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In lecture, we just went over the basics of angular momentum and how it compared to the equations we previously learned for the simple harmonic ocsillator (SHO).
<math>[x,p]=i{\hbar}</math>
no top rung
<math>[L_x,L_y]=i{\hbar}{L_z}</math>
has a top rung, <math>{L_z}{f_t}={\hbar}{l}{f_t}</math>; <math>{L^2}{f_t}={\lambda}{f_t}</math>
To go back to the lecture note list, click lec_notes
previous lecture note: lec_notes_1111
Main quiz 3 concepts: Quiz_3_1113
next lecture note: lec_notes_1118