The quenching cross section for the 0-0 first negative band of nitrogen is determined for temperatures between 78 K and 300 K. As the temperature increases above 78 K, the quenching reaches a maximum at approximately 140 K and then decreases as 300 K is approached. At temperatures on the order of 5000 K, quenching is reported to increase with temperature and must therefore reach a minimum at some intermediate temperature between 300 K and 5000 K. By comparison, quenching of the 5016 A helium line increases continuously over the temperature range 78 K to 300 K
International audienceShock layer radiation from atomic lines can represent the main source of radia...
Data from a pure nitrogen test series in the Electric Arc Shock Tube Facility were previously report...
A table-top set-up for studying gas kinetic processes in dense gases via time resolved optical spec...
The first part of this work is concerned, with the study of the fluorescence and quenching of beta i...
In-situ determinations of the quenching of O(1 D) atoms by N2 and O2 molecules were made from observ...
The kinetic mechanisms responsible for the excitation of the first-positive and first-negative emiss...
Ab initio calculation of vibrational excitation and de-excitation cross sections of N_2 by low-ener...
The measurement of rotational temperature by the electron-beam fluorescence technique is investigate...
Electron beam probe measurements of rotational and vibrational temperatures in static low-density ai
A high resolution spectrographic study has been made of the nitrogen first negative system as induce...
Laboratory measurements of rotational temperatures in static low density air with electron beam prob
A vehicle reentering Earth\u27s atmosphere at hypersonic velocities violently compresses the air in ...
The Calspan electron beam fluorescence (EBF) measurement system is described along with the results ...
The helium line ratio technique was used to determine electron temperatures in a toroidal steady-sta...
The temperature dependences of the quenching rate constants of the states N2 (${\rm C} \ {^{3}{ \rm...
International audienceShock layer radiation from atomic lines can represent the main source of radia...
Data from a pure nitrogen test series in the Electric Arc Shock Tube Facility were previously report...
A table-top set-up for studying gas kinetic processes in dense gases via time resolved optical spec...
The first part of this work is concerned, with the study of the fluorescence and quenching of beta i...
In-situ determinations of the quenching of O(1 D) atoms by N2 and O2 molecules were made from observ...
The kinetic mechanisms responsible for the excitation of the first-positive and first-negative emiss...
Ab initio calculation of vibrational excitation and de-excitation cross sections of N_2 by low-ener...
The measurement of rotational temperature by the electron-beam fluorescence technique is investigate...
Electron beam probe measurements of rotational and vibrational temperatures in static low-density ai
A high resolution spectrographic study has been made of the nitrogen first negative system as induce...
Laboratory measurements of rotational temperatures in static low density air with electron beam prob
A vehicle reentering Earth\u27s atmosphere at hypersonic velocities violently compresses the air in ...
The Calspan electron beam fluorescence (EBF) measurement system is described along with the results ...
The helium line ratio technique was used to determine electron temperatures in a toroidal steady-sta...
The temperature dependences of the quenching rate constants of the states N2 (${\rm C} \ {^{3}{ \rm...
International audienceShock layer radiation from atomic lines can represent the main source of radia...
Data from a pure nitrogen test series in the Electric Arc Shock Tube Facility were previously report...
A table-top set-up for studying gas kinetic processes in dense gases via time resolved optical spec...