Results 121 to 130 of about 34,461,409 (228)
SU(2) and SU(3) Yang-Mills thermodynamics and some implications
We sketch the development of effective theories for SU(2) and SU(3) Yang-Mills thermodynamics. The most important results are quoted and some implications for particle physics and cosmology are discussed.Comment: 18 pages, 5 figures, v3: consequences of ...
Hofmann, Ralf
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Running neutrino masses and mixing in a SU(4) x SU(2)^2 x U(1)_X model
In this talk, we discuss the implications of the renormalization group equations for the neutrino masses and mixing angles in a supersymmetric string-inspired SU(4) x SU(2)_L x SU(2)_R x U(1)_X model with matter in fundamental and antisymmetric tensor ...
A Psallidas +13 more
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Fermionic and parafermionic CFTs with su ̂ 2 $$ \hat{su}(2) $$ and su ̂ 3 $$ \hat{su}(3) $$ symmetry
We investigate two-dimensional conformal field theories (CFTs) with affine su ̂ 2 $$ \hat{su}(2) $$ and su ̂ 3 $$ \hat{su}(3) $$ algebra symmetry.
Kohki Kawabata
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SU(2/1) superchiral self-duality: a new quantum, algebraic and geometric paradigm to describe the electroweak interactions. [PDF]
Thierry-Mieg J, Jarvis P.
europepmc +1 more source
Orbital measures on SU(2)/SO(2)
We let U=SU(2) and K=SO(2) and denote N_{U}(K) the normalizer of K in U. For a an element of U\ N_{U} (K), we let \mu_{a} be the normalized singular measure supported in KaK. For p a positive integer, it was proved that \mu_{a}^{( p)}, the convolution of
Anchouche, Boudjemaa +2 more
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Supplement to the checklist of vascular plants of Guangxi, China(IX)
Eleven species of vascular plants are reported as new records to northwestern Guangxi of China, viz. Pteris amoena Blume in the Pteridaceae, Diplaziopsis cavaleriana (Christ)C. Chr. in the Diplaziopsidaceae, Diplazium nanchuanicum(W. M. Chu)Z. R.
SU Chunlan1, 2, NONG Suyun2, HUANG Yusong2, LIU Yan2*
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v1-Periodic 2-exponents of SU(2^e) and SU(2^e + 1)
8 ...
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SU(2) × SU(2) breaking and the Cabibbo angle
Abstract In a recent investigation of the transformation properties under chiral SU(3) × SU(3) of the hadron energy density H ( X ) Gell-Mann, Oakes and Renner have assumed the form H = H − H 0 − CU 8 where H is SU(3) × SU(3) invariant while U 0 and U 8 belong to the representation (3 ∗ , 3) + (3, 3 ∗ ) and have ...
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SU(4)⊗SU(2)L⊗SU(2)R as a surrogate SUSY GUT
Abstract We consider a supersymmetric SU (4)⊗ SU (2) L ⊗ SU (2) R model broken at 10 16 GeV, and propose natural solutions to the problems of Planck-scale unification and light fermion masses in this model. The resulting model shares many of the successes of conventional SUSY GUTs such as the successful prediction of sin 2 θ w and Yukawa ...
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