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topicsinqm
www.damtp.cam.ac.uk/user/tong/aqm/topics1.pdf2 Jul 2024: E, so the new Hamiltonian reads. H = 2. 2mr2 V (r) ex E. -
topicsinqm
www.damtp.cam.ac.uk/user/tong/aqm/topics2.pdf2 Jul 2024: Then, whenever we’re faced with a new problem we can root around in our toolbox,. ... and h;|p2(0)|;i = m!2. The position operator now evolves, governed by the new Hamiltonian H,. -
topicsinqm
www.damtp.cam.ac.uk/user/tong/aqm/topics6.pdf2 Jul 2024: transmission coecients. It is useful both because it highlights new features of the. ... We can also think about the S-matrix using our new basis of states. -
topicsinqm
www.damtp.cam.ac.uk/user/tong/aqm/topics4.pdf2 Jul 2024: 4. Atoms in Electromagnetic Fields. Our goal in this chapter is to understand how atoms interact with electromagnetic. fields. There will be several stages to our understanding. We start by looking at atoms. in constant, background electromagnetic -
topicsinqm
www.damtp.cam.ac.uk/user/tong/aqm/topics5.pdf2 Jul 2024: We’ll introduce. some new notation for this state that will become useful in the following section: we. -
topicsinqm
www.damtp.cam.ac.uk/user/tong/aqm/topics3.pdf2 Jul 2024: 3.5). and our new goal is to compute the expectation values h1/rin,l and h1/r2in,l for thehydrogen atom wavefunctions. ... This time, we introducea new “radial momentum” observable. p̃ = i@. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel5.pdf2 Jul 2024: We did it assuming that there was nothing new to find as we went. -
Preprint typeset in JHEP style - HYPER VERSION Lent ...
www.damtp.cam.ac.uk/user/tong/aqm/topicsinqm.pdf2 Jul 2024: E, so the new Hamiltonian reads. H = 2. 2m2 V (r)ex E.
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