#' Examples of results for j0j0 for a sweep of frequency, directions and a
#' number of different velocity distributions:
#'
#' * maxwellian
#' * bimaxwellian
#' * lorentzian
#' * ring
#' * bvtnorm
#' * slowdown_b0
#' * slowdown_b5
#'
#'
#' @format A tibble with 12642 rows and 10 variables:
#' \describe{
#' \item{k}{length of wave vector in 1/m}
#' \item{phi}{angle between wave vector and magnetic field in degrees}
#' \item{frequency }{in Hz}
#' \item{B}{Magnetic field strength in Tesla}
#' \item{particle}{particle name}
#' \item{integration_method}{name of integration method}
#' \item{directions}{string with direction names}
#' \item{A}{mass number}
#' \item{Z}{charge number}
#' \item{j0j0}{result for j0j0}
#' }
#'
#' @source File /data/raw/j0j0_examples
"j0j0_examples"
#' Examples of results for j0j0 for a sweep of frequency, directions and two
#' values of phi for a maxwellian distribution.
#'
#'
#' @format A tibble with 3618 rows and 10 variables:
#' \describe{
#' \item{k}{length of wave vector in 1/m}
#' \item{phi}{angle between wave vector and magnetic field in degrees}
#' \item{frequency }{in Hz}
#' \item{B}{Magnetic field strength in Tesla}
#' \item{particle}{particle name}
#' \item{integration_method}{name of integration method}
#' \item{directions}{string with direction names}
#' \item{A}{mass number}
#' \item{Z}{charge number}
#' \item{j0j0}{result for j0j0}
#' }
#'
#' @source File /data/raw/j0j0_examples
"maxwellian_example"
#' examples of results for j0j0 for a sweep of frequency and phi angle forthe
#' zz-component for three distributions:
#'
#' * maxwellian
#' * ring
#' * slowdown_b5
#'
#' @format A tibble with 12,642 rows and 10 variables:
#' \describe{
#' \item{k}{length of wave vector in 1/m}
#' \item{phi}{angle between wave vector and magnetic field in degrees}
#' \item{frequency }{in Hz}
#' \item{B}{Magnetic field strength in Tesla}
#' \item{particle}{particle name}
#' \item{integration_method}{name of integration method}
#' \item{directions}{string with direction names}
#' \item{A}{mass number}
#' \item{Z}{charge number}
#' \item{j0j0}{result for j0j0}
#' }
#'
#' @source File /data/raw/j0j0_examples
"phi_sweep"
#' Examples 1D velocity distributions at v_perp = 0
#'
#' * maxwellian
#' * ring
#' * slowdown_b5
#'
#' @format A data frame with 7000 rows and 8 variables:
#' \describe{
#' \item{name}{Distribution name}
#' \item{v_par}{Parallel velocity}
#' \item{v_perp}{Perpendiculer velocity}
#' \item{p_scale}{Momentum scale - used to scale momentum in integrals, so it is near 1}
#' \item{A}{mass number}
#' \item{p_par}{parallel momentum}
#' \item{p_perp}{perpendicular momentum}
#' \item{value}{momentum distribution value (i.e. density)}
#' }
#'
#' @source File /data/raw/j0j0_examples
"distribution_examples"
#' Examples of 2D velocity distributions with variation in both v_par and
#' v_perp for a number of velocity distributions:
#'
#' * maxwellian
#' * bimaxwellian
#' * lorentzian
#' * ring
#' * bvtnorm
#' * slowdown_b5
#' * slowdown_b0
#'
#' @format A data frame with 630000 rows and 8 variables:
#' \describe{
#' \item{name}{Distribution name}
#' \item{v_par}{Parallel velocity}
#' \item{v_perp}{Perpendiculer velocity}
#' \item{p_scale}{Momentum scale - used to scale momentum in integrals, so it is near 1}
#' \item{A}{mass number}
#' \item{p_par}{parallel momentum}
#' \item{p_perp}{perpendicular momentum}
#' \item{value}{momentum distribution value (i.e. density)}
#' }
#'
#' @source File /data/raw/j0j0_examples
"dist_2D_examples"
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