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To make this concrete without simulation, take the weak-field proper-time rate d/dt1+gz/ for a static height z in Earth’s field, so that holding two branches at a height difference z for coordinate time T gives g\, z\,T/ . For z=1\, and T=1\, , 1.09010^{-16}\, . Pair this with a single-photon optical clock transition near 698\, , comparable to the transition used in strontium-lattice-clock proposals for this kind of experiment [ 11 , 13 ] , giving 4.29510^{14}\, and E=h2.84610^{-19}\, , a mass excess …
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Symbol h
h is one of the signed contributions combined to compute the quantity on the left.
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Δnu is one of the signed contributions combined to compute the quantity on the left.
Read this term in its guide →Symbol J
J is one of the signed contributions combined to compute the quantity on the left.
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Equation 116 · Evolutionary Physics
The Clock That Comes Back Wrong by Exactly Its Mass
This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.
To make this concrete without simulation, take the weak-field proper-time rate d/dt1+gz/ for a static height z in Earth’s field, so that holding two branches at a height difference z for coordinate time T gives g\, z\,T/ . For z=1\, and T=1\, , 1.09010^{-16}\, . Pair this with a single-photon optical clock transition near 698\, , comparable to the transition used in strontium-lattice-clock proposals for this kind of experiment [ 11 , 13 ] , giving 4.29510^{14}\, and E=h2.84610^{-19}\, , a mass excess …