Equation 91 · The Clock That Comes Back Wrong by Exactly Its Mass
What does this equation mean?
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.
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.
Read it piece by piece
Symbol L_rm G
m G is part of the quantity the equation computes from the expression on the right.
Symbol m
m occurs above the fraction bar. The numerator is divided by the entire denominator below it.
Symbol v_r
occurs above the fraction bar. The numerator is divided by the entire denominator below it.
Symbol b
b is an input to the expression that computes the quantity on the left.
=
The expressions on both sides represent the same quantity under the stated assumptions.
See an illustrated explanation →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.
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.
See an illustrated explanation →Denominator: hbar
The complete quantity below the fraction bar; it must be nonzero for this division.
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 [] is precisely the recoil phase every stimulated-Raman atom interferometer already uses for its own calibration. Take a sodium atom, m=3.817510^{-26}\, , driven by a two-photon stimulated-Raman transition on the 589\, line, effective wavevector =2(2/589\,)=2.133510^{7}\, [ 16 ] . The associated recoil velocity is = /m=5.894\, . Hold the loop open for T=50\, , comparable to the short interrogation times of early stimulated-Raman interferometers, so the…
Read the full surrounding passage
The Galilei loop admits an exact, non-simulated numerical check of the whole chain, because [] is precisely the recoil phase every stimulated-Raman atom interferometer already uses for its own calibration. Take a sodium atom, m=3.817510^{-26}\, , driven by a two-photon stimulated-Raman transition on the 589\, line, effective wavevector =2(2/589\,)=2.133510^{7}\, [ 16 ] . The associated recoil velocity is = /m=5.894\, . Hold the loop open for T=50\, , comparable to the short interrogation times of early stimulated-Raman interferometers, so the translation leg is b=T=2.947\, . The loop area is b=T=1.73710^{-4}\, , and the phase debt is . 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 = /m by definition of a recoil kick, the same number equals T/m , the ordinary recoil phase used to extract /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 []=/(b)=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.
Sources cited in the surrounding passage
- [16] Atomic Interferometry Using Stimulated Raman Transitions ↗
- [14] The Feynman Path Integral Approach to Atomic Interferometry: A Tutorial ↗
These citations give research context. Read each source to check which claims it supports.
Return to The Clock That Comes Back Wrong by Exactly Its Mass