2016
DOI: 10.1080/00268976.2016.1155778
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The stability conditions of diatomic molecules via analogy with the stability theory of lasers

Abstract: The vibrational motion equations of both homo and hetero-nuclei diatomic molecules are here derived for the first time. A diatomic molecule is first considered as a one dimensional quantum mechanics oscillator. The second and third-order Hamiltonian operators are then formed by substituting the number operator for the quantum number in the corresponding vibrational energy eigenvalues. The expectation values of relative position and linear momentum operators of two oscillating atoms are calculated by solving He… Show more

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Cited by 3 publications
(15 citation statements)
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“…A heuristics model is introduced for constructing the vibrational Hamiltonian of a two-particle system in quantum mechanics. This model has already been implemented to form the vibrational [7] and rovibrational [23] Hamiltonians of diatomic molecules. Here, the vibrational Hamiltonian of Hydrogen-like atoms (5) has similarly defined as an infinite positive power series.…”
Section: Discussionmentioning
confidence: 99%
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“…A heuristics model is introduced for constructing the vibrational Hamiltonian of a two-particle system in quantum mechanics. This model has already been implemented to form the vibrational [7] and rovibrational [23] Hamiltonians of diatomic molecules. Here, the vibrational Hamiltonian of Hydrogen-like atoms (5) has similarly defined as an infinite positive power series.…”
Section: Discussionmentioning
confidence: 99%
“…been used [7]. The final vibrational equation of motion associated with the linear Hamiltonian ( 6) is then derived for the variable…”
Section: The Vibrational Hamiltonian In the Linear Regimementioning
confidence: 99%
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“…Our method for converting the energy eigenvalue of HLAs () to the corresponding Hamiltonian () has already been used for diatomic molecules [20]. The vibrational energy eigenvalue (VEE) of diatomic molecules is determined by substituting the Morse potential into the time‐independent Schrodinger equation as [21, 22] Eitalicvib=ω0n+1/2normalℏ2ω02/4De()ngoodbreak+1/22 where ω0 and De are the respective natural frequency and dissociation energy.…”
Section: Relativistic Vibrational Hamiltonianmentioning
confidence: 99%