Please use this identifier to cite or link to this item:
https://hdl.handle.net/10316/12905| DC Field | Value | Language |
|---|---|---|
| dc.contributor.author | Lima, E. P. de | - |
| dc.contributor.author | Salete, M. | - |
| dc.contributor.author | Leite, S. C. P. | - |
| dc.contributor.author | Policarpo, A. J. P. L. | - |
| dc.contributor.author | Alves, M. A. F. | - |
| dc.date.accessioned | 2010-03-15T14:44:53Z | - |
| dc.date.available | 2010-03-15T14:44:53Z | - |
| dc.date.issued | 1984-02 | - |
| dc.identifier.citation | IEEE Transactions on Nuclear Science. 31:1 (1984) 94-98 | en_US |
| dc.identifier.issn | 0018-9499 | - |
| dc.identifier.uri | https://hdl.handle.net/10316/12905 | - |
| dc.description.abstract | The dead length, 6, for t > 20 ms is well approximated by d=d0 exp(-t/t) for mixtures of argon-isobutane with benzene or TEA. d0 varies in an approximate linear way with the streamer charge and the systematics of t regarding the high voltage is also presented. Afterpulses are associated not only with wall effects but also with photoionization in the gas mixture itself. Interpretation of the data is attempted | en_US |
| dc.language.iso | eng | en_US |
| dc.publisher | IEEE | en_US |
| dc.rights | openAccess | en_US |
| dc.title | Dead Region Time Evolution and Afterpulses Development in SQS | en_US |
| dc.type | article | en_US |
| dc.identifier.doi | 10.1109/TNS.1984.4333218 | - |
| item.fulltext | Com Texto completo | - |
| item.openairecristype | http://purl.org/coar/resource_type/c_18cf | - |
| item.grantfulltext | open | - |
| item.languageiso639-1 | en | - |
| item.openairetype | article | - |
| item.cerifentitytype | Publications | - |
| Appears in Collections: | FCTUC Física - Artigos em Revistas Internacionais | |
Files in This Item:
| File | Description | Size | Format | |
|---|---|---|---|---|
| Dead Region Time Evolution.pdf | 1.74 MB | Adobe PDF | View/Open |
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