Bound State Solution to Schrodinger Equation With Modified Hylleraas Plus Inversely Quadratic Potential Using Supersymmetric Quantum Mechanics Approach
In this work, we obtained an approximate bound state solution to Schrodinger equation with modified
Hylleraass plus inversely quadratic potential using Supersymmetric quantum mechanics approach.
Applying perkeris approximation to the centrifugal term, we obtained the eigen-energy and the normalized
wave function using Gauss and confluent hypergeometric functions. We implement Fortran algorithm to
obtained the numerical result of the energy for the screening parameter α = 0.1,0.2,0.3, 0.4 0.5 and .
The result shows that the energy increases with an increase in the quantum state. The energy spectrum
shows increase in angular quantum state spacing as the screening parameter increases.
BOUND STATE SOLUTION TO SCHRODINGER EQUATION WITH MODIFIED HYLLERAAS PLUS INV...ijrap
In this work, we obtained an approximate bound state solution to Schrodinger equation with modified
Hylleraass plus inversely quadratic potential using Supersymmetric quantum mechanics approach.
Applying perkeris approximation to the centrifugal term, we obtained the eigen-energy and the normalized
wave function using Gauss and confluent hypergeometric functions. We implement Fortran algorithm to
obtained the numerical result of the energy for the screening parameter α = 0.1,0.2,0.3, 0.4 0.5 and .
The result shows that the energy increases with an increase in the quantum state. The energy spectrum
shows increase in angular quantum state spacing as the screening parameter increases.
ANALYTICAL SOLUTIONS OF THE MODIFIED COULOMB POTENTIAL USING THE FACTORIZATIO...ijrap
This document presents analytical solutions to the Schrödinger equation with a modified Coulomb potential using the factorization method. The energy levels and wave functions are obtained in terms of associated Laguerre polynomials. Energy eigenvalues are computed for selected elements like hydrogen, lithium, sodium, potassium and copper for various values of n and l. The results show the expected degeneracies and reduce to the Coulomb energy solution when appropriate limits are taken.
This document discusses light-matter interaction using a two-level atom model. It describes how an atom with only two energy levels can be modeled as a two-dimensional quantum mechanical system. The interaction of such a two-level atom with an electromagnetic field is then derived, leading to Rabi oscillations between the atomic energy levels driven by the field. Dissipative processes require a statistical description using the density operator formalism.
SOLUTIONS OF THE SCHRÖDINGER EQUATION WITH INVERSELY QUADRATIC HELLMANN PLUS ...ijrap
The solutions of the Schrödinger equation with inversely quadratic Hellmann plus Mie-type potential for
any angular momentum quantum number have been presented using the Nikiforov-Uvarov method. The
bound state energy eigenvalues and the corresponding un-normalized eigenfunctions are obtained in terms
of the Laguerre polynomials. Several cases of the potential are also considered and their eigen values obtained.
Bound- State Solution of Schrodinger Equation with Hulthen Plus Generalized E...ijrap
- The document discusses using the Nikiforov-Uvarov method to find bound state solutions to the Schrodinger equation with Hulthen plus generalized exponential Coulomb potential.
- The method is applied to obtain the energy eigenvalues and total wave function for the potential.
- A C++ algorithm is used to numerically calculate the energy values for different quantum states and screening parameter values.
Bound State Solution to Schrodinger Equation with Hulthen Plus Exponential Co...ijrap
In this work, we obtained an approximate bound state solution to Schrodinger with Hulthen plus
exponential Coulombic potential with centrifugal potential barrier using parametric Nikiforov-Uvarov
method. We obtained both the eigen energy and the wave functions to non -relativistic wave equations. We
implement Matlab algorithm to obtained the numerical bound state energies for various values of
adjustable screening parameter at various quantum state.. The developed potential reduces to Hulthen
potential and the numerical bound state energy conform to that of existing literature.
These slides are especially made to understand the postulates of quantum mechanics or chemistry better. easily simplified and at one place you will find each of relevant details about the 5 postulates. so go through it & trust me it will help you a lot if you are chemistry or a science student.
well done
This document summarizes a research paper that develops a three-dimensional mathematical model of heat transfer using the stream function approach and numerical solution via finite element methods. The modeling is based on conservation of mass, momentum, and energy. Differential equations for continuity, Navier-Stokes, and heat transfer are derived and expressed in terms of the stream function. The system is then converted to a variational formulation and discretized using finite elements to obtain a numerical solution.
BOUND STATE SOLUTION TO SCHRODINGER EQUATION WITH MODIFIED HYLLERAAS PLUS INV...ijrap
In this work, we obtained an approximate bound state solution to Schrodinger equation with modified
Hylleraass plus inversely quadratic potential using Supersymmetric quantum mechanics approach.
Applying perkeris approximation to the centrifugal term, we obtained the eigen-energy and the normalized
wave function using Gauss and confluent hypergeometric functions. We implement Fortran algorithm to
obtained the numerical result of the energy for the screening parameter α = 0.1,0.2,0.3, 0.4 0.5 and .
The result shows that the energy increases with an increase in the quantum state. The energy spectrum
shows increase in angular quantum state spacing as the screening parameter increases.
ANALYTICAL SOLUTIONS OF THE MODIFIED COULOMB POTENTIAL USING THE FACTORIZATIO...ijrap
This document presents analytical solutions to the Schrödinger equation with a modified Coulomb potential using the factorization method. The energy levels and wave functions are obtained in terms of associated Laguerre polynomials. Energy eigenvalues are computed for selected elements like hydrogen, lithium, sodium, potassium and copper for various values of n and l. The results show the expected degeneracies and reduce to the Coulomb energy solution when appropriate limits are taken.
This document discusses light-matter interaction using a two-level atom model. It describes how an atom with only two energy levels can be modeled as a two-dimensional quantum mechanical system. The interaction of such a two-level atom with an electromagnetic field is then derived, leading to Rabi oscillations between the atomic energy levels driven by the field. Dissipative processes require a statistical description using the density operator formalism.
SOLUTIONS OF THE SCHRÖDINGER EQUATION WITH INVERSELY QUADRATIC HELLMANN PLUS ...ijrap
The solutions of the Schrödinger equation with inversely quadratic Hellmann plus Mie-type potential for
any angular momentum quantum number have been presented using the Nikiforov-Uvarov method. The
bound state energy eigenvalues and the corresponding un-normalized eigenfunctions are obtained in terms
of the Laguerre polynomials. Several cases of the potential are also considered and their eigen values obtained.
Bound- State Solution of Schrodinger Equation with Hulthen Plus Generalized E...ijrap
- The document discusses using the Nikiforov-Uvarov method to find bound state solutions to the Schrodinger equation with Hulthen plus generalized exponential Coulomb potential.
- The method is applied to obtain the energy eigenvalues and total wave function for the potential.
- A C++ algorithm is used to numerically calculate the energy values for different quantum states and screening parameter values.
Bound State Solution to Schrodinger Equation with Hulthen Plus Exponential Co...ijrap
In this work, we obtained an approximate bound state solution to Schrodinger with Hulthen plus
exponential Coulombic potential with centrifugal potential barrier using parametric Nikiforov-Uvarov
method. We obtained both the eigen energy and the wave functions to non -relativistic wave equations. We
implement Matlab algorithm to obtained the numerical bound state energies for various values of
adjustable screening parameter at various quantum state.. The developed potential reduces to Hulthen
potential and the numerical bound state energy conform to that of existing literature.
These slides are especially made to understand the postulates of quantum mechanics or chemistry better. easily simplified and at one place you will find each of relevant details about the 5 postulates. so go through it & trust me it will help you a lot if you are chemistry or a science student.
well done
This document summarizes a research paper that develops a three-dimensional mathematical model of heat transfer using the stream function approach and numerical solution via finite element methods. The modeling is based on conservation of mass, momentum, and energy. Differential equations for continuity, Navier-Stokes, and heat transfer are derived and expressed in terms of the stream function. The system is then converted to a variational formulation and discretized using finite elements to obtain a numerical solution.
1) The document presents two theorems regarding the absolute weighted mean |,|kAδ-summability of orthogonal series.
2) Theorem 1 states that if a certain series involving the coefficients of the orthogonal series converges, then the orthogonal series is summable |,|kAδ almost everywhere.
3) Theorem 2 is more general, introducing a positive weight sequence ω(n). It states that if another series involving the coefficients and ω(n) converges, then the orthogonal series is summable |,|kAδ almost everywhere.
Analytical Solution Of Schrödinger Equation With Mie–Type Potential Using Fac...ijrap
we have obtained the analytical solution of Schrödinger wave equation with Mie – type potential
using factorization method. We have also obtained energy eigenvalues of our potential and the
corresponding wave function using an ansatz and then compare the result to standard Laguerre’s
differential equation. Under special cases our potential model reduces two well known potentials such as
Coulomb and the Kratzer Feus potentials.
The document summarizes general gyrokinetic theory, which describes a symmetry in magnetized plasmas. It discusses:
1) Developing geometric Vlasov-Maxwell equations on a 7D phase space defined as a fiber bundle over spacetime. This determines particle worldlines and realizes kinetic integrals as fiber integrals.
2) Constructing the infinite small generator of gyrosymmetry by applying Lie coordinate perturbation to the Poincare-Cartan-Einstein 1-form. This generates the most relaxed condition for gyrosymmetry.
3) Developing general gyrokinetic Vlasov-Maxwell equations in the gyrocenter coordinate system rather than new equations, automatically carrying over properties like conservation laws. The pullback
This document is Scott Shermer's master's thesis on instantons and perturbation theory in the 1-D quantum mechanical quartic oscillator. It begins by reviewing the harmonic oscillator and perturbation theory. It then discusses non-perturbative phenomena like instantons and Borel resummation. The focus is on obtaining the ground state energy of the quartic oscillator Hamiltonian using both perturbative and non-perturbative techniques, and addressing ambiguities that arise for negative coupling.
This document introduces the concept of gauge invariance and gauge field theories. It discusses both global and local gauge symmetries:
- Global gauge symmetries lead to conserved currents and charges via Noether's theorem. They result in massless scalar bosons if spontaneously broken.
- Local gauge symmetries require the introduction of gauge fields which transform in a way that cancels out non-invariant terms under local transformations. This avoids the massless bosons and allows gauge fields to acquire mass. Quantum electrodynamics possesses a local U(1) gauge symmetry.
- Non-Abelian gauge groups were introduced by Yang and Mills, allowing the construction of gauge field theories with non-commuting gauge groups. Covariant derivatives are
Gauge field theory describes fundamental interactions through the principle of local gauge invariance. Quantum mechanics respects the gauge invariance of electromagnetic fields by requiring a simultaneous change in phase of the wavefunction under gauge transformations of potentials. Insisting on local gauge freedom in quantum mechanics forces the introduction of gauge fields that interact with particles. Yang-Mills theory extends this concept to field theories by demanding local gauge invariance of the Lagrangian density. This dictates that gauge fields belong to the Lie algebra of the symmetry group and interact with matter fields through covariant derivatives. The Lagrangian includes terms for gauge fields constructed from an invariant field strength tensor.
The document presents a criterion for determining when a pair of weighted composition operators acting on a Hilbert space of analytic functions satisfies the Hypercyclicity Criterion. Specifically:
1. The Hypercyclicity Criterion is introduced and shown to be a sufficient condition for hypercyclicity of operator pairs.
2. A theorem is presented proving that if two weighted composition operators satisfy certain conditions regarding their weights and composition map, then their adjoint operators satisfy the Hypercyclicity Criterion and are thus hypercyclic.
3. A corollary shows that the adjoint of a multiplication operator by a non-constant multiplier intersecting the unit circle also satisfies the Hypercyclicity Criterion.
International Journal of Computational Engineering Research (IJCER) is dedicated to protecting personal information and will make every reasonable effort to handle collected information appropriately. All information collected, as well as related requests, will be handled as carefully and efficiently as possible in accordance with IJCER standards for integrity and objectivity.
This document summarizes research on simplifying calculations of scattering amplitudes, especially for tree-level amplitudes. It introduces the spinor-helicity formalism for writing compact expressions for amplitudes. It then discusses color decomposition in SU(N) gauge theory and the Yang-Mills Lagrangian. Specific techniques explored include BCFW recursion relations, an inductive proof of the Parke-Taylor formula, the 4-graviton amplitude and KLT relations, multi-leg shifts, and the MHV vertex expansion. The goal is to develop recursion techniques that vastly simplify calculations compared to traditional Feynman diagrams.
The International Journal of Engineering & Science is aimed at providing a platform for researchers, engineers, scientists, or educators to publish their original research results, to exchange new ideas, to disseminate information in innovative designs, engineering experiences and technological skills. It is also the Journal's objective to promote engineering and technology education. All papers submitted to the Journal will be blind peer-reviewed. Only original articles will be published.
The papers for publication in The International Journal of Engineering& Science are selected through rigorous peer reviews to ensure originality, timeliness, relevance, and readability.
This document provides an overview of a physics lecture on units, dimensions, and vectors. The lecture introduces students to the International System of Units (SI) and the metric system of measurement. It discusses the basic SI units of length, mass, and time. The lecture also covers dimensional analysis, which uses the dimensions of physical quantities to check the validity of equations. Vector concepts such as coordinate systems and vector components are also introduced. The document aims to equip medical sciences students with the fundamental physics concepts needed to understand measurements and quantitative relationships in physics.
International Journal of Engineering Research and Applications (IJERA) is an open access online peer reviewed international journal that publishes research and review articles in the fields of Computer Science, Neural Networks, Electrical Engineering, Software Engineering, Information Technology, Mechanical Engineering, Chemical Engineering, Plastic Engineering, Food Technology, Textile Engineering, Nano Technology & science, Power Electronics, Electronics & Communication Engineering, Computational mathematics, Image processing, Civil Engineering, Structural Engineering, Environmental Engineering, VLSI Testing & Low Power VLSI Design etc.
1) The document discusses exact solutions of nonequilibrium steady states in many-body quantum systems using the matrix product ansatz.
2) It presents an exactly solvable model of a boundary driven XXZ spin chain, where the nonequilibrium steady state can be represented as a matrix product operator with a quadratic algebra.
3) Transport properties like the spin conductivity can be computed exactly using conservation laws that emerge from the integrability of the model.
This document discusses solutions to the Klein-Gordon equation in Schwarzschild spacetime near a black hole's event horizon. Very near the horizon, the radial Klein-Gordon equation can be approximated as an oscillatory solution in Regge-Wheeler coordinates. These solutions are then expressed in terms of outgoing and ingoing coordinates, which have distinct analytic properties inside and outside the event horizon.
This document discusses solutions to the Klein-Gordon equation in Schwarzschild spacetime near a black hole's event horizon. Very near the horizon, the radial Klein-Gordon equation can be approximated as an oscillatory solution in Regge-Wheeler coordinates. The time and radial solutions are then expressed in terms of outgoing and ingoing coordinates, which leads to outgoing and ingoing waves with different analytic properties on either side of the event horizon.
Outgoing ingoingkleingordon spvmforminit_proceedfromfoxtrot jp R
This document discusses outgoing and ingoing Klein-Gordon waves near the event horizons of a black hole. It begins by introducing the Klein-Gordon equation of motion in the background of the Schwarzschild spacetime metric. It then presents the solution to this equation in product form and discusses the radial and time component equations. Finally, it recasts the radial equation using the Regge-Wheeler coordinate and shows that very near the horizon, the equation can be approximated as a simple oscillatory solution. The goal is to obtain outgoing and ingoing wave solutions that have different properties on either side of the black hole's event horizons.
Outgoing ingoingkleingordon spvmforminit_proceedfrom12dec18foxtrot jp R
This document discusses outgoing and ingoing Klein-Gordon waves near the event horizons of a black hole. It begins by introducing the Klein-Gordon equation of motion in the background of the Schwarzschild spacetime metric. It then presents the solution to this equation in product form and discusses the radial and time component equations. Finally, it recasts the radial equation using the Regge-Wheeler coordinate and shows that very near the horizon, the equation can be approximated as a simple oscillatory solution. The goal is to obtain outgoing and ingoing wave solutions that have different properties on either side of the black hole's event horizons.
The document summarizes the theoretical framework for studying quantum resonances in diatomic molecules using the Born-Oppenheimer approximation. It considers the Hamiltonian for a diatomic molecule, with coordinates for the two nuclei and one electron. By fixing angular momentum and applying a rotation, the problem can be reduced to studying an effective one-dimensional Hamiltonian as a function of the internuclear distance R. Under certain assumptions about the electronic eigenvalues and effective potentials, the Hamiltonian takes the form of particle in overlapping potential wells, setting up the problem of studying resonances between the wells.
EXACT SOLUTIONS OF SCHRÖDINGER EQUATION WITH SOLVABLE POTENTIALS FOR NON PT/P...ijrap
We have obtained explicitly the exact solutions of the Schrodinger equation with Non PT/PT symmetric
Rosen Morse II, Scarf II and Coulomb potentials. Energy eigenvalues and the corresponding
unnormalized wave functions for these systems for both Non PT and PT symmetric are also obtained using
the Nikiforov-Uvarov (NU) method.
Analytical Solutions of the Modified Coulomb Potential using the Factorizatio...ijrap
The document presents analytical solutions to the Schrodinger equation with a modified Coulomb potential using the factorization method. The radial part of the Schrodinger equation is solved using the factorization method, resulting in wave functions expressed in terms of associated Laguerre polynomials. Energy eigenvalues are obtained and presented for selected values of n and l for hydrogen, lithium, sodium, potassium, and copper.
Solutions of the Schrodinger Equation with Inversely Quadratic Hellmann Plus ...ijrap
The solutions of the Schrödinger equation with inversely quadratic Hellmann plus Mie-type potential for
any angular momentum quantum number have been presented using the Nikiforov-Uvarov method. The
bound state energy eigenvalues and the corresponding un-normalized eigenfunctions are obtained in terms
of the Laguerre polynomials. Several cases of the potential are also considered and their eigen values
obtained.
1) The document presents two theorems regarding the absolute weighted mean |,|kAδ-summability of orthogonal series.
2) Theorem 1 states that if a certain series involving the coefficients of the orthogonal series converges, then the orthogonal series is summable |,|kAδ almost everywhere.
3) Theorem 2 is more general, introducing a positive weight sequence ω(n). It states that if another series involving the coefficients and ω(n) converges, then the orthogonal series is summable |,|kAδ almost everywhere.
Analytical Solution Of Schrödinger Equation With Mie–Type Potential Using Fac...ijrap
we have obtained the analytical solution of Schrödinger wave equation with Mie – type potential
using factorization method. We have also obtained energy eigenvalues of our potential and the
corresponding wave function using an ansatz and then compare the result to standard Laguerre’s
differential equation. Under special cases our potential model reduces two well known potentials such as
Coulomb and the Kratzer Feus potentials.
The document summarizes general gyrokinetic theory, which describes a symmetry in magnetized plasmas. It discusses:
1) Developing geometric Vlasov-Maxwell equations on a 7D phase space defined as a fiber bundle over spacetime. This determines particle worldlines and realizes kinetic integrals as fiber integrals.
2) Constructing the infinite small generator of gyrosymmetry by applying Lie coordinate perturbation to the Poincare-Cartan-Einstein 1-form. This generates the most relaxed condition for gyrosymmetry.
3) Developing general gyrokinetic Vlasov-Maxwell equations in the gyrocenter coordinate system rather than new equations, automatically carrying over properties like conservation laws. The pullback
This document is Scott Shermer's master's thesis on instantons and perturbation theory in the 1-D quantum mechanical quartic oscillator. It begins by reviewing the harmonic oscillator and perturbation theory. It then discusses non-perturbative phenomena like instantons and Borel resummation. The focus is on obtaining the ground state energy of the quartic oscillator Hamiltonian using both perturbative and non-perturbative techniques, and addressing ambiguities that arise for negative coupling.
This document introduces the concept of gauge invariance and gauge field theories. It discusses both global and local gauge symmetries:
- Global gauge symmetries lead to conserved currents and charges via Noether's theorem. They result in massless scalar bosons if spontaneously broken.
- Local gauge symmetries require the introduction of gauge fields which transform in a way that cancels out non-invariant terms under local transformations. This avoids the massless bosons and allows gauge fields to acquire mass. Quantum electrodynamics possesses a local U(1) gauge symmetry.
- Non-Abelian gauge groups were introduced by Yang and Mills, allowing the construction of gauge field theories with non-commuting gauge groups. Covariant derivatives are
Gauge field theory describes fundamental interactions through the principle of local gauge invariance. Quantum mechanics respects the gauge invariance of electromagnetic fields by requiring a simultaneous change in phase of the wavefunction under gauge transformations of potentials. Insisting on local gauge freedom in quantum mechanics forces the introduction of gauge fields that interact with particles. Yang-Mills theory extends this concept to field theories by demanding local gauge invariance of the Lagrangian density. This dictates that gauge fields belong to the Lie algebra of the symmetry group and interact with matter fields through covariant derivatives. The Lagrangian includes terms for gauge fields constructed from an invariant field strength tensor.
The document presents a criterion for determining when a pair of weighted composition operators acting on a Hilbert space of analytic functions satisfies the Hypercyclicity Criterion. Specifically:
1. The Hypercyclicity Criterion is introduced and shown to be a sufficient condition for hypercyclicity of operator pairs.
2. A theorem is presented proving that if two weighted composition operators satisfy certain conditions regarding their weights and composition map, then their adjoint operators satisfy the Hypercyclicity Criterion and are thus hypercyclic.
3. A corollary shows that the adjoint of a multiplication operator by a non-constant multiplier intersecting the unit circle also satisfies the Hypercyclicity Criterion.
International Journal of Computational Engineering Research (IJCER) is dedicated to protecting personal information and will make every reasonable effort to handle collected information appropriately. All information collected, as well as related requests, will be handled as carefully and efficiently as possible in accordance with IJCER standards for integrity and objectivity.
This document summarizes research on simplifying calculations of scattering amplitudes, especially for tree-level amplitudes. It introduces the spinor-helicity formalism for writing compact expressions for amplitudes. It then discusses color decomposition in SU(N) gauge theory and the Yang-Mills Lagrangian. Specific techniques explored include BCFW recursion relations, an inductive proof of the Parke-Taylor formula, the 4-graviton amplitude and KLT relations, multi-leg shifts, and the MHV vertex expansion. The goal is to develop recursion techniques that vastly simplify calculations compared to traditional Feynman diagrams.
The International Journal of Engineering & Science is aimed at providing a platform for researchers, engineers, scientists, or educators to publish their original research results, to exchange new ideas, to disseminate information in innovative designs, engineering experiences and technological skills. It is also the Journal's objective to promote engineering and technology education. All papers submitted to the Journal will be blind peer-reviewed. Only original articles will be published.
The papers for publication in The International Journal of Engineering& Science are selected through rigorous peer reviews to ensure originality, timeliness, relevance, and readability.
This document provides an overview of a physics lecture on units, dimensions, and vectors. The lecture introduces students to the International System of Units (SI) and the metric system of measurement. It discusses the basic SI units of length, mass, and time. The lecture also covers dimensional analysis, which uses the dimensions of physical quantities to check the validity of equations. Vector concepts such as coordinate systems and vector components are also introduced. The document aims to equip medical sciences students with the fundamental physics concepts needed to understand measurements and quantitative relationships in physics.
International Journal of Engineering Research and Applications (IJERA) is an open access online peer reviewed international journal that publishes research and review articles in the fields of Computer Science, Neural Networks, Electrical Engineering, Software Engineering, Information Technology, Mechanical Engineering, Chemical Engineering, Plastic Engineering, Food Technology, Textile Engineering, Nano Technology & science, Power Electronics, Electronics & Communication Engineering, Computational mathematics, Image processing, Civil Engineering, Structural Engineering, Environmental Engineering, VLSI Testing & Low Power VLSI Design etc.
1) The document discusses exact solutions of nonequilibrium steady states in many-body quantum systems using the matrix product ansatz.
2) It presents an exactly solvable model of a boundary driven XXZ spin chain, where the nonequilibrium steady state can be represented as a matrix product operator with a quadratic algebra.
3) Transport properties like the spin conductivity can be computed exactly using conservation laws that emerge from the integrability of the model.
This document discusses solutions to the Klein-Gordon equation in Schwarzschild spacetime near a black hole's event horizon. Very near the horizon, the radial Klein-Gordon equation can be approximated as an oscillatory solution in Regge-Wheeler coordinates. These solutions are then expressed in terms of outgoing and ingoing coordinates, which have distinct analytic properties inside and outside the event horizon.
This document discusses solutions to the Klein-Gordon equation in Schwarzschild spacetime near a black hole's event horizon. Very near the horizon, the radial Klein-Gordon equation can be approximated as an oscillatory solution in Regge-Wheeler coordinates. The time and radial solutions are then expressed in terms of outgoing and ingoing coordinates, which leads to outgoing and ingoing waves with different analytic properties on either side of the event horizon.
Outgoing ingoingkleingordon spvmforminit_proceedfromfoxtrot jp R
This document discusses outgoing and ingoing Klein-Gordon waves near the event horizons of a black hole. It begins by introducing the Klein-Gordon equation of motion in the background of the Schwarzschild spacetime metric. It then presents the solution to this equation in product form and discusses the radial and time component equations. Finally, it recasts the radial equation using the Regge-Wheeler coordinate and shows that very near the horizon, the equation can be approximated as a simple oscillatory solution. The goal is to obtain outgoing and ingoing wave solutions that have different properties on either side of the black hole's event horizons.
Outgoing ingoingkleingordon spvmforminit_proceedfrom12dec18foxtrot jp R
This document discusses outgoing and ingoing Klein-Gordon waves near the event horizons of a black hole. It begins by introducing the Klein-Gordon equation of motion in the background of the Schwarzschild spacetime metric. It then presents the solution to this equation in product form and discusses the radial and time component equations. Finally, it recasts the radial equation using the Regge-Wheeler coordinate and shows that very near the horizon, the equation can be approximated as a simple oscillatory solution. The goal is to obtain outgoing and ingoing wave solutions that have different properties on either side of the black hole's event horizons.
The document summarizes the theoretical framework for studying quantum resonances in diatomic molecules using the Born-Oppenheimer approximation. It considers the Hamiltonian for a diatomic molecule, with coordinates for the two nuclei and one electron. By fixing angular momentum and applying a rotation, the problem can be reduced to studying an effective one-dimensional Hamiltonian as a function of the internuclear distance R. Under certain assumptions about the electronic eigenvalues and effective potentials, the Hamiltonian takes the form of particle in overlapping potential wells, setting up the problem of studying resonances between the wells.
Similar to Bound State Solution to Schrodinger Equation With Modified Hylleraas Plus Inversely Quadratic Potential Using Supersymmetric Quantum Mechanics Approach
EXACT SOLUTIONS OF SCHRÖDINGER EQUATION WITH SOLVABLE POTENTIALS FOR NON PT/P...ijrap
We have obtained explicitly the exact solutions of the Schrodinger equation with Non PT/PT symmetric
Rosen Morse II, Scarf II and Coulomb potentials. Energy eigenvalues and the corresponding
unnormalized wave functions for these systems for both Non PT and PT symmetric are also obtained using
the Nikiforov-Uvarov (NU) method.
Analytical Solutions of the Modified Coulomb Potential using the Factorizatio...ijrap
The document presents analytical solutions to the Schrodinger equation with a modified Coulomb potential using the factorization method. The radial part of the Schrodinger equation is solved using the factorization method, resulting in wave functions expressed in terms of associated Laguerre polynomials. Energy eigenvalues are obtained and presented for selected values of n and l for hydrogen, lithium, sodium, potassium, and copper.
Solutions of the Schrodinger Equation with Inversely Quadratic Hellmann Plus ...ijrap
The solutions of the Schrödinger equation with inversely quadratic Hellmann plus Mie-type potential for
any angular momentum quantum number have been presented using the Nikiforov-Uvarov method. The
bound state energy eigenvalues and the corresponding un-normalized eigenfunctions are obtained in terms
of the Laguerre polynomials. Several cases of the potential are also considered and their eigen values
obtained.
Analytical Solution Of Schrödinger Equation With Mie–Type Potential Using Fac...ijrap
we have obtained the analytical solution of Schrödinger wave equation with Mie – type potential
using factorization method. We have also obtained energy eigenvalues of our potential and the
corresponding wave function using an ansatz and then compare the result to standard Laguerre’s
differential equation. Under special cases our potential model reduces two well known potentials such as
Coulomb and the Kratzer Feus potentials
The document discusses solving the Schrodinger equation to obtain bound state solutions and scattering phase shifts for a modified trigonometric Scarf type potential. It presents the asymptotic iteration method used to find the approximate bound state energies. The scattering phase shift is then calculated by expressing the radial wavefunction as a hypergeometric function and analyzing its asymptotic behavior. The potential's effect on the eigenvalues and scattering is studied numerically.
Analytical Solution Of Schrodinger Equation With Mie-Type Potential Using Fac...ijrap
we have obtained the analytical solution of Schrödinger wave equation with Mie – type potential
using factorization method. We have also obtained energy eigenvalues of our potential and the
corresponding wave function using an ansatz and then compare the result to standard Laguerre’s
differential equation. Under special cases our potential model reduces two well known potentials such as
Coulomb and the Kratzer Feus potentials.
IOSR Journal of Applied Physics (IOSR-JAP) is an open access international journal that provides rapid publication (within a month) of articles in all areas of physics and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in applied physics. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
The document summarizes key concepts from elementary quantum physics that will be built upon in the text, including:
1) The time-dependent and time-independent Schrodinger equations, which describe the wave function and energy levels of quantum systems.
2) Observables in quantum physics are represented by operators, and the measurement of an observable leaves the system in an eigenstate of that operator.
3) The Heisenberg uncertainty principle limits the precision with which conjugate variables like position and momentum can be known simultaneously.
4) Angular momentum is quantized and can be decomposed into orbital and spin components, with associated quantum numbers and eigenstates. Operators for total and z-component angular
Exact Bound State Solution of Qdeformed Woods-Saxon Plus Modified Coulomb Pot...ijrap
In this work, we obtained an exact solution to Schrodinger equation using q-deformed Woods-Saxon plus
modified Coulomb potential Using conventional Nikiforov-Uvarov method. We also obtained the energy
eigen value and its associated total wave function . This potential with some suitable conditions reduces to
two well known potentials namely: the Yukawa and coulomb potential. Finally, we obtained the numerical
results for energy eigen value with different values of q as dimensionless parameter. The result shows that
the values of the energies for different quantum number(n) is negative(bound state condition) and increases
with an increase in the value of the dimensionless parameter(arbitrary constant). The graph in figure (1)
shows the different energy levels for a particular quantum number.
Exact Bound State Solution of Qdeformed Woods-Saxon Plus Modified Coulomb Pot...ijrap
1) The document presents an exact solution to the Schrodinger equation using a q-deformed Woods-Saxon plus modified Coulomb potential via the Nikiforov-Uvarov method.
2) Key results include obtaining the energy eigenvalues and total wave function. The potential reduces to Yukawa and Coulomb potentials under certain conditions.
3) Numerical results show the energy increases with the dimensionless parameter q and is negative, satisfying the bound state condition.
Schrodinger equation and its applications: Chapter 2Dr.Pankaj Khirade
Wave function and its physical significance, Schrodinger time dependent equation, Separation in time dependent and time independent parts, Operators in quantum Mechanics, Eigen functions and Eigen values, Particle in one dimensional and three dimensional box (Energy eigen values). Qualitative analysis of potential barrier Tunneling effect). Simple Harmonic Oscillator (Qualitative analysis of Zero point energy)
On Approach of Estimation Time Scales of Relaxation of Concentration of Charg...Zac Darcy
In this paper we generalized recently introduced approach for estimation of time scales of mass transport.
The approach have been illustrated by estimation of time scales of relaxation of concentrations of charge
carriers in high-doped semiconductor. Diffusion coefficients and mobility of charge carriers and electric
field strength in semiconductor could be arbitrary functions of coordinate.
Exact Solutions of the Klein-Gordon Equation for the Q-Deformed Morse Potenti...ijrap
This document presents an analysis of solving the Klein-Gordon equation for the q-deformed Morse potential using the Nikiforov-Uvarov method. The eigenfunctions and eigenvalues of the Klein-Gordon equation are obtained. It is found that the eigenfunctions can be expressed in terms of Laguerre polynomials. The energy eigenvalues and normalized eigenfunctions obtained agree with previous studies that used algebraic approaches.
Quark Model Three Body Calculations for the Hypertriton Bound StateIOSR Journals
Hyperspherical three body calculations are performed to study and review the various properties of
the hypertriton bound state nucleus
3H in the quark model using -N potentials. In these calculations we study
the different effects of the -N potentials on the hypertriton bound states as well as the separation energy B. A
combination of realistic two body N-N potentials with various - N potentials are considered. Complete
symmetric and mixed symmetric wave functions are introduced. using the renormalized Numerov method. The
agreement between the calculated
3H binding energies and the available experimental data basically depends
on the type of the -N interactions used in the calculations. It was found that the -N potentials are the most
effective part in the hypertriton binding energy as well as the separation energy B where the -N potentials is
very effective to bound or unbound the
3H hyper nucleus
Pacs numbers: 21.30. + y, 21.10.+dr,27.20.+n
He laplace method for special nonlinear partial differential equationsAlexander Decker
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by Daley, K.
Published in IJTP in 2009. http://adsabs.harvard.edu/abs/2009IJTP..tmp...67D
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Similar to Bound State Solution to Schrodinger Equation With Modified Hylleraas Plus Inversely Quadratic Potential Using Supersymmetric Quantum Mechanics Approach (20)
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Bound State Solution to Schrodinger Equation With Modified Hylleraas Plus Inversely Quadratic Potential Using Supersymmetric Quantum Mechanics Approach
1. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
DOI : 10.14810/ijrap.2015.4403 27
BOUND STATE SOLUTION TO SCHRODINGER
EQUATION WITH MODIFIED HYLLERAAS PLUS
INVERSELY QUADRATIC POTENTIAL USING
SUPERSYMMETRIC QUANTUM MECHANICS
APPROACH
Ituen .B.Okon1
, Oyebola Popoola2
and Eno.E. Ituen1
1
Department of Physics, University of Uyo, Uyo, Nigeria.
2
Department of Physics, University of Ibadan, Ibadan, Nigeria.
1
Department of Physics, University of Uyo, Uyo, Nigeria.
ABSTRACT
In this work, we obtained an approximate bound state solution to Schrodinger equation with modified
Hylleraass plus inversely quadratic potential using Supersymmetric quantum mechanics approach.
Applying perkeris approximation to the centrifugal term, we obtained the eigen-energy and the normalized
wave function using Gauss and confluent hypergeometric functions. We implement Fortran algorithm to
obtained the numerical result of the energy for the screening parameter 0.1,0.2,0.3,0.4 0.5
and
α = .
The result shows that the energy increases with an increase in the quantum state. The energy spectrum
shows increase in angular quantum state spacing as the screening parameter increases.
KEYWORDS
Schrodinger, Supersymmetric Quantum Mechanics Approach, Modified Hylleraass plus Inversely
Quadratic potential.
1. INTRODUCTION
Schrodinger wave equation belongs to non-relativistic wave equation. The total wave function of
any quantum mechanical system basically provides implicitly the relevant information about the
physical behavior of the system. Bound state solutions most time provides negative energies
because oftenly, the energy of the particle is less than the maximum potential energy therefore,
causing the particle to be trapped within the potential well. However, in a well that is infinitely
long, the particles can have positive energies and are still trapped within the potential well, hence
we can conclude that for infinitely long potential well, bound state energy of a particle is either
less than the potential at negative infinity( )
E < −∞ or less than the potential at positive infinity
( )
E < ∞ which provides the reason for obtaining both negative and positive bound state energies
predominantly in Klein-Gordon equation. A lot of authors developed interest in studying bound
state solutions majorly due to its scientific applications in both physical and chemical sciences in
particle, high energy Physics and molecular dynamics . [1-3].
2. International Journal of Recent adv
Different analytical techniques have been adopted by different authors in providing solutions to
relativistic and non- relativistic wave equations. These are: Nikifor
quantisation, asymptotic iteration method, supersymmetric quantum mechanics approach,
factorization method, tridiagonalisation method etc.[4
consideration are: woods-Saxon plus modified exponential
generalized exponential coulomb potential,
Teller, kratzer fues and Mie-Type potential, Eckart potential and
etc [11-20]. This paper is organized
introduced the concept of supersymmetric quantum mechanics approach. In section 3, we apply
the concept of supersymmetry to provide the solution to Schrodinger equation using the proposed
potential and obtained the energy eigen value and the wave function.. In section 4, we implement
an algorithm to obtained numerical computation for the resulting energy.
The modified Hylleraas plus inversely quadratic potential is given by
2
0 3
1
2 2
2
( )
1
r
r
v e
V r
e r
α
α
χ
χ
χ
−
−
−
= +
−
Where 3
χ is a constant , 1
χ and
against the inter-nuclear distance with various values of the screening parameter
1.0,2.0,3.0 4.0
and
α = is shown below. The chosen
graph which is quite different from the one for numerical computation.
2.THE CONCEPT OF SUPERYSYMMETRIC QUANTUM
MECHANICS(SUSYQM)
The supersymmetric approach deals with the partner Hamiltonian of the form
2
( )
2
p
H V x
m
± = +
Where P is the momentum and V(x) is the effective potential which can be expressed in terms of
super-potential as
2
( ) ( ) ( )
eff
V x x x
φ φ
±
′
= ±
The ground state energy is obtained as
International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
Different analytical techniques have been adopted by different authors in providing solutions to
relativistic wave equations. These are: Nikiforov-Uvarov method, exact
quantisation, asymptotic iteration method, supersymmetric quantum mechanics approach,
factorization method, tridiagonalisation method etc.[4-10] . Some of the potentials under
Saxon plus modified exponential coulomb potential, Hulthen plus
generalized exponential coulomb potential, Rosen-Morse, Hulthen, pseudo harmonic, Poschl
pe potential, Eckart potential and P-T symmetric Hulthen potential
20]. This paper is organized as follows: section 1 is the introduction. In section 2, we
introduced the concept of supersymmetric quantum mechanics approach. In section 3, we apply
the concept of supersymmetry to provide the solution to Schrodinger equation using the proposed
al and obtained the energy eigen value and the wave function.. In section 4, we implement
an algorithm to obtained numerical computation for the resulting energy.
The modified Hylleraas plus inversely quadratic potential is given by
and 2
χ are Hylleraas parameter. The graph of this potential
nuclear distance with various values of the screening parameter
is shown below. The chosen α is to enable one sees the nature of the
graph which is quite different from the one for numerical computation.
Figure a.
CEPT OF SUPERYSYMMETRIC QUANTUM
MECHANICS(SUSYQM)
The supersymmetric approach deals with the partner Hamiltonian of the form
Where P is the momentum and V(x) is the effective potential which can be expressed in terms of
The ground state energy is obtained as
ances in Physics (IJRAP) Vol.4, No.4, November 2015
28
Different analytical techniques have been adopted by different authors in providing solutions to
Uvarov method, exact
quantisation, asymptotic iteration method, supersymmetric quantum mechanics approach,
10] . Some of the potentials under
coulomb potential, Hulthen plus
Morse, Hulthen, pseudo harmonic, Poschl-
T symmetric Hulthen potential
as follows: section 1 is the introduction. In section 2, we
introduced the concept of supersymmetric quantum mechanics approach. In section 3, we apply
the concept of supersymmetry to provide the solution to Schrodinger equation using the proposed
al and obtained the energy eigen value and the wave function.. In section 4, we implement
(1)
are Hylleraas parameter. The graph of this potential
nuclear distance with various values of the screening parameter
one sees the nature of the
CEPT OF SUPERYSYMMETRIC QUANTUM
(2)
Where P is the momentum and V(x) is the effective potential which can be expressed in terms of
(3)
3. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
29
1
0 ( ) N
x Ce
φ− −
= (4)
where N is the normalization constant which for very simple cases can be determined using the
expression
0
( ) ( )
x
x
N x r dr
φ
= ∫
(5)
However, the superpotential satisfies shape invariant condition of the form
0 1 1
( , ) ( , ) ( )
V a x V a x R a
+ −
= + (6)
Where 1
a is a new set of parameter uniquely determined from the old set 0
a through the
mapping 0 1 0
: ( )
f a a f a
→ = (7)
The supersymmetric energy is determined as
1
( )
n
n s
s
E R a
=
= ∑ (8)
While higher order state solutions are obtained through the expression
( )
†
1
0 0
1
0 2
( )
( , ) ( , )
n
s
n n
s
n s
A a
a x a x
E E
φ φ
−
− −
=
=
−
∏ (9)
Where †
( )
s
A a is a raising ladder operator expressed as
†
( , )
s s
A a x
x
φ
∂
= − +
∂
(10)
3. RADIAL SOLUTION OF SCHRODINGER EQUATION
Schrodinger equation is given by
( )
2
2 2 2
2 ( 1)
( ) ( ) 0
nl
d R l l
E V r R r
dr r
µ +
+ − − =
h
(11)
Substituting equation (1) into (11) gives
2
2
0 3
1
2 2 2 2 2
2
2 ( 1)
( ) 0
1
r
nl r
v e
d R l l
E R r
dr e r r
α
α
χ
χ
µ
χ
−
−
+
+ + − − =
−
h
(12)
Let’s define suitable approximation to the centrifugal term as
( )
2 1
0
2 2
1
1 r
D
D
r e α
α −
= +
−
(13)
Substituting equation (13) into (12) and re-arranging gives
4. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
30
( )
2 2
2
2
0 1 0 3 1
1
2 2 2
2
2
2
2 0 3 0
0
2 2
2 2
1
( 1) ( )
1
2
2
( 1) ( )
r
r
v e v D
d R
l l D R r
dr e
v D
E
l l D R r
α
α
µ χ µ χ α
α
χ
µ χ α
µ
α
−
−
+ − − +
−
= − − + −
h h
h h
(14)
This can also be represented as
( )
2 2
2
2
0 3 1 0 1
1
2 2 2
2
2
2
2 0 3 0
0
2 2
2 2
1
( 1) ( )
1
2
2
( 1) ( )
r
r
v D v e
d R
l l D R r
dr e
v D
E
l l D R r
α
α
µ χ α µ χ
α
χ
µ χ α
µ
α
−
−
− + + −
−
= − − + −
h h
h h
(15)
Let’s define second order differential equation containing effective potential as
2
2
( )
( ) ( ) ( )
nl
eff nl nl nl
d R r
V r R r E R r
dr
− + = % (16)
In order to represent equation (15) in the form of equation (16) , then equation (15) is multiply by
-1.
( )
2 2
2
2
0 3 1 0 1
1
2 2 2
2
2
2
2 0 3 0
0
2 2
2 2
1
( 1) ( )
1
2
2
( 1) ( )
r
r
v D v e
d R
l l D R r
dr e
v D
E
l l D R r
α
α
µ χ α µ χ
α
χ
µ χ α
µ
α
−
−
− + + + −
−
= − + −
h h
h h
(17)
Comparing equation (17) to (16), we obtained the following:
( )
2 2
2
0 3 1 0 1
1
2 2
2
2
2
2 0 3 0
0
2 2
2 2
1
( ) ( 1)
1
2
2
( 1) (18 )
r
eff r
nl
v D v e
V r l l D
e
v D
E
E l l D b
α
α
µ χ α µ χ
α
χ
µ χ α
µ
α
−
−
= + + −
−
= − + −
h h
%
h h
(18).
Let
2
2
0 3 1
1
2
2
( 1)
v D
A l l D
µ χ α
α
= + +
h
and 0 1
2
2
2 v
B
µ χ
χ
= −
h
(19)
Then, the effective potential reduced to
( )
2
2
1
( )
1
r
eff r
V r A Be
e
α
α
−
−
= +
−
(20)
The super-potential suitable for the effective potential is given as
( )
1
2
2
( )
1 r
q
r q
e α
φ −
−
= +
−
(21)
In order to construct partner potential, we apply equation (6) by first taking the square and first
derivative of equation (21)
5. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
31
( )
2
1
2
2
2
( )
1
r
r
q e
r
e
α
α
α
φ
−
−
′ =
−
(22)
( ) ( )
2
2 2 1 2 1
2 2
2 2
2
( )
1 1
r r
q q q
r q
e e
α α
φ − −
= − +
− −
(23)
The partner potentials are
( ) ( ) ( )
2 2
2 2 1 2 1 2
2 2 2
2 2 2
2 2
( ) ( ) ( )
1 1 1
r
eff r r r
q q q q e
V r r r q
e e e
α
α α α
α
φ φ
−
+
− − −
′
= + = − + +
− − −
(24)
( ) ( ) ( )
2 2
2 2 1 2 1 2
2 2 2
2 2 2
2 2
( ) ( ) ( )
1 1 1
r
eff r r r
q q q q e
V r r r q
e e e
α
α α α
α
φ φ
−
−
− − −
′
= − = − + −
− − −
(25)
Equation (24) and (25) satisfies shape invariant condition.
3.1 CALCULATION OF GROUND STATE ENERGY
The ground state energy can be calculated by solving associated Riccati equation. This equation
is given as
2
0
( ) ( ) ( )
eff l
r r V r E
φ φ′
− = − % (26)
Where 0l
E
% is the ground state energy.
Substituting equation (20) and (25) into (26) and simplifying in decreasing order of exponent
gives rise to three pairs of simultaneous equations
1
2 2
0 1 2 2
2
l
A E q q q q
+ = + −
% (27)
1 1
2
0 2 2
2 2 2 2
l
B A E q q q q
α
− − = − + −
% (28)
2
0 2
l
E B q
− =
% (29)
Solving the following simultaneous equations then
2
1 2 2 ( )
q q q A B
= ± + + (30)
2
2
1 1
2 2
1 1
2 2
2 2
A B q A B q
q q
q q
α α
+ + + +
= − ⇒ =
(31)
The ground state energy is calculated using equation (29)
2 2
1 1
0 0
1 1
2 2
2 2
l l
A B q A B q
E B E B
q q
α α
+ + + +
= + ⇒ − = − −
% % (32)
6. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
32
3.2 CALULATION OF HIGHER ORDER SUPERSYMMETRIC ENERGY
Using the condition of shape invariant, higher order supersymmetric energy can be calculated as
using
1
( )
nl k
k
E R a
∞
−
=
= ∑ (33)
Equation (33) satisfying shape invariant condition can be evaluated as follows
1 0 1
2 0 2
3 0 3
1
( ) ( ) ( )
( ) ( ) ( )
( ) ( ) ( )
( ) ( ) ( )
n n n
R a R a R a
R a R a R a
R a R a R a
R a R a R a
−
= −
= −
= −
= −
(34)
Thus, there is one to one corresponding mapping as shown below.
1 1
0 0
1 0
1
:
:
:
:
:
n n
n
q q
a a
a a n
q a
q a
α
α
α
+
+
+
⇒
⇒
a
a
a
a
a
(35)
Therefore, using (35), equation (31) can be written as
2
2
2 2 0
1
2 2
1 0
2
2
2 2
A B q
A B q
q q
q q
α
α
+ +
+ +
= ⇒ =
(36)
Using equation (34), the following evaluations is carried out
2 2
0 1
1
0 1
2 2
1 2
2
1 2
2
2
3
2
3
2 3
2 2
0
1 0
2 2
( )
2 2
2 2
( )
2 2
2
2
( )
2 2
2 2
( )
2 2
n
nl k
k n
A B q A B q
R a
q q
A B q A B q
R a
q q
A B q
A B q
R a
q q
A B a A B a
E R a
a a
α α
α α
α
α
α α
∞
−
=
+ + + +
= −
+ + + +
= −
+ +
+ +
= −
+ + + +
= = −
∑
(37)
7. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
33
3.3 CALCULATION OF TOTAL ENERGY
The total energy is the sum of the ground state energy and higher order supersymmetric energy.
This is given as
0
nl nl l
E E E
= +
% % (38)
Sometimes, the ground state energy can be negative (bound State condition) like in hydrogen
atom which is about -13.6eV.
Hence, equation (38) can in this manner be expressed as
0
( )
nl nl l
E E E
= + −
% % (39)
Substituting equation (32) and (37) into (39) gives
2
2
n
nl
n
A B a
E B
a
α
+ +
= − +
% (40)
Let’s recall equation (30)
2 2
1 2 2 1 2
( ) ( ) , :
q q q A B q A B q
α α α
= ± + + ⇒ = ± + + a
If 1
: , :
n n n
a a n for q a
α
+
a a
Then ( )
2 2
( ) 1 ( )
n n
a n A B a n A B
α α α α α
= + ± + + ⇒ = + ± + +
(41)
Substituting equation (18b) and equation (41) into (40) and simplifying gives the total energy as
2 2
2 2 2
3 1 0 1 3 1 0 1
1 1
2 2 2
2
2 2 0 1
2
2
2
2
3 1 0 1
1
2 2
2
2 2
2
3 0
2 2 2 2
( 1) 2 1 ( 1)
2
2 2 2
2 1 ( 1)
( 1)
nl
D v D v
l l D n l l D
v
E
D v
n l l D
l l
D
µχα µ χ µχα µ χ
α α α
χ χ µ χ
µ χ
µχα µ χ
α α
χ
α
χα
+ + − + + ± + + −
=− −
+ ± + + −
+
+ +
h h h
h
h
h h
h 0
(42)
2
D
µ
Equation (42) is the energy equation for Hylleraas plus inversely quadratic potential. However,
because of the plus and minus accaompanied by the square root sign, equation (42) can be
expressed as follows:
2 2
2 2 2
3 1 0 1 3 1 0 1
1 1
2 2 2
2
2 2 0 1
2
2
2
2
3 1 0 1
1
2 2
2
2 2
2
3 0
2 2 2 2
( 1) 2 1 ( 1)
2
2 2 2
2 1 ( 1)
( 1)
nl
D v D v
l l D n l l D
v
E
D v
n l l D
l l
D
µχα µ χ µχα µ χ
α α α
χ χ µ χ
µ χ
µχα µ χ
α α
χ
α
χα
+ + − + + + + + −
=− −
+ + + + −
+
+ +
h h h
h
h
h h
h 0
(43)
2
D
µ
8. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
34
2 2
2 2 2
3 1 0 1 3 1 0 1
1 1
2 2 2
2
2 2 0 1
2
2
2
2
3 1 0 1
1
2 2
2
2 2
2
3 0
2 2 2 2
( 1) 2 1 ( 1)
2
2 2 2
2 1 ( 1)
( 1)
nl
D v D v
l l D n l l D
v
E
D v
n l l D
l l
D
µχα µ χ µχα µ χ
α α α
χ χ µ χ
µ χ
µχα µ χ
α α
χ
α
χα
+ + − + + − + + −
=− −
+ − + + −
+
+ +
h h h
h
h
h h
h 0
(44)
2
D
µ
3.4 CALCULATION OF THE WAVE FUNCTION
Furthermore, in order to calculate the radial wave function, we used the coordinate transformation
2 r
s e α
−
= into equation (16) and obtained the following
( )
2
0 1 0 3 0
2 2 2
2
2
0 1 3 0 3 1 0 1
2 2 2 2 2 2
2
3 0 3 1 0 1
2 2
( 1) 2
4 4 4 4
1 2 2 ( 1) ( 1)
1
(45)
(1 ) (1 ) 4 4 4 4 4
( 1) ( 1) 2
4 4 4 4 4
v l l D D E
s
s v D D l l D l l D
d R dR E
s
dr s s ds s s
D D l l D l l D E
χ χ µ
α χ α
χ χ χ µ
α χ α
χ χ µ
α
+
− + + −
−
+ +
+ + + + + + + −
− −
+ +
− + + + −
h
h
h
The corresponding radial wave function is then given by
( )
3 0 3 1 0 1
3 0 3 1 0 1
2 2
2 2
3 0 3 1 0 3 0 3 1 0
1 1
2 2
( 1) ( 1) 2
( 1) ( 1) 2 1
2 2 4 4 4 4 4
4 4 4 4 4
( 1) ( 1)
( 1) ( 1)
2 2
1 2 , 3 2
4 4 4 4 4 4 4 4
4 4
( ) (1 )
n
D D l l D l l D E
D D l l D l l D E
r r
nl n
D D l l D D D l l D
l l D l l D
E E
R r N e e
P
χ χ µ
χ χ µ
α α α
α
χ χ χ χ
µ µ
α
+ +
+ + − − + + + −
+ + + −
− −
+ +
+ +
+ + + + − + + + + −
= −
×
h
h
h
( )
2 2
2
1 2 r
e
α α
−
−
h
(46)
4. NUMERICAL COMPUTATION OF THE ENERGY EQUATION
Using equation (43), we implement Fortran algorithm to compute for the energy of the equation
in electron volt with various values of the screening parameter α . We use the following values
for our computation. 0 0 1 1 2 2
1
1.0, , 1.0, 1, 2, 1
12
V D D
µ χ χ χ
= = = = = = − = =
h .
9. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
35
Bound State energy with 0.1
α = for different quantum state
n l ( 0.1)
n
E eV
α = n l ( 0.1)
n
E eV
α = n l ( 0.1)
n
E eV
α = n l ( 0.1)
n
E eV
α =
0 0 -1.81557810 0 1 -1.83414400 0 2 -1.87091950 0 3 -1.92523000
1 0 -1.39580210 1 1 -1.40959080 1 2 -1.43698190 1 3 -1.47761940
2 0 -1.18513580 2 1 -1.19601170 2 2 -1.21765080 2 3 -1.24983630
3 0 -1.05848570 3 1 -1.06744430 3 2 -1.08528610 3 3 -1.11186640
4 0 -0.97394794 4 1 -0.98155713 4 2 -0.99672174 4 3 -1.01933810
5 0 -0.91351247 5 1 -0.92012280 5 2 -0.93330324 5 3 -0.95297605
6 0 -0.86815786 6 1 -0.87399983 6 2 -0.88565266 6 3 -0.90305570
7 0 -0.83286536 7 1 -0.83809840 7 2 -0.84853950 7 3 -0.86414030
8 0 -0.80462086 8 1 -0.80935950 8 2 -0.81881640 8 3 -0.83295200
Table 1
Bound State energy with 0.2
α = for different quantum state
( 0.2)
n
E eV
α = ( 0.2)
n
E eV
α = ( 0.2)
n
E eV
α = ( 0.2)
n
E eV
α =
0 0 -1.25588080 0 1 -1.29197690 0 2 -1.36170600 0 3 -1.46096090
1 0 -1.04142170 1 1 -1.06843020 1 2 -1.12113100 1 3 -1.19725980
2 0 -0.93265150 2 1 -0.95405185 2 2 -0.99604530 2 3 -1.05721940
3 0 -0.86688805 3 1 -0.88456786 3 2 -0.91938436 3 3 -0.97037660
4 0 -0.82283480 4 1 -0.83788250 4 2 -0.86758830 4 3 -0.91125740
5 0 -0.79126420 5 1 -0.80435646 5 2 -0.83024790 5 3 -0.86841345
6 0 -0.76752913 6 1 -0.77911305 6 2 -0.80205260 6 3 -0.83593720
7 0 -0.74903460 7 1 -0.75942045 7 2 -0.78000940 7 3 -0.81047153
8 0 -0.73421750 8 1 -0.74362910 8 2 -0.76230270 8 3 -0.78996754
Table 2
Bound State energy with 0.3
α = for different quantum state
( 0.3)
n
E eV
α = ( 0.3)
n
E eV
α = ( 0.3)
n
E eV
α = ( 0.3)
n
E eV
α =
0 0 -1.11232240 0 1 -1.16417930 0 2 -1.26113510 0 3 -1.39352740
1 0 -0.96447120 1 1 -1.00370690 1 2 -1.07845380 1 3 -1.18307350
2 0 -0.88827163 2 1 -0.91957426 2 2 -0.97985350 2 3 -1.06547440
3 0 -0.84179723 3 1 -0.86777450 3 2 -0.91814520 3 3 -0.99038374
4 0 -0.81049335 4 1 -0.83267320 4 2 -0.87588680 4 3 -0.93828130
5 0 -0.78797410 5 1 -0.80731654 5 2 -0.84513450 5 3 -0.90001200
6 0 -0.77099670 6 1 -0.78814130 6 2 -0.82175210 6 3 -0.87071250
7 0 -0.75773966 7 1 -0.77313274 7 2 -0.80337375 7 3 -0.84755990
8 0 -0.74710070 8 1 -0.76106584 8 2 -0.78854835 8 3 -0.8288036
Table 3
n l n l n l n l
n l n l n l n l
10. International Journal of Recent adv
Bound State energy with
( 0.4)
n
E eV
α =
0 0 -1.07219960 0 1
1 0 -0.95648575 1 1
2 0 -0.89565750 2 1
3 0 -0.85815040 3 1
4 0 -0.83271027 4 1
5 0 -0.81432050 5 1
6 0 -0.80040705 6 1
7 0 -0.78951290 7 1
8 0 -0.78075130 8 1
Bound State energy with
( 0.5)
n
E eV
α =
0 0 -1.07287570 0 1
1 0 -0.97570810 1 1
2 0 -0.92349565 2 1
3 0 -0.89090130 3 1
4 0 -0.86861694 4 1
5 0 -0.85241880 5 1
6 0 -0.84011304 6 1
7 0 -0.83044730 7 1
8 0 -0.82265410 8 1
Figure 1: The graph of energy against the distance for different quantum state with
n l n l
n l n l
International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
Bound State energy with 0.4
α = for different quantum state
( 0.4)
n
E eV
α = ( 0.4)
n
E eV
α = ( 0.4)
n
E eV
α
-1.13772730 0 2 -1.25619530 0 3 -1.41204810
-1.00673560 1 2 -1.10005060 1 3 -1.22680750
-0.93608590 2 2 -1.01235960 2 3 -1.11805080
-0.89188860 3 2 -0.95620050 3 3 -1.04651460
-0.86163010 4 2 -0.91715777 4 3 -0.99588360
-0.83961457 5 2 -0.88844097 5 3 -0.95816210
-0.82287750 6 2 -0.86643210 6 3 -0.92897120
-0.80972373 7 2 -0.84902660 7 3 -0.90571094
-0.79911387 8 2 -0.83491695 8 3 -0.88674080
Table 4
Bound State energy with 0.5
α = for different quantum state
( 0.5)
n
E eV
α = ( 0.5)
n
E eV
α = ( 0.5)
n
E eV
α
-1.15000000 0 2 -1.28518370 0 3 -1.45766960
-1.03571430 1 2 -1.14444880 1 3 -1.28834840
-0.97222220 2 2 -1.06231940 2 3 -1.18440910
-0.93181820 3 2 -1.00849700 3 3 -1.11411000
-0.90384614 4 2 -0.97049820 4 3 -1.06339450
-0.88333330 5 2 -0.94223930 5 3 -1.02507970
-0.86764705 6 2 -0.92040080 6 3 -0.99511280
-0.85526310 7 2 -0.90301790 7 3 -0.97103360
-0.84523810 8 2 -0.88885320 8 3 -0.95126210
Table 5
Figure 1: The graph of energy against the distance for different quantum state with α =
n l n l
n l n l
ances in Physics (IJRAP) Vol.4, No.4, November 2015
36
( 0.4)
E eV
α =
1.41204810
1.22680750
1.11805080
1.04651460
0.99588360
0.95816210
0.92897120
0.90571094
0.88674080
( 0.5)
E eV
α =
1.45766960
1.28834840
1.18440910
1.11411000
1.06339450
1.02507970
0.99511280
0.97103360
0.95126210
0.1
= .
11. International Journal of Recent adv
Figure 2:The graph of energy against the distance for different quantum state with
Figure 3: The graph of energy
Figure 4: The graph of energy against the distance for different quantum state with
International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
Figure 2:The graph of energy against the distance for different quantum state withα =
Figure 3: The graph of energy against the distance for different quantum state withα =
Figure 4: The graph of energy against the distance for different quantum state withα =
ances in Physics (IJRAP) Vol.4, No.4, November 2015
37
0.2
= .
0.3
= .
0.4
= .
12. International Journal of Recent adv
Figure 5. : The graph of energy against the distance for
CONCLUSION
We used supersymmetric quantum mechanics approach to obtained bound state solution to
Hylleraas plus inversely quadratic potential using Schrodinger equation. We also obtained eigen
energy and the wave function. The result shows that the energy is negativ
state condition and increases with an increase in quantum as shown in tables (1
graphical spectrum shows that the interspacing within the quantum state is more pronounce the
value of α increases. This can be shown from figures (1
ACKNOWLEDGEMENT
We are deeply grateful to the referees for their useful comments which we have significantly use
to improve the article.
REFERENCES
[1] OkonI.B , Ituen E.E, .Popoola O.O and Antia A.D.(2013),
Equation with Mie-Type Potential Using Factorisation Method”, International Journal of Recent
Advances In Physics, Vol.2, No.2, pp1
[2] Okon I.B, Isonguyo C.N, Ituen, E.E and Ikot A.N. (2014), “Energy Spectrum for
Molecules with Generalized Manning
(SUSY)”. Conference proceedings of Nigerian Institute of Physics, 2014.
[3] Okon I. B, Popoola O.O and Isonguyo. C.N (2014), “Exact Bound state
Woods-Saxon plus modified Coulomb Potential Using Conventional Nikiforov
International Journal of Recent Advances in Physics Vol. 3, No.4.
[4] Okon I.B and Popoola. O.O.(2015) ,”Bound state solution of Schrodinger e
plus generalised exponential coulomb potential using Nikiforov
Journal of Recent Advances in Physics. Vol.4, No.3.Doi:10.14810/ijrap.2015.4301.
[5] Isonguyo C. N, Okon, I. B and Ikot A. N (2013), “Semi
Hellmann potential using Supersymmetric Quantum Mechanics”, Journal of the
Nigerian Association of Mathematical Physics (NAMP Journal). Vol.25, No. 2,
pp121-126.
International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
Figure 5. : The graph of energy against the distance for different quantum state withα
We used supersymmetric quantum mechanics approach to obtained bound state solution to
Hylleraas plus inversely quadratic potential using Schrodinger equation. We also obtained eigen
energy and the wave function. The result shows that the energy is negative to ascertain bound
state condition and increases with an increase in quantum as shown in tables (1-5). The energy
graphical spectrum shows that the interspacing within the quantum state is more pronounce the
This can be shown from figures (1-5).
ACKNOWLEDGEMENT
We are deeply grateful to the referees for their useful comments which we have significantly use
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38
0.5
α = .
We used supersymmetric quantum mechanics approach to obtained bound state solution to
Hylleraas plus inversely quadratic potential using Schrodinger equation. We also obtained eigen
e to ascertain bound
5). The energy
graphical spectrum shows that the interspacing within the quantum state is more pronounce the
We are deeply grateful to the referees for their useful comments which we have significantly use
“Analytical Solutions of Schrodinger
Type Potential Using Factorisation Method”, International Journal of Recent
Some Diatomic
Rosen Potential Using Supersymmetric Quantum Mechanics
Solution of q-deformed
Uvarov Method”,
quation with Hulthen
Uvarov method”, International
13. International Journal of Recent advances in Physics (IJRAP) Vol.4, No.4, November 2015
39
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