diff --git a/TrimSP.html b/TrimSP.html index ee9964d..ba6d600 100644 --- a/TrimSP.html +++ b/TrimSP.html @@ -134,61 +134,142 @@
| EF | +
+
+
+ EF+ Cutoff energy of projectiles (in eV);+ must be greater than zero. + |
- | KK0 | +
+
+
+ KK0+ Maximum order of weak (simultaneous) collisions between projectiles and target atoms;+ must be between 0 and 4 (0 means no weak collisions included). + |
|
| ESB | +
+
+
+ ESB+ Surface binding energy for projectiles (in eV). + |
- | KK0R | +
+
+
+ KK0R+ Maximum order of weak (simultaneous) collisions between target atoms;+ must be between 0 and 4 (0 means no weak collisions included). + |
|
| SHEATH | +
+
+
+ SHEATH+ Sheath potential (in eV); typically 3 * kT (i.e., 3 * |projectile energy|). + |
- | KDEE1 | +
+
+
+ KDEE1+ Inelastic energy loss model for projectiles:+ 1 = nonlocal (Lindhard-Scharff); + 2 = local (Oen-Robinson); + 3 = equipartition of 1 & 2; + 4 = nonlocal (Anderson-Ziegler tables for hydrogen); + 5 = nonlocal (Ziegler tables for helium). + |
|
| ERC | +
+
+
+ ERC+ Recoil cutoff energy (in eV);+ usually equal to the surface binding energy. + |
- | KDEE2 | +
+
+
+ KDEE2+ Inelastic energy loss for target atoms:+ 1 = nonlocal (Lindhard-Scharff); + 2 = local (Oen-Robinson); + 3 = equipartition of 1 and 2. + |
|
| RD | +
+
+
+ RD+ Depth (in Å) to which recoils are followed.+ RD = 50 is usually sufficient for sputtering + (if the projectile energy is not too high). + Use RD = 100 * CW (i.e., the depth increment) for following the full cascade. + |
- | IPOT | +
+
+ IPOT+ Interaction potential between projectiles and target atoms:+ 1 = krypton-carbon (Kr-C) potential; + 2 = Molière potential; + 3 = Ziegler-Biersack-Littmark (ZBL) potential. |
|
| CA | +
+
+
+ CA+ Correction factor to the Firsov screening length for collisions between projectile and target atoms+ (only for application of the Molière potential); + usually on the order of ~1.0. + |
- | IPOTR | +
+
+
+ IPOTR+ Interaction potential between target atoms:+ 1 = krypton-carbon (Kr-C) potential; + 2 = Molière potential; + 3 = Ziegler-Biersack-Littmark (ZBL) potential. + |
@@ -196,12 +277,28 @@ |
| - | IRL | +
+
+
+ IRL+ 0 = no recoils are generated (i.e., no sputtering effects);+ used to speed up the calculation if only projectile ranges are of interest. + |
+ For further details see: +
+
+ W. Eckstein, Computer Simulation of Ion-Solid Interactions,
+ Springer Series in Materials Science, Vol. 10 (Springer-Verlag, Berlin, 1991).
+
+ https://doi.org/10.1007/978-3-642-73513-4
+
+