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Spectral intensity of the N2 emission in argon low-pressure arc discharges for lighting purposes
被引:24
|作者:
Friedl, R.
[1
,2
]
Fantz, U.
[1
,2
]
机构:
[1] Univ Augsburg, Lehrstuhl Expt Plasmaphys, D-86135 Augsburg, Germany
[2] EURATOM, Max Planck Inst Plasmaphys, D-85748 Garching, Germany
来源:
NEW JOURNAL OF PHYSICS
|
2012年
/
14卷
关键词:
COLLISIONAL-RADIATIVE MODEL;
ENERGY-POOLING REACTIONS;
ACTIVE NITROGEN;
CROSS-SECTIONS;
ELECTRON;
EXCITATION;
STATE;
ATOMS;
RECOMBINATION;
SPECTROSCOPY;
D O I:
10.1088/1367-2630/14/4/043016
中图分类号:
O4 [物理学];
学科分类号:
0702 ;
摘要:
Nitrogen is discussed as an alternative to hazardous mercury in lamps for general lighting. Molecular nitrogen bands emit in both the near-UV (the second positive system C-3 Pi(u) -> B-3 Pi(g)) and the visible spectral range (the first positive system B-3 Pi(g) -> A(3)Sigma(+)(u)), which reduces conversion losses. To analyse the potential of nitrogen, low-pressure arc discharges in an argon background were characterized by means of optical emission spectroscopy. The spectral intensity of the molecular nitrogen emission rises with increasing nitrogen content in the discharge and shows a maximum around 4 mbar of absolute pressure. With regard to the application as a light source, radiation efficiencies were determined, which are around 5% at maximum. In order to identify the main population processes a collisional radiative model for the nitrogen-argon system was established which reveals the high relevance of heavy-particle collisions due to a pressure of a few mbar. The decisive excitation reactions for the state N-2 C-3 Pi(u) are the well-known processes of energy pooling between metastable nitrogen molecules and energy transfer from metastable argon atoms. For the state N-2 B-3 Pi(g) the main population channels are collision-induced crossings within the nitrogen states, where the collision partner can be either a nitrogen molecule or an argon atom, and the quenching collisions with argon.
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页数:22
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