomenological profile of Zn orbifolds are also discussed, e.g. the existence of nondiagonal entries in the fermion mass matrices, which is related to a nontrivial structure of the Kobayashi-Maskawa matrix. Some theoretical results are also given, e.g. the non-participation of (1,2) moduli in twisted Yukawa couplings. Likewise, (1,1) moduli associated with fixed tori which are involved in the Yukawa coupling, do not affect the value of the coupling. We discuss the relevance of these facts for the supersymmetry breaking process.

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2

Cherchiglia, Adriano, Dominik Stöckinger, and Hyejung Stöckinger-Kim. "The muon g – 2 for low-mass pseudoscalar Higgs in the general 2HDM." EPJ Web of Conferences 179 (2018): 01022. http://dx.doi.org/10.1051/epjconf/201817901022.

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The two-Higgs doublet model is a simple and attractive extension of the Standard Model. It provides a possibility to explain the large deviation between theory and experiment in the muon g – 2 in an interesting parameter region: light pseudoscalar Higgs A, large Yukawa coupling to τ-leptons, and general, non-type II Yukawa couplings are preferred. This parameter region is explored, experimental limits on the relevant Yukawa couplings are obtained, and the maximum possible contributions to the muon g – 2 are discussed.

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3

KOBAYASHI, TATSUO. "MINIMAL STRING UNIFICATION AND YUKAWA COUPLINGS IN ORBIFOLD MODELS." International Journal of Modern Physics A 10, no. 10 (April 20, 1995): 1393–411. http://dx.doi.org/10.1142/s0217751x9500067x.

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We study the minimal supersymmetric standard model derived from ZN×ZM orbifold models. Moduli-dependent threshold corrections of gauge couplings are investigated to explain the measured values of the coupling constants. We also study the Yukawa couplings of the models. We find that the Z2×Z2×Z6′, Z3×Z6 and Z6×Z6 orbifold models have the possibility of deriving Yukawa couplings for the second and third generations as well as the measured gauge coupling constants. Allowed models are shown explicitly by combinations of modular weights for the matter fields.

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4

Sashikanta Singh, Konsam, and N. Nimai Singh. "Effects of the Variation of SUSY Breaking Scale on Yukawa and Gauge Couplings Unification." Advances in High Energy Physics 2015 (2015): 1–8. http://dx.doi.org/10.1155/2015/652029.

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The present analysis addresses an interesting primary question on how do the gauge and Yukawa couplings unification scales vary with varying SUSY breaking scalesms, assuming a single scale for all supersymmetric particles. It is observed that the gauge coupling unification scale increases withmswhereas third-generation Yukawa couplings unification scale decreases withms. The rising of the unification scale and also the mass of the color triplet multiplets is necessary to increase the proton decay lifetime; the analysis is carried out with two-loop RGEs for the gauge and Yukawa couplings within the minimal supersymmetric SU(5) model, while ignoring for simplicity the threshold effects of the heavy particles, which could be as large as a few percentages.

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5

LUCHA, WOLFGANG, and MICHAEL MOSER. "CLIFFORD ALGEBRAS IN FINITE QUANTUM FIELD THEORIES I." International Journal of Modern Physics A 13, no. 13 (May 20, 1998): 2047–73. http://dx.doi.org/10.1142/s0217751x98000901.

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Finite quantum field theories may be constructed from the most general renormalizable quantum field theory by forbidding, order by order in the perturbative loop expansion, all ultraviolet-divergent renormalizations of the physical parameters of the theory. The relevant finiteness conditions resulting from this requirement relate all dimensionless couplings in the theory. At first sight, Yukawa couplings which are equivalent to the generators of some Clifford algebra with identity element represent a very promising type of solutions of the condition for one-loop finiteness of the Yukawa couplings. However, under a few reasonable and simplifying assumptions about their particular structure, these Clifford-like Yukawa couplings prove to be in conflict with the requirements of one- and two-loop finiteness of the gauge coupling and of the absence of gauge anomalies, at least for all simple gauge groups up to and including rank 8.

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6

Giudice, Gian F., and Oleg Lebedev. "Higgs-dependent Yukawa couplings." Physics Letters B 665, no. 2-3 (July 2008): 79–85. http://dx.doi.org/10.1016/j.physletb.2008.05.062.

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7

Fraser, Sean, and Ernest Ma. "Anomalous Higgs Yukawa couplings." EPL (Europhysics Letters) 108, no. 1 (October 1, 2014): 11002. http://dx.doi.org/10.1209/0295-5075/108/11002.

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8

Branco, Gustavo C., and J. I. Silva-Marcos. "Non-hermitian Yukawa couplings?" Physics Letters B 331, no. 3-4 (July 1994): 390–94. http://dx.doi.org/10.1016/0370-2693(94)91069-3.

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9

Stephenson, D., and A. Thornton. "Non-perturbative Yukawa couplings." Physics Letters B 212, no. 4 (October 1988): 479–82. http://dx.doi.org/10.1016/0370-2693(88)91800-x.

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10

CVETIČ, MIRJAM, and PAUL LANGACKER. "NEW GAUGE BOSONS FROM STRING MODELS." Modern Physics Letters A 11, no. 15 (May 20, 1996): 1247–62. http://dx.doi.org/10.1142/s0217732396001260.

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We address the mass ranges of new neutral gauge bosons and constraints on the accompanying exotic particles as predicted by a class of superstring models. Under certain assumptions about the supersymmetry breaking parameters we show that breaking of an additional U(1)′ symmetry is radiative when the appropriate Yukawa couplings of exotic particles are of order one, analogous to the radiative breaking of the electroweak symmetry in the supersymmetric standard model due to the large top-quark Yukawa coupling. Such large Yukawa couplings occur for a large class of string models. The Z′ and exotic masses are either of [Formula: see text], or of a scale intermediate between the string and electroweak scales. In the former case, [Formula: see text] may be achieved without excessive fine-tuning, and is within future experimental reach.

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11

Cynolter, G., J. Kovács, and E. Lendvai. "Doublet–singlet model and unitarity." Modern Physics Letters A 31, no. 01 (January 3, 2016): 1650013. http://dx.doi.org/10.1142/s0217732316500139.

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We study the renormalizable singlet–doublet fermionic extension of the Standard Model (SM). In this model, the new vector-like fermions couple to the gauge bosons and to the Higgs via new Yukawa couplings that allow for nontrivial mixing in the new sector, providing a stable, neutral dark matter candidate. Approximate analytic formulae are given for the mass spectrum around the blind spots, where the dark matter candidate coupling to h or Z vanishes. We calculate the two particle scattering amplitudes in the model, impose the perturbative unitarity constraints and establish bounds on the Yukawa couplings.

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12

Strominger, Andrew. "Yukawa Couplings in Superstring Compactification." Physical Review Letters 55, no. 23 (December 2, 1985): 2547–50. http://dx.doi.org/10.1103/physrevlett.55.2547.

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13

Grza̧dkowski, B., and M. Linder. "Nonlinear evolution of Yukawa couplings." Physics Letters B 193, no. 1 (July 1987): 71–77. http://dx.doi.org/10.1016/0370-2693(87)90458-8.

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14

Branco, G. C., J. I. Silva-Marcos, and M. N. Rebelo. "Universal strength for Yukawa couplings." Physics Letters B 237, no. 3-4 (March 1990): 446–50. http://dx.doi.org/10.1016/0370-2693(90)91204-o.

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15

Anderson, Lara B., James Gray, Dan Grayson, Yang-Hui He, and André Lukas. "Yukawa Couplings in Heterotic Compactification." Communications in Mathematical Physics 297, no. 1 (March 19, 2010): 95–127. http://dx.doi.org/10.1007/s00220-010-1033-8.

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16

BHATTACHARYYA, GAUTAM, JOHN ELLIS, and K. SRIDHAR. "NEW LEP CONSTRAINTS ON SOME SUPERSYMMETRIC YUKAWA INTERACTIONS THAT VIOLATE R-PARITY." Modern Physics Letters A 10, no. 22 (July 20, 1995): 1583–91. http://dx.doi.org/10.1142/s0217732395001708.

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We consider one-loop corrections to partial widths of the Z induced by supersymmetric Yukawa interactions that violate R-parity. The precise experimental values of the leptonic Z partial widths bound these Yukawa couplings, with the most interesting constraints being those on couplings involving τ, since previous constraints on them were very mild.

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17

Chishtie, F. A., M. D. Lepage, D. GC McKeon, T. G. Steele, and I. Zakout. "Exact one-loop running couplings in the standard model." Canadian Journal of Physics 86, no. 9 (September 1, 2008): 1067–70. http://dx.doi.org/10.1139/p08-036.

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Taking the dominant couplings in the standard model to be the quartic scalar coupling, the Yukawa coupling of the top quark, and the SU(3) gauge coupling, we consider their associated running couplings to one-loop order. Despite the nonlinear nature of the differential equations governing these functions, we show that they can be solved exactly. The nature of these solutions is discussed and their singularity structure is examined. It is shown that for a sufficiently small Higgs mass, the quartic scalar coupling decreases with increasing energy scale and becomes negative, indicative of vacuum instability. This behavior changes for a Higgs mass greater than 168 GeV, beyond which this couplant increases with increasing energy scales and becomes singular prior to the ultraviolet pole of the Yukawa coupling. Upper and lower bounds on the Higgs mass corresponding to new physics at the TeV scale are obtained and compare favourably with the numerical results of the one-loop and two-loop analyses with inclusion of electroweak couplings.PACS Nos.: 11.10.Hi, 14.80.Bn

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18

PASUPATHY, J. "A CALCULATION OF HIGGS MASS IN THE STANDARD MODEL." Modern Physics Letters A 15, no. 26 (August 30, 2000): 1605–10. http://dx.doi.org/10.1142/s0217732300002140.

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The assumption that the ratio of the Higgs self-coupling to the square of its Yukawa coupling to the top is (almost) independent of the renormalization scale fixes the Higgs mass within narrow limits at m H =160 GeV using only the values of gauge couplings and top mass.

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19

Borzumati, Francesca, Glennys R. Farrar, Nir Polonsky, and Scott Thomas. "Soft Yukawa couplings in supersymmetric theories." Nuclear Physics B 555, no. 1-2 (August 1999): 53–115. http://dx.doi.org/10.1016/s0550-3213(99)00328-4.

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20

Candelas, P. "Yukawa couplings between (2, 1)-forms." Nuclear Physics B 298, no. 3 (March 1988): 458–92. http://dx.doi.org/10.1016/0550-3213(88)90351-3.

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21

Bena, Iosif, Sebastian de Haro, and Radu Roiban. "Generalized Yukawa couplings and matrix models." Nuclear Physics B 664, no. 1-2 (August 2003): 45–58. http://dx.doi.org/10.1016/s0550-3213(03)00434-6.

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22

Abdalgabar, Ammar, Mohammed Omer Khojali, Alan S. Cornell, Giacomo Cacciapaglia, and Aldo Deandrea. "Unification of gauge and Yukawa couplings." Physics Letters B 776 (January 2018): 231–35. http://dx.doi.org/10.1016/j.physletb.2017.11.033.

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23

Saldaña-Salazar, U. J. "A principle for the Yukawa couplings." Journal of Physics: Conference Series 761 (October 2016): 012064. http://dx.doi.org/10.1088/1742-6596/761/1/012064.

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24

Deandrea, Aldo. "Unification of gauge and Yukawa couplings." Journal of Physics: Conference Series 1271 (July 2019): 012016. http://dx.doi.org/10.1088/1742-6596/1271/1/012016.

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25

Braun, Volker, Yang-Hui He, and Burt A. Ovrut. "Yukawa couplings in heterotic standard models." Journal of High Energy Physics 2006, no. 04 (April 10, 2006): 019. http://dx.doi.org/10.1088/1126-6708/2006/04/019.

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26

Miyata, Hideo, Noriyasu Ohtsubo, and Hiroshi Sugimoto. "Yukawa couplings in Feigin-Fuchs construction." Physics Letters B 269, no. 3-4 (October 1991): 319–24. http://dx.doi.org/10.1016/0370-2693(91)90178-s.

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27

Kobayashi, Tatsuo, and Noriyasu Ohtsubo. "Allowed Yukawa couplings of orbifold models." Physics Letters B 262, no. 4 (June 1991): 425–31. http://dx.doi.org/10.1016/0370-2693(91)90616-x.

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28

Shigemitsu, Junko. "Renormalized yukawa couplings from the lattice." Physics Letters B 226, no. 3-4 (August 1989): 364–68. http://dx.doi.org/10.1016/0370-2693(89)91211-2.

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29

Kawarabayashi, Ken, and Koichi Ohta. "Yukawa couplings in meson-soliton scattering." Physics Letters B 216, no. 1-2 (January 1989): 205–11. http://dx.doi.org/10.1016/0370-2693(89)91396-8.

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30

Shigemitsu, Junko. "Renormalized Yukawa couplings from the lattice." Nuclear Physics B - Proceedings Supplements 17 (September 1990): 657–60. http://dx.doi.org/10.1016/0920-5632(90)90336-s.

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31

Antoniadis, I., E. Gava, K. S. Narain, and T. R. Taylor. "Superstring threshold corrections to Yukawa couplings." Nuclear Physics B 407, no. 3 (October 1993): 706–24. http://dx.doi.org/10.1016/0550-3213(93)90095-7.

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32

SKARKE, HARALD. "TOWARDS FINITENESS WITHOUT SUPERSYMMETRY." International Journal of Modern Physics A 09, no. 05 (February 20, 1994): 711–26. http://dx.doi.org/10.1142/s0217751x94000339.

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Some aspects of finite quantum field theories in 3+1 dimensions are discussed. A model with nonsupersymmetric particle content and vanishing one- and two-loop beta functions for the gauge coupling and one-loop beta functions for Yukawa couplings is presented.

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33

LUCHA, WOLFGANG, and FRANZ F. SCHÖBERL. "A PARTICULAR CLASS OF GUTS WITH VANISHING ONE-LOOP BETA FUNCTIONS." International Journal of Modern Physics A 09, no. 32 (December 30, 1994): 5791–800. http://dx.doi.org/10.1142/s0217751x94002399.

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By explicit solution of the one-loop finiteness conditions for gauge and quartic scalar-boson self-interaction coupling constants, a particular class of grand unified theories with vanishing Yukawa couplings as well as vanishing one-loop renormalization-group beta functions is constructed.

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34

GRANDITS, PETER. "TOWARDS A CLASSIFICATION OF FINITE FIELD THEORIES." Modern Physics Letters A 09, no. 27 (September 7, 1994): 2555–67. http://dx.doi.org/10.1142/s0217732394002410.

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We consider the finiteness conditions on the Yukawa couplings of a general quantum field theory for gauge groups SU (n)(n>6) and a rather general particle content. It is shown that in the class of theories considered (149 different particle contents), only two models are able to fulfill the finiteness conditions. Only one of these is supersymmetric. For the nonsupersymmetric one the appropriate Yukawa couplings are constructed explicitly.

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35

Hou, Wei-Shu. "Bootstrap Dynamical Symmetry Breaking." Advances in High Energy Physics 2013 (2013): 1–19. http://dx.doi.org/10.1155/2013/650617.

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Despite the emergence of a 125 GeV Higgs-like particle at the LHC, we explore the possibility of dynamical electroweak symmetry breaking by strong Yukawa coupling of very heavy new chiral quarksQ. Taking the 125 GeV object to be a dilaton with suppressed couplings, we note that the Goldstone bosonsGexist as longitudinal modesVLof the weak bosons and would couple toQwith Yukawa couplingλQ. WithmQ≳700 GeV from LHC, the strongλQ≳4could lead to deeply boundQQ¯states. We postulate that the leading “collapsed state,” the color-singlet (heavy) isotriplet, pseudoscalarQQ¯mesonπ1, isGitself, and a gap equation without Higgs is constructed. Dynamical symmetry breaking is affected via strongλQ, generatingmQwhile self-consistently justifying treatingGas massless in the loop, hence, “bootstrap,” Solving such a gap equation, we find thatmQshould be several TeV, orλQ≳4π, and would become much heavier if there is a light Higgs boson. For such heavy chiral quarks, we find analogy with theπ−Nsystem, by which we conjecture the possible annihilation phenomena ofQQ¯→nVLwith high multiplicity, the search of which might be aided by Yukawa-boundQQ¯resonances.

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36

CERESOLE, A., R. D’AURIA, S. FERRARA, W. LERCHE, and J. LOUIS. "PICARD-FUCHS EQUATIONS AND SPECIAL GEOMETRY." International Journal of Modern Physics A 08, no. 01 (January 10, 1993): 79–113. http://dx.doi.org/10.1142/s0217751x93000047.

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We investigate the system of holomorphic differential identities implied by special Kählerian geometry of four-dimensional N=2 supergravity. For superstring compactifications on Calabi-Yau threefolds these identities are equivalent to the Picard-Fuchs equations of algebraic geometry that are obeyed by the periods of the holomorphic three-form. For one variable they reduce to linear fourth-order equations which are characterized by classical W generators; we find that the instanton corrections to the Yukawa couplings are directly related to the nonvanishing of w4. We also show that the symplectic structure of special geometry can be related to the fact that the Yukawa couplings can be written as triple derivatives of some holomorphic function F. Moreover, we give the precise relationship of the Yukawa couplings of special geometry with three-point functions in topological field theory.

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37

ILTAN, E. O. "THE RADIATIVE h0(A0)→γγ DECAYS IN THE TWO-HIGGS DOUBLET MODEL." Modern Physics Letters A 19, no. 29 (September 21, 2004): 2215–25. http://dx.doi.org/10.1142/s0217732304014823.

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We study the radiative h0(A0)→γγ decays in the framework of the general two-Higgs doublet model, the so-called model III. We estimate the decay width of the processes at the order of magnitude of 10-2 GeV for the intermediate values of the Yukawa couplings. We observe that the analysis of the two-photon system provides a comprehensive information for the complex nature of the Yukawa couplings and therefore, the source of the CP violation.

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38

IOANNISIAN, ARA, and APOSTOLOS PILAFTSIS. "LABORATORY LIMITS ON THEORIES WITH STERILE NEUTRINOS IN THE BULK." International Journal of Modern Physics A 16, supp01c (September 2001): 931–33. http://dx.doi.org/10.1142/s0217751x01008527.

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We discuss the phenomenological consequences of theories which describe sterile neutrinos in large extra dimensions, in the so-called bulk. We briefly outline how the cumulative non-decoupling effect due to the tower of Kaluza-Klein singlet neutrinos may equivalently be described by a higher-dimensional effective theory with original order-unity Yukawa couplings. Based on this cumulative phenomenon, we obtain strong constraints on the fundamental quantum gravity scale and/or on the higher-dimensional Yukawa couplings.

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39

HABA, N., and N. OKAMURA. "YUKAWA INTERACTION FROM A SUPERSYMMETRIC COMPOSITE MODEL." Modern Physics Letters A 13, no. 10 (March 28, 1998): 759–67. http://dx.doi.org/10.1142/s0217732398000826.

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We present a composite model that is based on nonperturbative effects of N=1 supersymmetric SU (NC) gauge theory with Nf=NC+1 flavors. In this letter, we consider NC=7, where all fields of one generation (quarks, leptons and Higgs) are bound states of preons and anti-preons. When SU (7)H coupling becomes strong. Yukawa couplings of quarks and leptons are generated dynamically. We show the one-generation model first and then we try to extend it to the three-generation model.

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40

KOBAYASHI, TATSUO, NORIYASU OHTSUBO, and KAZUTAKA TANIOKA. "THE Z4 × Z4 ORBIFOLD MODEL AT AN ENHANCEMENT POINT AND THE 26 MODEL." International Journal of Modern Physics A 08, no. 20 (August 10, 1993): 3553–63. http://dx.doi.org/10.1142/s0217751x93001430.

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We construct a "shifted" Z4 × Z4 orbifold model equivalent to a twisted Z4 × Z4 orbifold model at an enhancement point. It is proved that the N = 2 algebra of the 26 model is coincident with that of the "shifted" orbifold model. The correspondence between the Z4 × Z4 orbifold model and the 26 model is investigated with respect to massless spectra and Yukawa couplings. Also studied are Yukawa couplings and some other aspects of the models away from the enhancement point.

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41

Gepner, Doron. "Yukawa couplings for Calabi-Yau string compactification." Nuclear Physics B 311, no. 1 (December 1988): 191–204. http://dx.doi.org/10.1016/0550-3213(88)90147-2.

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42

Kobayashi, Tatsuo, and Oleg Lebedev. "Heterotic Yukawa couplings and continuous Wilson lines." Physics Letters B 566, no. 1-2 (July 2003): 164–70. http://dx.doi.org/10.1016/s0370-2693(03)00560-4.

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43

Lebedev, Oleg. "CP violation with Higgs-dependent Yukawa couplings." Physics Letters B 697, no. 1 (February 2011): 58–62. http://dx.doi.org/10.1016/j.physletb.2011.01.048.

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44

Whisnant, K., Bing-Lin Young, and X. Zhang. "Unitarity and anomalous top-quark Yukawa couplings." Physical Review D 52, no. 5 (September 1, 1995): 3115–18. http://dx.doi.org/10.1103/physrevd.52.3115.

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45

Faraggi, Alon E. "Yukawa couplings in superstring-derived standardlike models." Physical Review D 47, no. 11 (June 1, 1993): 5021–28. http://dx.doi.org/10.1103/physrevd.47.5021.

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46

Leontaris, G. K. "Yukawa couplings in F-theory SU(5)." Fortschritte der Physik 59, no. 11-12 (July 18, 2011): 1154–58. http://dx.doi.org/10.1002/prop.201100052.

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47

Griest, Kim, and Marc Sher. "Radiative corrections due to enhanced Yukawa couplings." Physical Review D 33, no. 7 (April 1, 1986): 2039–42. http://dx.doi.org/10.1103/physrevd.33.2039.

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48

Cremades, D., L. E. Ibanez, and F. Marchesano. "Computing Yukawa Couplings from Magnetized Extra Dimensions." Journal of High Energy Physics 2004, no. 05 (June 2, 2004): 079. http://dx.doi.org/10.1088/1126-6708/2004/05/079.

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49

Cremades, Daniel, Luis E. Ibánez, and Fernando Marchesano. "Yukawa couplings in intersecting D-brane models." Journal of High Energy Physics 2003, no. 07 (July 16, 2003): 038. http://dx.doi.org/10.1088/1126-6708/2003/07/038.

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50

Mandal, Gautam, and Spenta R. Wadia. "Non-renormalization of Yukawa couplings on orbifolds." Physics Letters B 195, no. 4 (September 1987): 547–53. http://dx.doi.org/10.1016/0370-2693(87)91571-1.

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