Body frames in the separation of collective angles in quantum N-body problems

Journal of Chemical Physics

Volumn 120, Issue 17, 2004, Pages 7861-7876

  Meremianin, A V ^a  

^a UNIVERSITY OF FREIBURG   (Germany)

Author keywords

[No Author keywords available]

Indexed keywords

EIGENVALUES AND EIGENFUNCTIONS; HAMILTONIANS; MATRIX ALGEBRA; METHOD OF MOMENTS; PARAMETER ESTIMATION; POTENTIAL ENERGY; PROBLEM SOLVING; TENSORS; VECTORS;

BODY-FIXED REFERENCE FRAMES; PLANAR SYSTEMS; VIBRO-ROTATIONAL COUPLINGS;

QUANTUM THEORY;

EID: 2442543088     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.1687672     Document Type: Article

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51. ij, A is not a vector in a physical space, rather it is a set of three scalar functions depending only on internal coordinates.
52. The first Eckart condition is the requirement that the origin of the BF is located in the center of mass of the whole system.
53. For distinctness, we took a positive branch of the square root.
54. n square roots.
55. Strictly speaking, we should provide I and J with labels indicating that they are taken at the equilibrium configuration of the system. However, for the sake of shortness we do not do that.