• Quantum Zeno Effect pixel-art physics T-shirt, white tee, front view

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Zeno

Quantum Zeno Effect / The Observer Physics

\[P_{\text{stay}}(t) \approx 1 - \left(\frac{t}{\tau_Z}\right)^{2}, \qquad \tau_Z = \frac{\hbar}{\Delta H}\]
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Stare at a pot and it never boils. Quantum mechanics has its own version. Zeno embodies the quantum Zeno effect: measure a quantum system often enough and its evolution is suppressed. Zeno wears it in pixel art on a unisex tee. The physics panel below has the equation, every symbol and the sources.

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Details

Size & fitS–5XL

Unisex heavy cotton (Gildan 5000), classic fit.

Unisex tee size chart, inches
SizeWidthLengthSleeve
S182815.1
M202916.5
L223018
XL243119.5
2XL263221
3XL283322.4
4XL303423.7
5XL323525

Ter vergelijking: maat M is 20 in (50.80 cm) breed, ongeveer 3.143 × 1034 Plancklengtes (lP = 1.616255 × 10−35 m). Een meetlint is sneller.

Measurements in inches, ±1.5 in tolerance.

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Returns & replacements21 days

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The physics

Each time you measure an unstable quantum system you reset it, and right after a reset its chance of having changed grows only with the square of the time. So if you look often enough, it barely gets the chance to change at all: a watched quantum pot never boils.

The arrow is drawn. You are watching. Nothing happens.

Zeno of Elea argued that a flying arrow, at any single instant, is not moving, so when does it move? About twenty-four centuries later, in 1977, Baidyanath Misra and George Sudarshan showed that quantum mechanics contains a version of the paradox that actually holds: a system observed often enough does not leave the state it started in.

The reason is in the first moments. A quantum state does not begin to change at a steady rate. For short times, the chance that it has changed grows with the square of the elapsed time. Check it n times instead of once and each check starts the clock again; you pay n small squares instead of one large one, and as n grows the total goes toward zero.

In 1990, at NIST in Boulder, Wayne Itano, Daniel Heinzen, John Bollinger and David Wineland put about 5,000 beryllium ions in a Penning trap. A 256-millisecond radio-frequency pulse was tuned to carry every ion from one hyperfine level to another. During the pulse they hit the ions with short flashes of ultraviolet light: 1, 2, 4, and so on up to 64. Each flash asked one question: which level are you in? Ions in one level scattered a few photons. Ions in the other scattered none, and were measured anyway. With one flash at the end, nearly all the ions made the transition. With 64 flashes, nearly none did. For 64 ideal measurements, \(\tfrac{1}{2}\left[1-\cos^{64}(\pi/64)\right]\) comes to under 4 percent.

What the flashes do to the wavefunction is still argued over. "Collapse" is one reading, and Leslie Ballentine published an objection to it in 1991. The suppression itself is measured.

Zeno holds the bow because you are looking.

Equations

\[P_{\text{stay}}(t) \approx 1 - \left(\frac{t}{\tau_Z}\right)^{2}, \qquad \tau_Z = \frac{\hbar}{\Delta H}\]
\[P_{1\to 2}(n) = \tfrac{1}{2}\left[1 - \cos^{n}\!\left(\tfrac{\pi}{n}\right)\right]\]
Symbols
SymbolMeaningUnit
\(P_{\text{stay}}\) probability the system is still in its initial state (dimensionless) \(\mathrm{1}\)
\(t\) time since preparation \(\mathrm{s}\)
\(\tau_Z\) Zeno time (short-time scale of decay) \(\mathrm{s}\)
\(\hbar\) reduced Planck constant \(\mathrm{J·s}\)
\(\Delta H\) energy spread of the initial state, √(⟨H²⟩ − ⟨H⟩²) \(\mathrm{J}\)
\(P_{1\to 2}(n)\) probability of completing a driven π-pulse transition when interrupted by n ideal measurements \(\mathrm{1}\)
\(n\) number of equally spaced measurements during the pulse \(\mathrm{1}\)

Source Misra, B.; Sudarshan, E. C. G. (1977). The Zeno’s paradox in quantum theory. Journal of Mathematical Physics 18, 756–763.doi.org/10.1063/1.523304 (opens in a new tab)