Potassium's principal doublet consists of the lines at and at ; the fine-structure…
PHYSICS · Multi-part · Fermi University Physics · Atomic, Molecular & Optical Physics · Many-electron atoms and the periodic table · Radiative transitions, external fields and collisions
Reading the Spectrum, Ch Atoms in a magnetic field: moments, the Zeeman effect and the Paschen-Back limit
Problem
Potassium's principal doublet consists of the lines 42P3/2→42S1/2 at 766.49nm and 42P1/2→42S1/2 at 769.90nm; the fine-structure interval of the 4p level is 57.7cm−1. A spectrum recorded in an unknown magnetic field shows one of the two lines, but the record does not say which. Its components sit at −0.623, −0.374, −0.125, +0.125, +0.374 and +0.623cm−1 from the zero-field position of the line. Take μBB/hc=0.467cm−1 per tesla.
((a)) Evaluate gJ for the three levels from the Lande formula, and work out the weak-field pattern of each line in units of μBB. Decide which line was recorded, using only features of the pattern that do not depend on the size of the field, and state the number of components in the recorded pattern.
((b)) Find B in tesla, and report the ratio μBB/(hc×57.7cm−1) as a check that the field is weak for the 4p level.
((c)) State how many components the other line of the doublet would show in the same field, and predict the size of its component shifts, in cm−1, from the centre outward. Give the smallest wavelength separation between two neighbouring components of that line, in nm.