Discrete energy level of schrodinger's equation

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SUMMARY

The discrete energy levels of Schrödinger's equation arise primarily from boundary conditions. For example, in the hydrogen atom, the boundary condition \(\Psi \rightarrow 0\) as \(r \rightarrow \infty\) results in discrete radial solutions and corresponding energy levels. Similarly, the one-dimensional "particle in a box" model demonstrates that setting \(\Psi = 0\) at the box's walls leads to discrete energy solutions. While quantum confinement also influences energy levels, the primary cause of discreteness is indeed the boundary conditions imposed on the system.

PREREQUISITES
  • Understanding of Schrödinger's equation
  • Familiarity with boundary conditions in differential equations
  • Basic knowledge of quantum mechanics concepts
  • Experience with classical wave phenomena, such as string oscillations
NEXT STEPS
  • Research the implications of boundary conditions in quantum mechanics
  • Study the concept of quantum confinement in various physical systems
  • Explore the mathematical solutions of the "particle in a box" model
  • Investigate the relationship between energy levels and boundary conditions in different quantum systems
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Students of quantum mechanics, physicists exploring wave-particle duality, and educators teaching advanced topics in quantum theory.

feynmann
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Is it true that the discrete energy level of Schrödinger's equation is due to boundary condition?
What is the definition of boundary condition?
 
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A simple example is provided by a (classical) guitar string. The guitarist controls the boundary conditions by fingering the strings in various positions. The notes and harmonics for a given fingering will be a discrete set.
 
For the hydrogen atom, the boundary condition is that \Psi \rightarrow 0 as r \rightarrow \infty. This gives discrete solutions for the radial part of \Psi, with correspondingly discrete energies.

For the one-dimensional "particle in a box" that most all undergraduates learn as their first example of solving the Schrödinger equation, the boundary condition is that \Psi = 0 at the "walls" of the box. This likewise leads to discrete solutions with discrete energies.
 
Boundary conditions for a second order differential equation are two numerical conditions for the general solution containing two arbitrary constants. These conditions "pick up" (select) the physically right solution. For a string oscillations they signify that the string is fixed at its ends (does not move). So any perturbation of the string is reflected from the ends making survive only discrete (proper) frequencies due to constructive/destructive interference.

Bob.
 
jtbell said:
For the hydrogen atom, the boundary condition is that \Psi \rightarrow 0 as r \rightarrow \infty. This gives discrete solutions for the radial part of \Psi, with correspondingly discrete energies.

For the one-dimensional "particle in a box" that most all undergraduates learn as their first example of solving the Schrödinger equation, the boundary condition is that \Psi = 0 at the "walls" of the box. This likewise leads to discrete solutions with discrete energies.

Is the discrete solutions due to quantum confinement or boundary condition?
They are not the same, right?
 
what is "quantum confinement"?
 
feynmann said:
Is the discrete solutions due to quantum confinement or boundary condition?
They are not the same, right?

It is due to the boundary conditions. If you have large systems, the discrete solutions are however so close to each other that they are often treated as a quasicontinuum. For example the phonon dispersion of a bulk solid is usually drawn as a continuous curve of energy versus k although the allowed values are discrete. There are so many possible states close to each other, that this seems sensible. Strong confinement now leads to a large difference in energy between the energy levels (see the particle in a box problem), so that the discreteness becomes easily noticeable.
 

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