D 2 and H 2 Stark recurrence spectra have been measured at scaled energies of = −2.3 and = −3.2. An isotope shift in the scaled-action locations of recurrence peaks is found and explained by the increased density of states associated with perturbing rotational series. This reinforces the insight gained in previous work on the correspondence between the structures of a quantum spectrum and its classical periodic orbits. PACS number(s): 32.60.+i, 32.80.Ee Recently, Wright et al.[1] measured the Stark recurrence spectrum of H 2 and observed two primitive recurrences in the spectrum due to the presence in the photoabsorption spectrum of two Rydberg series converging to different rotational core states. Diffractive inelastic scattering recurrence peaks were also found resulting from configuration interaction between the two Rydberg series. We have carried out a new set of measurements using both H 2 and D 2 in order to study the effect of mass on these recurrences.The experimental apparatus used is identical to that in Ref.[1] with the only change being a different experimenter and the use of D 2 as well as H 2 . A brief outline of the experiment follows. A 4-keV D 2 + ion beam is neutralized in potassium vapor and the resulting neutral molecules in the 2pπ c 3 u metastable state are excited to Rydberg states in the presence of an electric field using a tunable dye-laser system. The Rydberg states are field ionized and the resulting ions detected with a channel plate. A field-ionization spectrum is recorded over the principal-quantum-number range of n = 16 to 26 while holding the scaled energy = EF −1/2 constant. The energy E is the electron binding energy relative to a Rydberg-series limit and F is the applied electric field. This maintains the classical dynamics unchanged over the entire spectrum [2]. The scaled spectrum is Fourier transformed to obtain the recurrence spectrum, i.e., signal strength versus orbit scaled action S [3]. Figure 1 shows the measured recurrence spectrum of D 2 (upper panel) and H 2 (lower panel) at = −3.2 and Fig. 2 shows the spectrum at = −2.3, both for scaled action up to S = 4.0. Both energies are beyond the Inglis-Teller limit with two (three) n manifolds overlapping for = −3.2 ( = −2.3). We refer the reader to Ref. [1] for additional details about molecular recurrence spectra.The peak labeled p in the figures is the primitive (smallestaction) recurrence associated with the scaled Rydberg excitation series (R = 1 for H 2 and R = 2 for D 2 , where R is the rotational quantum number). This peak occurs at scaled action S = 1 due to scaling. Each recurrence spectrum is normalized such that this peak has unit height. The peak labeled p in the figures is due to the presence in the photoabsorption spectrum of interloping Rydberg series (R > 1 in H 2 and R > 2 in D 2 ). As can be seen in the figures, p is at lower action than p. This occurs because the interloper series in both the H 2 and D 2 spectra is at a lower principal-quantum-number range compared to the main series and has larger e...