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P460 - real H atom1 The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects.

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Presentation on theme: "P460 - real H atom1 The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects."— Presentation transcript:

1 P460 - real H atom1 The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects (spin-orbit and hyperfine e-A) relativistic corrections Also have Lamb shift due to electron “self- interaction”. Need QED (Dirac eq.) and depends on H wavefunction at r=0 (source of electric field). Very small and skip in this course (first calculated by Bethe using perturbation theory on train from Long Island to Ithaca. Bethe also in film Fat Man and Little Boy....)

2 P460 - real H atom2 Spin-Orbit Interactions A non-zero orbital angular momentum L produces a magnetic field electron sees it. Its magnetic moment interacts giving energy shift in rest frame of electron, B field is (see book/ER): convert back to lab frame (Thomas precession due to non-inertial frame gives a factor of 2 – Dirac eq gives directly). Energy depends on spin-orbit coupling

3 P460 - real H atom3 Spin-Orbit: Quantum Numbers The spin-orbit coupling (L*S) causes m l and m s to no longer be “good” quantum numbers spin-orbit interactions changes energy. In atomic physics, small perturbation, and can still use H spatial and spin wave function as very good starting point. Large effects in nuclear physics (and will see energy ordering very different due to couplings). So in atomic just need expectation value of additional interaction

4 P460 - real H atom4 SL Expectation value Determine expectation value of the spin-orbit interaction using perturbation theory. Assume J,L,S are all “good” quantum numbers (which isn’t true) assume H wave function is ~eigenfunction of perturbed potential

5 P460 - real H atom5 SL Expectation value To determine the energy shift, also need the expectation value of the radial terms using Laguerre polynomials put all the terms together to get spin-orbit energy shift. =0 if l=0 n=2 L=0,1 J=3/2, L=1 J=1/2 L=0 J=1/2 L=1 with relativistic j=3/2 j=1/2

6 P460 - real H atom6 Numerology have but and so

7 P460 - real H atom7 Spin Orbit energy shift For 2P state. N=2, L=1, J= 3/2 or 1/2 and so energy split between 2 levels is L=1 J=3/2 j=1/2

8 P460 - real H atom8 Relativistic Effects Solved using non-relativistic S.E. can treat relativistic term (Krel) as a perturbation can use virial theorem

9 P460 - real H atom9 Relativistic+spin-orbit Effects by integrating over the radial wave function combine spin-orbit and relativistic corrections energy levels depend on only n+j (!). Dirac equation gives directly (not as perturbation). For n=2 have:

10 P460 - real H atom10 Energy Levels in Hydrogen Degeneracy = 2j+1 spectroscopic notation: nL j with L=0 S=state, L=1 P-state, L=2 D-state also can note spin “doublet” is single electron with s=1/2 E N=1 N=3 N=2 # states

11 P460 - real H atom11 Zeeman Effect:External B Field Energy shift depends on m j and removes any remaining degeneracy. Now two fields (internal and external) and details of splitting depends on relative strengths Unless S=0, the magnetic moment and the total angular momentum are not in the same direction (and aren’t in B direction). For weak external field, manipulating the dot products gives B=0 B>0

12 P460 - real H atom12 Zeeman Effect  L=+-1  m=0,+1,-1 strong field

13 P460 - real H atom13 Zeeman Effect:External B Field Assume that weak B field (if strong then L and S won’t couple) B field off  1 photon energy B field on  6 photon energies (with their energy depending on the g factor and on the B field One of the first indicators that the electron had intrinsic angular momentum s=1/2 B=0 B>0

14 P460 - real H atom14 Hyperfine Splitting Many nuclei also have spin p,n have S=1/2. Made from 3 S=1/2 quarks (plus additional quarks and antiquarks and gluons). G- factors are 5.58 and -3.8 from this (-2 for electron). Nuclear g-factors/magnetic moments complicated. Usually just use experimental number for Hydrogen. Let I be the nuclear spin (1/2) have added terms to energy. For S-states, L=0 and can ignore that term

15 P460 - real H atom15 Hyperfine Splitting Electron spin couples to nuclear spin so energy difference between spins opposite and aligned. Gives 21 cm line for hydrogen (and is basis of NMR/MRI)


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