“…We construct a Hamiltonian diffeomorphism with support near the sphere ∂B(3) displacing L(1, 2) ∪ L(2, 1) from a neighborhood of the cylinder T . This is equivalent to constructing a Hamiltonian isotopy of L(1, 2) ∪ L(2, 1), where the Lagrangian tori remain close to ∂B (3). It is convenient to use symplectic polar coordinates (R 1 , θ 1 , R 2 , θ 2 ) where…”