2019
DOI: 10.1007/s00894-019-4040-5
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Rotation-vibrational energies for some diatomic molecules with improved Rosen–Morse potential in D-dimensions

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Cited by 25 publications
(11 citation statements)
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“…Based on this manipulation, we can further represent the MPETP as the following improved form, U()r=De1ere/kqer/kq2. This improved version tells us that the MPETP is entirely identical to the Tietz potential for diatomic molecules . The emergence of the improved Tietz potential and its special cases has attracted great attention in the physical and chemical community due to a combination of simple forms and effective applications, including relativistic and nonrelativistic treatments of molecular vibrational energies and predictions of thermochemical quantities for some diatomics . Through the introduction of the dissociation energy and equilibrium bond length as direct parameter identifications, we have overcome the fault that the potential parameters appearing in the original MPETP given in Equation lack explicit physical definitions.…”
Section: Improved Mpetpmentioning
confidence: 99%
“…Based on this manipulation, we can further represent the MPETP as the following improved form, U()r=De1ere/kqer/kq2. This improved version tells us that the MPETP is entirely identical to the Tietz potential for diatomic molecules . The emergence of the improved Tietz potential and its special cases has attracted great attention in the physical and chemical community due to a combination of simple forms and effective applications, including relativistic and nonrelativistic treatments of molecular vibrational energies and predictions of thermochemical quantities for some diatomics . Through the introduction of the dissociation energy and equilibrium bond length as direct parameter identifications, we have overcome the fault that the potential parameters appearing in the original MPETP given in Equation lack explicit physical definitions.…”
Section: Improved Mpetpmentioning
confidence: 99%
“…One can compare Equation () with the following equation [21, 56–59], d2Ritalicds2+trueτ˜()sσ()sdRds+trueσ˜()sσ2()sR=0, where lefttrueτfalse˜s=1s,σs=s1s,σfalse˜s=As2+BsC. Let us consider the solution of Equation () in following form, R()s=ϕ()sy()s. Then one may obtain [56], σ()sy()s+τ()sy()s+italicνy()s=0, and lefttrueϕs=eπsσsds, where lefttrueπs=σsτfalse˜s2±()σs...…”
Section: The Methodologymentioning
confidence: 99%
“…quarks-fundammental constituents of hadrons and other areas of modern chemistry [22,23] and physics [24].…”
Section: The Trm Oscillatormentioning
confidence: 99%
“…In this work, we extend the research area to construct the minimum-uncertainty coherent states of the hyperbolic Rosen-Morse (HRM) [16] and trigonometric Rosen-Morse (TRM) oscillators [17]. Those models are widely used in many areas of exact sciences including quantum chromodynamics (quark interactions) [18], N-fold supersymmetries in Schrödinger, Pauli and Dirac equations [19], SUSYQM [17,20], the theory of molecular vibrations [16,21] and other fields of modern chemistry [22,23] and physics [24].…”
Section: Introductionmentioning
confidence: 99%