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Equation 27 · The Clock That Comes Back Wrong by Exactly Its Mass

What does this equation mean?

[Ki,Pj]=iℏ m δij 1,[K_i,P_j]=i\hbar\,m\,\delta_{ij}\,\mathbb 1,

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Inputs and operationsihbarmdelta_ijmathbb 1
Result or condition[K_i,P_j]
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

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.

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KiK_i

Symbol K_i

KiK_i is part of the quantity the equation computes from the expression on the right.

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PjP_j

Symbol P_j

PjP_j is part of the quantity the equation computes from the expression on the right.

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ii

Symbol i

i is part of the quantity the equation computes from the expression on the right.

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mm

Symbol m

the mass.

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δij\delta_{ij}

Symbol delta_ij

deltaia_ij is an input to the expression that computes the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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subscript

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.

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How to interpret it

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What the article says around this equation

They do not commute. The defining fact of the nonrelativistic symmetry group, established by Bargmann and sharpened by Lévy-Leblond, is that its faithful quantum representations require a centrally extended algebra in which [Ki,Pj]=iℏ m δij 1[K_i,P_j]=i\hbar\,m\,\delta_{ij}\,\mathbb 1. with mass m appearing not as an eigenvalue to be measured state by state but as a fixed number multiplying the identity operator across an entire representation [ 1 , 2 ] . This is what “central” means: the commutator commutes with everything, including K\mathbf K and P\mathbf P themselves.

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