Supplementary information

From the following article:

How Cooper pairs vanish approaching the Mott insulator in Bi2Sr2CaCu2O8+delta

Y. Kohsaka, C. Taylor, P. Wahl, A. Schmidt, Jhinhwan Lee, K. Fujita, J. W. Alldredge, K. McElroy, Jinho Lee, H. Eisaki, S. Uchida, D.-H. Lee & J. C. Davis

Nature 454, 1072-1078(28 August 2008)

doi:10.1038/nature07243

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Supplementary Information

This file contains Supplementary Methods; Supplementary Tables S1-S4; Supplementary Discussion; additional references and Supplementary Figures S1-S7 with Legends.
This file includes the detailed methods used to extract quasiparticle momentum space properties from the Fourier transform of real space data. It includes tables of the doping dependence of various extracted parameters as well as a discussion of the impact of the doping dependence of the Bogoliubov arc end points on non-dispersive wavevectors. This Supplementary Figures illustrate the doping dependence of the properties depicted in the main text figures.

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Supplementary Video 1

This movie shows the Fourier transform of the real space conductance ratio maps for the TC = 88K sample of Bi2Sr2CaCu2O8+delta. It demonstrates strongly dispersing wave vectors at low bias voltages and non-dispersive wave vectors at high bias voltages.

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Supplementary Video 2

This movie shows the Fourier transform of the real space conductance ratio maps for the TC = 74K sample of Bi2Sr2CaCu2O8+delta. It demonstrates strongly dispersing wave vectors at low bias voltages and non-dispersive wave vectors at high bias voltages.

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Supplementary Video 3

This movie shows the Fourier transform of the real space conductance ratio maps for the TC = 45K sample of Bi2Sr2Ca0.8Dy0.2Cu2O8+delta. It demonstrates strongly dispersing wave vectors at low bias voltages and non-dispersive wave vectors at high bias voltages

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Supplementary Video 4

This movie shows shoes the Fourier transform of the real space conductance ratio maps for the TC = 20K sample of Bi2Sr2Ca0.8Dy0.2Cu2O8+delta. It demonstrates strongly dispersing wave vectors at low bias voltages and non-dispersive wave vectors at high bias voltages.

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