Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite
The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite ca...
Ausführliche Beschreibung
Autor*in: |
Ozturk, Sevgul [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
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2015 |
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Übergeordnetes Werk: |
Enthalten in: IEEE transactions on plasma science - New York, NY : IEEE, 1973, 43(2015), 6, Seite 1839-1844 |
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Übergeordnetes Werk: |
volume:43 ; year:2015 ; number:6 ; pages:1839-1844 |
Links: |
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DOI / URN: |
10.1109/TPS.2015.2422579 |
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Katalog-ID: |
OLC1966516754 |
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520 | |a The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. | ||
650 | 4 | |a β-irradiation | |
650 | 4 | |a discharges (electric) | |
650 | 4 | |a radiation absorbed dose 1 kGy | |
650 | 4 | |a plasma light intensity | |
650 | 4 | |a radiation defect centers | |
650 | 4 | |a plasma production | |
650 | 4 | |a nanoporous zeolite | |
650 | 4 | |a conductivity | |
650 | 4 | |a material porosity | |
650 | 4 | |a Charge carrier processes | |
650 | 4 | |a Radiation effects | |
650 | 4 | |a gas discharge system | |
650 | 4 | |a discharge currents | |
650 | 4 | |a porous surfaces | |
650 | 4 | |a Plasmas | |
650 | 4 | |a beta-ray effects | |
650 | 4 | |a Dielectrics | |
650 | 4 | |a nonthermal plasma generation | |
650 | 4 | |a β-radiation | |
650 | 4 | |a electrical properties | |
650 | 4 | |a pressure | |
650 | 4 | |a zeolites | |
650 | 4 | |a trapped electrons | |
650 | 4 | |a ZC surface | |
650 | 4 | |a AP microplasmas | |
650 | 4 | |a pressure 1 atm to 0.01 torr | |
650 | 4 | |a plasma generation | |
650 | 4 | |a porosity | |
650 | 4 | |a charge trapping effects | |
650 | 4 | |a optical properties | |
650 | 4 | |a breakdown voltage | |
650 | 4 | |a zeolite cathode | |
650 | 4 | |a Surface discharges | |
650 | 4 | |a current-voltage characteristics | |
650 | 4 | |a atmospheric pressure | |
650 | 4 | |a irradiated porous zeolite | |
650 | 4 | |a electron emission | |
650 | 4 | |a Discharge | |
650 | 4 | |a Radiation | |
650 | 4 | |a Conductivity | |
650 | 4 | |a Electrical currents | |
650 | 4 | |a Atmospheric pressure | |
650 | 4 | |a Zeolites | |
650 | 4 | |a Porous materials | |
700 | 1 | |a Ozer, Metin |4 oth | |
700 | 1 | |a Bulur, Enver |4 oth | |
700 | 1 | |a Salamov, Bahtiyar G |4 oth | |
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10.1109/TPS.2015.2422579 doi PQ20160617 (DE-627)OLC1966516754 (DE-599)GBVOLC1966516754 (PRQ)c2101-efc3906bb524739426722126dcfd0f0a048a0787a7054800373a1ba5bcbfe84b0 (KEY)0058744320150000043000601839plasmagenerationinagasdischargesystemwithirradiate DE-627 ger DE-627 rakwb eng 530 DNB 33.80 bkl Ozturk, Sevgul verfasserin aut Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. β-irradiation discharges (electric) radiation absorbed dose 1 kGy plasma light intensity radiation defect centers plasma production nanoporous zeolite conductivity material porosity Charge carrier processes Radiation effects gas discharge system discharge currents porous surfaces Plasmas beta-ray effects Dielectrics nonthermal plasma generation β-radiation electrical properties pressure zeolites trapped electrons ZC surface AP microplasmas pressure 1 atm to 0.01 torr plasma generation porosity charge trapping effects optical properties breakdown voltage zeolite cathode Surface discharges current-voltage characteristics atmospheric pressure irradiated porous zeolite electron emission Discharge Radiation Conductivity Electrical currents Atmospheric pressure Zeolites Porous materials Ozer, Metin oth Bulur, Enver oth Salamov, Bahtiyar G oth Enthalten in IEEE transactions on plasma science New York, NY : IEEE, 1973 43(2015), 6, Seite 1839-1844 (DE-627)129391379 (DE-600)184848-3 (DE-576)014776553 0093-3813 nnns volume:43 year:2015 number:6 pages:1839-1844 http://dx.doi.org/10.1109/TPS.2015.2422579 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7108072 http://search.proquest.com/docview/1689887525 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 33.80 AVZ AR 43 2015 6 1839-1844 |
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10.1109/TPS.2015.2422579 doi PQ20160617 (DE-627)OLC1966516754 (DE-599)GBVOLC1966516754 (PRQ)c2101-efc3906bb524739426722126dcfd0f0a048a0787a7054800373a1ba5bcbfe84b0 (KEY)0058744320150000043000601839plasmagenerationinagasdischargesystemwithirradiate DE-627 ger DE-627 rakwb eng 530 DNB 33.80 bkl Ozturk, Sevgul verfasserin aut Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. β-irradiation discharges (electric) radiation absorbed dose 1 kGy plasma light intensity radiation defect centers plasma production nanoporous zeolite conductivity material porosity Charge carrier processes Radiation effects gas discharge system discharge currents porous surfaces Plasmas beta-ray effects Dielectrics nonthermal plasma generation β-radiation electrical properties pressure zeolites trapped electrons ZC surface AP microplasmas pressure 1 atm to 0.01 torr plasma generation porosity charge trapping effects optical properties breakdown voltage zeolite cathode Surface discharges current-voltage characteristics atmospheric pressure irradiated porous zeolite electron emission Discharge Radiation Conductivity Electrical currents Atmospheric pressure Zeolites Porous materials Ozer, Metin oth Bulur, Enver oth Salamov, Bahtiyar G oth Enthalten in IEEE transactions on plasma science New York, NY : IEEE, 1973 43(2015), 6, Seite 1839-1844 (DE-627)129391379 (DE-600)184848-3 (DE-576)014776553 0093-3813 nnns volume:43 year:2015 number:6 pages:1839-1844 http://dx.doi.org/10.1109/TPS.2015.2422579 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7108072 http://search.proquest.com/docview/1689887525 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 33.80 AVZ AR 43 2015 6 1839-1844 |
allfields_unstemmed |
10.1109/TPS.2015.2422579 doi PQ20160617 (DE-627)OLC1966516754 (DE-599)GBVOLC1966516754 (PRQ)c2101-efc3906bb524739426722126dcfd0f0a048a0787a7054800373a1ba5bcbfe84b0 (KEY)0058744320150000043000601839plasmagenerationinagasdischargesystemwithirradiate DE-627 ger DE-627 rakwb eng 530 DNB 33.80 bkl Ozturk, Sevgul verfasserin aut Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. β-irradiation discharges (electric) radiation absorbed dose 1 kGy plasma light intensity radiation defect centers plasma production nanoporous zeolite conductivity material porosity Charge carrier processes Radiation effects gas discharge system discharge currents porous surfaces Plasmas beta-ray effects Dielectrics nonthermal plasma generation β-radiation electrical properties pressure zeolites trapped electrons ZC surface AP microplasmas pressure 1 atm to 0.01 torr plasma generation porosity charge trapping effects optical properties breakdown voltage zeolite cathode Surface discharges current-voltage characteristics atmospheric pressure irradiated porous zeolite electron emission Discharge Radiation Conductivity Electrical currents Atmospheric pressure Zeolites Porous materials Ozer, Metin oth Bulur, Enver oth Salamov, Bahtiyar G oth Enthalten in IEEE transactions on plasma science New York, NY : IEEE, 1973 43(2015), 6, Seite 1839-1844 (DE-627)129391379 (DE-600)184848-3 (DE-576)014776553 0093-3813 nnns volume:43 year:2015 number:6 pages:1839-1844 http://dx.doi.org/10.1109/TPS.2015.2422579 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7108072 http://search.proquest.com/docview/1689887525 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 33.80 AVZ AR 43 2015 6 1839-1844 |
allfieldsGer |
10.1109/TPS.2015.2422579 doi PQ20160617 (DE-627)OLC1966516754 (DE-599)GBVOLC1966516754 (PRQ)c2101-efc3906bb524739426722126dcfd0f0a048a0787a7054800373a1ba5bcbfe84b0 (KEY)0058744320150000043000601839plasmagenerationinagasdischargesystemwithirradiate DE-627 ger DE-627 rakwb eng 530 DNB 33.80 bkl Ozturk, Sevgul verfasserin aut Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. β-irradiation discharges (electric) radiation absorbed dose 1 kGy plasma light intensity radiation defect centers plasma production nanoporous zeolite conductivity material porosity Charge carrier processes Radiation effects gas discharge system discharge currents porous surfaces Plasmas beta-ray effects Dielectrics nonthermal plasma generation β-radiation electrical properties pressure zeolites trapped electrons ZC surface AP microplasmas pressure 1 atm to 0.01 torr plasma generation porosity charge trapping effects optical properties breakdown voltage zeolite cathode Surface discharges current-voltage characteristics atmospheric pressure irradiated porous zeolite electron emission Discharge Radiation Conductivity Electrical currents Atmospheric pressure Zeolites Porous materials Ozer, Metin oth Bulur, Enver oth Salamov, Bahtiyar G oth Enthalten in IEEE transactions on plasma science New York, NY : IEEE, 1973 43(2015), 6, Seite 1839-1844 (DE-627)129391379 (DE-600)184848-3 (DE-576)014776553 0093-3813 nnns volume:43 year:2015 number:6 pages:1839-1844 http://dx.doi.org/10.1109/TPS.2015.2422579 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7108072 http://search.proquest.com/docview/1689887525 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 33.80 AVZ AR 43 2015 6 1839-1844 |
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10.1109/TPS.2015.2422579 doi PQ20160617 (DE-627)OLC1966516754 (DE-599)GBVOLC1966516754 (PRQ)c2101-efc3906bb524739426722126dcfd0f0a048a0787a7054800373a1ba5bcbfe84b0 (KEY)0058744320150000043000601839plasmagenerationinagasdischargesystemwithirradiate DE-627 ger DE-627 rakwb eng 530 DNB 33.80 bkl Ozturk, Sevgul verfasserin aut Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. β-irradiation discharges (electric) radiation absorbed dose 1 kGy plasma light intensity radiation defect centers plasma production nanoporous zeolite conductivity material porosity Charge carrier processes Radiation effects gas discharge system discharge currents porous surfaces Plasmas beta-ray effects Dielectrics nonthermal plasma generation β-radiation electrical properties pressure zeolites trapped electrons ZC surface AP microplasmas pressure 1 atm to 0.01 torr plasma generation porosity charge trapping effects optical properties breakdown voltage zeolite cathode Surface discharges current-voltage characteristics atmospheric pressure irradiated porous zeolite electron emission Discharge Radiation Conductivity Electrical currents Atmospheric pressure Zeolites Porous materials Ozer, Metin oth Bulur, Enver oth Salamov, Bahtiyar G oth Enthalten in IEEE transactions on plasma science New York, NY : IEEE, 1973 43(2015), 6, Seite 1839-1844 (DE-627)129391379 (DE-600)184848-3 (DE-576)014776553 0093-3813 nnns volume:43 year:2015 number:6 pages:1839-1844 http://dx.doi.org/10.1109/TPS.2015.2422579 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7108072 http://search.proquest.com/docview/1689887525 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 33.80 AVZ AR 43 2015 6 1839-1844 |
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Ozturk, Sevgul ddc 530 bkl 33.80 misc β-irradiation misc discharges (electric) misc radiation absorbed dose 1 kGy misc plasma light intensity misc radiation defect centers misc plasma production misc nanoporous zeolite misc conductivity misc material porosity misc Charge carrier processes misc Radiation effects misc gas discharge system misc discharge currents misc porous surfaces misc Plasmas misc beta-ray effects misc Dielectrics misc nonthermal plasma generation misc β-radiation misc electrical properties misc pressure misc zeolites misc trapped electrons misc ZC surface misc AP microplasmas misc pressure 1 atm to 0.01 torr misc plasma generation misc porosity misc charge trapping effects misc optical properties misc breakdown voltage misc zeolite cathode misc Surface discharges misc current-voltage characteristics misc atmospheric pressure misc irradiated porous zeolite misc electron emission misc Discharge misc Radiation misc Conductivity misc Electrical currents misc Atmospheric pressure misc Zeolites misc Porous materials Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite |
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530 DNB 33.80 bkl Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite β-irradiation discharges (electric) radiation absorbed dose 1 kGy plasma light intensity radiation defect centers plasma production nanoporous zeolite conductivity material porosity Charge carrier processes Radiation effects gas discharge system discharge currents porous surfaces Plasmas beta-ray effects Dielectrics nonthermal plasma generation β-radiation electrical properties pressure zeolites trapped electrons ZC surface AP microplasmas pressure 1 atm to 0.01 torr plasma generation porosity charge trapping effects optical properties breakdown voltage zeolite cathode Surface discharges current-voltage characteristics atmospheric pressure irradiated porous zeolite electron emission Discharge Radiation Conductivity Electrical currents Atmospheric pressure Zeolites Porous materials |
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ddc 530 bkl 33.80 misc β-irradiation misc discharges (electric) misc radiation absorbed dose 1 kGy misc plasma light intensity misc radiation defect centers misc plasma production misc nanoporous zeolite misc conductivity misc material porosity misc Charge carrier processes misc Radiation effects misc gas discharge system misc discharge currents misc porous surfaces misc Plasmas misc beta-ray effects misc Dielectrics misc nonthermal plasma generation misc β-radiation misc electrical properties misc pressure misc zeolites misc trapped electrons misc ZC surface misc AP microplasmas misc pressure 1 atm to 0.01 torr misc plasma generation misc porosity misc charge trapping effects misc optical properties misc breakdown voltage misc zeolite cathode misc Surface discharges misc current-voltage characteristics misc atmospheric pressure misc irradiated porous zeolite misc electron emission misc Discharge misc Radiation misc Conductivity misc Electrical currents misc Atmospheric pressure misc Zeolites misc Porous materials |
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ddc 530 bkl 33.80 misc β-irradiation misc discharges (electric) misc radiation absorbed dose 1 kGy misc plasma light intensity misc radiation defect centers misc plasma production misc nanoporous zeolite misc conductivity misc material porosity misc Charge carrier processes misc Radiation effects misc gas discharge system misc discharge currents misc porous surfaces misc Plasmas misc beta-ray effects misc Dielectrics misc nonthermal plasma generation misc β-radiation misc electrical properties misc pressure misc zeolites misc trapped electrons misc ZC surface misc AP microplasmas misc pressure 1 atm to 0.01 torr misc plasma generation misc porosity misc charge trapping effects misc optical properties misc breakdown voltage misc zeolite cathode misc Surface discharges misc current-voltage characteristics misc atmospheric pressure misc irradiated porous zeolite misc electron emission misc Discharge misc Radiation misc Conductivity misc Electrical currents misc Atmospheric pressure misc Zeolites misc Porous materials |
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ddc 530 bkl 33.80 misc β-irradiation misc discharges (electric) misc radiation absorbed dose 1 kGy misc plasma light intensity misc radiation defect centers misc plasma production misc nanoporous zeolite misc conductivity misc material porosity misc Charge carrier processes misc Radiation effects misc gas discharge system misc discharge currents misc porous surfaces misc Plasmas misc beta-ray effects misc Dielectrics misc nonthermal plasma generation misc β-radiation misc electrical properties misc pressure misc zeolites misc trapped electrons misc ZC surface misc AP microplasmas misc pressure 1 atm to 0.01 torr misc plasma generation misc porosity misc charge trapping effects misc optical properties misc breakdown voltage misc zeolite cathode misc Surface discharges misc current-voltage characteristics misc atmospheric pressure misc irradiated porous zeolite misc electron emission misc Discharge misc Radiation misc Conductivity misc Electrical currents misc Atmospheric pressure misc Zeolites misc Porous materials |
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plasma generation in a gas discharge system with irradiated porous zeolite |
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Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite |
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The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. |
abstractGer |
The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. |
abstract_unstemmed |
The influence of pressure [from atmospheric pressure (AP) to 10 -2 torr] and β-radiation (1-kGy β doses) on the current-voltage characteristics, charge trapping effects in porous surfaces, and breakdown voltage (U B ) in AP microplasmas are discussed for the first time. This is due to the zeolite cathode (ZC) exposure to β-radiation resulting in substantial decreases in the U B , discharge currents, and conductivity due to increase in porosity of the material. Results indicated the enhancement of plasma light intensity and electron emission from the ZC surface with the release of trapped electrons which are captured by the defect centers following β-irradiation. The porosity of the ZC and radiation defect centers has a significant influence on the electrical and optical properties of the devices manufactured on its base. |
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Plasma Generation in a Gas Discharge System With Irradiated Porous Zeolite |
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http://dx.doi.org/10.1109/TPS.2015.2422579 http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7108072 http://search.proquest.com/docview/1689887525 |
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