<p>The discovery of the C<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> fullerene opened new horizons to design carbon nanostructures with targeted electronic structure as well as transport and optical properties. For example, endohedral <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> molecules were proposed as candidates for functional quantum architectures to store and manipulate encased atomic and molecular qubits. Recent advances in cryogenic buffer-gas cooling and frequency-comb spectroscopy have enabled rovibrational quantum-state-resolved measurements of gas-phase <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation>, revealing rotational fine structure reflecting its high icosahedral symmetry. Here, we present a perturbative quantum description of the <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> molecule interacting with a buffer gas of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(^{40}\)</EquationSource> </InlineEquation>Ar atoms at temperatures of order 150&#xa0;K, including a detailed analysis of their electronic structure, their interaction anisotropies, and the collision-induced rotational quenching of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> in its vibrational and electronic ground state. The role of the icosahedral symmetry on the collisional dynamics is emphasized leading to a complex dependence on the <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> rotational quantum number. Finally, we compute the isotropic and anisotropic static and dynamic dipole polarizability of <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> in its absolute ground state in order to evaluate the long-range, van der Waals interaction between <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> </InlineEquation>C<InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(_{60}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(^{40}\)</EquationSource> </InlineEquation>Ar.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Quantum scattering of fullerene \(^{12}\)C\(_{60}\) with rare gas atoms and its selection rules for rotational quenching

  • Alexander Petrov,
  • Anna Linnik,
  • Jacek Kłos,
  • Eite Tiesinga,
  • Svetlana Kotochigova

摘要

The discovery of the C \(_{60}\) fullerene opened new horizons to design carbon nanostructures with targeted electronic structure as well as transport and optical properties. For example, endohedral \(^{12}\) C \(_{60}\) molecules were proposed as candidates for functional quantum architectures to store and manipulate encased atomic and molecular qubits. Recent advances in cryogenic buffer-gas cooling and frequency-comb spectroscopy have enabled rovibrational quantum-state-resolved measurements of gas-phase \(^{12}\) C \(_{60}\) , revealing rotational fine structure reflecting its high icosahedral symmetry. Here, we present a perturbative quantum description of the \(^{12}\) C \(_{60}\) molecule interacting with a buffer gas of \(^{40}\) Ar atoms at temperatures of order 150 K, including a detailed analysis of their electronic structure, their interaction anisotropies, and the collision-induced rotational quenching of \(^{12}\) C \(_{60}\) in its vibrational and electronic ground state. The role of the icosahedral symmetry on the collisional dynamics is emphasized leading to a complex dependence on the \(^{12}\) C \(_{60}\) rotational quantum number. Finally, we compute the isotropic and anisotropic static and dynamic dipole polarizability of \(^{12}\) C \(_{60}\) in its absolute ground state in order to evaluate the long-range, van der Waals interaction between \(^{12}\) C \(_{60}\) and \(^{40}\) Ar.