“…One may also find similar rigid string solutions with ln S scaling of E − S at large spin with two non-zero spins S 1 , S 2 , i.e. moving in the whole AdS 5 [16,42,54,55,43] subject to the rigid string ansatz (3.24), i.e. t = κτ, ρ = ρ(σ), θ = θ(σ), φ 1 = ω 1 τ, φ 2 = ω 2 τ .…”