Figure 1.
Diagonal upper level –matrix elements as a function of time for a single (the same) plasma microfield realization, with and without a magnetic field. The only effect of the magnetic field is assumed to be the linear Zeeman splitting. It is seen that the addition of the magnetic field results in a slower drop of the U-matrix elements.
Figure 1.
Diagonal upper level –matrix elements as a function of time for a single (the same) plasma microfield realization, with and without a magnetic field. The only effect of the magnetic field is assumed to be the linear Zeeman splitting. It is seen that the addition of the magnetic field results in a slower drop of the U-matrix elements.
Figure 2.
calculation with the full plasma microfield (solid) and only its z-component (dashed). The only effect of the magnetic field is assumed to be the linear Zeeman splitting. It is clear that the nonadiabatic component is only a minor correction. Both the and components are shown.
Figure 2.
calculation with the full plasma microfield (solid) and only its z-component (dashed). The only effect of the magnetic field is assumed to be the linear Zeeman splitting. It is clear that the nonadiabatic component is only a minor correction. Both the and components are shown.
Figure 3.
component of the calculation with the full plasma microfield (solid) and only its z-component (dashed). Spiralling trajectories are still not allowed, but the Zeeman effect is included to all orders.
Figure 3.
component of the calculation with the full plasma microfield (solid) and only its z-component (dashed). Spiralling trajectories are still not allowed, but the Zeeman effect is included to all orders.
Figure 4.
component of the calculation with the full plasma microfield (solid) and only its z-component (dashed). Spiralling trajectories are still not allowed, but the Zeeman effect is included to all orders.
Figure 4.
component of the calculation with the full plasma microfield (solid) and only its z-component (dashed). Spiralling trajectories are still not allowed, but the Zeeman effect is included to all orders.
Figure 5.
calculation at , eV for (a) shielded electron and ions at B = 500 T (dashed), (b) unshielded electrons and ions at B = 500 T (dotted), and (c) shielded electrons and ions, but no spiralling (solid).
Figure 5.
calculation at , eV for (a) shielded electron and ions at B = 500 T (dashed), (b) unshielded electrons and ions at B = 500 T (dotted), and (c) shielded electrons and ions, but no spiralling (solid).
Figure 6.
calculation at , eV, and no magnetic field. Shown are the profiles under the joint action of electrons and ions (solid) and with electron perturbers only (dashed). It is clear that the ion contribution is substantial or even dominant for B = 0.
Figure 6.
calculation at , eV, and no magnetic field. Shown are the profiles under the joint action of electrons and ions (solid) and with electron perturbers only (dashed). It is clear that the ion contribution is substantial or even dominant for B = 0.
Figure 7.
Sample –component of , where is the random ion microfield in the x direction (solid) and (dotted) with the Zeeman splitting.
Figure 7.
Sample –component of , where is the random ion microfield in the x direction (solid) and (dotted) with the Zeeman splitting.
Figure 8.
Four components of the line under a magnetic field of 2000 T with strong magnetic field effects accounted for, but spiralling not accounted for. The dashed line is the B = 0 autocorrelation function. Three of these components (solid) display a sawtooth-like oscillatory behaviour, while the other one does not (dotted).
Figure 8.
Four components of the line under a magnetic field of 2000 T with strong magnetic field effects accounted for, but spiralling not accounted for. The dashed line is the B = 0 autocorrelation function. Three of these components (solid) display a sawtooth-like oscillatory behaviour, while the other one does not (dotted).
Figure 9.
Sample component of , with as the random electron microfield in the x direction (solid) and (dotted).
Figure 9.
Sample component of , with as the random electron microfield in the x direction (solid) and (dotted).
Figure 10.
profiles for B = 2000 T without spiralling, but strong B effects accounted for. Shown are the calculations with electrons and ions (solid), only the adiabatic component of electrons and ions (dashed), only electrons (dotted), and only the adiabatic component of electrons (dash-dotted).
Figure 10.
profiles for B = 2000 T without spiralling, but strong B effects accounted for. Shown are the calculations with electrons and ions (solid), only the adiabatic component of electrons and ions (dashed), only electrons (dotted), and only the adiabatic component of electrons (dash-dotted).
Figure 11.
profiles for B = 2000 T without spiralling, but strong B effects accounted for. Shown are the calculations with electrons and ions (solid), only the adiabatic component of electrons and ions (dashed), only electrons (dotted), and only the adiabatic component of electrons (dash-dotted).
Figure 11.
profiles for B = 2000 T without spiralling, but strong B effects accounted for. Shown are the calculations with electrons and ions (solid), only the adiabatic component of electrons and ions (dashed), only electrons (dotted), and only the adiabatic component of electrons (dash-dotted).
Figure 12.
Typical case for ions, where , so that impact parameters in () contribute, and even these contribute only partially.
Figure 12.
Typical case for ions, where , so that impact parameters in () contribute, and even these contribute only partially.
Figure 13.
and line profiles for the line with and without spiralling and without the strong B term for B = 300 T.
Figure 13.
and line profiles for the line with and without spiralling and without the strong B term for B = 300 T.
Figure 14.
and line profiles for the line with and without spiralling and without the strong B term for B = 500 T.
Figure 14.
and line profiles for the line with and without spiralling and without the strong B term for B = 500 T.
Figure 15.
and line profiles for the line with and without spiralling and without the strong B term for B = 2000 T.
Figure 15.
and line profiles for the line with and without spiralling and without the strong B term for B = 2000 T.
Figure 16.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 16.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 17.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 17.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 18.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 18.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 19.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 19.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 20.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 20.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 21.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 21.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 22.
Comparison of spiralling calculations for with and without the account of the strong B-term for B = 300 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 22.
Comparison of spiralling calculations for with and without the account of the strong B-term for B = 300 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 23.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 500 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 23.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 500 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 24.
Comparison of spiralling calculations for with and without the account of the strong B-term for B = 2000 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 24.
Comparison of spiralling calculations for with and without the account of the strong B-term for B = 2000 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 25.
and line profiles for the line with and without spiralling and without the strong B term for B = 300 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 25.
and line profiles for the line with and without spiralling and without the strong B term for B = 300 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 26.
and line profiles for the line with and without spiralling and without the strong B term for B = 500 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 26.
and line profiles for the line with and without spiralling and without the strong B term for B = 500 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 27.
and line profiles for the line with and without spiralling and without the strong B term for B = 2000 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dash-dotted) and (dotted) directions, and by spiralling electrons and ions in the (solid) and (dashed) directions.
Figure 27.
and line profiles for the line with and without spiralling and without the strong B term for B = 2000 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dash-dotted) and (dotted) directions, and by spiralling electrons and ions in the (solid) and (dashed) directions.
Figure 28.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 28.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 29.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 29.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 30.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 30.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 31.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 31.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 32.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 32.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 33.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 33.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 34.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 300 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 34.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 300 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 35.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 500 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 35.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 500 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 36.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 2000 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 36.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 2000 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 37.
and line profiles for the line with and without spiralling and without the strong B term for B = 300 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 37.
and line profiles for the line with and without spiralling and without the strong B term for B = 300 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 38.
and line profiles for the line with and without spiralling and without the strong B term for B = 500 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 38.
and line profiles for the line with and without spiralling and without the strong B term for B = 500 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 39.
and line profiles for the line with and without spiralling and without the strong B term for B = 2000 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 39.
and line profiles for the line with and without spiralling and without the strong B term for B = 2000 T. Shown are the profiles broadened by nonspiralling electrons and ions for the (dashed) and (dash-dotted) directions, and by spiralling electrons and ions in the (solid) and (dotted) directions.
Figure 40.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 40.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 41.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 41.
Comparison of the profiles with and without spiralling for B = 300 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 42.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 42.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 43.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 43.
Comparison of the profiles with and without spiralling for B = 500 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 44.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 44.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 45.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 45.
Comparison of the profiles with and without spiralling for B = 2000 T. The strong B term is neglected. Shown are the profiles broadened by nonspiralling electrons and ions (solid), nonspiralling electrons only (dotted), spiralling electrons and ions (dashed), and spiralling electrons only (dash-dotted).
Figure 46.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 300 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 46.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 300 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 47.
Comparison of spiralling calculations for with and without the account of the strong B-term for B = 500 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 47.
Comparison of spiralling calculations for with and without the account of the strong B-term for B = 500 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 48.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 2000 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 48.
Comparison of spiralling calculations for with and without account of the strong B-term for B = 2000 T. Shown are the profiles with the account of the strong B-term for the (dashed) and (solid) components and without the account of the strong B-term for the (dotted) and (dash-dotted) components.
Figure 49.
autocorrelation functions for B = 0, 300, 500 T (solid), and 2000 T. For the 0, 300, and 500 T, the and components practically coincide. For B = 2000 T, the (dotted) and (dashed) components differ and are shown as such.
Figure 49.
autocorrelation functions for B = 0, 300, 500 T (solid), and 2000 T. For the 0, 300, and 500 T, the and components practically coincide. For B = 2000 T, the (dotted) and (dashed) components differ and are shown as such.
Table 1.
Number of perturbers required for with T = 4 ps.
Table 1.
Number of perturbers required for with T = 4 ps.
B | Model | Electrons | Ions | | | | | | |
---|
300 | NS | 4827 | 242 | 0.225 | 6.82 | | | | |
300 | S | 3033 | 272 | 0.225 | 6.82 | | | | |
500 | NS | 4827 | 242 | 0.135 | 4.1 | | | | |
500 | S | 2631 | 285 | 0.135 | 4.1 | | | | |
2000 | NS | 4827 | 242 | 0.03 | 1.02 | | | | |
2000 | S | 2219 | 464 | 0.03 | 0.9078 | | | | |
Table 2.
Number of perturbers required for with T = 3.5 ps.
Table 2.
Number of perturbers required for with T = 3.5 ps.
B () | Model | Electrons | Ions | | | | | | |
---|
300 | NS | 3764 | 225 | 0.225 | 6.83 | 1.17 | 0.0332 | 3.865 | 3.32 |
300 | S | 2654 | 248 | 0.225 | 6.83 | 0.85 | | 3.56 | 4.37 |
500 | NSg | 3764 | 225 | 0.135 | 4.1 | 1.17 | 0.0332 | 3.865 | 3.32 |
500 | S | 2302 | 260 | 0.135 | 4.1 | 0.737 | | 3.72 | 4.6 |
2000 | NS | 3764 | 225 | 0.0338 | 1.02 | 1.17 | 0.0332 | 3.865 | 3.32 |
2000 | S | 1942 | 430 | 0.0338 | 1.02 | 0.62 | | 5.51 | 8.23 |
Table 3.
Number of perturbers required for with T = 0.7 ps.
Table 3.
Number of perturbers required for with T = 0.7 ps.
B () | Model | Electrons | Ions | | | | | | |
---|
300 | NS | 836 | 128 | 0.225 | 6.83 | | | 0.773 | |
300 | S | 531 | 151 | 0.225 | 6.83 | 0.17 | | | |
500 | NS | 836 | 128 | 0.135 | 4.1 | | | 0.773 | |
500 | S | 460 | 159 | 0.135 | 4.1 | | | 0.49 | 4.59 |
2000 | NS | 836 | 128 | 0.0338 | 1.02 | | | 0.773 | 3.32 |
2000 | S | 388 | 265 | 0.0338 | 1.02 | | | 0.868 | 7.6 |