* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download PH301
Density functional theory wikipedia , lookup
Schrödinger equation wikipedia , lookup
Franck–Condon principle wikipedia , lookup
Quantum state wikipedia , lookup
Path integral formulation wikipedia , lookup
Identical particles wikipedia , lookup
EPR paradox wikipedia , lookup
Renormalization group wikipedia , lookup
Hydrogen atom wikipedia , lookup
Canonical quantization wikipedia , lookup
Density matrix wikipedia , lookup
Quantum decoherence wikipedia , lookup
Wave–particle duality wikipedia , lookup
Hidden variable theory wikipedia , lookup
Symmetry in quantum mechanics wikipedia , lookup
Copenhagen interpretation wikipedia , lookup
Quantum electrodynamics wikipedia , lookup
Theoretical and experimental justification for the Schrödinger equation wikipedia , lookup
Coherent states wikipedia , lookup
De Broglie–Bohm theory wikipedia , lookup
Interpretations of quantum mechanics wikipedia , lookup
Many-worlds interpretation wikipedia , lookup
Relativistic quantum mechanics wikipedia , lookup
Measurement in quantum mechanics wikipedia , lookup
PH301 Quantum Computer Assignment The program for quantum calculations is made by the Consortium for Upper-level Physics Software. Double-click on the CUPS icon on any of the computers in the Swenson computer lab that runs Windows 95. The software starts up with a list of choices, choose “Quantum Mechanics.” Part I – Uncertainty Principle The quantum mechanics program starts up in the "Uncertainty Principle" section, and displays a Gaussian or "minimum uncertainty" wavepacket. Only the probability densities for the spatial (on the left) and momentum (on the right) state wave functions are shown. Note that a convenient (if unconventional) set of units is used. Distances are in nm, and momenta are in units of /nm. Change the slider control for Delta p to four different values: 0.1, 0.5, 2.0, 6.0 (or as close as you can get). The program calculates a new Gaussian wavefunction that has that value of momentum uncertainty. It will recalculate the uncertainty in position and reposition the Delta x slider accordingly. After each adjustment of the Delta p slider, record the value of Delta p and Delta x. Calculate the product of Delta p and Delta x for each case. Now we'll try a different shape for the wavefunction. Choose "Wavefunction Parameters" from the "Parameters" menu. Select "Triangle," and click OK. Record the value of Delta p and Delta x. Calculate the product of Delta p and Delta x for this case. To within roundoff errors, does it seem that the uncertainty principle holds? Why do you think the Gaussian shape wavefunction is called a "minimum uncertainty" wavefunction? Part II – Stationary States Choose “Bound Particles in a Well” from “Section” menu. The program begins with the finite square well potential. Let’s make it do a more complicated example: the harmonic oscillator. To do this, choose “Well Parameters” from the “Parameters” menu. Select “User Defined Well,” and define the well as V(x)=150*x^2 (like a spring: V=1/2 kx2) with a domain from -1 to 1. Click OK. Press F3 to begin the attempt to find the wavefunction for the ground state of the harmonic oscillator. Sketch the computer’s first attempt (the white curve). Why can’t this function be a real wavefunction? Press F3 repeatedly until the wavefunction appears to fit all the requirements of a real wavefunction. How many steps does it take? Continue pressing F3 until the computer program is also satisfied that it fits all requirements – that is until it displays the energy of the ground state in the box on the right, and starts over with another impossible wavefunction in an attempt to find the second energy level wavefunction. Now press F2, which makes it run quickly through the process of finding wavefunctions. Once it has calculated all the wavefunctions, it will display them on the right, with the ground state at the bottom. Now let’s look at how a wavefunction will vary with time. Choose “Wavefunction Parameters” from the “Parameters” menu. Make a wavefunction that is a combination of the first three energy levels, by setting component 1 to n=1 and A=0.33, component 2 to n=2 and A=0.33, and component 3 to n=3 and A=0.33. Note that since this wavefunction is made up of three different energy levels (with equal amplitude of 0.33), it does not have a definite energy. Click OK. The wavefunction at t=0 is displayed on the left (the real part in blue, the imaginary part in green). Pay particular attention to the probability density graphed in purple, because this is what can be determined from experiment. To see how the probability density changes with time, press F2 -- run. Describe the behavior of the probability density function. Press F2 to stop. Now make a wavefunction that has a definite energy, E1, by choosing “Wavefunction Parameters,” and setting component 1 to n=1 and A=1, component 2 to n=2 and A=0, and component 3 to n=3 and A=0. Click OK. Press F2 -- run. Describe the behavior of the probability density function. Press F2 to stop. Now make a wavefunction that has a definite energy, E2, by choosing “Wavefunction Parameters,” and setting component 1 to n=1 and A=0, component 2 to n=2 and A=1, and component 3 to n=3 and A=0. Click OK. Press F2 -- run. Describe the behavior of the probability density function. Why do you suppose a state with definite energy is called a “stationary state”? When you are finished, choose “Exit Program” from the “File” menu. Then choose “Exit Program” from the main menu. You will be returned to the DOS screen. Type “exit” at the DOS prompt to return to Windows 95.