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Equation 57 · The Clock That Comes Back Wrong by Exactly Its Mass

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c→∞c\to\infty

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cc

Symbol c

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The two pictures are not independent theories that happen to share a symbol. The Galilei phase is the c→\to∞\infty residue of the Poincaré non-extension, and the residue can be taken explicitly rather than asserted. Write the energy operator for a system at rest as H=Mc2c^2+HNRH_{\rm NR} , separating the rest energy from whatever nonrelativistic energy — kinetic, internal — sits on top of it. The relativistic loop phase becomes

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