coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the major radius on the grid (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/r_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/r_fourier(:,:)"

type = "dynamic"

units = "m"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the Height on the grid (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/z_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/z_fourier(:,:)"

type = "dynamic"

units = "m"

cocos_label_transformation = "psi_like"

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cocos_transformation_expression = ".fact_psi"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the poloidal flux at the grid in the poloidal plane (when relevant for the chosen grid). The poloidal flux is integral of magnetic field passing through a contour defined by the intersection of a flux surface passing through the point of interest and a Z=constant plane. If the integration surface is flat, the surface normal vector is in the increasing vertical coordinate direction, Z, namely upwards."

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/psi_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/psi_fourier(:,:)"

type = "dynamic"

units = "Wb"

cocos_label_transformation = "pol_angle_like"

cocos_leaf_name_aos_indices = "equilibrium.time_slice{i}.profiles_2d{j}.theta_fourier"

cocos_transformation_expression = ".fact_dtheta"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of poloidal angle on the grid (when relevant for the chosen grid). The poloidal angle is centered on the magnetic axis and oriented such that (grad rho_tor_norm, grad theta, grad phi) form a right-handed set where grad rho_tor_norm points away from the magnetic axis."

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/theta_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/theta_fourier(:,:)"

type = "dynamic"

units = "rad"

cocos_label_transformation = "b0_like"

cocos_leaf_name_aos_indices = "equilibrium.time_slice{i}.profiles_2d{j}.phi_fourier"

cocos_transformation_expression = ".sigma_b0_eff"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the toroidal flux (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/phi_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/phi_fourier(:,:)"

type = "dynamic"

units = "Wb"

cocos_label_transformation = "ip_like"

cocos_leaf_name_aos_indices = "equilibrium.time_slice{i}.profiles_2d{j}.j_phi_fourier"

cocos_transformation_expression = ".sigma_ip_eff"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the toroidal plasma current density (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/j_phi_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/j_phi_fourier(:,:)"

type = "dynamic"

units = "A.m^-2"

cocos_label_transformation = "ip_like"

cocos_leaf_name_aos_indices = "equilibrium.time_slice{i}.profiles_2d{j}.j_parallel_fourier"

cocos_transformation_expression = ".sigma_ip_eff"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the quantity defined as (j.B)/B0 where j and B are the current density and magnetic field vectors and B0 is the (signed) vacuum toroidal magnetic field strength at the geometric reference point (R0,Z0). It is formally not the component of the plasma current density parallel to the magnetic field"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/j_parallel_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/j_parallel_fourier(:,:)"

type = "dynamic"

units = "A.m^-2"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the R component of the poloidal magnetic field (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/b_field_r_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/b_field_r_fourier(:,:)"

type = "dynamic"

units = "T"

cocos_label_transformation = "b0_like"

cocos_leaf_name_aos_indices = "equilibrium.time_slice{i}.profiles_2d{j}.b_field_phi_fourier"

cocos_transformation_expression = ".sigma_b0_eff"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the toroidal component of the magnetic field (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/b_field_phi_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/b_field_phi_fourier(:,:)"

type = "dynamic"

units = "T"

coordinate1 = "time_slice(itime)/profiles_2d(i1)/grid/dim1"

coordinate2 = "time_slice(itime)/profiles_2d(i1)/grid/dim2"

data_type = "CPX_2D"

documentation = "Fourier components of the Z component of the magnetic field (when relevant for the chosen grid)"

introduced_with_version = "4.2.0"

path = "time_slice/profiles_2d/b_field_z_fourier"

path_doc = "time_slice(itime)/profiles_2d(i1)/b_field_z_fourier(:,:)"

type = "dynamic"

units = "T"