Abstract:The infrared spectrum of single oxygen carbon sulfide (OCS) molecules was measured inside large superfluid pure helium-4 droplets and nonsuperfluid pure helium-3 droplets, both consisting of about 10(4) atoms. In the helium-4 droplets, sharp rotational lines were observed, whereas in helium-3 only a broad peak was found. This difference is interpreted as evidence that the narrow rotational lines, which imply free rotations, are a microscopic manifestation of superfluidity. Upon addition of 60 helium-4 atoms to… Show more
“…7 (a)), the relative amplitudes only decrease in the case of the high-lying level beats (4,5) and (5,6), whereas the lower beats (3, 4) remain constant or even rise [(0, 1), (1,2), and (2, 3)] in amplitude in proportion to the sum of all.…”
The vibrational wave-packet dynamics of diatomic rubidium molecules (Rb2) in triplet states formed on the surface of superfluid helium nanodroplets is investigated both experimentally and theoretically. Detailed comparison of experimental femtosecond pump-probe spectra with dissipative quantum dynamics simulations reveals that vibrational relaxation is the main source of dephasing. The rate constant for vibrational relaxation in the first excited triplet state 1 3 Σ + g is found to be constant γ ≈ 0.5 ns −1 for the lowest vibrational levels v < ∼ 15 and to increase sharply when exciting to higher energies.
“…7 (a)), the relative amplitudes only decrease in the case of the high-lying level beats (4,5) and (5,6), whereas the lower beats (3, 4) remain constant or even rise [(0, 1), (1,2), and (2, 3)] in amplitude in proportion to the sum of all.…”
The vibrational wave-packet dynamics of diatomic rubidium molecules (Rb2) in triplet states formed on the surface of superfluid helium nanodroplets is investigated both experimentally and theoretically. Detailed comparison of experimental femtosecond pump-probe spectra with dissipative quantum dynamics simulations reveals that vibrational relaxation is the main source of dephasing. The rate constant for vibrational relaxation in the first excited triplet state 1 3 Σ + g is found to be constant γ ≈ 0.5 ns −1 for the lowest vibrational levels v < ∼ 15 and to increase sharply when exciting to higher energies.
“…The microscopic version of the Andronikashvili experiment was first conducted by Grebenev et al in 1998. [8] They measured the rovibrational spectrum of OCS doped in a 4 He droplet with thousands of atoms at T 5 0.37 K. In the spectrum, the group observed a well-resolved rotational structure with a rotational inertia greater than that of a free OCS molecule.…”
The idea of a macroscopic Andronikashvili experiment used to measure superfluid fraction of bulk liquid 4 He can be ported into the realm of spectroscopic studies to measure the superfluid fraction of microscopic systems at the nanoscale. Theoretical studies are needed to fully unravel the superfluid information contained in such a microscopic Andronikashvili experiment. Two aspects of the theoretical studies, the generation of accurate and efficient potential energy surfaces, and the methodology of path-integral Monte Carlo simulations are briefly introduced in this article.
“…In fact, spectroscopic probes of molecular impurities in helium droplets have shown that while 4 He clusters result in superfluid behavior with free-rotor-like molecular spectra, 3 He atoms behave as a normal fluid and the impurity spectra are of hindered-rotor type. 1 Since 4 He atoms are composite spinless bosons and 3 He atoms are fermionic particles with a nuclear spin equal to 1/2, one fundamental question has concerned the influence of the spin and the antisymmetry of the fermionic 3 He wave-functions in providing such different response to the molecular rotation. QuantumChemistry (QC)-like Nuclear-Orbital (NO) approaches, first introduced by Jungwirth and Krylov, 2 map the problem onto an electronic structure-like problem by considering the helium atoms as pseudo-electrons and the dopant molecule as a structured pseudo-nucleus, replacing Coulomb interactions by van der Waals He-He and He-dopant pair potentials.…”
An interface between the APMO code and the electronic structure package MOLPRO is presented. The any particle molecular orbital APMO code [González et al., Int. J. Quantum Chem. 108, 1742 implements the model where electrons and light nuclei are treated simultaneously at Hartree-Fock or second-order Möller-Plesset levels of theory. The APMO-MOLPRO interface allows to include highlevel electronic correlation as implemented in the MOLPRO package and to describe nuclear quantum effects at Hartree-Fock level of theory with the APMO code. Different model systems illustrate the implementation: 4 He 2 dimer as a protype of a weakly bound van der Waals system; isotopomers of [He-H-He] + molecule as an example of a hydrogen bonded system; and molecular hydrogen to compare with very accurate non-Born-Oppenheimer calculations. The possible improvements and future developments are outlined.
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