SUMMARY
The discussion centers on the concepts of the one-dimensional infinite potential well, specifically addressing the stationary states and their representation through Fourier series. Participants clarify that the stationary states, represented by the wave function $$\Psi_n(x,t) = \sqrt{\frac{2}{a}}\sin \left( \frac{n \pi x}{a} \right) e^{-i E_n t / \hbar}$$, can be expressed as a linear combination of these states. The confusion arises regarding the expansion of a constant function in a Fourier sine series, which is explained as being constant only at time t=0, with time dependence emerging subsequently. The relationship between Fourier series and the infinite square well is established through the coefficients $$c_n$$ that define the wave function's evolution.
PREREQUISITES
- Understanding of quantum mechanics principles, particularly stationary states.
- Familiarity with Fourier series and their mathematical representation.
- Knowledge of wave functions and their time evolution in quantum systems.
- Basic grasp of the infinite potential well model in quantum mechanics.
NEXT STEPS
- Study the derivation of stationary states in the infinite potential well using quantum mechanics textbooks.
- Learn about the mathematical formulation of Fourier series and their applications in quantum mechanics.
- Explore the concept of wave function evolution over time in quantum systems.
- Investigate the implications of probability density in stationary states and its time independence.
USEFUL FOR
Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators looking to clarify concepts related to the infinite potential well and Fourier series.