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Inquiry Question 3: What evidence supports the relativistic model of the universe?

Investigate experimental and observational evidence for special relativity, including atmospheric and accelerator muon decay, GPS clock corrections, and the routine use of relativistic mechanics in particle physics

A focused answer to the HSC Physics Module 7 dot point on evidence for special relativity. Atmospheric muon flux at sea level, accelerator muon lifetimes, the daily GPS clock corrections (combined SR and GR), and the routine use of relativistic mechanics in particle physics.

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. The answer
  3. Examples in context

What this dot point is asking

NESA wants you to give concrete experimental and observational evidence that special relativity is correct. The standard items are atmospheric and accelerator muon measurements, GPS satellite clock corrections, and the routine validation of relativistic kinematics in particle physics.

The answer

1. Atmospheric muons

Cosmic rays striking the upper atmosphere produce muons at altitudes around 1010 to 1515 km. Muons are unstable, with proper lifetime t0=2.2t_0 = 2.2 μ\mus and typical speeds of 0.99c0.99c or more.

Non-relativistic prediction
In one proper lifetime, a muon at 0.99c0.99c travels about 650650 m, so almost no muons should reach the ground.
Relativistic prediction
At 0.99c0.99c, γ7.09\gamma \approx 7.09. The Earth-frame lifetime is γt016\gamma t_0 \approx 16 μ\mus, and the muon travels about 4.64.6 km in one dilated lifetime. A measurable fraction (about 10%10\% on average) survives to sea level.
Measurement
The Rossi-Hall experiment (1941) compared muon flux at the top of Mount Washington (elevation 19001900 m) and at sea level. The ratio matched the relativistic prediction and ruled out the non-relativistic one by orders of magnitude. Modern detectors confirm this to high precision.
The same effect in the muon frame
From the muon's point of view, its own lifetime is just 2.22.2 μ\mus. What changes is the distance to the ground: the atmosphere is length-contracted to 1010 km /γ=1.4/ \gamma = 1.4 km, which a 0.99c0.99c muon can comfortably cross in one proper lifetime. The two frames agree on the observed outcome (10% transit fraction) by different routes.

Muon survival fraction versus altitude descended through the atmosphere A graph of the percentage of an original population of ten kilometre altitude cosmic ray muons still surviving as they descend toward sea level at zero point nine nine c. The relativistic curve is an exponential decay that falls from one hundred percent at the top of the atmosphere to about twelve percent at ten kilometres, with six data points on the curve. A steep dashed reference curve shows the non relativistic prediction, which collapses to almost zero within about one kilometre. altitude descended (km) muons surviving (%) 246810 255075100 non-relativistic prediction relativistic: L = γv t₀ ≈ 4.6 km ≈18% at 8 km Far more muons survive than the non-relativistic curve predicts.

2. Accelerator muons

The Bailey et al. experiment (CERN, 1977) stored muons in a circular ring at γ29.3\gamma \approx 29.3 (v0.9994cv \approx 0.9994 c). The lab-frame lifetime was measured to be about 6464 μ\mus, 29.329.3 times the rest-frame 2.22.2 μ\mus, in agreement with t=γt0t = \gamma t_0 to better than 0.1%0.1\%. The muons' centripetal acceleration in the storage ring was enormous (1018g\sim 10^{18} g), confirming that time dilation depends only on instantaneous speed, not on acceleration.

Two equivalent frame explanations for muon survival to sea level Two panels compare the Earth frame and the muon rest frame. In the Earth frame panel the atmosphere is a full ten kilometres thick and the muon clock runs slow so its lifetime is dilated to about sixteen microseconds, long enough to cross. In the muon frame panel the muon clock ticks normally at two point two microseconds but the atmosphere is length contracted to about one point four kilometres, short enough to cross in that time. Both panels conclude the same observed survival fraction. Earth frame ground μ 10 km atmosphere clock dilated: t = γt₀ ≈ 16 μs muon lifetime stretched, atmosphere full length Muon frame ground μ L = L₀ ⁄ γ ≈ 1.4 km clock normal: t₀ = 2.2 μs Different mechanism, same result: about 10% of muons reach the ground.

3. GPS satellite clocks

GPS satellites orbit at 20200\sim 20\,200 km altitude with orbital speed 3.87\sim 3.87 km/s. A GPS receiver determines position by measuring the time-of-flight from at least four satellites, so the onboard clocks must agree with ground time to within a few nanoseconds to give metre-level positions.

Two relativistic effects shift the satellite clock rate:

  • Special relativity (motion). A moving clock runs slow by Δt/t12(v/c)28.3×1011\Delta t / t \approx -\tfrac{1}{2}(v/c)^2 \approx -8.3 \times 10^{-11}, equivalent to 7.2-7.2 μ\mus per day.
  • General relativity (altitude). A clock higher in Earth's gravitational potential runs fast by Δt/t+gh/c2+5.3×1010\Delta t / t \approx +g h / c^2 \approx +5.3 \times 10^{-10}, equivalent to +45.8+45.8 μ\mus per day.

Net: the satellite clock runs about +38.6+38.6 μ\mus per day faster than a ground clock. The correction is applied by adjusting the satellite's onboard oscillator frequency before launch (set slightly slow at 10.2299999954310.22999999543 MHz instead of the design 10.2310.23 MHz), and minor residual corrections are computed each day. Without these corrections, GPS positions would drift by about 1111 km per day - a clear failure of the system.

GPS is therefore an everyday technology that validates both special and general relativity in real time.

4. Particle physics kinematics

Every collision experiment at a modern accelerator (LHC at CERN, Belle II at KEK, RHIC at Brookhaven) is analysed with relativistic kinematics:

  • Energy-momentum conservation uses the four-vector form, E2=(pc)2+(mc2)2E^2 = (pc)^2 + (mc^2)^2, not the non-relativistic E=p2/(2m)E = p^2 / (2m).
  • Track reconstruction in magnetic fields assumes r=p/(qB)r = p / (q B) with p=γmvp = \gamma m v, not the non-relativistic version.
  • Invariant masses of resonances (the Z boson, the Higgs boson) are reconstructed from decay products using the relativistic combination m2c4=E2(pc)2m^2 c^4 = E^2 - (pc)^2.

If any of this were wrong, particle identification and discoveries would fail. The Higgs boson was discovered in 2012 by reconstructing decays such as HγγH \to \gamma \gamma and HZZ4H \to ZZ \to 4\ell, with invariant masses calculated using exactly the special-relativity machinery. The agreement of cross-sections, lifetimes and decay products with relativistic predictions at the per-cent level (or better) is the most thoroughly tested aspect of any physical theory.

5. Other supporting evidence

Ives-Stilwell experiment (1938)
A direct test of relativistic Doppler shift using hydrogen ion beams; agreed with relativity to a few per cent at the time and now to better than 10910^{-9}.
Hafele-Keating experiment (1971)
Atomic clocks flown on commercial aircraft eastward and westward around the world differed from a stationary ground clock by amounts predicted by SR (motion) and GR (altitude) combined.
Pound-Rebka experiment (1959)
Measured gravitational redshift of 14.414.4-keV gamma photons over 22.522.5 m using the Mossbauer effect; supports general relativity, complementing SR evidence.
Modern atomic-clock comparisons
Optical lattice clocks at NIST can detect altitude differences of a few centimetres through gravitational time dilation.

Examples in context

Example 1. Australian-built GPS receivers and the 38.7μs/day38.7 \mu\text{s}/\text{day} correction. GPS satellites orbiting at v=3.87 km/sv = 3.87 \text{ km/s} and altitude 20,200 km20{,}200 \text{ km} experience two relativistic effects: SR time dilation slows their clocks by ΔtSR=(v2/2c2)×86,400=7.2μs/day\Delta t_{SR} = -(v^2/2c^2) \times 86{,}400 = -7.2 \mu\text{s}/\text{day}, while general-relativistic altitude makes them tick faster by +45.9μs/day+45.9 \mu\text{s}/\text{day}. Net correction: +38.7μs/day+38.7 \mu\text{s}/\text{day}. A Geoscience Australia GPS reference station at Yarragadee, WA, has measured this drift to better than 10910^{-9} precision over decades. Without the correction, positions would degrade by 11 km/day\sim 11 \text{ km}/\text{day}, making the system useless for navigation.

Example 2. Hafele-Keating-style experiment from Sydney. Two atomic clocks, one flown around the world eastward on a Sydney-London-Sydney commercial route at v240 m/sv \approx 240 \text{ m/s} for 24 h\sim 24 \text{ h} (86,400 s86{,}400 \text{ s}), the other left at Sydney Observatory. SR slowdown: (v2/2c2)×t=(2402/2×9×1016)×86,400=2.8×108 s=28 ns(v^2/2c^2) \times t = (240^2 / 2 \times 9 \times 10^{16}) \times 86{,}400 = 2.8 \times 10^{-8} \text{ s} = 28 \text{ ns}. (GR speedup at 11 km11 \text{ km} altitude adds +50 ns\sim +50 \text{ ns}.) These nanosecond-level effects, predicted by SR and confirmed first by Hafele and Keating in 1971, demonstrate that moving clocks really do run slow. Caesium atomic clocks resolve the 30 ns\sim 30 \text{ ns} difference easily.

Exam-style practice questions

Practice questions written in the style of NESA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

2021 HSC4 marksMuons produced at an altitude of 10 km travel toward the Earth at 0.99c. Their proper lifetime is 2.2 microseconds. Show, using a relativistic and a non-relativistic calculation, why the observed flux of muons at sea level is evidence for special relativity.
Show worked answer →

Non-relativistic prediction. In 2.22.2 μ\mus a muon at 0.99c0.99c travels:

dNR=vt0=0.99×3.0×108×2.2×106=6.5×102d_{\text{NR}} = v t_0 = 0.99 \times 3.0 \times 10^8 \times 2.2 \times 10^{-6} = 6.5 \times 10^{2} m =650= 650 m.

This is far less than 1010 km, so essentially no muons should survive to sea level. The expected flux ratio would be exp(10000/650)exp(15.4)2×107\exp(-10000 / 650) \approx \exp(-15.4) \approx 2 \times 10^{-7}.

Relativistic prediction. Lorentz factor:

γ=1/10.9801=1/0.0199=1/0.1411=7.09\gamma = 1 / \sqrt{1 - 0.9801} = 1 / \sqrt{0.0199} = 1 / 0.1411 = 7.09.

Earth-frame lifetime: t=γt0=7.09×2.2×106=1.56×105t = \gamma t_0 = 7.09 \times 2.2 \times 10^{-6} = 1.56 \times 10^{-5} s.

Distance covered in this dilated lifetime: d=vt=0.99×3.0×108×1.56×105=4.6×103d = v t = 0.99 \times 3.0 \times 10^8 \times 1.56 \times 10^{-5} = 4.6 \times 10^3 m =4.6= 4.6 km.

So in one dilated lifetime the muons travel 4.64.6 km, comparable to the 1010 km distance. The expected flux ratio is exp(10000/4600)exp(2.17)0.11\exp(-10000 / 4600) \approx \exp(-2.17) \approx 0.11.

Measurement: about 10%10\% of muons reach sea level, matching the relativistic prediction. The non-relativistic prediction is wrong by six orders of magnitude. Markers reward both calculations and a clear comparison with experiment.

2020 HSC3 marksExplain why GPS satellites must apply a daily clock correction of approximately 38 microseconds to operate correctly, identifying which parts of the correction come from special relativity and which from general relativity.
Show worked answer →

A GPS satellite orbits at about 2020020\,200 km altitude at a speed of about 3.873.87 km/s. Two relativistic effects shift its onboard clock relative to a clock at the Earth's surface:

Special relativity (time dilation due to motion): the satellite's clock runs slow as seen from the ground because the satellite is moving. The shift is:

ΔtSR/t12(v/c)212(3870/3×108)28.3×1011\Delta t_{\text{SR}} / t \approx -\tfrac{1}{2} (v/c)^2 \approx -\tfrac{1}{2} (3870 / 3 \times 10^8)^2 \approx -8.3 \times 10^{-11},

which is about 7.2-7.2 μ\mus per day (the clock loses time).

General relativity (gravitational time dilation): a clock at high altitude in a weaker gravitational potential ticks faster than a clock at the surface. The shift is:

ΔtGR/t+gΔh/c2+5.3×1010\Delta t_{\text{GR}} / t \approx + g \Delta h / c^2 \approx +5.3 \times 10^{-10},

which is about +45.8+45.8 μ\mus per day (the clock gains time).

Net effect: +45.87.2+38.6+45.8 - 7.2 \approx +38.6 μ\mus per day faster than ground clocks. Without applying this correction, GPS positions would drift by about 1111 km per day (since light travels 0.30.3 m per ns). The correction is hard-coded into the satellite oscillator frequencies before launch.

Markers reward identifying both effects with correct signs, the net magnitude, and the consequence for position accuracy.

Practice questions

Original practice questions graded from foundation to exam level, each with a full worked solution. Try them before revealing the solution.

foundation2 marksState one piece of experimental evidence for time dilation and one piece of experimental evidence for length contraction, each in a single sentence.
Show worked solution →

Time dilation. More atmospheric muons reach sea level than a non-relativistic calculation predicts, because their lab-frame lifetime t=γt0t = \gamma t_0 is stretched.

Length contraction. In the muon's own rest frame, the 10 km10\ \text{km} atmosphere is contracted to L=L0/γ1.4 kmL = L_0 / \gamma \approx 1.4\ \text{km}, short enough to cross in one proper lifetime.

Marks: one for a correct, clearly time-dilation example, one for a correct, clearly length-contraction example (not the same experiment described twice in different words).

foundation3 marksA muon travels at v=0.95cv = 0.95c. Calculate its Lorentz factor γ\gamma, giving your answer to three significant figures.
Show worked solution →

γ=11v2/c2\gamma = \dfrac{1}{\sqrt{1 - v^2/c^2}}

γ=110.952=110.9025=10.0975=10.3122\gamma = \dfrac{1}{\sqrt{1 - 0.95^2}} = \dfrac{1}{\sqrt{1 - 0.9025}} = \dfrac{1}{\sqrt{0.0975}} = \dfrac{1}{0.3122}

γ=3.20\gamma = 3.20.

Marks: one for the correct formula, one for correctly substituting v/c=0.95v/c = 0.95, one for γ=3.20\gamma = 3.20 to three significant figures.

foundation3 marksMuons are created at an altitude of 8.0 km8.0\ \text{km} and travel toward the ground at v=0.95cv = 0.95c, with proper lifetime t0=2.2 μst_0 = 2.2\ \mu\text{s}. Using γ=3.20\gamma = 3.20 (from the previous question), find the distance a muon travels, on average, in one lab-frame lifetime.
Show worked solution →

Lab-frame (dilated) lifetime: t=γt0=3.20×2.2×106=7.04×106 st = \gamma t_0 = 3.20 \times 2.2 \times 10^{-6} = 7.04 \times 10^{-6}\ \text{s}.

Distance travelled: d=vt=(0.95×3.00×108)(7.04×106)=2.0×103 m=2.0 kmd = v t = (0.95 \times 3.00 \times 10^8)(7.04 \times 10^{-6}) = 2.0 \times 10^{3}\ \text{m} = 2.0\ \text{km}.

Marks: one for t=γt0t = \gamma t_0 correctly evaluated, one for d=vtd = vt correctly evaluated, one for the final answer 2.0 km2.0\ \text{km} with correct unit and sig figs.

core4 marksIn the muon's own rest frame, the 9.0 km9.0\ \text{km} thickness of atmosphere it must cross is length-contracted. Using v=0.99cv = 0.99c (γ=7.09\gamma = 7.09), calculate the contracted thickness, and explain why this length-contraction argument predicts the same survival fraction as the time-dilation argument made in the Earth frame.
Show worked solution →

Contracted length. L=L0γ=9.0×1037.09=1.3×103 m=1.3 kmL = \dfrac{L_0}{\gamma} = \dfrac{9.0 \times 10^3}{7.09} = 1.3 \times 10^{3}\ \text{m} = 1.3\ \text{km}.

Why the two arguments agree. In the Earth frame, the muon's lifetime is dilated to t=γt0t = \gamma t_0, so it covers a distance γvt0\gamma v t_0 before decaying - long enough to cross the (uncontracted) 9.0 km9.0\ \text{km}. In the muon's own frame, the muon's lifetime is just the proper time t0t_0, but the atmosphere it must cross is contracted to L0/γL_0/\gamma, which is short enough for it to cross in that undilated time. Both descriptions are self-consistent applications of the same relative motion, and both correctly predict that a substantial fraction of muons survive to the ground - special relativity guarantees the two frames agree on the observable outcome (how many muons reach sea level).

Marks: one for L=L0/γL = L_0/\gamma correctly evaluated, one for L=1.3 kmL = 1.3\ \text{km} with unit, one for stating the ground frame uses dilated time, one for stating the muon frame uses contracted length and that both frames predict the same observed survival fraction.

core4 marksThe figure shows the percentage of a cosmic-ray muon population (created at altitude 10 km10\ \text{km}, v=0.99cv = 0.99c) still surviving as a function of altitude descended. **(a)** Describe the shape of the curve. **(b)** Using the points at 2 km2\ \text{km} (64.9%64.9\%) and 8 km8\ \text{km} (17.8%17.8\%), find the gradient of ln(fraction surviving)\ln(\text{fraction surviving}) against altitude. **(c)** Hence find the decay length LL this implies, and compare it with L=γvt0L = \gamma v t_0.
Show worked solution →

(a) The curve is an exponential decay: it falls steeply at first and flattens as altitude descended increases, consistent with a constant-probability decay process (radioactive-decay-like survival, N=N0ex/LN = N_0 e^{-x/L}).

(b) Taking natural logs of the surviving percentage at each point: ln(0.649)=0.432\ln(0.649) = -0.432 and ln(0.178)=1.726\ln(0.178) = -1.726.

Gradient =Δ(lnf)Δx=(1.726)(0.432)82=1.2946=0.216 km1= \dfrac{\Delta(\ln f)}{\Delta x} = \dfrac{(-1.726) - (-0.432)}{8 - 2} = \dfrac{-1.294}{6} = -0.216\ \text{km}^{-1}.

(c) Since f=ex/Lf = e^{-x/L}, lnf=x/L\ln f = -x/L, so the gradient equals 1/L-1/L: L=10.216=4.6 kmL = \dfrac{1}{0.216} = 4.6\ \text{km}.

This matches L=γvt0=7.09×(0.99×3.00×108)×2.2×106=4.6×103 m=4.6 kmL = \gamma v t_0 = 7.09 \times (0.99 \times 3.00 \times 10^8) \times 2.2 \times 10^{-6} = 4.6 \times 10^{3}\ \text{m} = 4.6\ \text{km} from the relativistic prediction, confirming the graph is consistent with time-dilated muon decay.

Marks: one for correctly describing the exponential shape, one for a correctly computed gradient (allow 0.20-0.20 to 0.23 km1-0.23\ \text{km}^{-1}), one for L4.6 kmL \approx 4.6\ \text{km} from the gradient, one for comparing it with γvt0\gamma v t_0 and concluding they agree.

exam6 marksEvaluate the claim that atmospheric muon decay is convincing evidence for special relativity, referring to both the time-dilation and length-contraction explanations and to the size of the discrepancy with the non-relativistic prediction.
Show worked solution →

Band-6 plan. (1) State the non-relativistic prediction and why it fails. (2) Give the Earth-frame (time-dilation) explanation with the numbers. (3) Give the muon-frame (length-contraction) explanation and note it predicts the same outcome. (4) Quantify the discrepancy and state the experimental confirmation. (5) Reach an explicit judgement on how convincing the evidence is.

Model answer. Muons created at about 10 km10\ \text{km} altitude have a proper lifetime of only t0=2.2 μst_0 = 2.2\ \mu\text{s} and travel at roughly 0.99c0.99c. Non-relativistically, a muon travels only vt0650 mv t_0 \approx 650\ \text{m} in one lifetime, so the fraction expected to survive 10 km10\ \text{km} to sea level is of order 10710^{-7} - essentially none.

In the Earth frame, special relativity dilates the muon's lifetime to t=γt0t = \gamma t_0. At v=0.99cv = 0.99c, γ7.09\gamma \approx 7.09, so t1.6×105 st \approx 1.6 \times 10^{-5}\ \text{s} and the muon travels d=vt4.6 kmd = vt \approx 4.6\ \text{km} in one dilated lifetime - comparable to the 10 km10\ \text{km} path, giving a survival fraction of order 10%10\%.

Equivalently, in the muon's own rest frame its lifetime is still just t0t_0, but the 10 km10\ \text{km} atmosphere is length-contracted to L=L0/γ1.4 kmL = L_0/\gamma \approx 1.4\ \text{km}, which is short enough to cross before decaying. The two frames disagree about which quantity changes (time in the Earth frame, length in the muon frame) but agree exactly on the observable: about 10%10\% of the muons reach sea level.

Experiments such as the Rossi-Hall comparison of muon flux atop Mount Washington versus at sea level, and later accelerator storage-ring measurements of muon lifetime at γ29.3\gamma \approx 29.3 (agreeing with t=γt0t = \gamma t_0 to better than 0.1%0.1\%), measure exactly this survival fraction and match the relativistic prediction, not the non-relativistic one - which is wrong by roughly six orders of magnitude. Because the non-relativistic and relativistic predictions differ so enormously, and because two independent relativistic descriptions (time dilation and length contraction) converge on the same measured outcome, atmospheric and accelerator muon decay is very strong, near-conclusive observational evidence for special relativity.

Marker's note: the top band gives both numerical predictions (non-relativistic and relativistic), explains the discrepancy is orders of magnitude not a small correction, presents BOTH frame explanations and states they agree on the observable, and closes with an explicit judgement of how convincing the evidence is. A response giving only the time-dilation calculation without the length-contraction frame or a judgement caps in the middle band.

exam7 marksAssess the significance of GPS satellite clock corrections and routine relativistic kinematics in particle accelerators as evidence for special relativity, compared with the muon-decay evidence.
Show worked solution →

Band-6 plan. Thesis: GPS and accelerator kinematics extend the case beyond a single decay-rate measurement to continuous, high-precision, technological confirmation. Cover (1) GPS: what the correction is, why it is needed, and what would happen without it; (2) accelerator kinematics: the routine reliance on relativistic energy-momentum and why discovery physics would fail otherwise; (3) compare robustness/precision with muon decay; (4) explicit judgement of significance.

Model answer. GPS satellites orbit at about 20200 km20\,200\ \text{km} altitude at v3.87 km/sv \approx 3.87\ \text{km/s}. Special relativity predicts their onboard clocks run slow relative to the ground by about 7.2 μs7.2\ \mu\text{s} per day (motion, ΔtSR/t12(v/c)2\Delta t_{\text{SR}}/t \approx -\tfrac{1}{2}(v/c)^2), while general relativity predicts they run fast by about 45.8 μs45.8\ \mu\text{s} per day (altitude). The net +38.6 μs+38.6\ \mu\text{s} per day correction is built into the satellite oscillators before launch. If special relativity were wrong, the SR term would be mis-sized and GPS positions would drift by kilometres within a day - yet global positioning works to metre accuracy every day, continuously testing the prediction in a way a single decay experiment cannot.

Relativistic kinematics is also load-bearing in every accelerator experiment. Energy-momentum conservation is applied as E2=(pc)2+(mc2)2E^2 = (pc)^2 + (mc^2)^2, not the Newtonian E=p2/2mE = p^2/2m, and particle tracks are reconstructed with relativistic momentum p=γmvp = \gamma m v. Resonances such as the Higgs boson are identified from invariant masses m2c4=E2(pc)2m^2c^4 = E^2 - (pc)^2 of their decay products. None of this machinery works, and no new particle could be correctly identified, if special relativity were false - so every successful discovery (including the 2012 Higgs boson) is an additional, independent confirmation.

Compared with muon decay, which is a striking but single-purpose demonstration of t=γt0t = \gamma t_0, GPS and accelerator kinematics are significant because they are continuous (millions of GPS fixes daily), applied at a completely different energy/speed regime (near-orbital speeds for GPS versus ultra-relativistic speeds in accelerators), and embedded in technologies whose failure would be immediately obvious. Weighing the muon evidence (large, unambiguous discrepancy with the non-relativistic prediction) against the GPS/accelerator evidence (continuous, high-precision, and practically consequential), together they form a body of evidence spanning many orders of magnitude in speed and energy, which is why special relativity is considered one of the most rigorously tested theories in physics.

Marker's note: the top band explains the GPS correction with both signed contributions, links accelerator kinematics to a concrete example (the Higgs boson or equivalent), explicitly compares the type of evidence to muon decay (continuous/technological versus a single measurement), and reaches a stated judgement of overall significance. A response that only restates the GPS numbers without the comparison or the particle-physics kinematics caps below the top band.

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