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Equation 91 · The Clock That Comes Back Wrong by Exactly Its Mass

What does this equation mean?

Φ[LG]=m vrbℏ≈6.29×104 rad.\Phi[\mathcal L_{\rm G}]=\frac{m\,v_rb}{\hbar}\approx6.29\times10^{4}\ \text{rad}.

Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.

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Divide byhbar
This relates toPhi[mathcal L_rm G]
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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Φ\Phi

Symbol Phi

the single measured phase.

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LGL_{\rm G}

Symbol L_rm G

LrL_rm G is part of the quantity the equation computes from the expression on the right.

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mm

Symbol m

m occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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vrv_r

Symbol v_r

vrv_r occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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bb

Symbol b

b is an input to the expression that computes the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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fraction

fraction

Divide the expression above the line by the one below it.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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superscript

superscript

A raised number can be a power. When it is a label or bound, it selects a case or the upper limit of a sum; the formula’s structure distinguishes these uses.

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m vrbm\,v_rb

Numerator: mv_rb

The complete quantity above the fraction bar.

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ℏ\hbar

Denominator: hbar

The complete quantity below the fraction bar; it must be nonzero for this division.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

The Galilei loop admits an exact, non-simulated numerical check of the whole chain, because Φ\Phi[LG\mathcal L_{\rm G}] is precisely the recoil phase every stimulated-Raman atom interferometer already uses for its own calibration. Take a sodium atom, m=3.8175×\times10^{-26}\,kg\mathrm{kg} , driven by a two-photon stimulated-Raman transition on the 589\,nm\mathrm{nm} line, effective wavevector keffk_{\rm eff}=2(2π\pi/589\,nm\mathrm{nm})=2.1335×\times10^{7}\,m−1\mathrm{m^{-1}} [ 16 ] . The associated recoil velocity is vrv_r=ℏ\hbar keffk_{\rm eff}/m=5.894\,cm s−1\mathrm{cm\,s^{-1}} . Hold the loop open for T=50\,ms\mathrm{ms} , comparable to the short interrogation times of early stimulated-Raman interferometers, so the…
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The Galilei loop admits an exact, non-simulated numerical check of the whole chain, because Φ\Phi[LG\mathcal L_{\rm G}] is precisely the recoil phase every stimulated-Raman atom interferometer already uses for its own calibration. Take a sodium atom, m=3.8175×\times10^{-26}\,kg\mathrm{kg} , driven by a two-photon stimulated-Raman transition on the 589\,nm\mathrm{nm} line, effective wavevector keffk_{\rm eff}=2(2π\pi/589\,nm\mathrm{nm})=2.1335×\times10^{7}\,m−1\mathrm{m^{-1}} [ 16 ] . The associated recoil velocity is vrv_r=ℏ\hbar keffk_{\rm eff}/m=5.894\,cm s−1\mathrm{cm\,s^{-1}} . Hold the loop open for T=50\,ms\mathrm{ms} , comparable to the short interrogation times of early stimulated-Raman interferometers, so the translation leg is b=vrv_rT=2.947\,mm\mathrm{mm} . The loop area is vrv_rb=vr2v_r^2T=1.737×\times10^{-4}\,m2 s−1\mathrm{m^2\,s^{-1}} , and the phase debt is Φ[LG]=m vrbℏ≈6.29×104 rad\Phi[\mathcal L_{\rm G}]=\frac{m\,v_rb}{\hbar}\approx6.29\times10^{4}\ \text{rad}. This is an exact analytic evaluation of the formula derived above for stated, idealized parameters — not a simulation, not a measurement, and not the output of any code run for this article. It is offered as illustrative, and it carries a built-in consistency check: because vrv_r=ℏ\hbar keffk_{\rm eff}/m by definition of a recoil kick, the same number equals ℏ\hbar keff2k_{\rm eff}^2T/m , the ordinary recoil phase used to extract ℏ\hbar/m in precision atom-interferometry measurements through the general path-integral formalism for atomic interferometry [ 14 ] . The two expressions are algebraically identical, so this is a check that the loop construction reproduces a quantity the field already measures by an independent route, not new physics. Inverting the formula returns mopm_{\rm op}[LG\mathcal L_{\rm G}]=ℏ\hbarΦ\Phi/(vrv_rb)=m exactly, because the phase was defined from m in the first place. That circularity is the point of this section: it isolates what an idealized, confound-free evaluation looks like, so the next two sections can show exactly what breaks the idealization.

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