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