Here α = 1, 2 labels the top and bottom layer within a bi- layer labeled by j, and r is the in-plane coordinate

We need to assume that at equilibrium, a local pairing amplitude exists so that a phase of the local pairing order parameter, ∆α,j(r) = | ∆α,j(r) | eiϕα,j (r), is defined

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Parametrically amplified Josephson plasma waves in YBa_2Cu_3O_(6+x): evidence for local superconducting fluctuations up to the pseudogap temperature $T^*$

cond-mat.supr-con · 2025-05-06 · conditional · novelty 6.0

Local pairing amplitude with short-range phase coherence exists in the pseudogap phase of YBCO up to T*, enabling parametric amplification of Josephson plasma waves via a Floquet framework.

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Parametrically amplified Josephson plasma waves in YBa_2Cu_3O_(6+x): evidence for local superconducting fluctuations up to the pseudogap temperature $T^*$ cond-mat.supr-con · 2025-05-06 · conditional · none · ref 1
Local pairing amplitude with short-range phase coherence exists in the pseudogap phase of YBCO up to T*, enabling parametric amplification of Josephson plasma waves via a Floquet framework.

Here α = 1, 2 labels the top and bottom layer within a bi- layer labeled by j, and r is the in-plane coordinate

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