The canonical commutation relation between the variables involved in this relation implies that no state can be an eigenstate of the variables at the same time. This relation 
The canonical commutation relation between the variables involved in this relation implies that no state can be an eigenstate of the variables at the same time. This relation is a special case of the Robertson-Schrödinger inequality, and it was introduced through a thought experiment that involved a gamma-ray microscope. One way of representing this principle involves energy and time, and this principle states that electrons can only have definite positions when they are in a state in which their energy is undefined. For 10 points, name this principle which states that the momentum and position of a particle cannot be precisely measured simultaneously.
The canonical commutation relation between the variables involved in this relation implies that no state can be an eigenstate of the variables at the same time.