The High-Lying Vibrational Levels and Dissociation Energy of the a3Sigma+u State of 7Li2.

Perturbation-facilitated optical-optical double resonance (PFOODR) has been used to access the 2(3)Pig state of 7Li2 via the excitation scheme using two single-mode tunable lasers. The selected () mixed level provides a gateway through which the triplet manifold can be accessed. Fluorescence from single rovibrational levels of 2(3)Pig to the state was detected at high resolution using a Fourier transform spectrometer. Transitions to v = 0-9 in the state were observed, covering the potential well almost to the dissociation limit. The data were analyzed using a near dissociation expansion (NDE) technique and the resulting vibrational and rotational parameters were used to calculate a new RKR potential curve which reproduced the observed energy levels to within a rms error of 0.02 cm-1. The following parameters were obtained for the state: D0 = 301.829 +/- 0.015 cm-1, De = 333.69 +/- 0.10 cm-1, Te = 8183.12 +/- 0.12 cm-1. Copyright 1999 Academic Press.

On the 5d 1Pig --> 2 (1)Sigma+u and 5d 1Pig --> C 1Piu Fluorescence in 7Li2.

Following excitation of the 5d 1Pig Rydberg state of 7Li2 by optical-optical double resonance, fluorescence has been observed in the infrared region to the 2 (1)Sigma+u and C 1Piu states. Analysis of high-resolution Fourier transform spectra yields term energies and rotational constants of the lowest seven vibrational levels of the inner well of the 2 (1)Sigma+u "double minimum" state. The equilibrium term value and dissociation energy have been determined to be Te = 30101.45 +/- 0.12 cm-1 and De = 5621.3 +/- 0.2 cm-1. The v = 0 and 1 levels of the C 1Piu state have been analyzed, resulting in new values of Te = 30551.0 +/- 0.1 cm-1 and De = 7773.3 +/- 0.2 cm-1. Copyright 1998 Academic Press.

Chirp-free nanosecond laser amplifier for precision spectroscopy.

We describe a simple method for greatly reducing optical phase perturbations in a nanosecond pulsed dye amplifier. The laser dye mix is tailored to produce a susceptibility near zero at the operating wavelength. Frequency shifts are reduced to less than 3 MHz, and frequency chirping to less than 10 MHz, without significant loss of amplified power. This technique has been used to improve the accuracy of precision far-UV wavelength measurements in H(2) to ~7 parts in 10(9).