Data

The LisbOn KInetics (LoKI) Suite requires quality data to deliver useful predictions on the behaviour of low-temperature plasmas. Thus, the development of tools is accompanied by the consolidation of state-of-the-art kinetic schemes for various gases and gaseous mixtures.


The procedure involves:
(i) the critical assessment of data (electron scattering cross sections and heavy-species rate coefficients);
(ii) the validation of kinetic schemes, by comparing simulation results with experimental measurements (mainly obtained by optical and mass spectroscopy diagnostics) for the intensities of the main radiative line/band transitions and/or the densities of the main excited species in the plasma;
(iii) the public release of electron scattering cross sections for momentum-transfer, excitation to electronic / vibrational / rotational states, attachment and ionization, through the IST-Lisbon database on the open-access website LXCat (currently in the process of migration to the new LXCat 3.0 and the LXCat (future) databases);
(iv) the distribution / publication of the kinetic schemes and data as KInetic Testbeds (KITs) (to be hosted in the new ChemCat database).

The LoKI-Suite tools and data leverage the expertise in the field of non-equilibrium low-temperature plasmas accumulated over many years by the Portuguese group N-Plasmas Reactive: Modelling and Engineering (N-PRiME).

The current efforts focus on argon, helium, nitrogen, oxygen, hydrogen, carbon monoxide, carbon dioxide, ammonia, tetrafluoromethane, and related mixtures, delivering kinetics schemes for these systems (see graphs below).

Presently, LoKI-Suite gives open-acess to the following kinetic schemes, available at LoKI-GM/Code/Input
  • Oxygen, published at
    T. C. Dias, C. Fromentin, L. L. Alves, A. T. del Caz, T. Silva and V. Guerra
    A reaction mechanism for oxygen plasmas
    Plasma Sources Sci. Technol. 32 084003 (2023)
  • Carbon dioxide (no vibrations), based on the chemistry published at
    A. F. Silva, A. S. Morillo-Candás, A. Tejero-del-Caz, L. L. Alves, O. Guaitella and V. Guerra
    A reaction mechanism for vibrationally-cold low-pressure CO2 plasmas
    Plasma Sources Sci. Technol. 29 125020 (2020)
  • Nitrogen (no vibrations), based on the chemistry published at
These studies include also identifying consistent cross section sets for electron collisions with the following atoms/molecules:
  • Ar (collisions with ground-state Ar(1S0); swarm validated);
  • He (collisions with ground-state He(1S0); swarm validated);
  • N2 (collisions with ground-state N2(X) and N2(X,v=0); swarm validated), N2-vib (with N2(X,v=1-10)), N2-rot (with N2(X,v=0,J=0-30) ΔJ=2).
    The latter two datagroups are clustered under Nitrogen at LXCat;
  • N (collisions with ground-state N(4S)), N-elec (with N(2D) and N(2P)).
    These datagroups are clustered under Nitrogen at LXCat;
  • O2 (collisions with ground-state O2(X) and O2(X,v=0); swarm validated), O2-vib (with O2(X,v=0-41)), O2-rot (with O2(X,v=0,J=1-29) ΔJ=2), O2-elec (with excited electronic states, namely O2(a1Δg, b1Σ+g)).
    The latter three datagroups are clustered under Oxygen;
  • O (collisions with ground-state O(3P)), O-elec (with excited electronic states, namely O-).
    These datagroups are clustered under Oxygen;
  • O3 (collisions with ground-state O3(X)).
    This datagroup is clustered under Oxygen;
  • H2 (collisions with ground-state H2(X) and H2(X,v=0); swarm validated), H2-vib (with H2(X,v=1-15)), H2-rot (with H2(X,v=0,J=0-5) ΔJ=2), H2-elec (for electron recombination of H2+ and H3+).
    The latter three datagroups are clustered under Hydrogen;
  • H (collisions with ground-state H(1s)), H-elec (with H(2s), H(2p), H(3), H(4) and H(5)).
    These datagroups are clustered under Hydrogen;
  • CO2 (collisions with ground-state CO2(X) and CO2(X,v=000); swarm validated);
  • CO (collisions with ground-state CO(X) and CO(X,v=0); swarm validated), CO-rot (with CO(X,v=0,J=0-17) ΔJ=1);
  • CO_anis (collisions with ground-state CO(X) and CO(X,v=0) to be adopted when anisotropic scattering for rotational collisions is also considered; swarm validated), CO_dipint-rot (dipole-integral cross sections for rotational excitation with CO(X,v=0,J=0-25) ΔJ=1), CO_dipmt-rot (dipole-momentum-transfer cross sections for rotational excitation with CO(X,v=0,J=0-25) ΔJ=1), CO_quadint-rot (quadrupole-integral cross sections for rotational excitation with CO(X,v=0,J=0-24) ΔJ=2).
    These datagroups are clustered under CO_anis.
  • NH3: (collisions with ground-state NH3(X); swarm validated), NH3-rot (with NH3(X,v=0,J=0) ΔJ=1-5).
    These datagroups are published in the new LXCat (future) database.

Argon KIT - results

The figures show example results, obtained for argon plasmas at low and moderate pressures, with the simulation tool LisbOn KInetics - LoKI: the electron energy distribution function (1); the distribution of the electron power-density (2); and the densities of charged and neutral species (3).

Helium KIT - results

The figures show example results, obtained for helium plasmas at low and moderate pressures, with the simulation tool LisbOn KInetics - LoKI: the electron energy distribution function (1); the distribution of the electron power-density (2); and the densities of charged and neutral species (3).

Nitrogen KIT - results

The figures show example results, obtained for nitrogen plasmas at low and high-pressures, with the simulation tool LisbOn KInetics - LoKI: the electron energy distribution function (1); the distribution of the electron power-density (2); the densities of atomic / molecular charged and neutral species (3); and the distribution of densities for the vibrational excited states with the electronic ground-state N2(X) (4).

Oxygen KIT - results

The figures show example results, obtained for oxygen plasmas at low and moderate pressures, with the simulation tool LisbOn KInetics - LoKI: the electron energy distribution function (1); the distribution of the electron power-density (2); the densities of atomic / molecular charged and neutral species (3); and the distribution of densities for the vibrational excited states with the electronic ground-state O2(X) (4).