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Detection and Electric Field Quenching of Nitrogen Atoms in the (2S2P('3)3S)SEXTUPLET-S(5/2) Metastable Autoionizing State.

Hari Prasad Garg

Published Jan 1, 1976• 0 citations
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Detection of nitrogen atoms in the 2s(2p)$sup 3$3s $sup 6$S/sub 5/2/ metastable autoionizing state

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Metastable nitrogen atoms, produced by electron-impact dissociation of N/ sub 2/, have been detected in time-of-flight apparatuses locatcd at Oregon State University and at University of California at Berkeley. Two different types of metastable atoms are detected; one type resembies Rydberg hydrogen atoms, while the other does not. The measured natural lifetime for the non-Rydberg atoms is 100 plus or minus 25 mu see. Additional infonnation regarding the identity of both types of metastable atoms is obtained by observing their quenching in a static electric field. The field-dependent decay constant for the Rydberg atoms is essentially a step function, and these atoms are entirely quenched by a field of 1.5 kV/cm. Both results are consistent with theory if the Rydberg atoms are in levels with principal quantum number greater than 25. The field-dependent decay constant for the non-Rydherg atoms varies quadratically with the strength of the applied electric field. In a field of 4 kV/cm applied along a 6-cm length of flight path, the value of this decay constant is 0.3 x 10/sup 6/ sec/sup -1/. The quenching results, together with the lifetime measurement, are a strong more » indication that the non-Rydberg atoms detected in the time-of-flight spectra are nitrogen atoms in the 2s(2p)/sup 3/3s /sup 6/S/sub 5/2/ metastable autoionizing state. (a uth) « less

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Detection of Nitrogen Atoms in the 2s(2p)33sS526 Metastable Autoionizing State

Clifford E. Fairchild, Hari Prasad Garg, C. E. Johnson

Metastable nitrogen atoms, produced by electron-impact dissociation of ${\mathrm{N}}_{2}$, have been detected in time-of-flight apparatuses located at Oregon State University and at University of California at Berkeley. Two different types of metastable atoms are detected; one type resembles Rydberg hydrogen atoms, while the other does not. The measured natural lifetime for the non-Rydberg atoms is 100 \ifmmode\pm\else\textpm\fi{} 25 \ensuremath{\mu}sec. Additional information regarding the identity of both types of metastable atoms is obtained by observing their quenching in a static electric field. The field-dependent decay constant for the Rydberg atoms is essentially a step function, and these atoms are entirely quenched by a field of 1.5 kV/cm. Both results are consistent with theory if the Rydberg atoms are in levels with principal quantum number greater than 25. The field-dependent decay constant for the non-Rydberg atoms varies quadratically with the strength of the applied electric field. In a field of 4 kV/cm applied along a 6-cm length of flight path, the value of this decay constant is 0.3 \ifmmode\times\else\texttimes\fi{} ${10}^{6}$ ${\mathrm{sec}}^{\ensuremath{-}1}$. The quenching results, together with the lifetime measurement, are a strong indication that the non-Rydberg atoms detected in the time-of-flight spectra are nitrogen atoms in the $2s{(2p)}^{3}3s^{6}S_{\frac{5}{2}}$ metastable autoionizing state.

Physical Review A•Aug 1, 1973•7 citations
Detection of nitrogen atoms in the 2s(2p)$sup 3$3s sup6sup 6sup6S/sub 5/2/ metastable autoionizing state
Metastable nitrogen atoms, produced by electron-impact dissociation of N/ sub 2/, have been detected in time-of-flight apparatuses locatcd at Oregon State University and at University of California at Berkeley. Two different types of metastable atoms are detected; one type resembies Rydberg hydrogen atoms, while the other does not. The measured natural lifetime for the non-Rydberg atoms is 100 plus or minus 25 mu see. Additional infonnation regarding the identity of both types of metastable atoms is obtained by observing their quenching in a static electric field. The field-dependent decay constant for the Rydberg atoms is essentially a step function, and these atoms are entirely quenched by a field of 1.5 kV/cm. Both results are consistent with theory if the Rydberg atoms are in levels with principal quantum number greater than 25. The field-dependent decay constant for the non-Rydherg atoms varies quadratically with the strength of the applied electric field. In a field of 4 kV/cm applied along a 6-cm length of flight path, the value of this decay constant is 0.3 x 10/sup 6/ sec/sup -1/. The quenching results, together with the lifetime measurement, are a strong more » indication that the non-Rydberg atoms detected in the time-of-flight spectra are nitrogen atoms in the 2s(2p)/sup 3/3s /sup 6/S/sub 5/2/ metastable autoionizing state. (a uth) « less
Metastable nitrogen atoms, produced by electron-impact dissociation of N2{\mathrm{N}}_{2}N2​, have been detected in time-of-flight apparatuses located at Oregon State University and at University of California at Berkeley. Two different types of metastable atoms are detected; one type resembles Rydberg hydrogen atoms, while the other does not. The measured natural lifetime for the non-Rydberg atoms is 100 \ifmmode\pm\else\textpm\fi{} 25 \ensuremath{\mu}sec. Additional information regarding the identity of both types of metastable atoms is obtained by observing their quenching in a static electric field. The field-dependent decay constant for the Rydberg atoms is essentially a step function, and these atoms are entirely quenched by a field of 1.5 kV/cm. Both results are consistent with theory if the Rydberg atoms are in levels with principal quantum number greater than 25. The field-dependent decay constant for the non-Rydberg atoms varies quadratically with the strength of the applied electric field. In a field of 4 kV/cm applied along a 6-cm length of flight path, the value of this decay constant is 0.3 \ifmmode\times\else\texttimes\fi{} 106{10}^{6}106 ${\mathrm{sec}}^{\ensuremath{-}1}$. The quenching results, together with the lifetime measurement, are a strong indication that the non-Rydberg atoms detected in the time-of-flight spectra are nitrogen atoms in the 2s(2p)33s6S522s{(2p)}^{3}3s^{6}S_{\frac{5}{2}}2s(2p)33s6S25​​ metastable autoionizing state.