Analytic model of the cathode region of a short glow discharge in light gases

Kolobov, Vladimir; Tsendin, L. D.

doi:10.1103/physreva.46.7837

Cited by 134 publications

(152 citation statements)

References 55 publications

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“…±Ñ ÄÔÇÌ ÄÇÓÑâÕÐÑÔÕË, ÇÐÅÏáÓ ÑÜÖÜÂÎ ÐÇÑÃØÑAEËÏÑÔÕß ÃÑÎÇÇ ÕÑÚÐÑÅÑ ÍÑÎËÚÇÔÕÄÇÐÐÑÅÑ ÑÒËÔÂ-ÐËâ àÎÇÍÕÓÑÐÐÑÌ ÍËÐÇÕËÍË, ÍÑÅAEÂ, ÐÂÒÓËÏÇÓ, ÒËÔÂÎ: "... ¥ÂÐÐÞÇ ÍÎÂÔÔËÚÇÔÍÑÌ ÍËÐÇÕËÚÇÔÍÑÌ ÕÇÑÓËË ÒÑÎÇÊÐÞ AEÎâ ÒÓÑÔÕÞØ ÅÓÖÃÞØ ÑÙÇÐÑÍ ËÎË AEÎâ ËÔÒÑÎßÊÑÄÂÐËâ Ä ÕÇØ ÔÎÖÚÂâØ, ÍÑÅAEÂ ÑÕÔÖÕÔÕÄÖáÕ ËÎË ÐÇ ÏÑÅÖÕ ÃÞÕß ÏÂÕÇÏÂ-ÕËÚÇÔÍË ÑÃÓÂÃÑÕÂÐÞ ÃÑÎÇÇ ÕÑÚÐÞÇ AEÂÐÐÞÇ" [17].°AEÐÂÍÑ ÍËÐÇÕËÚÇÔÍÑÇ ÖÓÂÄÐÇÐËÇ Ä ÇÅÑ ÓÂÃÑÕÂØ ÐÇ ÑÃÔÖÉAEÂÇÕÔâ Ë ËÏâ ¢ÑÎßÙÏÂÐÂ ÖÒÑÏËÐÂÇÕÔâ ÎËÛß Ä ÔÄâÊË Ô ÔÑÑÕÐÑÛÇ-ÐËÇÏ ¢ÑÎßÙÏÂÐÂ ÏÇÉAEÖ àÎÇÍÕÓÑÐÐÑÌ ÍÑÐÙÇÐÕÓÂÙËÇÌ Ë àÎÇÍÕÓÑÔÕÂÕËÚÇÔÍËÏ ÒÑÕÇÐÙËÂÎÑÏ. ¥Îâ àÕÑÅÑ ÐÂÚÂÎßÐÑÅÑ àÕÂÒÂ ØÂÓÂÍÕÇÓÇÐ ÕÑÕ ×ÂÍÕ, ÚÕÑ Ä ×ÖÐAEÂÏÇÐÕÂÎßÐÞØ ÏÑÐÑÅÓÂ×ËâØ [20 ë 22] [120,121] ÂÃÎáAEÂÇÏÞÇ Ä S-, P-Ë R-ÔÕÓÂÕÂØ ¶²¿ ÕÂÍÉÇ ØÑÓÑÛÑ ÔÑÅÎÂÔÖáÕÔâ Ô àÕÑÌ ÍÂÓÕËÐÑÌ.°AEÐÂÍÑ, Ä ÑÕÎËÚËÇ ÑÕ S-ÔÕÓÂÕ p 1 Ë P-ÔÕÓÂÕ, ÖÔÕÂÐÑÄËÄÛËÇÔâ R-ÔÕÓÂÕÞ ËÏÇáÕ AEÄÇ ÓÇÊÑÐÂÐÔÐÞØ ÕÓÂÇÍÕÑÓËË, ÍÑÕÑÓÞÏ ÔÑÑÕÄÇÕ-ÔÕÄÖáÕ ÓÂÊÎËÚÐÞÇ ÊÐÂÚÇÐËâ AEË××ÇÓÇÐÙËÂÎßÐÑÅÑ ÒÑÕÑÍÂ F 1 , F 2 . ³ÎÇAEÖÇÕ, ÑAEÐÂÍÑ, ÑÕÏÇÕËÕß, ÚÕÑ ÔÂÏÑÔÑÅÎÂÔÑÄÂÐ-ÐÂâ ÕÇÑÓËâ S-, P-Ë R-ÔÕÓÂÕ ÒÑÍÂ ÑÕÔÖÕÔÕÄÖÇÕ.¯ÇâÔÐÞÏ ÑÔÕÂÈÕÔâ ÕÂÍÉÇ ÕÑ, ÄÑÊÏÑÉÐÞ ÎË Ä AEÇÌÔÕÄËÕÇÎßÐÑÔÕË ÔÕÓÂÕÞ, ÔÑÑÕÄÇÕÔÕÄÖáÜËÇ AEÓÖÅËÏ ÊÐÂÚÇÐËâÏ p.…”

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Nonlocal electron kinetics in gas discharge plasma

Tsendin¹

2010

Usp. Fiz. Nauk

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Nonlocal electron kinetics in gas discharge plasma

Tsendin¹

2010

Usp. Fiz. Nauk

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“…4,5 This is unfortunately an intrinsic feature of cathode-fall dominated discharges, in general, which are the typical discharges generated in conventional PDP cells. 8,10 A sufficiently large ion flux to a cathode for emitting secondary electrons is inevitable to sustain the discharges. Recently, it was reported that PDPs with high-Xe-content gas mixtures have the potential for improving luminous efficiency under a conventionally used driving scheme.…”

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confidence: 99%

Discharge efficiency in high-Xe-content plasma display panels

Hayashi

Heusler

Hagelaar

et al. 2004

Journal of Applied Physics

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We study theoretically the overall output performance and the dominating reaction processes of the vacuum ultraviolet ͑UV͒ radiation production in high-Xe partial pressures in plasma display panels ͑PDPs͒ with Ne-Xe gas mixtures. A two-dimensional self-consistent fluid model is applied for the simulations of discharges and UV radiation in sustaining phases of PDPs. The UV intensity increases with the Xe partial pressure ( P Xe ). The discharge efficiency also increases with P Xe . The resonant radiation from Xe( 3 P 1 ) dominates for 3.5%, while that from Xe 2 ( 3 ⌺ u ϩ ) becomes dominant over Xe( 3 P 1 ) for 10%-30%. Remarkably for 30%, the intensity from Xe 2 ( 1 ⌺ u ϩ ) is even larger than that from Xe( 3 P 1 ). It is found that for higher P Xe , the UV radiation mainly consists of the excimer radiation from Xe 2 ( 1 ⌺ u ϩ ) and Xe 2 ( 3 ⌺ u ϩ ). Here, Xe( 3 P 1 ) does not play a role itself as the UV radiator of the resonant radiation ͑147 nm͒, but as the precursor to Xe 2 ( 1 ⌺ u ϩ ), which results in the excimer radiation ͑173 nm͒.

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“…The Townsend approximation is based on the assumption that the ionization frequency can be parameterized only by the value of the local electric field. As it was pointed out in paper [13], the sheath width in the regime of dc and RFC discharges automatically shrinks to a small value which is comparable with the relaxation length of electrons even at high pressures. This implies that such an approximation is not valid for any discharge pressure.…”

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confidence: 91%