I. Introduction The Lambert problem is one of the most extensively studied problems in astrodynamics as its solution is a building block for many problems, including interplanetary transfer optimization, rendezvous missions design, collision avoidance maneuvers design, and orbit determination. Although this problem was solved more than 200 years ago [1], many researchers are still working on devising robust and efficient resolution procedures [2, 3], including analytical approximations [4]. In particular, when the transfer time is long, Lambert's problem becomes a multi-revolution Lambert's problem (MRLP) which has the additional difficulty of admitting many solutions associated with different number of revolutions. More specifically, there exists 2N max + 1 number of solutions to a MRLP, in which N max is the maximum number of revolutions compatible with the time-of-flight of interest [5]. The original formulation of Lambert's problem is based on two-body dynamics. However, when the MRLP solutions are used to design missions around a planetary body or for orbit determination and data association problems, the effect of perturbations cannot be neglected. The perturbations, e.g. J 2 or atmospheric drag, can cause large violations of the terminal constraints, up to the point that classical Lambert's solutions fail to provide a good initial guess for the multi-revolution perturbed Lambert problem (MRPLP). Different methods have been proposed over the years to solve perturbed Lambert's problems. Engles and Junkins [6] proposed a variation-of-parameter approach combined with Kustaanheimo-Stiefel (KS) transformation to algebraically solve the J 2 perturbed problem. Bai and Junkins [7] proposed a modified Chebyshev-Picard iteration (MCPI) method for the solution of two-point boundary values problems, which was later regularized by Woollands et al. [8] using the KS time transformation and applied to high-fidelity dynamics. Der [9] developed a Lambert solver that can be modified to include the effect of J 2 − J 4 via a targeting technique based on Vinti's approximation. However, these approaches are not suitable for cases with many revolutions, due to the fact that the initial Keplerian guess for the velocity is not close to the perturbed one. More recently, Yang et al. [10] developed a homotopic approach suitable for solving the MRPLP, which they applied to the design of rendezvous missions around Mars. This approach employs a homotopy on the residuals. For each of the multiple solutions of the MRLP, a sequence of MRPLP is solved for decreasing values of the homotopic parameter.