Richard L. Hall
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Richard L. Hall has a total of 53 co-authors. Here are the top co-authors by number of shared publications:
- Nasser Saad
School of Mathematical and Computational Sciences, University of Prince Edward Island, Charlottetown, PE C1A 4P3, Canada
36 shared publications Nasser Saad
University of Prince Edward Island 2 Department of Mathematics and Statistics 550 University Avenue, Charlottetown, Prince Edward Island C1A 4P3, Canada
33 shared publications- Wolfgang Lucha
Institute for High Energy Physics, Austrian Academy of Sciences, Nikolsdorfergasse 18, A-1050 Vienna, Austria
25 shared publications - Hakan Ciftci
Gazi Üniversitesi, Fen-Edebiyat Fakültesi, Fizik Bölümü, 06500 Teknikokullar-Ankara, Turkey
12 shared publications Hakan Ciftci
11 shared publicationsWolfgang Lucha
Austrian Academy of Sciences 2 Institute for High Energy Physics Nikolsdorfergasse 18, A-1050 Vienna, Austria
11 shared publications
Latest Publications
- 17 September 2019
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 134 (9) , 449
General comparison theorems for the Klein-Gordon equation in d dimensions
- 17 September 2019
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 134 (9) , 449
General comparison theorems for the Klein-Gordon equation in d dimensions
- Open Access
- 1 February 2019
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 60 (2) , 029901
Publisher’s Note: “Exact normalized eigenfunctions for general deformed Hulthén potentials” [J. Math. Phys. 59, 122103 (2018)]
- 1 February 2019
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 60 (2) , 029901
Open AccessPublisher’s Note: “Exact normalized eigenfunctions for general deformed Hulthén potentials” [J. Math. Phys. 59, 122103 (2018)]
- Open Access
Exact normalized eigenfunctions for general deformed Hulthén potentials
The exact solutions of Schr\"odinger's equation with the deformed Hulth\'en potential $V_q(x)=-{\mu\, e^{-\delta\,x }}/({1-q\,e^{-\delta\,x}}),~ \delta,\mu, q>0$ are given, along with a closed--form formula for the normalization constants of the eigenfunctions for arbitrary $q>0$. The Crum-Darboux transformation is then used to derive the corresponding exact solutions for the extended Hulth\'en potentials $V(x)= -{\mu\, e^{-\delta\,x }}/({1-q\,e^{-\delta\,x}})+ {q\,j(j+1)\, e^{-\delta\,x }}/({1-q\,e^{-\delta\,x}})^2, j=0,1,2,\dots.$ A general formula for the new normalization condition is also provided.Open AccessExact normalized eigenfunctions for general deformed Hulthén potentials
The exact solutions of Schr\"odinger's equation with the deformed Hulth\'en potential $V_q(x)=-{\mu\, e^{-\delta\,x }}/({1-q\,e^{-\delta\,x}}),~ \delta,\mu, q>0$ are given, along with a closed--form formula for the normalization constants of the eigenfunctions for arbitrary $q>0$. The Crum-Darboux transformation is then used to derive the corresponding exact solutions for the extended Hulth\'en potentials $V(x)= -{\mu\, e^{-\delta\,x }}/({1-q\,e^{-\delta\,x}})+ {q\,j(j+1)\, e^{-\delta\,x }}/({1-q\,e^{-\delta\,x}})^2, j=0,1,2,\dots.$ A general formula for the new normalization condition is also provided. - 1 December 2018
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 59 (12) , 122103
Exact normalized eigenfunctions for general deformed Hulthén potentials
The exact solutions of Schrödinger’s equation with the deformed Hulthén potential Vq(x) = −μ e−δ x/(1 − q e−δ x), δ, μ, q > 0 are given, along with a closed-form formula for the normalization constants of the eigenfunctions for arbitrary q > 0. The Crum-Darboux transformation is then used to derive the corresponding exact solutions for the extended Hulthén potentials A general formula for the new normalization condition is also provided.- 1 December 2018
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 59 (12) , 122103
Exact normalized eigenfunctions for general deformed Hulthén potentials
The exact solutions of Schrödinger’s equation with the deformed Hulthén potential Vq(x) = −μ e−δ x/(1 − q e−δ x), δ, μ, q > 0 are given, along with a closed-form formula for the normalization constants of the eigenfunctions for arbitrary q > 0. The Crum-Darboux transformation is then used to derive the corresponding exact solutions for the extended Hulthén potentials A general formula for the new normalization condition is also provided.- Open Access
The $d$-dimensional softcore Coulomb potential and the generalized confluent Heun equation
An analysis of the generalized confluent Heun equation $(\alpha_2r^2+\alpha_1r)\,y''+(\beta_2r^2+\beta_1r+\beta_0)\,y'-(\varepsilon_1r+\varepsilon_0)\,y=0$ in $d$-dimensional space, where $\{\alpha_i, \beta_i, \varepsilon_i\}$ are real parameters, is presented. With the aid of these general results, the quasi exact solvability of the Schr\"odinger eigenproblem generated by the softcore Coulomb potential $V(r)=-e^2Z/(r+b),\, b>0$, is explicitly resolved. Necessary and sufficient conditions for polynomial solvability are given. A three-term recurrence relation is provided to generate the coefficients of polynomial solutions explicitly. We prove that these polynomial solutions are sources of finite sequences of orthogonal polynomials. Properties such as recurrence relations, Christoffel-Darboux formulas, and the moments of the weight function are discussed. We also reveal a factorization property of these polynomials which permits the construction of other interesting related sequences of orthogonal polynomials.Open AccessThe $d$-dimensional softcore Coulomb potential and the generalized confluent Heun equation
An analysis of the generalized confluent Heun equation $(\alpha_2r^2+\alpha_1r)\,y''+(\beta_2r^2+\beta_1r+\beta_0)\,y'-(\varepsilon_1r+\varepsilon_0)\,y=0$ in $d$-dimensional space, where $\{\alpha_i, \beta_i, \varepsilon_i\}$ are real parameters, is presented. With the aid of these general results, the quasi exact solvability of the Schr\"odinger eigenproblem generated by the softcore Coulomb potential $V(r)=-e^2Z/(r+b),\, b>0$, is explicitly resolved. Necessary and sufficient conditions for polynomial solvability are given. A three-term recurrence relation is provided to generate the coefficients of polynomial solutions explicitly. We prove that these polynomial solutions are sources of finite sequences of orthogonal polynomials. Properties such as recurrence relations, Christoffel-Darboux formulas, and the moments of the weight function are discussed. We also reveal a factorization property of these polynomials which permits the construction of other interesting related sequences of orthogonal polynomials. - 1 October 2018
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 59 (10) , 102105
Thed-dimensional softcore Coulomb potential and the generalized confluent Heun equation
An analysis of the generalized confluent Heun equation (α2r2 + α1r) y″ + (β2r2 + β1r + β0) y′ − (ε1r + ε0) y = 0 in d-dimensional space, where {αi, βi, εi} are real parameters, is presented. With the aid of these general results, the quasi-exact solvability of the Schrödinger eigenproblem generated by the softcore Coulomb potential V(r) = −e2Z/(r + b), b > 0, is explicitly resolved. Necessary and sufficient conditions for polynomial solvability are given. A three-term recurrence relation is provided to generate the coefficients of polynomial solutions explicitly. We prove that these polynomial solutions are sources of finite sequences of orthogonal polynomials. Properties such as the recurrence relations, Christoffel-Darboux formulas, and moments of the weight function are discussed. We also reveal a factorization property of these polynomials which permits the construction of other interesting related sequences of orthogonal polynomials.
- 1 October 2018
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 59 (10) , 102105
Thed-dimensional softcore Coulomb potential and the generalized confluent Heun equation
An analysis of the generalized confluent Heun equation (α2r2 + α1r) y″ + (β2r2 + β1r + β0) y′ − (ε1r + ε0) y = 0 in d-dimensional space, where {αi, βi, εi} are real parameters, is presented. With the aid of these general results, the quasi-exact solvability of the Schrödinger eigenproblem generated by the softcore Coulomb potential V(r) = −e2Z/(r + b), b > 0, is explicitly resolved. Necessary and sufficient conditions for polynomial solvability are given. A three-term recurrence relation is provided to generate the coefficients of polynomial solutions explicitly. We prove that these polynomial solutions are sources of finite sequences of orthogonal polynomials. Properties such as the recurrence relations, Christoffel-Darboux formulas, and moments of the weight function are discussed. We also reveal a factorization property of these polynomials which permits the construction of other interesting related sequences of orthogonal polynomials.
- Open Access
Exact and approximate solutions of Schrödinger's equation with hyperbolic double-well potentials
Analytic and approximate solutions for the energy eigenvalues generated by the hyperbolic potentials $V_m(x)=-U_0\sinh^{2m}(x/d)/\cosh^{2m+2}(x/d),\,m=0,1,2,\dots$ are constructed. A byproduct of this work is the construction of polynomial solutions for the confluent Heun equation along with necessary and sufficient conditions for the existence of such solutions based on the evaluation of a three-term recurrence relation. Very accurate approximate solutions for the general problem with arbitrary potential parameters are found by use of the {\it asymptotic iteration method}.Open AccessExact and approximate solutions of Schrödinger's equation with hyperbolic double-well potentials
Analytic and approximate solutions for the energy eigenvalues generated by the hyperbolic potentials $V_m(x)=-U_0\sinh^{2m}(x/d)/\cosh^{2m+2}(x/d),\,m=0,1,2,\dots$ are constructed. A byproduct of this work is the construction of polynomial solutions for the confluent Heun equation along with necessary and sufficient conditions for the existence of such solutions based on the evaluation of a three-term recurrence relation. Very accurate approximate solutions for the general problem with arbitrary potential parameters are found by use of the {\it asymptotic iteration method}. - 22 June 2016
- Published by World Scientific Pub Co Pte Ltd in International Journal of Modern Physics E
- Vol. 25 (06)
Sharp comparison theorems for the Klein–Gordon equation in d dimensions
- 22 June 2016
- Published by World Scientific Pub Co Pte Ltd in International Journal of Modern Physics E
- Vol. 25 (06)
Sharp comparison theorems for the Klein–Gordon equation in d dimensions
- 18 April 2016
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 131 (4) , 1-13
Refined comparison theorems for the Dirac equation with spin and pseudo-spin symmetry in d dimensions
- 18 April 2016
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 131 (4) , 1-13
Refined comparison theorems for the Dirac equation with spin and pseudo-spin symmetry in d dimensions
- Open AccessSharp comparison theorems for the Klein--Gordon equation in $d$ dimensionsWe establish sharp (or `refined') comparison theorems for the Klein--Gordon equation. We show that the condition $V_a\le V_b$, which leads to $E_a\le E_b$, can be replaced by the weaker assumption $U_a\le U_b$ which still implies the spectral ordering $E_a\le E_b$. In the simplest case, for $d=1$, $U_i(x)=\int_0^x V_i(t)dt$, $i=a$ or $b$, and for $d>1$, $U_i(r)=\int_0^r V_i(t) t^{d-1}dt$, $i=a$ or $b$. We also consider sharp comparison theorems in the presence of a scalar potential $S$ (a `variable mass') in addition to the vector term $V$ (the time component of a $4$-vector). The theorems are illustrated by a variety of explicit detailed examples.Open AccessSharp comparison theorems for the Klein--Gordon equation in $d$ dimensionsWe establish sharp (or `refined') comparison theorems for the Klein--Gordon equation. We show that the condition $V_a\le V_b$, which leads to $E_a\le E_b$, can be replaced by the weaker assumption $U_a\le U_b$ which still implies the spectral ordering $E_a\le E_b$. In the simplest case, for $d=1$, $U_i(x)=\int_0^x V_i(t)dt$, $i=a$ or $b$, and for $d>1$, $U_i(r)=\int_0^r V_i(t) t^{d-1}dt$, $i=a$ or $b$. We also consider sharp comparison theorems in the presence of a scalar potential $S$ (a `variable mass') in addition to the vector term $V$ (the time component of a $4$-vector). The theorems are illustrated by a variety of explicit detailed examples.