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Equation 3 · More Is Different: Emergence and Phase Transitions

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Rb:{K}⟶{K′}\mathcal{R}_b : \{K\} \longrightarrow \{K'\}

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Rb\mathcal{R}_b

Symbol R_b

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KK

Symbol K

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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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Take a system described by a set of couplings, coarse-grain it by integrating out the shortest-wavelength degrees of freedom, then rescale lengths so the cutoff returns to its original value. The result is a system of the same form with different couplings. Iterating defines a flow on the space of all possible Hamiltonians: Rb:{K}⟶{K′}\mathcal{R}_b : \{K\} \longrightarrow \{K'\}. A critical point corresponds to a fixed point of this flow, a Hamiltonian that maps to itself, which is exactly the scale-invariance the diverging correlation length demanded. Linearising the map about the fixed point,

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