Presentation - Oxford Physics
... The periodicity of f(x) in register B is now reflected in register A by entanglement Second Fourier transform: reorganise register A to move a random offset into the overall phase of the state makes the (inverse) period appear in measured result. ...
... The periodicity of f(x) in register B is now reflected in register A by entanglement Second Fourier transform: reorganise register A to move a random offset into the overall phase of the state makes the (inverse) period appear in measured result. ...
D NAME: 1. Which of the following phenomena could not be expla
... Prove that, given a pair of normalized but not orthogonal functions ψ1 and ψ2, the function ψ3 = ψ2 – Sψ1 is orthogonal to ψ1 if S is the overlap integral of ψ1 and ψ2. Is ψ3 normalized? (Use the back of the page if necessary). ...
... Prove that, given a pair of normalized but not orthogonal functions ψ1 and ψ2, the function ψ3 = ψ2 – Sψ1 is orthogonal to ψ1 if S is the overlap integral of ψ1 and ψ2. Is ψ3 normalized? (Use the back of the page if necessary). ...
Chapter 7 - Quantum Numbers, Orbitals, and Electron
... En RH 2 for n = 1, 2, 3, ... (Applies only to H atom!!) ...
... En RH 2 for n = 1, 2, 3, ... (Applies only to H atom!!) ...
Wave
... – There is a tradeoff between particle and wave character. – Depending on the width of the wave packet, an object can be more like a particle or like a wave. – A particle (short wave packet) has a well-defined position, and a wave (long packet) has a well-defined momentum. ...
... – There is a tradeoff between particle and wave character. – Depending on the width of the wave packet, an object can be more like a particle or like a wave. – A particle (short wave packet) has a well-defined position, and a wave (long packet) has a well-defined momentum. ...
... possible values of the angular momentum. Calculate the energy eigenvalues. What is the energy difference between the ground state of zero angular momentum and the first rotational state? Show that this approaches infinity as N . Contrast this with the comparable energy for a “nicked” cylinder, wh ...
... possible values of the angular momentum. Calculate the energy eigenvalues. What is the energy difference between the ground state of zero angular momentum and the first rotational state? Show that this approaches infinity as N . Contrast this with the comparable energy for a “nicked” cylinder, wh ...
