Abstract. We give an upper bound of a Hamiltonian displacement energy of a unit disk cotangent bundle D * M in a cotangent bundle T * M , when the base manifold M is an open Riemannian manifold. Our main result is that the displacement energy is not greater than Cr(M ), where r(M ) is the inner radius of M , and C is a dimensional constant. As an immediate application, we study symplectic embedding problems of unit disk cotangent bundles. Moreover, combined with results in symplectic geometry, our main result shows the existence of short periodic billiard trajectories and short geodesic loops.1. Introduction 1.1. Displacement energy. Displacement energy is an important quantity in symplectic geometry, introduced by H. Hofer [9]. First we recall its definition. Let (X, ω) be a symplectic manifold. For any H ∈ C ∞ (X), its Hamiltonian vector field X H is definedc denotes the set of compactly supported smooth functions) and 0 ≤ t ≤ 1, H t ∈ C ∞ c (X) is defined as H t (x) := H(t, x) and its Hofer norm H is defined as Then ω M := dλ M is a symplectic form on T * M.