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University Quantum Field Theory I · unit UQFTI-01

Natural Units, Relativistic States and the Feynman Propagator

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

Natural units, the metric, and back to seconds and barns: infer an input with uncertainty

Natural units set ħ = c = 1, so energy, momentum and mass share the unit GeV while lengths and times are measured in GeV⁻¹; ħc = 197.327 MeV fm and ħ = 6.582 × 10⁻²⁵ GeV s convert back to SI. Use the supplied topic model Y_out = -24.181634-log(a)-k, where Y_out is log₁₀(time/s) (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; log(x) means log₁₀x. a is Mantissa a in E = a × 10ᵏ GeV, dimensionless. Keep k (Power of ten k) = -1 fixed. For this exercise use only 1.95519 ≤ a ≤ 9.03481 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 = -23.979162, with a bounded reading uncertainty ±0.023759. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown a by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.000707962, 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

log₁₀(time/s) against a

Predictions from the supplied Natural units, the metric, and back to seconds and barns 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): log₁₀(time/s)

log₁₀(time/s) against aPredictions from the supplied Natural units, the metric, and back to seconds and barns 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: a: Mantissa a in E = a × 10ᵏ GeV. Vertical axis: log₁₀(time/s). Exact values are available in the data table below.-24.164-23.985-23.805-23.626-23.4461.6723.5845.4957.4069.318xy

Horizontal axis (x): a: Mantissa a in E = a × 10ᵏ GeV

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

Reading 1a: Mantissa a in E = a × 10ᵏ GeV: 1.955log₁₀(time/s): -23.47
Read the exact data as a table
log₁₀(time/s) against a — supplied values
a: Mantissa a in E = a × 10ᵏ GeVlog₁₀(time/s)
1.9551875-23.47282241201869
3.72509375-23.752771207177016
5.494999999999999-23.92160169675951
7.264906249999999-24.042864014316024
9.0348125-24.137553144051314

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(a) = 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(1.95519) = -23.4728 and Y_out(9.03481) = -24.1376. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives a_line = 1.95519 + (-23.9792 − -23.4728)(9.03481 − 1.95519)/(-24.1376 − -23.4728) = 7.34789. 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 a = 6.27376; substituting back gives Y_out = -23.979162.
  4. The interpolation error in the input is |a_line − a| = 1.07413. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = -24.002921 and -23.955403. Sort the roots even if the response decreases: 5.93976 ≤ a ≤ 6.62654.
  6. The lower and upper input deviations are 0.334 and 0.352781. 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 a ≈ 6.27376; compatible interval [5.93976, 6.62654]. Endpoint interpolation gives 7.34789.

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

Extra challenging · 02

What Advanced QM supplies, quoted and restated: infer an input with uncertainty

Advanced QM's free-field toolkit is the set of exact results about non-interacting quantum fields, their modes, vacuum amplitude, commutator, spin sums, statistics and Coulomb-gauge photons, that this course quotes by topic code and builds interactions on without re-deriving. Use the supplied topic model Y_out = exp(-sqrt(max(r*r - t*t, 0))*m/197.327), where Y_out is TAIL e^(−m√(−x²)), SPACELIKE ONLY (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sqrt(x) means √x; exp(x) means eˣ; max(a,b) selects the larger value. m is Particle mass m, measured in MeV. Keep t (Time separation t = x⁰ − y⁰) = 0.8 fm; r (Spatial distance r) = 2 fm fixed. For this exercise use only 195.625 MeV ≤ m ≤ 904.375 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 = 0.0029282981, with a bounded reading uncertainty ±0.00040555. 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 0.070875 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

TAIL e^(−m√(−x²)), SPACELIKE ONLY against m

Predictions from the supplied What Advanced QM supplies, quoted and restated 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): TAIL e^(−m√(−x²)), SPACELIKE ONLY

TAIL e^(−m√(−x²)), SPACELIKE ONLY against mPredictions from the supplied What Advanced QM supplies, quoted and restated 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: Particle mass m / MeV. Vertical axis: TAIL e^(−m√(−x²)), SPACELIKE ONLY. Exact values are available in the data table below.-0.0062650.037540.081350.12520.169167.3358.6550741.4932.7xy

Horizontal axis (x): m: Particle mass m / MeV

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

Reading 1m: Particle mass m / MeV: 195.6TAIL e^(−m√(−x²)), SPACELIKE ONLY: 0.1625
Read the exact data as a table
TAIL e^(−m√(−x²)), SPACELIKE ONLY against m — supplied values
m: Particle mass m / MeVTAIL e^(−m√(−x²)), SPACELIKE ONLY
195.6250.16247682798322646
372.81250.03133034237161927
5500.006041417507388916
727.18749999999990.0011649641445236124
904.37499999999990.00022463957446506368

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(195.625) = 0.162477 and Y_out(904.375) = 0.00022464. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives m_line = 195.625 + (0.0029283 − 0.162477)(904.375 − 195.625)/(0.00022464 − 0.162477) = 892.565 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 = 627.962 MeV; substituting back gives Y_out = 0.0029282981.
  4. The interpolation error in the input is |m_line − m| = 264.602 MeV. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.0025227481 and 0.0033338481. Sort the roots even if the response decreases: 614 MeV ≤ m ≤ 644.01 MeV.
  6. The lower and upper input deviations are 13.9629 MeV and 16.0478 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 ≈ 627.962 MeV; compatible interval [614, 644.01] MeV. Endpoint interpolation gives 892.565 MeV.

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

Extra challenging · 03

Invariant normalisation and the Poincaré group on Fock space: infer an input with uncertainty

Invariant normalisation is the choice ⟨p|q⟩ = (2π)³ 2E_p δ³(p − q) for one-particle states, the one normalisation every inertial frame agrees on, so that a Lorentz transformation acts on states as a unitary operator that simply relabels p as Λp. Use the supplied topic model Y_out = (exp(y0+eta)+exp(-(y0+eta)))/(exp(y0)+exp(-(y0))), where Y_out is ENERGY RATIO E′/E (dimensionless). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; exp(x) means eˣ. eta is Boost rapidity η, dimensionless. Keep y0 (Packet rapidity y₀) = 0.3; m (Mass m) = 0.5 GeV fixed. For this exercise use only -0.2625 ≤ eta ≤ 0.7875 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 = 1.185054, with a bounded reading uncertainty ±0.034163. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown eta by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.000105, 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

ENERGY RATIO E′/E against eta

Predictions from the supplied Invariant normalisation and the Poincaré group on Fock space 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): ENERGY RATIO E′/E

ENERGY RATIO E′/E against etaPredictions from the supplied Invariant normalisation and the Poincaré group on Fock space 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: eta: Boost rapidity η. Vertical axis: ENERGY RATIO E′/E. Exact values are available in the data table below.0.93241.1011.2691.4371.605-0.3045-0.0210.26250.5460.8295xy

Horizontal axis (x): eta: Boost rapidity η

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

Reading 1eta: Boost rapidity η: -0.2625ENERGY RATIO E′/E: 0.9573
Read the exact data as a table
ENERGY RATIO E′/E against eta — supplied values
eta: Boost rapidity ηENERGY RATIO E′/E
-0.262499999999999960.957300619728209
01
0.262499999999999961.1120022128088525
0.52499999999999991.301069328752839
0.78749999999999991.5803042345064902

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(eta) = 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(-0.2625) = 0.957301 and Y_out(0.7875) = 1.5803. The target lies between them. On the selected branch the response is strictly increasing.
  2. Endpoint interpolation gives eta_line = -0.2625 + (1.18505 − 0.957301)(0.7875 − -0.2625)/(1.5803 − 0.957301) = 0.121352. 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 eta = 0.378; substituting back gives Y_out = 1.185054.
  4. The interpolation error in the input is |eta_line − eta| = 0.256648. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 1.150891 and 1.219217. Sort the roots even if the response decreases: 0.326973 ≤ eta ≤ 0.424958.
  6. The lower and upper input deviations are 0.0510275 and 0.0469578. 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 eta ≈ 0.378; compatible interval [0.326973, 0.424958]. Endpoint interpolation gives 0.121352.

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

Extra challenging · 04

Wigner's little group: mass, spin and helicity: infer an input with uncertainty

The little group of a four-momentum k is the set of Lorentz transformations that leave k unchanged; its unitary representations supply the spin label of the states |p, σ⟩: 2j + 1 rotation states when m > 0, one Lorentz-invariant helicity when m = 0. Use the supplied topic model Y_out = deg(atan2(beta/sqrt(1-beta^2)*sqrt(1+u^2), u)), where Y_out is MOMENTUM TURN α (°). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sqrt(x) means √x; deg converts radians to degrees; atan2(y,x) is the angle of the vector (x,y), in radians. u is Particle momentum |p|/m, dimensionless. Keep beta (Observer speed β along −y) = 0.8; j (Spin j) = 0.5 fixed. For this exercise use only 1.15188 ≤ u ≤ 8.94812 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 = 53.5178 °, with a bounded reading uncertainty ±0.032576 °. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown u by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.000779625, 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

MOMENTUM TURN α against u

Predictions from the supplied Wigner's little group: mass, spin and helicity 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): MOMENTUM TURN α / °

MOMENTUM TURN α against uPredictions from the supplied Wigner's little group: mass, spin and helicity 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: u: Particle momentum |p|/m. Vertical axis: MOMENTUM TURN α / °. Exact values are available in the data table below.53.0154.9556.8958.8260.760.842.9455.057.1559.26xy

Horizontal axis (x): u: Particle momentum |p|/m

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

Reading 1u: Particle momentum |p|/m: 1.152MOMENTUM TURN α / °: 60.47
Read the exact data as a table
MOMENTUM TURN α against u — supplied values
u: Particle momentum |p|/mMOMENTUM TURN α / °
1.151875000000000260.47491427260283
3.100937499999999754.480685679758245
5.0553.65754953171523
6.99906249999999953.40758615011419
8.94812553.30062888379445

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(u) = 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(1.15188) = 60.4749 ° and Y_out(8.94812) = 53.3006 °. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives u_line = 1.15188 + (53.5178 − 60.4749)(8.94812 − 1.15188)/(53.3006 − 60.4749) = 8.71213. 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 u = 5.90758; substituting back gives Y_out = 53.5178 °.
  4. The interpolation error in the input is |u_line − u| = 2.80454. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 53.485224 ° and 53.550376 °. Sort the roots even if the response decreases: 5.67014 ≤ u ≤ 6.17681.
  6. The lower and upper input deviations are 0.237447 and 0.269229. 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 u ≈ 5.90758; compatible interval [5.67014, 6.17681]. Endpoint interpolation gives 8.71213.

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

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