Hamiltonian Operator: Difference vs. E?

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Is there any difference between Hamiltonian operator and E? Or do we describe H as an operation that is performed over (psi) to give us E as a function of (psi)??
 
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physicsfirzen said:
Is there any difference between Hamiltonian operator and E? Or do we describe H as an operation that is performed over (psi) to give us E as a function of (psi)??

Usually, H is an operator, and E is a real number, its eigenvalue. For example, for a free particle,

H = -\frac{\hbar^2}{2m} \frac{\partial^2}{\partial x^2}

When applied to \psi(x) = e^{ikx} you get:

H \psi = \frac{\hbar^2 k^2}{2m} \psi

So for this particular \psi, E = \frac{\hbar^2 k^2}{2m}, which is a real number.
 
Adding to what steven said, any wave function (or more generally, quantum state) does not fulfill the time-independent SE. This only happens for the eigenstates of the Hamiltonian (in fact the time independent SE is just the eigenstate equation for H). The time dependent SE describes how any quantum state evolves, not only the Hamiltonian eigenstates (although if we know the evolution of the eigenstates, i.e., for all possible E in the time independent equation, then we can easily reconstruct the general time evolution).
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA
If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!
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