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We have seen that for open systems the (formula presented)’s are quantized according to the special constraints (13). In the thermodynamic limit this constraint is fulfilled, e.g., by (formula presented) (formula presented). The “phase shift” (formula presented) appears in the expression (16) of the density and the correlation functions (for (formula presented) through the parameter (formula presented). The solution of this transcendental equation at, leads to (formula presented). Therefore, it is sufficient to assume (formula presented) in the large (formula presented) expansion of the terms contributing to the density and correlation functions
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We have seen that for open systems the (formula presented)’s are quantized according to the special constraints (13). In the thermodynamic limit this constraint is fulfilled, e.g., by (formula presented) (formula presented). The “phase shift” (formula presented) appears in the expression (16) of the density and the correlation functions (for (formula presented) through the parameter (formula presented). The solution of this transcendental equation at smallp leads to (formula presented). Therefore, it is sufficient to assume (formula presented) in the large (formula presented) expansion of the terms contributing to the density and correlation functions.
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