1995
DOI: 10.1007/bf01338398
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The binding of alkali atoms to the surfaces of liquid helium and hydrogen

Abstract: AIkali atoms have been shown previously to have only unstable binding states inside liquid He-4. We calculate the equilibrium configurations and binding energies of single alkali atoms near the liquid-vapor interface of He-4 and He-3. A simple interface model is used to predict the surface deformation due to the presence of the atoms. A more realistic density functional model yields somewhat higher energies in the case of He-4. For all alkali atoms, we find the surface binding energies to be around 10 to 20 K.… Show more

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Cited by 110 publications
(108 citation statements)
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“…16) (e.g., the ratio among the number of p-H 2 molecules and alkali metal atoms are 10/3 and 2/1, respectively). The cause for the large equilibrium density in the Na case, as compared to that of the Rb system, is related to the decrease of the core size of the AM-H 2 interaction (i.e., σ = 4.54Å in the Rb-H 2 case), which makes the surface available to p-H 2 molecules larger (we note that the depth of the potential wells in both Na-H 2 and Rb-H 2 interactions are very similar, i.e., 30 and 28 K, respectively 25 ). Regarding the stabilization of possible pseudocommensurate solid phases, we investigated the three crystal structures shown in Fig.…”
Section: Resultsmentioning
confidence: 97%
See 1 more Smart Citation
“…16) (e.g., the ratio among the number of p-H 2 molecules and alkali metal atoms are 10/3 and 2/1, respectively). The cause for the large equilibrium density in the Na case, as compared to that of the Rb system, is related to the decrease of the core size of the AM-H 2 interaction (i.e., σ = 4.54Å in the Rb-H 2 case), which makes the surface available to p-H 2 molecules larger (we note that the depth of the potential wells in both Na-H 2 and Rb-H 2 interactions are very similar, i.e., 30 and 28 K, respectively 25 ). Regarding the stabilization of possible pseudocommensurate solid phases, we investigated the three crystal structures shown in Fig.…”
Section: Resultsmentioning
confidence: 97%
“…24 The interactions between Na atoms and H 2 molecules are described with a Lennard-Jones potential of the form V LJ (r) = 4 [(σ/r) 12 − (σ/r) 6 ], with parameters taken from Ref. 25, namely σ = 4.14Å and = 30 K. The kinetic energy of the Na atoms has been also neglected since this is expected to be much smaller than the typical energy scale of p-H 2 molecules (i.e., 10-100 K).…”
Section: Methods and Simulation Detailsmentioning
confidence: 99%
“…In case of surface doping with Ca, we assume a dimple depth of 7 Å [33]. According to Ancilotto et al [34], a single K atom is located in a dimple of depth 2.3 Å. Since such a shallow dimple cannot be implemented in a fcc lattice of discrete He atoms, we neglect the dimple for K dopants.…”
Section: Simulationsmentioning
confidence: 99%
“…Due to the large mass of Rb and Cs atoms compared to that of He, we describe them as classical particles in the dynamics while their effect on the statics is incorporated as an external field acting upon the droplet [14,53]. Accordingly, the energy of the system is written as…”
Section: B Dft For Bosonsmentioning
confidence: 99%