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University Physics IV · topic UPIV-09.06

Intrinsic spin, spinors, and the Pauli matrices

Connect the ideas, make your working visible, and test the result. Use the hints when you need a starting point; open the full solution after your attempt.

Further practice

Work through a fresh case before tackling the extension.

Further practice · 01

Intrinsic spin, spinors and the Pauli matrices: predict a finite change

Intrinsic spin is an angular momentum a particle carries as an internal property: it obeys the same commutation relations as orbital angular momentum but depends on no coordinate, so its state is a finite column of complex numbers rather than a function of space. Use the supplied topic model Y_out = cosd((th-th0)/2), where Y_out is AMPLITUDE cos((Θ−Θ₀)/2) (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sind/cosd/tand use degrees. th0 is Prepared direction Θ₀, measured in °. Keep th (Analyser angle Θ) = 90 ° fixed. For this exercise use only 19.125 ° ≤ th0 ≤ 85.275 ° on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. Calculate Y_out at th0 = 33.678 ° and 42.939 °. Find the signed output change ΔY_out and the average sensitivity ΔY_out/Δth0 across this interval. State whether the response increases or decreases; distinguish this interval average from a derivative at one point.

Explore the question data

AMPLITUDE cos((Θ−Θ₀)/2) against th0

Predictions from the supplied Intrinsic spin, spinors and the Pauli matrices model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): AMPLITUDE cos((Θ−Θ₀)/2)

AMPLITUDE cos((Θ−Θ₀)/2) against th0Predictions from the supplied Intrinsic spin, spinors and the Pauli matrices model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: th0: Prepared direction Θ₀ / °. Vertical axis: AMPLITUDE cos((Θ−Θ₀)/2). Exact values are available in the data table below.0.80740.85720.90690.95671.00716.4834.3452.270.0687.92xy

Horizontal axis (x): th0: Prepared direction Θ₀ / °

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1th0: Prepared direction Θ₀ / °: 19.13AMPLITUDE cos((Θ−Θ₀)/2): 0.8147
Read the exact data as a table
AMPLITUDE cos((Θ−Θ₀)/2) against th0 — supplied values
th0: Prepared direction Θ₀ / °AMPLITUDE cos((Θ−Θ₀)/2)
19.1250.8147484825274895
35.66250.8896655492327864
52.20.9460853588275453
68.737500000000010.9828348730558712
85.2750.9991500236519368

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

Substitute each value of th0 separately while keeping every other input fixed, then subtract in the same order.

Reveal the worked solution
  1. At th0 = 33.678 °, substitute into Y_out = cosd((th-th0)/2): Y₀ = 0.881625.
  2. At th0 = 42.939 °, the same fixed-parameter model gives Y₁ = 0.916848.
  3. Signed change: ΔY_out = Y₁ − Y₀ = 0.0352228; the input change is Δth0 = 9.261 °.
  4. Average sensitivity is ΔY_out/Δth0 = 0.00380334 1 per °. Its positive sign means that this response increases over the specified interval.
  5. This is a secant slope between two settings. It equals a point derivative only for a locally linear relation or in a justified small-interval limit.

Answer Y₀ = 0.881625, Y₁ = 0.916848; ΔY_out = 0.0352228; average sensitivity = 0.00380334 1 per °.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.

Extra challenging questions

Work through the linked stages and explain what each result means.

Extra challenging · 01

Intrinsic spin, spinors and the Pauli matrices: infer an input with uncertainty

Intrinsic spin is an angular momentum a particle carries as an internal property: it obeys the same commutation relations as orbital angular momentum but depends on no coordinate, so its state is a finite column of complex numbers rather than a function of space. Use the supplied topic model Y_out = cosd((th-th0)/2), where Y_out is AMPLITUDE cos((Θ−Θ₀)/2) (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sind/cosd/tand use degrees. th0 is Prepared direction Θ₀, measured in °. Keep th (Analyser angle Θ) = 90 ° fixed. For this exercise use only 19.125 ° ≤ th0 ≤ 85.275 ° on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. A reading gives Y_out = 0.96473336, with a bounded reading uncertainty ±0.0051625. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown th0 by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.006615 °, using a numerical bracket if required. Find the full input interval consistent with the bounded reading uncertainty and compare it with a symmetric input-error assumption. Do not assume that the supplied calibration points prove monotonicity outside this branch.

Explore the question data

AMPLITUDE cos((Θ−Θ₀)/2) against th0

Predictions from the supplied Intrinsic spin, spinors and the Pauli matrices model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): AMPLITUDE cos((Θ−Θ₀)/2)

AMPLITUDE cos((Θ−Θ₀)/2) against th0Predictions from the supplied Intrinsic spin, spinors and the Pauli matrices model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: th0: Prepared direction Θ₀ / °. Vertical axis: AMPLITUDE cos((Θ−Θ₀)/2). Exact values are available in the data table below.0.80740.85720.90690.95671.00716.4834.3452.270.0687.92xy

Horizontal axis (x): th0: Prepared direction Θ₀ / °

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1th0: Prepared direction Θ₀ / °: 19.13AMPLITUDE cos((Θ−Θ₀)/2): 0.8147
Read the exact data as a table
AMPLITUDE cos((Θ−Θ₀)/2) against th0 — supplied values
th0: Prepared direction Θ₀ / °AMPLITUDE cos((Θ−Θ₀)/2)
19.1250.8147484825274895
35.66250.8896655492327864
52.20.9460853588275453
68.737500000000010.9828348730558712
85.2750.9991500236519368

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

The model's endpoint predictions bracket the reading. Solve Y_out(th0) = Y_measured and then solve again at Y_measured − u and Y_measured + u; a nonlinear inverse can give unequal input deviations.

Reveal the worked solution
  1. Endpoint predictions are Y_out(19.125) = 0.814748 and Y_out(85.275) = 0.99915. The target lies between them. On the selected branch the response is strictly increasing.
  2. Endpoint interpolation gives th0_line = 19.125 + (0.964733 − 0.814748)(85.275 − 19.125)/(0.99915 − 0.814748) = 72.9288 °. This estimates the inverse of the endpoint chord, rather than assuming that chord is the physical model.
  3. Use the actual equation, not the chord, and bracket its root. Evaluating the midpoint and retaining the sign-changing half-interval gives th0 = 59.4765 °; substituting back gives Y_out = 0.96473336.
  4. The interpolation error in the input is |th0_line − th0| = 13.4523 °. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.95957086 and 0.96989586. Sort the roots even if the response decreases: 57.3044 ° ≤ th0 ≤ 61.8112 °.
  6. The lower and upper input deviations are 2.17208 ° and 2.33472 °. They differ because the inverse response is nonlinear; a symmetric error bar would only be a local approximation. This interval includes reading uncertainty only, not model error or uncertainty in fixed inputs.

Answer th0 ≈ 59.4765 °; compatible interval [57.3044, 61.8112] °. Endpoint interpolation gives 72.9288 °.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.