This file explains all of the variables in each of the datasets that accompany: Smith AP et al. '3D Properties in (RE)BCO Tapes Measured in Fields up to 35T'

dataset: Figure 1.csv
r		=	Normalised interlayer coupling parameter (ratio of interlayer superelectron coupling energy to the temperature KbT)
T* - Klemm	=	Dimensional Crossover Temperature according to the Klemm model
T* - LD		=	Dimensional Crossover Temperature according to the Lawrence Doniach model

dataset: Figure 2.csv
These data correspond to measurements performed on a segment of Fujikura tape without artifical pinning centres

Temperature	=	Temperature in Kelvin
Bc2 0deg	=	Measured value of Bc2 from susceptibility data with B||c
Bc2 30deg	=	Measured value of Bc2 from susceptibility data with B at 30degrees to c
Bc2 60deg	=	Measured value of Bc2 from susceptibility data with B at 60degrees to c
Bc2 AGL 0deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B||c
Bc2 AGL 30deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B at 30degrees to c
Bc2 AGL 60deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B at 60degrees to c
Bc2 AGL 90deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B||ab
Bc2 Klemm 0deg	=	Fitted value of Bc2 using Klemm's theory with B||c
Bc2 Klemm 30deg	=	Fitted value of Bc2 using Klemm's theory with B at 30degrees to c
Bc2 Klemm 60deg	=	Fitted value of Bc2 using Klemm's theory with B at 60degrees to c
Bc2 Klemm 90deg	=	Fitted value of Bc2 using Klemm's theory with B||ab

dataset: Figure 3.csv
These data correspond to measurements performed on a segment of Superpower tape with artifical pinning centres

Temperature	=	Temperature in Kelvin
Bc2 0deg	=	Measured value of Bc2 from susceptibility data with B||c
Bc2 30deg	=	Measured value of Bc2 from susceptibility data with B at 30degrees to c
Bc2 60deg	=	Measured value of Bc2 from susceptibility data with B at 60degrees to c
Bc2 AGL 0deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B||c
Bc2 AGL 30deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B at 30degrees to c
Bc2 AGL 60deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B at 60degrees to c
Bc2 AGL 90deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B||ab
Bc2 Klemm 0deg	=	Fitted value of Bc2 using Klemm's theory with B||c
Bc2 Klemm 30deg	=	Fitted value of Bc2 using Klemm's theory with B at 30degrees to c
Bc2 Klemm 60deg	=	Fitted value of Bc2 using Klemm's theory with B at 60degrees to c
Bc2 Klemm 90deg	=	Fitted value of Bc2 using Klemm's theory with B||ab

dataset: Figure 4.csv
These data correspond to measurements performed on a segment of Superpower tape without artifical pinning centres

Temperature	=	Temperature in Kelvin
Bc2 0deg	=	Measured value of Bc2 from susceptibility data with B||c
Bc2 30deg	=	Measured value of Bc2 from susceptibility data with B at 30degrees to c
Bc2 60deg	=	Measured value of Bc2 from susceptibility data with B at 60degrees to c
Bc2 AGL 0deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B||c
Bc2 AGL 30deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B at 30degrees to c
Bc2 AGL 60deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B at 60degrees to c
Bc2 AGL 90deg	=	Fitted value of Bc2 using Anisotropic Ginzburg-Landau theory with B||ab
Bc2 Klemm 0deg	=	Fitted value of Bc2 using Klemm's theory with B||c
Bc2 Klemm 30deg	=	Fitted value of Bc2 using Klemm's theory with B at 30degrees to c
Bc2 Klemm 60deg	=	Fitted value of Bc2 using Klemm's theory with B at 60degrees to c
Bc2 Klemm 90deg	=	Fitted value of Bc2 using Klemm's theory with B||ab