1. "Calculate Curves" Group

1.1 "Depth-dose curve" mode

• D_e(z) [energy deposition as a function of depth]
  or
  (r₀/E₀)D_e(z) [scaled energy deposition as a function of scaled depth; r₀ = continuous slowing-down approximation range of incident electrons]
• Additional results: r₀ , R_ex , R_av , z_av , h_N , h_E , D_e(0) , D_e^max and D_e(z_max)
  The last three parameters are also obtained in scaled quantities.

1.2 "Bremsstrahlung dose" mode

• D_eb(z) [energy-deposition distribution via bremsstrahlung]
  or
  (r₀/E₀)D_eb(z) [scaled energy-deposition distribution via bremsstrahlung]
• Additional results: r₀ , R_ex , R_av , z_av , h_N , h_E , D_eb(0) , D_eb^max and D_eb(z_max)
  The last three parameters are also obtained in scaled quantities.

1.3 "Depth-charge curve" mode

• D_cp(z) [charge-deposition distribution due to primary electrons]
  or
  r₀D_cp(z) [scaled charge-deposition distribution due to primary electrons]
• Additional results: r₀ , R_ex , R_av , z_av , h_N , h_E , D_cp(0) , D_cp^max and D_cp(z_max)
  The last three parameters are also obtained in scaled quantities.

1.4 "Transmission curve" mode

• k(x) [number-transmission ratio as a function of absorber thickness or as a function of scaled absorber thickness]
• Additional results: r₀ , R_ex and R_av

2.1 "Dose and charge" mode

• D_e(z) and D_cp(z) [see 1.1 and 1.3]
  or
  (r₀/E₀)D_e(z) and r₀D_cp(z)
• Additional results: r₀  , R_ex , h_N , h_E

2.2 "Dose components" mode

• D_eb(z) (see 1.2) and D_ec(z) [energy- deposition distribution via collision]
  or
  (r₀/E₀)D_eb(z) and (r₀/E₀)D_ec(z)
• Additional results: r₀  , R_ex , h_pE and h_E

2.3 "Transmission and reflection" mode

• h_N(E) [number-reflection ratio as a function of incident energy] and k(E) [number-transmission ratio as a function of incident energy]
• Additional results: r₀  , R_ex and R_av

2.4 "Energy-reflection ratios" mode

• h_E [energy-reflection ratio of electrons as a function of incident energy] and
  h_pE [energy-reflection ratio of photons as a function of incident energy]
  
• Additional results: h_E(E_min) , h_E(E_max) , h_pE^max , h_pE(E_min) and h_pE(E_min)

3.1 "Dose in elemental absorbers" mode

• D_e(z) or (r₀/E₀)D_e(z) [see 1.1]
  calculated by the algorithm is compared with the ITS Monte Carlo results for elemental absobers.

3.2 "Dose in non-elemental absorbers" mode

• The same comparison as above is made for light compounds and mixtures.

3.2 "Charge in elemental absorbers" mode

• D_cp(z) or r₀D_cp(z) [see 1.1]
  calculated by the formulla is compared with the ITS Monte Carlo results for elemental absobers.

• h_E: energy-reflection ratio of electrons
• h_pE: energy-reflection ratio of photons
• h_N: number-reflection ratio of electrons
• r₀: continuous slowing-down approximation range
• R_av: average reach, originally proposed as average depth of electron penetration
• R_ex: extrapolated range
• z_av: average penetration depth, also called projected range