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Published equation contexts

d(hg^,hg)=d(g^,g)d(h\hat g,hg)=d(\hat g,g)

Why this formula appears here

The central mathematical test is simple to state. Apply a common frame transformation h to the physical description. Covariance sends g and g^\hat g to hg and hg^\hat g , or to the appropriate left/right action fixed by convention. A left-invariant distance satisfies d(hg^,hg)=d(g^,g)d(h\hat g,hg)=d(\hat g,g). The Haar measure is invariant, and the transformed POVM produces the correspondingly transformed outcome probabilities. Therefore the integration region defining success is merely relabeled. The value of pϵ(F)p_\epsilon(F) , and hence Rϵ,δR_{\epsilon,\delta} , should not change.

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g^\hat g

Symbol hat g

hat g is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

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Published contexts (1)

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d(hg^,hg)=d(g^,g).d(h\hat g,hg)=d(\hat g,g).

Equation 63 · Evolutionary Physics

A Reference Frame Becomes Classical by Publishing Its Orientation

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.

The central mathematical test is simple to state. Apply a common frame transformation h to the physical description. Covariance sends g and g^\hat g to hg and hg^\hat g , or to the appropriate left/right action fixed by convention. A left-invariant distance satisfies d(hg^,hg)=d(g^,g)d(h\hat g,hg)=d(\hat g,g). The Haar measure is invariant, and the transformed POVM produces the correspondingly transformed outcome probabilities. Therefore the integration region defining success is merely relabeled. The value of pϵ(F)p_\epsilon(F) , and hence Rϵ,δR_{\epsilon,\delta} , should not change.

Meanings in this article

  • gg: the covariance sends.
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