Abstract

We have measured depletion spectra of the heteronuclear (85Rb87Rb+) dimer cation complexed with up to 10 He atoms. Two absorption bands are observed between 920 and 250 nm. The transition into the repulsive 12Σu+ state of HeRb2+ gives rise to a broad feature at 790 nm (12,650 cm−1); it exhibits a blueshift of 98 cm−1 per added He atom. The transition into the bound 12Πu state of HeRb2+ reveals vibrational structure with a band head at ≤ 15,522 cm−1, a harmonic constant of 26 cm−1, and a spin–orbit splitting of ≤ 183 cm−1. The band experiences an average redshift of − 38 cm−1 per added He atom. Ab initio calculations rationalize the shape of the spectra and spectral shifts with respect to the number of helium atoms attached. For a higher number of solvating helium atoms, symmetric solvation on both ends of the Rb2+ ion is predicted.

Highlights

  • Helium nanodroplets have been used as nanocryostats to isolate atoms or molecules at a temperature of 0.4 K, or to form new weakly bound aggregates [1,2,3]

  • Alkali metal atoms reside on the surface of He droplets due to the short-range Pauli repulsion between their s valence electrons and surrounding helium atoms counteracting the Published as part of the special collection of articles “Festschrift in honor of Fernand Spiegelmann”

  • The ion beam was guided into the extraction region of a high-resolution time-of-flight mass spectrometer (TOFMS) where it was merged with a laser beam from a tunable light source (EKSPLA NT242, line width 5 ­cm−1, pulse duration 3–6 ns, repetition rate 1 kHz)

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Summary

Introduction

Helium nanodroplets have been used as nanocryostats to isolate atoms or molecules at a temperature of 0.4 K, or to form new weakly bound aggregates [1,2,3]. They offer a unique quantum solvent for studying small and large dopant clusters, neutral or ionic, which can in turn be investigated by electronic or infrared spectroscopy [4]. Alkali metal atoms reside on the surface of He droplets due to the short-range Pauli repulsion between their s valence electrons and surrounding helium atoms counteracting the Published as part of the special collection of articles “Festschrift in honor of Fernand Spiegelmann”

Present Address
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Experiment
Calculations
Results and discussion
Method
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Conclusions
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Full Text
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