add explanatory text for the "other" simulation parameters
- also include link to Eckstein's book
This commit is contained in:
+110
-13
@@ -134,61 +134,142 @@
|
||||
<div id="Other" class="tabcontent">
|
||||
<table cellpadding="5">
|
||||
<tr>
|
||||
<td>EF</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>EF</summary>
|
||||
Cutoff energy of projectiles (in eV);<br>
|
||||
must be greater than zero.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parEF" id="parEF" type="number" size="7" step="0.1" value="0.5">
|
||||
</td>
|
||||
<td>KK0</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>KK0</summary>
|
||||
Maximum order of weak (simultaneous) collisions between projectiles and target atoms;<br>
|
||||
must be between 0 and 4 (0 means no weak collisions included).
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parKK0" id="parKK0" type="number" step="1" min="0" max="4" value="2">
|
||||
</td>
|
||||
</tr>
|
||||
<tr>
|
||||
<td>ESB</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>ESB</summary>
|
||||
Surface binding energy for projectiles (in eV).
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parESB" id="parESB" type="number" size="7" step="0.1" value="0.0">
|
||||
</td>
|
||||
<td>KK0R</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>KK0R</summary>
|
||||
Maximum order of weak (simultaneous) collisions between target atoms;<br>
|
||||
must be between 0 and 4 (0 means no weak collisions included).
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parKK0R" id="parKK0R" type="number" step="1" min="0" max="4" value="2">
|
||||
</td>
|
||||
</tr>
|
||||
<tr>
|
||||
<td>SHEATH</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>SHEATH</summary>
|
||||
Sheath potential (in eV); typically 3 * kT (i.e., 3 * |projectile energy|).
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parSHEATH" id="parSHEATH" type="number" size="7" step="0.1" value="0.0">
|
||||
</td>
|
||||
<td>KDEE1</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>KDEE1</summary>
|
||||
Inelastic energy loss model for projectiles:<br>
|
||||
1 = nonlocal (Lindhard-Scharff);<br>
|
||||
2 = local (Oen-Robinson);<br>
|
||||
3 = equipartition of 1 & 2;<br>
|
||||
4 = nonlocal (Anderson-Ziegler tables for hydrogen);<br>
|
||||
5 = nonlocal (Ziegler tables for helium).
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parKDEE1" id="parKDEE1" type="number" step="1" min="1" max="5" value="4">
|
||||
</td>
|
||||
</tr>
|
||||
<tr>
|
||||
<td>ERC</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>ERC</summary>
|
||||
Recoil cutoff energy (in eV);<br>
|
||||
usually equal to the surface binding energy.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parERC" id="parERC" type="number" size="7" step="0.1" value="0.0">
|
||||
</td>
|
||||
<td>KDEE2</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>KDEE2</summary>
|
||||
Inelastic energy loss for target atoms:<br>
|
||||
1 = nonlocal (Lindhard-Scharff);<br>
|
||||
2 = local (Oen-Robinson);<br>
|
||||
3 = equipartition of 1 and 2.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parKDEE2" id="parKDEE2" type="number" step="1" min="1" max="3" value="3">
|
||||
</td>
|
||||
</tr>
|
||||
<tr>
|
||||
<td>RD</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>RD</summary>
|
||||
Depth (in Å) to which recoils are followed.<br>
|
||||
RD = 50 is usually sufficient for sputtering<br>
|
||||
(if the projectile energy is not too high).<br>
|
||||
Use RD = 100 * CW (i.e., the depth increment) for following the full cascade.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parRD" id="parRD" type="number" size="7" step="0.1" value="50.0">
|
||||
</td>
|
||||
<td>IPOT</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>IPOT</summary>
|
||||
Interaction potential between projectiles and target atoms:<br>
|
||||
1 = krypton-carbon (Kr-C) potential;<br>
|
||||
2 = Molière potential;<br>
|
||||
3 = Ziegler-Biersack-Littmark (ZBL) potential.</details></td>
|
||||
<td>
|
||||
<input name="parIPOT" id="parIPOT" type="number" step="1" min="1" max="3" value="2">
|
||||
</td>
|
||||
</tr>
|
||||
<tr>
|
||||
<td>CA</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>CA</summary>
|
||||
Correction factor to the Firsov screening length for collisions between projectile and target atoms<br>
|
||||
(only for application of the Molière potential);<br>
|
||||
usually on the order of ~1.0.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parCA" id="parCA" type="number" size="7" step="0.1" value="1.0">
|
||||
</td>
|
||||
<td>IPOTR</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>IPOTR</summary>
|
||||
Interaction potential between target atoms:<br>
|
||||
1 = krypton-carbon (Kr-C) potential;<br>
|
||||
2 = Molière potential;<br>
|
||||
3 = Ziegler-Biersack-Littmark (ZBL) potential.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parIPOTR" id="parIPOTR" type="number" step="1" min="0" max="3" value="1">
|
||||
</td>
|
||||
@@ -196,12 +277,28 @@
|
||||
<tr>
|
||||
<td></td>
|
||||
<td></td>
|
||||
<td>IRL</td>
|
||||
<td>
|
||||
<details>
|
||||
<summary>IRL</summary>
|
||||
0 = no recoils are generated (i.e., no sputtering effects);<br>
|
||||
used to speed up the calculation if only projectile ranges are of interest.
|
||||
</details>
|
||||
</td>
|
||||
<td>
|
||||
<input name="parIRL" id="parIRL" type="number" step="1" min="0" max="2" value="0">
|
||||
</td>
|
||||
</tr>
|
||||
</table>
|
||||
<p>
|
||||
For further details see:
|
||||
</p>
|
||||
<p>
|
||||
W. Eckstein, <i>Computer Simulation of Ion-Solid Interactions</i>,<br>
|
||||
Springer Series in Materials Science, Vol. 10 (Springer-Verlag, Berlin, 1991).<br>
|
||||
<a href="https://doi.org/10.1007/978-3-642-73513-4">
|
||||
https://doi.org/10.1007/978-3-642-73513-4
|
||||
</a>
|
||||
</p>
|
||||
</div>
|
||||
</div>
|
||||
</td></tr>
|
||||
|
||||
Reference in New Issue
Block a user