Superconductivity through Quantum Critical Fluctuations in the ...

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Correlation function in the Quantum critical RegionVortices are confined; they do not contribute to the dynamics.Above the critical value , the “warps” proliferate and disorder theVelocity field. The correlation functions can be calculated exactly.Correlation function of the Order Parameter atPhysical Reason: Interactions of topological defects (warps)is spatially local and logarithmic in time.
Theory of the Loop OrderPhysics beyond the Hubbard ModelThree-Orbital Model with on-site and nearest neighbor Interactions.oocuUse Operator identity:Vn i n j = V/2 |J ij | 2 + n i + n j ).J ij = ic + i c j + H.C. ⇥ current operator in the link (i j)SupposeV2 < J ij >= x ij .Then effective kinetic energy parameter on the link (i j) ist ij + ix ij = |˜t ij |e ia ij.This is equivalent to a vector potentiala ijon the link (i j).
Page 1 and 2: Superconductivity through Quantum C
Page 3 and 4: Universal Phase DiagramTAntiferroma
Page 5 and 6: Fermi-Arc Phenomena:A New paradigm
Page 7 and 8: Any theoretical ideas and calculati
Page 10 and 11: Effect of Fluctuations on Single-pa
Page 12 and 13: If there is a region of Quantum-cri
Page 14 and 15: s but simply characterized temperat
Page 16 and 17: For quantum-fluctuations in the dis
Page 18 and 19: Fluctuations of the pseudogap order
Page 20 and 21: Superconductivity through Quantum C
Page 22 and 23: angle independence of the Eliashber
Page 24 and 25: Pairing VertexScattering through π
Page 26 and 27: Deducing the Fluctuation Spectra Co
Page 28 and 29: dI/dV ⇥ SdI/dV ⇥ N( )2 F (⇥)
Page 30 and 31: High Resolution Laser ARPES data. Z
Page 32 and 33: The Eliashberg functionAnalysis on
Page 34 and 35: How could one imagine superconducti
Page 36 and 37: TQuantum-critical fluctuationsof th
Page 38 and 39: Quantum Critical Fluctuations(Vivek
Page 40 and 41: t finite temperature where the corr
Page 42 and 43: ppose we separate m into the usual
Page 46: Definitive Evidence that there is a

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