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University Advanced Quantum Mechanics · course UAQM

University Advanced Quantum Mechanics

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.

Extra challenging questions

A selection from this pathway. Open a topic below for its complete practice and challenge set.

Extra challenging · 01

Wigner's theorem: every symmetry is unitary or antiunitary: infer an input with uncertainty

A symmetry is a one-to-one map of rays that keeps every transition probability |⟨a|b⟩|², and Wigner's theorem says it is carried out by an operator that is either unitary or antiunitary, fixed up to one overall phase. Use the supplied topic model Y_out = 3*sqrt(3)/8*sind(th)^2*sind(90-th), where Y_out is IM B (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sqrt(x) means √x; sind/cosd/tand use degrees. th is Polar angle θ of a, b, c, measured in °. Keep chi (Rotation χ about z, applied after) = 45 °; s (Type s: +1 unitary, −1 antiunitary) = 1 fixed. For this exercise use only 56.8375 ° ≤ th ≤ 82.5625 ° 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 = 0.17741851, with a bounded reading uncertainty ±0.010735. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown th by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.0025725 °, 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

IM B against th

Predictions from the supplied Wigner's theorem: every symmetry is unitary or antiunitary 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): IM B

IM B against thPredictions from the supplied Wigner's theorem: every symmetry is unitary or antiunitary 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: th: Polar angle θ of a, b, c / °. Vertical axis: IM B. Exact values are available in the data table below.0.076020.12090.16580.21070.255655.8162.7569.776.6583.59xy

Horizontal axis (x): th: Polar angle θ of a, b, c / °

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

Reading 1th: Polar angle θ of a, b, c / °: 56.84IM B: 0.249
Read the exact data as a table
IM B against th — supplied values
th: Polar angle θ of a, b, c / °IM B
56.83750.24898290403971113
63.268750.23304670803299413
69.70.19821825562703652
76.131250.14674362213060246
82.56250.08266796225957404

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(th) = 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(56.8375) = 0.248983 and Y_out(82.5625) = 0.082668. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives th_line = 56.8375 + (0.177419 − 0.248983)(82.5625 − 56.8375)/(0.082668 − 0.248983) = 67.9068 °. 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 th = 72.5298 °; substituting back gives Y_out = 0.17741851.
  4. The interpolation error in the input is |th_line − th| = 4.62293 °. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.16668351 and 0.18815351. Sort the roots even if the response decreases: 71.1221 ° ≤ th ≤ 73.8505 °.
  6. The lower and upper input deviations are 1.40768 ° and 1.32075 °. 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 th ≈ 72.5298 °; compatible interval [71.1221, 73.8505] °. Endpoint interpolation gives 67.9068 °.

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

Extra challenging · 02

The spin-dependent amplitude g(θ) + i h(θ) σ⋅n: infer an input with uncertainty

For a spin-half particle scattering from a spin-zero target, the amplitude is the 2 × 2 spin matrix M = g(θ) + i h(θ) σ⋅n, where g leaves the spin alone, h acts through the spin component along the normal n to the scattering plane, and an unpolarised beam scatters with dσ/dΩ = |g|² + |h|². Use the supplied topic model Y_out = -2*deg(atan(w*kb^2*sind(th)/4)), where Y_out is SPIN ROTATION ABOUT n (°). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sind/cosd/tand use degrees; deg converts radians to degrees; unmarked trigonometric functions use radians. th is Marker angle θ, measured in °. Keep kb (Momentum times range kb) = 2.5; w (Spin-orbit depth ratio W/U) = 0.4 fixed. For this exercise use only 94.725 ° ≤ th ≤ 160.875 ° 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 = -47.628653 °, with a bounded reading uncertainty ±2.431 °. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown th 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

SPIN ROTATION ABOUT n against th

Predictions from the supplied The spin-dependent amplitude g(θ) + i h(θ) σ⋅n 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): SPIN ROTATION ABOUT n / °

SPIN ROTATION ABOUT n against thPredictions from the supplied The spin-dependent amplitude g(θ) + i h(θ) σ⋅n 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: th: Marker angle θ / °. Vertical axis: SPIN ROTATION ABOUT n / °. Exact values are available in the data table below.-65.46-54.48-43.49-32.5-21.5292.08109.9127.8145.7163.5xy

Horizontal axis (x): th: Marker angle θ / °

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

Reading 1th: Marker angle θ / °: 94.72SPIN ROTATION ABOUT n / °: -63.84
Read the exact data as a table
SPIN ROTATION ABOUT n against th — supplied values
th: Marker angle θ / °SPIN ROTATION ABOUT n / °
94.725-63.835572394075136
111.26249999999999-60.43779102071531
127.8-52.56463894734074
144.3375-40.04155729129355
160.875-23.144833057771717

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(th) = 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(94.725) = -63.8356 ° and Y_out(160.875) = -23.1448 °. The target lies between them. On the selected branch the response is strictly increasing.
  2. Endpoint interpolation gives th_line = 94.725 + (-47.6287 − -63.8356)(160.875 − 94.725)/(-23.1448 − -63.8356) = 121.072 °. 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 th = 135.077 °; substituting back gives Y_out = -47.628653 °.
  4. The interpolation error in the input is |th_line − th| = 14.0043 °. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = -50.059653 ° and -45.197653 °. Sort the roots even if the response decreases: 131.66 ° ≤ th ≤ 138.243 °.
  6. The lower and upper input deviations are 3.41685 ° and 3.16616 °. 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 th ≈ 135.077 °; compatible interval [131.66, 138.243] °. Endpoint interpolation gives 121.072 °.

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

Extra challenging · 03

Covariant notation and the Klein-Gordon equation: infer an input with uncertainty

The Klein-Gordon equation, (1/c²)∂²φ/∂t² − ∇²φ + (mc/ħ)²φ = 0, is the wave equation obtained by making E²/c² − p² = m²c² an operator identity with E = iħ∂/∂t and p = −iħ∇; written as (□ + (mc/ħ)²)φ = 0 it has the same form in every inertial frame. Use the supplied topic model Y_out = 197.327/m, where Y_out is COMPTON LENGTH ħ/mc (fm). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793. m is Rest energy mc², measured in MeV. Keep p (Momentum pc) = 100 MeV fixed. For this exercise use only 30.1875 MeV ≤ m ≤ 179.813 MeV 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 = 1.6246421 fm, with a bounded reading uncertainty ±0.079086 fm. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown m by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.0149625 MeV, 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

COMPTON LENGTH ħ/mc against m

Predictions from the supplied Covariant notation and the Klein-Gordon equation 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): COMPTON LENGTH ħ/mc / fm

COMPTON LENGTH ħ/mc against mPredictions from the supplied Covariant notation and the Klein-Gordon equation 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: m: Rest energy mc² / MeV. Vertical axis: COMPTON LENGTH ħ/mc / fm. Exact values are available in the data table below.0.87982.3483.8175.2866.75424.264.6105145.4185.8xy

Horizontal axis (x): m: Rest energy mc² / MeV

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

Reading 1m: Rest energy mc² / MeV: 30.19COMPTON LENGTH ħ/mc / fm: 6.537
Read the exact data as a table
COMPTON LENGTH ħ/mc against m — supplied values
m: Rest energy mc² / MeVCOMPTON LENGTH ħ/mc / fm
30.18756.536712215320911
67.593752.919308368007397
1051.8793047619047618
142.406251.3856624972569673
179.81251.0974042405283282

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(m) = 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(30.1875) = 6.53671 fm and Y_out(179.813) = 1.0974 fm. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives m_line = 30.1875 + (1.62464 − 6.53671)(179.813 − 30.1875)/(1.0974 − 6.53671) = 165.309 MeV. 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 m = 121.459 MeV; substituting back gives Y_out = 1.6246421 fm.
  4. The interpolation error in the input is |m_line − m| = 43.8504 MeV. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 1.5455561 fm and 1.7037281 fm. Sort the roots even if the response decreases: 115.821 MeV ≤ m ≤ 127.674 MeV.
  6. The lower and upper input deviations are 5.63804 MeV and 6.21504 MeV. 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 m ≈ 121.459 MeV; compatible interval [115.821, 127.674] MeV. Endpoint interpolation gives 165.309 MeV.

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

Extra challenging · 04

Dirac's requirements and the algebra of α and β: infer an input with uncertainty

Dirac's requirements are that the Hamiltonian H = cα⋅p + βmc² be Hermitian and square to p²c² + m²c⁴; they hold exactly when α₁, α₂, α₃ and β are Hermitian, square to 1 and anticommute in pairs, which no ordinary numbers can do. Use the supplied topic model Y_out = 1.022*m*sqrt(max(1-s^2,0)), where Y_out is SOLID GAP AT ITS MINIMUM (MeV). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sqrt(x) means √x; max(a,b) selects the larger value. s is Overlap s, where αβ + βα = 2s, dimensionless. Keep m (Mass m in electron masses) = 1 mₑ; p0 (Probe momentum p₀) = 1 MeV/c fixed. For this exercise use only 0.10625 ≤ s ≤ 0.89375 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 = 0.82767559 MeV, with a bounded reading uncertainty ±0.028281 MeV. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown s by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.00007875, 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

SOLID GAP AT ITS MINIMUM against s

Predictions from the supplied Dirac's requirements and the algebra of α and β 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): SOLID GAP AT ITS MINIMUM / MeV

SOLID GAP AT ITS MINIMUM against sPredictions from the supplied Dirac's requirements and the algebra of α and β 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: s: Overlap s, where αβ + βα = 2s. Vertical axis: SOLID GAP AT ITS MINIMUM / MeV. Exact values are available in the data table below.0.43610.58670.73730.88791.0390.074750.28740.50.71260.9252xy

Horizontal axis (x): s: Overlap s, where αβ + βα = 2s

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

Reading 1s: Overlap s, where αβ + βα = 2s: 0.1062SOLID GAP AT ITS MINIMUM / MeV: 1.016
Read the exact data as a table
SOLID GAP AT ITS MINIMUM against s — supplied values
s: Overlap s, where αβ + βα = 2sSOLID GAP AT ITS MINIMUM / MeV
0.106251.0162149156766742
0.3031250.9739157214363764
0.50.8850779626676962
0.69687499999999990.7329708435271745
0.89374999999999990.45843386092625193

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(s) = 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(0.10625) = 1.01621 MeV and Y_out(0.89375) = 0.458434 MeV. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives s_line = 0.10625 + (0.827676 − 1.01621)(0.89375 − 0.10625)/(0.458434 − 1.01621) = 0.372438. 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 s = 0.586625; substituting back gives Y_out = 0.82767559 MeV.
  4. The interpolation error in the input is |s_line − s| = 0.214187. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.79939459 MeV and 0.85595659 MeV. Sort the roots even if the response decreases: 0.54639 ≤ s ≤ 0.623044.
  6. The lower and upper input deviations are 0.0402351 and 0.0364194. 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 s ≈ 0.586625; compatible interval [0.54639, 0.623044]. Endpoint interpolation gives 0.372438.

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

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