280 likes | 375 Views
Expectation values and uncertainties II (including free particles). SMXR355 2005. http://www.cmmp.ucl.ac.uk/~swz/courses/SMXR355.html For hard copy: give me your address. Stationary state:. Free (non-interacting) particle:. kinetic energy operator. So it can not be normalized to unity:
E N D
Expectation values and uncertainties II(including free particles) SMXR355 2005 http://www.cmmp.ucl.ac.uk/~swz/courses/SMXR355.html For hard copy: give me your address
Free (non-interacting) particle: kinetic energy operator
So it can not be normalized to unity: It is NOT a wave function that represents a realizable state of the particle
Completeness of the momentum eigenfunctions Fourier transform
For free particles: energy eigenvalues form a continuum of unbound solutions → instead of sums, integrals
Time evolution Time dependence of amplitude function for the expansion of the initial wave packet in momentum and energy eigenfunctions Using energy eigenvalues
amplitudes: for a given set of eigenfunctions, the amplitudes completely specify the state of the system normalization → if system is in eigenstate, only one measurement →
completely specifies state at time t amplitude for position x Note:
when specified for all completely specify wave function
Heisenberg’s uncertainty principle for both free and bound particles It is impossible to prepare any state of a one particle quantum system for which the product (x)(px) is less than ħ/2