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In the context of planar holography, integrability plays an important role for solving certain massless quantum field theories such as N=4 SYM theory.
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Note that the p j 2 p_{j}^{2} are unconstrained and the m j m_{j} are generic; we have x j μ = x 1 μ − ∑ k < j p k μ x^{\mu}_{j}=x^{\mu}_{1}-\sum\displaylimits_{k<j}p^{\mu}_{k} and x n + 1 μ = x 1 μ x_{n+1}^{\mu}=x_{1}^{\mu}
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In these cases one acts on massive legs with the generators of the massive symmetry and on massless legs with the usual dual-conformal generators obtained by dropping the mass terms in ( 2
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Switching on the internal mass m 0 m_{0} , only the combination P ^ \mathaccentV h a t 05 E μ + P ^ extra \mathaccentV h a t 05 E μ \mathrm{\mathaccent 866{P}}^{\mathaccentV{hat}05E\mu}+\mathrm{\mathaccent 866{P}}^{\mathaccentV{hat}05E\mu}_{\text{extra}} is a symmetry
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Note that this equation arises from the differential operator P ^ extra \mathaccentV h a t 05 E μ \mathrm{\mathaccent 866{P}}^{\mathaccentV{hat}05E\mu}_{\text{extra}} , while the rest of P ^ \mathrm{\mathaccent 866{P}} trivially annihilates I 2 I_{2} . This is a generic feature for two-point invariants
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