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Rydberg states of the nitrogen moleculea)

Sunggi Chung, Chun C. Lin, Edward T. P. Lee

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Abstract

Rydberg states (1,3Σg+, 1,3Σu+, 1,3Πg, and 1,3Πu) of N2 that converge to the N2+ (X 2Σg+) ion have been calculated. The core orbitals are taken as those of the free N2+(X 2Σg+) ion. The Rydberg electron wave functions are expanded by one-center basis functions which are solution of an electron moving in a sphericalized potential of the N2+(X 2Σg+) ion. This expansion converges rapidly since the basis functions are already a fairly good representation of the Rydberg states especially for the higher ones. The use of one-center expansion allows us to examine the mixing of the basis functions of different angular-momentum quantum number l in the Rydberg states which is found to be generally small. Energy levels are reported for singlet and triplet Rydberg states of the Σ and Π types (Λ=0,1) with l from 0–9 and n through 11. The Rydberg levels with l≥4 are entirely hydrogenic. For lower l the quantum defect varies significantly with n within a given l series. Also a wide range of quantum defect is found for different states. Transitions among the various Rydberg series produce a very rich spectrum in the long-wave infrared region.

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What this paper is about

Rydberg states (1,3Σg+, 1,3Σu+, 1,3Πg, and 1,3Πu) of N2 that converge to the N2+ (X 2Σg+) ion have been calculated. The core orbitals are taken as those of the free N2+(X 2Σg+) ion. The Rydberg electron wave functions are expanded by one-center basis functions which are solution of an electron moving in a sphericalized potential of the N2+(X 2Σg+) ion. This expansion converges rapidly since the basis functions are already a fairly good representation of the Rydberg states especially for the higher ones. The use of one-center expansion allows us to examine the mixing of the basis functions of different angular-momentum quantum number l in the Rydberg states which is found to be generally small. Energy levels are reported for singlet and triplet Rydberg states of the Σ and Π types (Λ=0,1) with l from 0–9 and n through 11. The Rydberg levels with l≥4 are entirely hydrogenic. For lower l the quantum defect varies significantly with n within a given l series. Also a wide range of quantum defect is found for different states. Transitions among the various Rydberg series produce a very rich spectrum in the long-wave infrared region.

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Available abstract

Rydberg states (1,3Σg+, 1,3Σu+, 1,3Πg, and 1,3Πu) of N2 that converge to the N2+ (X 2Σg+) ion have been calculated. The core orbitals are taken as those of the free N2+(X 2Σg+) ion. The Rydberg electron wave functions are expanded by one-center basis functions which are solution of an electron moving in a sphericalized potential of the N2+(X 2Σg+) ion. This expansion converges rapidly since the basis functions are already a fairly good representation of the Rydberg states especially for the higher ones. The use of one-center expansion allows us to examine the mixing of the basis functions of different angular-momentum quantum number l in the Rydberg states which is found to be generally small. Energy levels are reported for singlet and triplet Rydberg states of the Σ and Π types (Λ=0,1) with l from 0–9 and n through 11. The Rydberg levels with l≥4 are entirely hydrogenic. For lower l the quantum defect varies significantly with n within a given l series. Also a wide range of quantum defect is found for different states. Transitions among the various Rydberg series produce a very rich spectrum in the long-wave infrared region.

Key concepts: Rydberg formula, Quantum defect, Atomic physics, Hydrogen spectral series, Principal quantum number, Rydberg atom, Wave function, Rydberg matter

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