Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films
Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decre...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Oh, Hyungon [verfasserIn] Cho, Kyoungah [verfasserIn] Kim, Sangsig [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of the Korean Physical Society - Berlin : Springer, 1968, 67(2015), 4 vom: Aug., Seite 638-642 |
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| Übergeordnetes Werk: |
volume:67 ; year:2015 ; number:4 ; month:08 ; pages:638-642 |
| Links: |
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| DOI / URN: |
10.3938/jkps.67.638 |
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| Katalog-ID: |
SPR032721250 |
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| 520 | |a Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. | ||
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| 700 | 1 | |a Kim, Sangsig |e verfasserin |4 aut | |
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10.3938/jkps.67.638 doi (DE-627)SPR032721250 (SPR)jkps.67.638-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Oh, Hyungon verfasserin aut Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. Nitrogen-doped amorphous carbon (dpeaa)DE-He213 DC magnetron sputtering (dpeaa)DE-He213 Bonding state (dpeaa)DE-He213 Cho, Kyoungah verfasserin aut Kim, Sangsig verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 67(2015), 4 vom: Aug., Seite 638-642 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:67 year:2015 number:4 month:08 pages:638-642 https://dx.doi.org/10.3938/jkps.67.638 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 67 2015 4 08 638-642 |
| spelling |
10.3938/jkps.67.638 doi (DE-627)SPR032721250 (SPR)jkps.67.638-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Oh, Hyungon verfasserin aut Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. Nitrogen-doped amorphous carbon (dpeaa)DE-He213 DC magnetron sputtering (dpeaa)DE-He213 Bonding state (dpeaa)DE-He213 Cho, Kyoungah verfasserin aut Kim, Sangsig verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 67(2015), 4 vom: Aug., Seite 638-642 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:67 year:2015 number:4 month:08 pages:638-642 https://dx.doi.org/10.3938/jkps.67.638 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 67 2015 4 08 638-642 |
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10.3938/jkps.67.638 doi (DE-627)SPR032721250 (SPR)jkps.67.638-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Oh, Hyungon verfasserin aut Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. Nitrogen-doped amorphous carbon (dpeaa)DE-He213 DC magnetron sputtering (dpeaa)DE-He213 Bonding state (dpeaa)DE-He213 Cho, Kyoungah verfasserin aut Kim, Sangsig verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 67(2015), 4 vom: Aug., Seite 638-642 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:67 year:2015 number:4 month:08 pages:638-642 https://dx.doi.org/10.3938/jkps.67.638 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 67 2015 4 08 638-642 |
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10.3938/jkps.67.638 doi (DE-627)SPR032721250 (SPR)jkps.67.638-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Oh, Hyungon verfasserin aut Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. Nitrogen-doped amorphous carbon (dpeaa)DE-He213 DC magnetron sputtering (dpeaa)DE-He213 Bonding state (dpeaa)DE-He213 Cho, Kyoungah verfasserin aut Kim, Sangsig verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 67(2015), 4 vom: Aug., Seite 638-642 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:67 year:2015 number:4 month:08 pages:638-642 https://dx.doi.org/10.3938/jkps.67.638 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 67 2015 4 08 638-642 |
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10.3938/jkps.67.638 doi (DE-627)SPR032721250 (SPR)jkps.67.638-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Oh, Hyungon verfasserin aut Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. Nitrogen-doped amorphous carbon (dpeaa)DE-He213 DC magnetron sputtering (dpeaa)DE-He213 Bonding state (dpeaa)DE-He213 Cho, Kyoungah verfasserin aut Kim, Sangsig verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 67(2015), 4 vom: Aug., Seite 638-642 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:67 year:2015 number:4 month:08 pages:638-642 https://dx.doi.org/10.3938/jkps.67.638 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 67 2015 4 08 638-642 |
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|
| author |
Oh, Hyungon |
| spellingShingle |
Oh, Hyungon ddc 530 bkl 33.00 misc Nitrogen-doped amorphous carbon misc DC magnetron sputtering misc Bonding state Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films |
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530 ASE 33.00 bkl Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films Nitrogen-doped amorphous carbon (dpeaa)DE-He213 DC magnetron sputtering (dpeaa)DE-He213 Bonding state (dpeaa)DE-He213 |
| topic |
ddc 530 bkl 33.00 misc Nitrogen-doped amorphous carbon misc DC magnetron sputtering misc Bonding state |
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ddc 530 bkl 33.00 misc Nitrogen-doped amorphous carbon misc DC magnetron sputtering misc Bonding state |
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ddc 530 bkl 33.00 misc Nitrogen-doped amorphous carbon misc DC magnetron sputtering misc Bonding state |
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Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films |
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Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films |
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Oh, Hyungon |
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Journal of the Korean Physical Society |
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Oh, Hyungon Cho, Kyoungah Kim, Sangsig |
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| title_sort |
effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films |
| title_auth |
Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films |
| abstract |
Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. |
| abstractGer |
Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. |
| abstract_unstemmed |
Abstract In this study, we investigate the effect of the deposition pressure on the electrical properties of nitrogen-doped amorphous carbon (a-C:N) films deposited by using an unbalanced DC magnetron sputtering method. As the deposition pressure is decreased from 9 to 1 mTorr, the resistivity decreases from 7.88 to 2.68 × 10 −2 Ω·cm while the deposition rate increases from 3.5 to 4.4 nm/min. The decrease in resistivity is caused by increases in both the carrier concentration and mobility. As the pressure is decreased, the carrier concentration increases from 1.9 × $ 10^{14} $ to 7.8 × $ 10^{20} $ cm −3, and the mobility increases from 0.01 to 0.3 $ cm^{2} $/V·sec. X-ray photoelectron spectroscopy and Raman spectroscopy reveal that the improved electrical properties of the film deposited at a lower pressure are the result of a higher fraction of $ sp^{2} $ bonding. |
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Effect of deposition pressure on the electrical properties of nitrogen-doped amorphous carbon films |
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https://dx.doi.org/10.3938/jkps.67.638 |
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Cho, Kyoungah Kim, Sangsig |
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10.3938/jkps.67.638 |
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2024-07-03T14:24:13.638Z |
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