## Description of the Calculator

### This program provides range, initial kinetic energy, final kinetic energy, or linear energy transfer for a specified projectile-target combination. The interface is task-driven, which the user can select from the drop-down menu below.

Range — See the Notes section for details on how the program calculates this. Returns range in g/cm^{2}.

Initial Kinetic Energy — This task obtains the initial kinetic energy of the projectile by first finding the placement of `depth`

within the range table `trange(abs,i)`

, then interpolating these neighboring values in terms of the energy table `tenerg(i)`

. Returns initial kinetic energy in MeV/n.

Final Kinetic Energy — This task integrates $\mathrm{d} E/\mathrm{d} x$ to find the change in kinetic energy, with the initial kinetic energy pointed to by `second`

(in MeV/n), and the target thickness (depth) pointed to by `third`

(in g/cm^{2}). Returns final kinetic energy in MeV/n.

Linear Energy Transfer — This task is a straight evaluation of $\mathrm{d} E/\mathrm{d} x$, including any stopping power corrections the user chooses. Here `second`

has the same meaning as in the $\text{KE}_f$ task, but `third`

now acts as a switch for Restricted Energy Loss (REL). Returns LET in keV/$\mu$m.

You can download a write-up of stopping power theory here [PDF].

### These are the stopping power corrections available. The defaults, marked in red, are appropriate for most situations.

FD // The density effect correction $\delta/2$ accounts for the phenomenon that, in a dense medium, the field which perturbs electrons far from the projectile track is modified by the dielectric polarization of the atoms between the distant electrons and the projectile. This correction is required.

FE // The correction due to electron capture accounts for the fact that the bare nuclear charge of the projectile $Z_0$ is reduced and can thus be replaced by the effective projectile charge $Z_1$.

FSH // The shell correction arises when the velocity of the projectile is comparable to the velocities of the electrons in the target atoms. Why? The Bethe-Bloch stopping power formula is derived on the assumption that the velocity of the incident particle is large compared to the velocities of the atomic electrons with which it interacts. When this condition is not satisfied, shell corrections are needed which are available for heavy particles but not for electrons.

FLE // The Leung, or relativistic shell correction, is a small effect which is due to relativistic inner shell electrons in very heavy targets. See P.T. Leung, Phys. Rev. A 40, 5417 (1989) and P.T. Leung, Phys. Rev. A 60, 2562 (1999) for details.

FKIN // The kinematic correction $f_\text{FKIN}$ accounts for the finite mass of the nucleus in electron-projectile collisions. This is an estimate of the ultrarelativistic kinematic correction from S.P. Ahlen, Rev. Mod. Phys. 52, 121 (1980). It is a correction to the finite mass (as opposed to size) of the nucleus in relativistic electron-nucleus collisions.

FRAD // This is the radiative correction $f_\text{FRAD}$ discussed in S.P. Ahlen, Rev. Mod. Phys. 52, 121 (1980). It arises from bremsstrahlung of scattered electrons in ultrarelativistic collisions. The form here is that of V.Z. Jankus, Phys. Rev. 90, 4 (1953). The parameter $Q$ from that paper is here equal to the geometric mean between the electron rest energy and $2 m_\text{e} c^2 \gamma$.

FLS // The Lindhard-Sørensen (LS) correction $f_\text{FLS}$ replaces the Bloch-Mott-Ahlen group. In their paper Lindhard and Sørensen show that the low-energy limit of the LS correction is exactly the Bloch correction. Furthermore, by using exact solutions to the Dirac equation, the LS correction automatically incorporates Mott scattering and is relativistically correct.

FNS // In their paper Lindhard and Sørensen also derive a correction due to the finite size of atomic nuclei. This is possible because exact solutions to the Dirac equation exist for any spherically symmetric potential.

FBA // The factor $f_\text{FBA}$ takes into account target polarization effects for low-energy distant electronic collisions that produce a multiplicative correction to the energy loss.

FBR // This correction $f_\text{FBR}$ accounts for bremsstrahlung emitted directly from the projectile in the effective field of the target nuclei.