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Mimicking classical noise in ion channels by quantum decoherence. [PDF]
Seifi M, Soltanmanesh A, Shafiee A.
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How Vibrational Notations Can Spoil Infrared Spectroscopy: A Case Study on Isolated Methanol. [PDF]
Dinu DF +6 more
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Selecting Initial Conditions for Trajectory-Based Nonadiabatic Simulations. [PDF]
Janoš J, Slavíček P, Curchod BFE.
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Observation of dynamic non-Hermitian skin effects. [PDF]
Li Z +5 more
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Novel Criteria to Provide a Locality/Normality Degree in Molecules and Their Relevance in Physical Chemistry. [PDF]
Suárez E, Guzmán-Juárez O, Lemus R.
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Anharmonic Grassmann oscillator. II
Physical Review D, 1990An analysis of the anharmonic fermion oscillator, possessing an $\mathrm{Sp}(2)\ifmmode\times\else\texttimes\fi{}\mathrm{O}(N)$ symmetry, is presented. The complete solution is given for $N=2 \mathrm{and} 3$, and the general features for arbitrary $N$ are spelled out.
, Delbourgo, , Jones, , White
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Anharmonic oscillators revisited
International Journal of Non-Linear Mechanics, 1985A large class of anharmonic oscillators represented by the Hamiltonian \(H(p,q)=(1/2)p^ 2+(1/2)q^ 2+\lambda q^{\alpha}\) (\(\alpha\) integer \(>2)\) is considered. Owing to an integration technique using the Lagrange-Bürmann theorem the solution of the motion equation is given in terms of series of Gauss hypergeometric functions.
Codaccioni, J. P., Caboz, R.
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Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences, 1978
Accurate eigenvalues and eigenfunctions of the anharm onic oscillator ( H = p 2 + x 2 + λx 4 , λ > 0) and the quartic oscillator ( H = p 2 + x
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Accurate eigenvalues and eigenfunctions of the anharm onic oscillator ( H = p 2 + x 2 + λx 4 , λ > 0) and the quartic oscillator ( H = p 2 + x
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