What Are Eigenstates and Their Role in Quantum Mechanics?

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SUMMARY

Eigenstates in quantum mechanics are defined as states with a specific energy that remains constant over time. Any arbitrary state can be expressed as a linear combination of these eigenstates, with coefficients Cn serving as weighting factors. The probabilities of measuring a particular energy value E_n are given by the squared magnitudes of these coefficients, |c_n|^2. Upon measurement, the wave function collapses to the corresponding energy-eigenstate, ensuring that energy measurements remain quantized.

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I've read the chapter but it hasn't helped. Eigenstates are states with a definite amount of energy independent on time? and then any other state is a linear combination of the eigenstates, with some Cn acting as a weighting factor...is there a limitation on what the Cn's can be? otherwise, wouldn't non-stationary states be unquantized?
 
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In fact, the [itex]|c_n|^2[/itex] are the probabilities of measuring the energy value [itex]E_n[/itex]. Remember that quantum mechanics assumes that the wave function collapses to an energy-eigenstate when the energy is measured, so the measured energy is still quantized.

This "collapse" means the wavefunction is

[itex]\Psi = \sum \limits _n c_n \varphi_n[/itex] before the energy is measured, where the [itex]|c_n|^2[/itex] say how probable it is to measure energy [itex]E_n[/itex].

Right after the measurement of energy [itex]E_n[/itex], the wavefunction collapses to

[itex]\Psi = \varphi_n[/itex].
 

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