We prove that the number of Reeb chords between a Legendrian submanifold and its contact Hamiltonian push-off is at least the sum of the Z2-Betti numbers of the submanifold, provided that the contact isotopy is sufficiently small when compared to the smallest Reeb chord on the Legendrian. Moreover, the established invariance enables us to use two different contact forms: one for the count of Reeb chords and another for the measure of the smallest length, under the assumption that there is a suitable symplectic cobordism from the latter to the former. The size of the contact isotopy is measured in terms of the oscillation of the contact Hamiltonian, together with the maximal factor by which the contact form is shrunk during the isotopy. The main tool used is a Mayer-Vietoris sequence for Lagrangian Floer homology, obtained by "neck-stretching" and "splashing." 1 4 GEORGIOS DIMITROGLOU RIZELL AND MICHAEL G. SULLIVAN Corollary 1.7. Let Λ ⊂ (Y, ξ) be a Legendrian submanifold and let α 0 be a (not necessarily generic) contact form on (Y, ξ) which is relatively hypertight, i.e. for which σ(α 0 , Λ) = +∞. Suppose that Λ ′ is Legendrian isotopic to Λ. For any choice of contact form α, we then have the boundgiven that the latter chords are transverse.Proof. The contact form α can be written as α = e f α 0 for some real-valued function f :After a sufficiently small perturbation of the contact form α − it may be assumed to be generic, while the inequality e A H osc < σ(α − , Λ) is still satisfied for the contact Hamiltonian generating the isotopy from Λ to φ 1 α,Ht (Λ). Since it is possible to assume that α − = e g α holds for some smooth function g : Y → (0, 1) also after the perturbation, the result now follows directly from Corollary 1.6.Example 1.8. The following are well-known examples of Legendrian submanifolds satisfying σ(α 0 , Λ) = +∞ to which the above corollary can be applied.(1) The zero section of the one-jet space (J 1 M, dz − λ M ) of a closed manifold M endowed with its canonical contact form α std = dz − λ M ; i.e. λ M is the Liouville form on T * M and z is the canonical coordinate on the R-factor of J 1 M = T * M × R;(2) A fiber of the unit cotangent bundle S * M ⊂ T * M with contact form α 0 = λ M | T (S * M ) induced by a Riemannian metric on M having non-positive sectional curvature (recall that such a Riemannian manifold has no closed contractible geodesics, even without assuming periodicity); and(3) The conormal lift of a sub-torus (S 1 ) k × {1} n−k ⊂ (S 1 ) n inside the unit cotangent bundle S * (S 1 ) n , with contact form α 0 induced by the canonical flat metric on (S 1 ) n = R n /Z n .In another direction, define the α-displacement energy of a Legendrian Λ in (Y, kerα) to be disp(α, Λ) := inf Ht e A H osc where the infimum is taken over all contact Hamiltonians such that there are no α-Reeb chords between φ 1 α,Ht (Λ) and Λ or vice versa. (Set this infimum to +∞ if no such Hamiltonian exists.) Suppose Λ − , Λ + ⊂ Y are two Legendrians which are Lagrangian concordant in the symplectization (R×Y, ...