For an electron in the infinite spherical well of radius nm treated in Chapter 11

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Central potentials and canonical three-dimensional systems · Central potentials and canonical three-dimensional systems

Quantum Mechanics: From the Photon to the Hydrogen Atom, Ch The hydrogen atom

Problem

For an electron in the infinite spherical well of radius 1.001.00 nm treated in Chapter 11, the three lowest levels are 0.3760.376 eV (with l=0l=0), 0.7690.769 eV (with l=1l=1) and 1.271.27 eV (with l=2l=2). In hydrogen, by contrast, the n=2n=2 level contains both the 2s2s and the 2p2p states at −3.40-3.40 eV, both with orbital angular momentum L=l(l+1) ℏL=\sqrt{l(l+1)}\,\hbar. In both problems each ll carries 2l+12l+1 values of mlm_l and the electron has two spin states; V(r)V(r) enters only the radial equation, so the angular factor YlmlY_l^{m_l} is identical in the two problems for the same ll (Chapter 11). The proton is a fixed point charge. ((a)) How many independent states, counting spin, does each of the three lowest well levels hold, in order of increasing energy? ((b)) How many independent states, counting spin, lie at hydrogen's n=2n=2 energy? ((c)) The well's l=1l=1 level and hydrogen's 2p2p state both carry L=2 ℏL=\sqrt2\,\hbar. Are their full three-dimensional wave functions therefore identical? Referring to how V(r)V(r) enters the separated equations, say in one or two sentences what is shared between them and what is not.

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