The Hamiltonian operator is a fundamental concept in quantum mechanics that represents the total energy of a system, encompassing both kinetic and potential energies. It plays a crucial role in the formulation of the Schrödinger equation, which describes how quantum states evolve over time, and is used extensively in variational methods to approximate solutions for complex systems. Additionally, the Hamiltonian is a Hermitian operator, which ensures real eigenvalues that correspond to measurable energy levels.
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