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Comparison of X-ray diffraction patterns of La 2 CuO 4+ from different crystals at room temperature Pia Jensen

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(h,k,0.00)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.05)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.10)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.15)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.20)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.25)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.30)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.35)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.40)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.45)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.50)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.55)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.60)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.65)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.70)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.75)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.80)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.85)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.90)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,0.95)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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(h,k,1.00)-layer LSCO_01_long LSCO_07_long LSCO_03_long

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