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Equation 45 · Part 3 · The Clock That Comes Back Wrong by Exactly Its Mass

Symbol Phi

mop[LG]=ℏ Φ[LG]b⋅v.m_{\rm op}[\mathcal L_{\rm G}]=\frac{\hbar\,\Phi[\mathcal L_{\rm G}]}{\mathbf b\cdot\mathbf v}.
Φ\Phi

What this part means

dimensionless as a phase must be, and mass is recoverable from it as [displayed formula].

Its job in the formula

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

Where the article explains it

The loop invariant b\mathbf b⋅\cdotv\mathbf v carries units of m2 s−1\mathrm{m^2\,s^{-1}} , exactly the units of ℏ\hbar/mass\text{mass} , so Φ\Phi is dimensionless as a phase must be, and mass is recoverable from it as mop[LG]=ℏ Φ[LG]b⋅vm_{\rm op}[\mathcal L_{\rm G}]=\frac{\hbar\,\Phi[\mathcal L_{\rm G}]}{\mathbf b\cdot\mathbf v}.

The passage around this formula

…phase debt : what the representation charges for a loop the classical group considered free. The loop invariant b\mathbf b⋅\cdotv\mathbf v carries units of m2 s−1\mathrm{m^2\,s^{-1}} , exactly the units of ℏ\hbar/mass\text{mass} , so Φ\Phi is dimensionless as a phase must be, and mass is recoverable from it as mop[LG]=ℏ Φ[LG]b⋅vm_{\rm op}[\mathcal L_{\rm G}]=\frac{\hbar\,\Phi[\mathcal L_{\rm G}]}{\mathbf b\cdot\mathbf v}. Because m enters only through the fixed central charge and b\mathbf b,v\mathbf v are the loop’s own declared parameters, mopm_{\rm op}[LG\mathcal L_{\rm G}] does not depend on which inertial frame is used to…

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Learn the underlying idea

A variable is a named place for a value. Its letter is a local label: x can mean position in one formula and a data point in another.

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