Searcharxiv⌕ Search

arXiv subjects

E. H. Saidi

Publications and source records attributed to E. H. Saidi.

43 records · Page 3Linked to original sources

On HyperKahler Singularities

Using a geometric realization of the $SU(2)_R$ symmetry and a procedure of factorisation of the gauge and $SU(2)_R$ charges, we study the small instanton singularities of the Higgs branch of supersymmetric $U(1)^r$ gauge theories with eight supercharges. We derive new solutions for the moduli space of vacua preserving manifestly the eight supercharges. In particular, we obtain an extension of the ordinary ADE singularities for hyperKahler manifolds and show that the classical moduli space of vacua is in general given by cotangent bundles of compact weighted projective spaces.

hep-th↗

Explicit Derivation of Yang-Mills Self-Dual Solutions on non-Commutative Harmonic Space

We develop the noncommutative harmonic space (NHS) analysis to study the problem of solving the non-linear constraint eqs of noncommutative Yang-Mills self-duality in four-dimensions. We show that this space, denoted also as NHS($η,θ$), has two SU(2) isovector deformations $η^{(ij)}$ and $θ^{(ij)}$ parametrising respectively two noncommutative harmonic subspaces NHS($η,0$) and NHS($0,θ$) used to study the self-dual and anti self-dual noncommutative Yang-Mills solutions. We formulate the Yang-Mills self-dual constraint eqs on NHS($η,0$) by extending the idea of harmonic analyticity to linearize them. Then we give a perturbative self-dual solution recovering the ordinary one. Finally we present the explicit computation of an exact self-dual solution.

hep-th↗

On the confining potential in 4d $SU(N_c)$ gauge theory with dilaton

Using the formal analogy between the Dick superstring inspired model of ref.[6] and the problem of building of Eguchi Hanson metric in 4d N=2 harmonic superspace (hs), we derive a general formula for the quark-quark interaction potential V(r) including the Dick confining potential. The interquark potential V(r) depends on the dilaton-gluon coupling and may be related to the parameterization of confinement by the quark and gluon vacuum condensates. It is also shown how the axion field may be incorporated in agreement with 10d type IIB superstring requirements. Others features are also discussed.

hep-th↗

Hyperkahler Singularities in Superstrings Compactification and 2d N=4 Conformal Field Theory

We study the singularities of the Higgs branch of supersymmetric U(1)^r gauge theories with eight supercharges. We derive new solutions for the moduli space of vacua preserving manifestly the eight supercharges by using a geometric realization of the SU(2)_R symmetry and a separation procedure of the gauge and SU(2)_R charges, which allow us to put the hypermultiplet vacua in a form depending on a parameter $γ$. For $γ=1$, we obtain new models which flow in the infrared to 2d N=(4,4) conformal models and we show that the classical moduli spaces are given by intersecting cotangent weighted complex projective spaces containing the small instanton singularity, discussed in [17], as a leading special case. We also make comments regarding the d$2d N=4 conformal Liouville description of the Higgs branch throat by following the analysis of [18]. Other features are also discussed.

hep-th↗

More Insight into Heavy Quark Masses from QCD

Using the non-relativistic version of Borel sum rules, combined to the very accurate experimental information on the Charmonium and Upsilon spectra, we rigorously investigate the Euclidean mass of the Charm and Bottom quark. Our analysis is performed with an improved expansion of the heavy current correlator in the infinite heavy quark mass limit. The optimal results, which take into account the most recent world average values of the strong coupling constant, as well as a conservative range of the gluon condensate, are: m_c^Eucl=1.20+-0.034 GeV and m_b^Eucl=4.18+-0.037 GeV. Their conversions to the corresponding pole mass and running mass give respectively: M_c=1.49+-0.08 GeV, M_b=4.65+-0.06 GeV and m_c(m_c)=1.21+-0.08 GeV, m_b(m_b)=4.20+-0.06 GeV in good agreement with the most recent direct estimates.

hep-ph↗

Three Graded Modified Classical Yang-Baxter Equations and Integrable Systems

The $6 = 3\times 2$ huge Lie algebra $Ξ$ of all local and non local differential operators on a circle is applied to the standard Adler-Kostant-Symes (AKS) R-bracket sckeme. It is shown in particular that there exist three additional Lie structures, associated to three graded modified classical Yang-Baxter(GMCYB) equations. As we know from the standard case, these structures can be used to classify in a more consitent way a wide class of integrable systems. Other algebraic properties are also presented.

solv-int↗

On the N=2 U(1) supercovariant Lax formalism and WA(n-1|n-1)^(1) symmetries

We introduce the concept of conformal spin gradation of the untwisted affine Lie superalgebra $\hat A(n-1| n-1)^{(1)}$ to study the $W\hat A (n-1| n-1)^{(1)}$ Miura transformation. We show that the essential of $\hat A(n-1| n-1)^{(1)}$ may be read from the conformal spin gradation of the canonical vector basis of the $SL(n| n)$ vector representation space $V_{2n}$ and a spectral parameter $μ$. We give the generic formula of their conformal spin weights. Then, we set up the fundamentals of a manifestly $N=2 U(1)$ Lax formalism leading to a manifestly $N=2 W\hat A(n-1| n-1)^{(1)}$ Miura transformation. Its explicit form is obtained and is shown to have a similar structure as in the N=0 case. Both $N=0 W\hat A(n-1)^{(1)}$ and $N=2 W\hat A(n-1| n-1)^{(1)}$ Miura transformations involve $(n-1) N=0$ and N=2 conserved currents with integer conformal spins. The leading cases are discussed. Using the U(1) charge of the N=2 algebra, we develop also a new method of constructing N=2 superfield realizations of the N=2 higher spin supercurrents. Among other results, we find that in general there are three series of $(n-1)$ higher conformal spin N=2 supercurrents. The usual N=2 super $W$ currents are the only hermitian ones. At the $n=3$ level, we find a new Feigin Fuchs type extension of the conformal spin one N=2 supercurrent. Such a feature, which has no analogue at the $n=2$ level, is also present for $n>3$. Finally, we give the N=2 superfield formulation of the N=2 Boussinesq equation and its generalization involving complex N=2 supercurrents.

hep-th↗