diff --git a/lecture_notes/4-11/overview b/lecture_notes/4-11/overview new file mode 100644 index 0000000..c13578c --- /dev/null +++ b/lecture_notes/4-11/overview @@ -0,0 +1,25 @@ + Review of Exam 2 +━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━━ + +V = ⎧ 1/2 k r² (x>0) + ⎨ + ⎩ ∞ (x<0) + + Gives the set L𝓍,L²,H due to x-symmetry + +(pic) schrodinger equations for radial and angular components + +(pic x2) working through asymptotic behaviours of diffEQ + +followed asymptotic approach and then set up a series polynomial solution +for the final F(r) + +(pic) still working through derivatives of the polynomial solution + +(pic) Use the "series shift" to combine terms. + +(pic) basically just continuing to prepare terms (2/r dR/dr in this case) +to plug back into the main differential equation + +the final answer gives a relationship between the coeffiecients cᵢ. + diff --git a/lecture_notes/4-6/lectures b/lecture_notes/4-6/lectures new file mode 100644 index 0000000..5400704 --- /dev/null +++ b/lecture_notes/4-6/lectures @@ -0,0 +1,19 @@ +reestablish fundamental brakets + + spin Z operators + + raising/lowering operators (lowering erased before pic) + + commutations relations (erased before pic) + +Now setup a two-spin system + + (pic) Look at general operator expressions ?? in different spaces ?? + + Take direct product of A and B + +(pic) Developed 𝐒 using raising lowering operators + + (pic: last y should be an x) Proved this. + + diff --git a/lecture_notes/4-6/overview b/lecture_notes/4-6/overview new file mode 100644 index 0000000..7e5da6b --- /dev/null +++ b/lecture_notes/4-6/overview @@ -0,0 +1,39 @@ +reestablish fundamental brakets + + spin Z operators + + raising/lowering operators (lowering erased before pic) + + commutations relations (erased before pic) + +Now setup a two-spin system + + (pic) Look at general operator expressions ?? in different spaces ?? + + Take direct product of A and B + +(pic) Developed 𝐒 using raising lowering operators + + (pic: last y should be an x) Proved this. + + +(pic x2) Still missing a 1/2 somewhere! But moving on to see proper solutions of direct product. + + Eigenvalues are + + 𝐒² = ħ² S(S+1) = ⎧ 2ħ² + ⎨ + ⎩ 0ħ² + + 𝐒 = ⎧ 1 (3 eigenstates) + ⎨ + ⎩ 0 (1 eigenstate) + + (pic) Plugging back to direct product matrix + +(pic) FOUND PROBLEM of -1/2 from the up/down raising/lowering operator interactions + +(pic) finished diagonalizing operator product + + +