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[PDF] Top 20 Four-point functions in N=2 superconformal field theories

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Four-point functions in N=2 superconformal field theories

Four-point functions in N=2 superconformal field theories

... (138) satisfies both requirements. To prove its uniqueness, we argue as follows. Firstly, at the lowest level in the θ + expansion there is a single SU(2) invariant combination of the three harmonics with the ... See full document

36

Invariants of toric seiberg duality

Invariants of toric seiberg duality

... 3 2 R[X]. In principle, this superconformal R-charge is an unknown non-anomalous combination of all the global U (1) symmetries of the ...the superconformal R-symmetry, so one might worry that the ... See full document

44

Four point functions of lowest weight CPOs in N = 4 SYM(4) in supergravity approximation

Four point functions of lowest weight CPOs in N = 4 SYM(4) in supergravity approximation

... a four-point function of arbitrary CPOs requires the con- struction of the effective 5D gravity action with all cubic terms involving two fields s I and with all s I -dependent quar- tic terms, the problem ... See full document

12

Thermal Soliton Correlation Functions in Theories with a Z(N) Symmetry

Thermal Soliton Correlation Functions in Theories with a Z(N) Symmetry

... in theories with a Z N   ...scalar field in  1 1   - dimensions described by a theory with Z N   symmetry, we are naturally led to a SG theory in the phase of this field ... See full document

5

Chiral Green's functions in superconformal field theory

Chiral Green's functions in superconformal field theory

... The definition of linear independence is that if a linear combination of a set of linearly independent terms vanishes, then all coefficients must vanish independently. Hence, to prove that a set of terms are linearly ... See full document

32

Symmetries in Three Dimensional Superconformal Quantum Field Theories

Symmetries in Three Dimensional Superconformal Quantum Field Theories

... the superconformal index of the ABJM theory ...1, 2 the ABJM theory has monopole operators which are conformal primaries of dimension 2 and transform as vectors under Lorenz ...an N = 4 d = 3 ... See full document

140

Typicality, Black Hole Microstates and Superconformal Field Theories

Typicality, Black Hole Microstates and Superconformal Field Theories

... In [1], generating functions for enumerating mesonic BPS operators in these SCFTs were derived. This counting was extended to include baryonic operators in [2, 3], but in the present paper we consider only ... See full document

49

Localization and Dualities in Three Dimensional Superconformal Field Theories

Localization and Dualities in Three Dimensional Superconformal Field Theories

... with N = 2, 2 ∗ , or 4 super Yang-Mills theory, the former two being deformations of the latter by adding infinite and finite mass, respectively, for the adjoint chiral ...is superconformal, ... See full document

121

Entanglement entropy in integrable quantum systems

Entanglement entropy in integrable quantum systems

... free theories and non local models, integrable systems exist only in two ...a 2+0 or 1+1 dimensional ...to 2+0 dimensional theories as classical statistical bi-dimensional ...quantum ... See full document

241

Three Point Identities and Inequalities for n-time Differential Functions

Three Point Identities and Inequalities for n-time Differential Functions

... A premature Gr¨ uss inequality is embodied in the following theorem which was proved in the paper [29]. It provides a sharper bound than the above Gr¨ uss in- equality. The term premature is used to denote the fact that ... See full document

26

Arguments towards a c-theorem from branch-point twist fields

Arguments towards a c-theorem from branch-point twist fields

... Branch point twist fields are on the one hand twist fields, that is they are associated to an internal symmetry of the theory under consideration, and on the other hand they are related to branch points of ... See full document

11

Higher particle form factors of branch point twist fields in integrable quantum field theories

Higher particle form factors of branch point twist fields in integrable quantum field theories

... Entanglement is the most distinct and bizarre of all quantum phenomena. The idea that the quantum states of objects so wide apart from each other that they are not even causally con- nected can be entangled seems ... See full document

28

Statutory Interpretation: Four Theories in Disarray

Statutory Interpretation: Four Theories in Disarray

... Statutory Interpretation Four Theories in Disarray SMU Law Review Volume 53 | Issue 1 Article 6 2000 Statutory Interpretation Four Theories in Disarray J Clark Kelso Charles D Kelso Follow this and ad[.] ... See full document

41

On Common Fixed Point for Four Maps  in 2- metric Space

On Common Fixed Point for Four Maps in 2- metric Space

... of 2-metric space, many authors established an analogue of Banach’s Contraction principle in 2-metric ...fixed point theorem in 2-metric ...fixed point theorem in 2- metric ... See full document

5

The non-relativistic limits of the Maxwell and Dirac equations: the role of Galilean and gauge invariance

The non-relativistic limits of the Maxwell and Dirac equations: the role of Galilean and gauge invariance

... illustrate four properties of the non-relativistic limits of relativistic theories: (a) that a massless relativistic field may have a meaningful non- relativistic limit, (b) that a relativistic ... See full document

27

The politics of public enterprises in the third world : the ASEAN case

The politics of public enterprises in the third world : the ASEAN case

... Figure 4.1 shows the significance of political factors: how the growth of the public enterprise sector (whether it expands or reduces) is affected by various political events, such as wars, coup d'etat, changes of ... See full document

564

N=2 gauge theories: Congruence subgroups, coset graphs, and modular surfaces

N=2 gauge theories: Congruence subgroups, coset graphs, and modular surfaces

... The Schreier-Cayley coset graphs for the genus zero, torsion-free congruence sub- groups from the classification were subsequently studied in [2, 3], a distinguished set of trivalent finite graphs thus emerged, ... See full document

44

Gauge string duality for superconformal deformations of N=4 super Yang Mills theory

Gauge string duality for superconformal deformations of N=4 super Yang Mills theory

... depend only on the angles of the 5-sphere and are constant when restricted to configurations from the sl(2) sector). Therefore, the spin chain Landau-Lifshitz action matches the string action as in the undeformed ... See full document

52

Functional N Representability in 2 Matrix, 1 Matrix, and Density Functional Theories

Functional N Representability in 2 Matrix, 1 Matrix, and Density Functional Theories

... approximate 2-RDM formed by the product of the Hartree-Fock 2-RDM times a correlation ... 2  ...not N-representable, the mathematical proof of this fact was presented by Morrison in 1993 ... See full document

10

Canonical Set Theory for Classic Mathematics A Linear Order On Finite Groups and Structures, with a Natural Extension to Infinite Structures

Canonical Set Theory for Classic Mathematics A Linear Order On Finite Groups and Structures, with a Natural Extension to Infinite Structures

... We need an extra rule for defining an equivalence class on finite trees. If a tree has two identical branches we substitute these two identical branches with a single branch, the successor. This process is called ... See full document

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