“…22,32,34,41,43 The quantum structure has been studied in detail using models of the confining potential, sometimes combined with cage-induced modifications of the rotational and vibrational characteristics of the guest molecule. 32,33,35,36,[43][44][45][46][47][48][49][50][51][52][53][54][55][56] There are two main ways to describe the interaction potential between the encapsulated species and the cage. One approach describes the interaction potential as a sum over many two-body Lennard-Jones (LJ) functions involving each endohedral atom and all 60 carbon atoms of the cage, [44][45][46]49,50,52,53,55,56 sometimes introducing "additional sites" on the endohedral species as well.…”
Section: Introductionmentioning
confidence: 99%
“…32,33,35,36,[43][44][45][46][47][48][49][50][51][52][53][54][55][56] There are two main ways to describe the interaction potential between the encapsulated species and the cage. One approach describes the interaction potential as a sum over many two-body Lennard-Jones (LJ) functions involving each endohedral atom and all 60 carbon atoms of the cage, [44][45][46]49,50,52,53,55,56 sometimes introducing "additional sites" on the endohedral species as well. 46,52,53 One disadvantage of this approach is that the summed potential has an undesirable dependence on the precise radius of the encapsulating fullerene cage.…”
Section: Introductionmentioning
confidence: 99%
“…One approach describes the interaction potential as a sum over many two-body Lennard-Jones (LJ) functions involving each endohedral atom and all 60 carbon atoms of the cage, [44][45][46]49,50,52,53,55,56 sometimes introducing "additional sites" on the endohedral species as well. 46,52,53 One disadvantage of this approach is that the summed potential has an undesirable dependence on the precise radius of the encapsulating fullerene cage. An alternative approach, which we call "model-free," describes the interaction potential as a sum of orthogonal spatial functions.…”
The interactions between atoms and molecules may be described by a potential energy function of the nuclear coordinates. Nonbonded interactions between neutral atoms or molecules are dominated by repulsive forces at a short range and attractive dispersion forces at a medium range. Experimental data on the detailed interaction potentials for nonbonded interatomic and intermolecular forces are scarce. Here, we use terahertz spectroscopy and inelastic neutron scattering to determine the potential energy function for the nonbonded interaction between single He atoms and encapsulating C 60 fullerene cages in the helium endofullerenes 3 He@C 60 and 4 He@C 60 , synthesized by molecular surgery techniques. The experimentally derived potential is compared to estimates from quantum chemistry calculations and from sums of empirical two-body potentials.
“…22,32,34,41,43 The quantum structure has been studied in detail using models of the confining potential, sometimes combined with cage-induced modifications of the rotational and vibrational characteristics of the guest molecule. 32,33,35,36,[43][44][45][46][47][48][49][50][51][52][53][54][55][56] There are two main ways to describe the interaction potential between the encapsulated species and the cage. One approach describes the interaction potential as a sum over many two-body Lennard-Jones (LJ) functions involving each endohedral atom and all 60 carbon atoms of the cage, [44][45][46]49,50,52,53,55,56 sometimes introducing "additional sites" on the endohedral species as well.…”
Section: Introductionmentioning
confidence: 99%
“…32,33,35,36,[43][44][45][46][47][48][49][50][51][52][53][54][55][56] There are two main ways to describe the interaction potential between the encapsulated species and the cage. One approach describes the interaction potential as a sum over many two-body Lennard-Jones (LJ) functions involving each endohedral atom and all 60 carbon atoms of the cage, [44][45][46]49,50,52,53,55,56 sometimes introducing "additional sites" on the endohedral species as well. 46,52,53 One disadvantage of this approach is that the summed potential has an undesirable dependence on the precise radius of the encapsulating fullerene cage.…”
Section: Introductionmentioning
confidence: 99%
“…One approach describes the interaction potential as a sum over many two-body Lennard-Jones (LJ) functions involving each endohedral atom and all 60 carbon atoms of the cage, [44][45][46]49,50,52,53,55,56 sometimes introducing "additional sites" on the endohedral species as well. 46,52,53 One disadvantage of this approach is that the summed potential has an undesirable dependence on the precise radius of the encapsulating fullerene cage. An alternative approach, which we call "model-free," describes the interaction potential as a sum of orthogonal spatial functions.…”
The interactions between atoms and molecules may be described by a potential energy function of the nuclear coordinates. Nonbonded interactions between neutral atoms or molecules are dominated by repulsive forces at a short range and attractive dispersion forces at a medium range. Experimental data on the detailed interaction potentials for nonbonded interatomic and intermolecular forces are scarce. Here, we use terahertz spectroscopy and inelastic neutron scattering to determine the potential energy function for the nonbonded interaction between single He atoms and encapsulating C 60 fullerene cages in the helium endofullerenes 3 He@C 60 and 4 He@C 60 , synthesized by molecular surgery techniques. The experimentally derived potential is compared to estimates from quantum chemistry calculations and from sums of empirical two-body potentials.
“…The spectroscopy and dynamics of guest molecules in H 2 O@C 60 and other LMEFs are dominated by nuclear quantum effects (NQEs), 59,110,118 especially for the low temperatures (typically ranging from 1.5 K to about 30 K) at which the spectroscopic measurements are usually carried out. The NQEs arise from a combination of quantization of the translational c.m.…”
Section: Applicationsmentioning
confidence: 99%
“…These calculations 58 also showed that the TR level structure of H 2 O@C 60 exhibits all of the key qualitative features identified previously for H 2 @C 60 . 56,59,118,127…”
The methodological advances made in recent years have significantly extended the range and dimensionality of noncovalently bound, hydrogen-bonded and Van der Waals, molecular complexes for which full-dimensional and fully coupled...
We introduce an efficient
quantum fully coupled computational scheme
within the multiconfiguration time-dependent Hartree (MCTDH) approach
to handle the otherwise extremely costly computations of translational–rotational–vibrational
states and energies of light-molecule endofullenes. Quantum calculations
on energy levels are reported for a water molecule inside C
60
fullerene by means of such a systematic approach that includes all
nine degrees of freedom of H
2
O@C
60
and does
not consider restrictions above them. The potential energy operator
is represented as a sum of natural potentials employing the
n
-mode expansion, along with the exact kinetic energy operator,
by introducing a set of Radau internal coordinates for the H
2
O molecule. On the basis of the present rigorous computations, various
aspects of the quantized intermolecular dynamics upon confinement
of H
2
O@C
60
are discussed, such as the rotational
energy level splitting and the significant frequency shifts of the
encapsulated water molecule vibrations. The impact of water encapsulation
on quantum features is explored, and insights into the nature of the
underlying forces are provided, highlighting the importance of a reliable
first-principles description of the guest–host interactions.
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