* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Thursday afternoon
Quantum state wikipedia , lookup
Theoretical and experimental justification for the Schrödinger equation wikipedia , lookup
Coherent states wikipedia , lookup
Canonical quantization wikipedia , lookup
Relativistic quantum mechanics wikipedia , lookup
Bra–ket notation wikipedia , lookup
Compact operator on Hilbert space wikipedia , lookup
Symmetry in quantum mechanics wikipedia , lookup
Renormalization group wikipedia , lookup
Coupled cluster wikipedia , lookup
Density matrix wikipedia , lookup
Physics 541 A quantum approach to condensed matter physics Syracuse students - please put homework from all of you in one envelope and mail to me no later than Thursday afternoon. If you are not ready by that time, then mail your homework separately. Mail it to: Prof Philip Taylor Dept of Physics CWRU Cleveland OH 44106-7079 CWRU students - please put your individual homework in my mail box no later than Thursday afternoon. Recapitulation of Class 4 Hartree-Fock approximation gives an answer that is worse than if we just ignored interactions! Recapitulation of Class 5 To second order in V Look for approach that could give plasmons Problem: What operator creates plasma oscillations? Quasiparticle excitations vs collective excitations Equation-of-motion approach Can we find an operator like this for the Coulomb gas? Can we find an operator like Try this for the Coulomb gas? After lots of work: So this operator is good if q is big, but not if it is small. Can we find an operator like this for the Coulomb gas? doesn’t work Try the density fluctuation operator We know that so we just sum this over all p Interaction terms cancel, so still no good! Remember that plasmon energy squared is linear in the coupling Could it be that Let’s miss out a few steps and go to the result -- becomes is really special! For small q is really special! What is happening? Screening! Small q -- screening possible. Plasmons are relevant excitations Large q -- screening impossible. Quasiparticles are relevant excitations Can this be related to the concept of a dielectric constant? Terms linear in U can be written as with Look at a sample term in Ueff