Results 11 to 20 of about 140 (98)
The main goal of this paper is to introduce the notion of stabilizers in EQ-algebras and develop stabilizer theory in EQ-algebras. In the paper, we introduce (fuzzy) left and right stabilizers and investigate some related properties of them.
Cheng Xiao Yun +3 more
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Multileptonic signals of co-annihilating left-right supersymmetric dark matter [PDF]
20 pages, 4 figures, revised ...
Chatterjee, Arindam +6 more
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The Armendariz module and its application to the Ikeda-Nakayama module
A ring R is called a right Ikeda-Nakayama (for short IN-ring) if the left annihilator of the intersection of any two right ideals is the sum of the left annihilators, that is, if ℓ(I∩J)=ℓ(I)+ℓ(J) for all right ideals I and J of R. R is called Armendariz
M. Tamer Koşan
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Left annihilator of identities with generalized derivations in prime and semiprime rings
Let R be a noncommutative prime ring of char (R) ≠ 2, F a generalized derivation of R associated to the derivation d of R and I a nonzero ideal of R. Let S ⊆ R. The left annihilator of S in R is denoted by lR(S) and defined by lR (S) = {x ∈ R | xS = 0}. In the present paper, we study the left annihilator of the sets {F (x)◦n F (y)−x◦n y | x, y ∈ I} and
openaire +2 more sources
The main goal of this paper is to introduce the notion of stabilizers in \(L\)-algebras and develop stabilizer theory in \(L\)-algebras. In this paper, we introduced the notions of left and right stabilizers and investigated some related properties of ...
Gholam Reza Rezaei, Mona Aaly Kologani
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Positron Annihilation Lifetime Analysis of Left- and Right-Handed Alanine Single Crystals
Studies of the interaction of polarized light or particles (including electrons, e(-), or positrons, e(+)) with asymmetric forms of matter has been of interest to scientists since the discovery of chirality and the subsequent development of particle physics.
Eren, B. +4 more
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Generalized derivations with left annihilator conditions in prime and semiprime rings
Let R be a prime ring with its Utumi ring of quotients U, C = Z(U) be the extended centroid of R, H and G two generalized derivations of R, L a noncentral Lie ideal of R, I a nonzero ideal of R. The left annihilator of S ⊆ R is denoted by lR(S) and defined by lR(S) = {x ∈ R| xS = 0}. Suppose that S = {H(un)un +unG(un) | u ∈ L} and T = {H(xn)xn +xnG(xn)
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Triplet quenching pathway control with molecular dyads enables the identification of a highly oxidizing annihilator class. [PDF]
Bertrams MS +4 more
europepmc +1 more source
We accomplish for the first time the next-to-leading-order computation of the weak annihilation contribution to the exclusive electroweak penguin decays $B \to \left \{K, π\right \} \ell^{+} \ell^{-}$ with an energetic light-flavour meson, which is an essential missing piece of the complete QCD correction to the matrix elements of hadronic operators in
Huang, Yong-Kang +3 more
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Metal-Organic Bichromophore Lowers the Upconversion Excitation Power Threshold and Promotes UV Photoreactions. [PDF]
Li H +4 more
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