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Numerical Simulation of an Atomic Cluster Explosion

The calculated time-history of a cluster of 5000 Xe atoms irradiated by a 200-fs, 780-nm laser pulse with a peak intensity of 1016 W cm-2 is illustrated in Fig. 1. The time-dependence of the nanoplasma parameters clearly shows field enhancement in the cluster, a resonance in the heating and an extremely rapid expansion (explosion) of the nanoplasma. The peak of the laser pulse is at t = 0 fs. At around t = -280 fs, when the intensity is ~4 x 1013 W cm-2, a small number of free electrons are created through tunnel ionization?. The electron density rises to reach 3ncrit at t = -270 fs [Fig. 1(c)]. At this point the field in the cluster is enhanced [Fig. 1(a)] and more electrons are liberated through tunnel, laser-driven and thermal ionization. The electron density is now higher than 3ncrit and the field inside the cluster is shielded from the external laser field. The tunnel and laser-driven ionization rates fall off, but electrons are still created through thermal collisions.

From t = -50 fs onwards, some electrons are able to leave the cluster, as the mean? electron temperature is in the region of 100–1000 eV and the escape energy is ~200–2000 eV. The combined effect of the free-streaming of electrons out of the cluster and the hydrodynamic expansion of the cluster is that the electron density starts to fall, after peaking at over 50ncrit. The field in the cluster again starts to rise as the electron density drops, so the tunnel and laser-driven ionization rates increase while the thermal collisional ionization rate falls. Near the peak of the laser pulse, at t = -12 fs, the electron density in the cluster drops to 3ncrit. The resonantly increased heating rate causes the electron temperature in the cluster to soar to 25 keV [Fig. 1(b)]. The field in the cluster is also strongly enhanced and the peak intensity in the cluster reaches 2 x 1016 W cm-2, twice the intensity outside. The electron free-streaming rate increases sharply as a significant number of electrons have energies above the then 4-keV escape energy.

The total charge on the cluster increases to 5.5 x 104e, resulting in the Coulomb pressure? increasing to 10 Mbar [Fig. 1(d)]. However, this is small compared to the hydrodynamic pressure? due to the hot electrons of 200 Mbar. This pressure causes a sharp increase in the cluster expansion velocity. This is the explosion of the cluster. Once the nanoplasma density has dropped to ≈1017 cm-3, the final expansion velocity of electrons and ions is 3.3 x 107 cm s-1, which corresponds to a maximum ion energy of ~80 keV. The final electron energy is much lower, only 30 eV, a consequence of their much lighter mass. However, electrons that free streamed away from the nanoplasma have energies in the 0.2–2 keV range. (underline added)

This simulation shows an extremely energetic laser–cluster interaction, with ion energies close to 100 keV and electron energies of several keV. We will see that these predictions are borne out in experiments.

Atomic Clusters Figure 1



See Also

3.14 - Vortex Theory of Atomic Motions
3.23 - Hydrodynamic Equations - Vortex Motions
5.8.5 - The complete Contraction Expansion Cycle is as follows
9.27 - Expansion and Contraction
13.04 - Atomic Subdivision
16.15 - Negative Electricity is Expansion
Atomic
Atomic Cluster Heating
Atomic Cluster Ionization
Atomic Cluster X-Ray Emission
Atomic Clusters
Atomic Force
atomic mass
atomic number
atomic theory
atomic triplet
atomic weight
diatomic
Egyptian fraction expansion
expansion
Figure 13.06 - Atomic Subdivision
Figure 14.10 - Proportionate Tonal Relations dictate Contraction or Expansion
Figure 3.28 - Compression and Expansion Forces in Gyroscopic Motions
Figure 9.10 - Phases of a Wave as series of Expansions and Contractions
Figure 9.5 - Phases of a Wave as series of Expansions and Contractions
Force-Atomic
Formation of Atomic Clusters
Hydrodynamic Expansion
InterAtomic
Ionization Energy
Laser Cluster Interactions
Law of Atomic Dissociation
Law of Atomic Pitch
Law of Oscillating Atomic Substances
Law of Pitch of Atomic Oscillation
Law of Variation of Atomic Oscillation by Electricity
Law of Variation of Atomic Oscillation by Sono-thermism
Law of Variation of Atomic Oscillation by Temperature
Law of Variation of Atomic Pitch by Electricity and Magnetism
Law of Variation of Atomic Pitch by Rad-energy
Law of Variation of Atomic Pitch by Temperature
Law of Variation of Pitch of Atomic Oscillation by Pressure
Models of Laser Cluster Interactions
monatomic
Nanoplasma
subatomic


Page last modified on Wednesday 05 of June, 2013 03:27:49 MDT

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