Abstract
The rate of ionization of nitrogen at 300 K and at gas pressures of 1 to 30 Torr is considerably increased by admixing neutral molecules of electronically excited nitrogen, N*
2
. This effect is demonstrated by measuring the corresponding decrease in electric strength as a function of the population of the excited species. These are produced in a weak electric discharge which is maintained at one end of a long tube filled with N
2
. From there they diffuse into the test region at the other end where a high frequency electric field is applied to determine electric breakdown voltage of the partially excited gas. Gas contamination is avoided by using external electrodes throughout. The population of N*
2
in the test region is varied by changing the gas pressure and the distance between the test region and the source whose activity is kept constant. It is found that at a pressure of about 1 Torr and a distance of 10 cm the electric strength of N
2
+ N*
2
is up to 15% smaller than that of N
2
. The presence of N*
2
is also detected by the colour change of a metal oxide powder with which it reacts; for example, pale green MoO
3
exposed to N*
2
is reduced to blue MoO
2
within 10 to 100s. From the time interval between the exposure of the powder to the gas and the colour change, the relative concentration of N*
2
is obtained as a function of distance in a 4 cm wide tube up to 80 cm from the source at pressures up to 30 Torr when the system is kept in a steady state. In addition, the time dependence of the concentration along the tube is observed in the non-steady state. A colour test with calcium shows that outside the source nitrogen atoms are negligible in numbers. Also by means of a platinum resistance wire the total energy flux and the number of N*
2
is measured and, with an electron emission detector, their spatial distribution is again confirmed. Analysis of the results shows that the extremely slow decay of N*
2
at lower pressures is essentially controlled by spontaneous radiation and wall collisons, whereas collision deactivation sets in above about 10 Torr. It is concluded that the bulk of N*
2
outside the source is in the A(
3
∑
u
+
) state with a free life of 12 s and a concentration of about 10
13
particles/cm
3
at 1 Torr; hence 1 part in 10
4
of N
2
are electronically excited. The efficiency of wall deactivation to the ground state of N
2
by Pyrex glass and platinum is found to be 3 × 10
-5
and 3 × 10
-3
respectively, the efficiency of electron emission from platinum is about 10
-7
excited molecules per electron collected and the upper bound of the activation energy for reducing MoO
3
is 6.1 eV, the zero vibrational level of the A state. Since the potential energy of two A state molecules is smaller than the ionization energy of N
2
, deactivation by ionization along the tube is not feasible. However, enhancement of ionization can occur in an electric field when electrons collide with such long-lived excited molecules thus raising them to higher vibrational levels so that pairs with a potential energy ≥ ionization energy can produce ionization on collision.
Reference64 articles.
1. rose from ^ 103 s in r : B rennen (1966) 1965 to present value
2. W entink & sta te filled m ainly b y Isaacson (1967) cascading B rom er & Spieweck
3. (1967)
4. B decays into A ; t : B rennen (1966) electron collision Benson (1968)
5. filled from 52 + ; e r : K e n ty (1961 3A Udecays into B 1967)
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