Boundary Liouville field theory: boundary three-point function

By B. Ponsot, J. Teschner. 2002

162 citations recorded by the source corpus.

Subfields: Applied Mathematics, Geometry and Topology

View Paper: https://www.semanticscholar.org/paper/d144dcb70502969bd4ffa8033ccedad9fc884d88

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In Applied Mathematics

In Geometry and Topology

Citations in the corpus

Classical and quantum D-branes in 2D string theory (2003, methodology): “By using the results of [16] it is possible to show that taking μ → 0 preserves the reflection relation (2.”
Open String Creation by S-Branes (2002, background): “(Ordinary boundary Liouville theories have been studied in [16-18].”
D-brane Decay in Two-Dimensional String Theory (2003, methodology): “First we have D-branes which are extended along the Liouville direction that were studied in [34,35,40].”
Rolling tachyons from Liouville theory (2003, unknown): “[28, 29, 30, 31, 32] for some formulas concerning the models with c ≥ 25).”
Loop and surface operators in $ \mathcal{N} = 2 $ gauge theory and Liouville modular geometry (2009, background): “These eigen states have been explicitly constructed in [27].”
Strings from Tachyons (2003, background): “…units) via geff ≃ 1/µ, (11) or as related to the value of T at the location ϕ = 0 of the “dilaton wall” (i.e. where the string coupling is of order 1) via T (0) ≃ µ 2 log µ. (12) The action (9) has only one single propagating degree of freedom, which we can take to be the closed string tachyon T .”
Liouville Field Theory — A decade after the revolution (2004, unknown): “The result is [157] C321 (Q−β3)β2β1 = Γb(2Q− β1 − β2 − β3)Γb(β2 + β3 − β1)Γb(Q+ β2 − β1 − β3)Γb(Q+ β3 − β1 − β2) Γb(2β3 −Q)Γb(Q− 2β2)Γb(Q− 2β1)Γb(Q) × (πμγ(b2)b2−2b(2))(β3−β2−β1)/2bb3 + σ1 − σ3)Sb(Q+ β3 − σ3 − σ1) Sb(β2 + σ2 − σ3)Sb(Q+ β2 − σ3 − σ2) × 1 i ∫ i∞ −i∞ dt Sb(U1 + t)Sb(U2 + t)Sb(U3 + t)Sb”
Exact vs. semiclassical target space of the minimal string (2004, unknown): “By thinking of the target space as the moduli space of FZZT branes, parametrized by the boundary cosmological constant x, we see that classically it consists of a Riemann surface Mp,q which is a p-sheeted cover of the complex x plane.”
FROM 4d SUPERCONFORMAL INDICES TO 3d PARTITION FUNCTIONS (2011, background): “A recent intriguing conjecture made in [17] concerns a connection of the partition function for 3d N = 4 SYM theory with SU(2) gauge group with a kernel of the 2d Liouville field theory connecting conformal blocks in different channels [43] (see also [44]).”