Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials

Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks pr...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Xu, Yi [verfasserIn] He, Ying Yang, Yanfang

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2014

Schlagwörter:	Resonance Peak Shot Noise Transmission Probability Periodic Potential Fano Factor

Anmerkung:	© Springer-Verlag Berlin Heidelberg 2014

Übergeordnetes Werk:	Enthalten in: Applied physics - Berlin : Springer, 1973, 115(2014), 3 vom: 24. Apr., Seite 721-729
Übergeordnetes Werk:	volume:115 ; year:2014 ; number:3 ; day:24 ; month:04 ; pages:721-729

Links:	Volltext

DOI / URN:	10.1007/s00339-014-8423-2

Katalog-ID:	SPR004139844

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520			\|a Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices.
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publishDate	2014
allfields	10.1007/s00339-014-8423-2 doi (DE-627)SPR004139844 (SPR)s00339-014-8423-2-e DE-627 ger DE-627 rakwb eng Xu, Yi verfasserin aut Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2014 Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. Resonance Peak (dpeaa)DE-He213 Shot Noise (dpeaa)DE-He213 Transmission Probability (dpeaa)DE-He213 Periodic Potential (dpeaa)DE-He213 Fano Factor (dpeaa)DE-He213 He, Ying aut Yang, Yanfang aut Enthalten in Applied physics Berlin : Springer, 1973 115(2014), 3 vom: 24. Apr., Seite 721-729 (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:115 year:2014 number:3 day:24 month:04 pages:721-729 https://dx.doi.org/10.1007/s00339-014-8423-2 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_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_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 115 2014 3 24 04 721-729
spelling	10.1007/s00339-014-8423-2 doi (DE-627)SPR004139844 (SPR)s00339-014-8423-2-e DE-627 ger DE-627 rakwb eng Xu, Yi verfasserin aut Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2014 Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. Resonance Peak (dpeaa)DE-He213 Shot Noise (dpeaa)DE-He213 Transmission Probability (dpeaa)DE-He213 Periodic Potential (dpeaa)DE-He213 Fano Factor (dpeaa)DE-He213 He, Ying aut Yang, Yanfang aut Enthalten in Applied physics Berlin : Springer, 1973 115(2014), 3 vom: 24. Apr., Seite 721-729 (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:115 year:2014 number:3 day:24 month:04 pages:721-729 https://dx.doi.org/10.1007/s00339-014-8423-2 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_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_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 115 2014 3 24 04 721-729
allfields_unstemmed	10.1007/s00339-014-8423-2 doi (DE-627)SPR004139844 (SPR)s00339-014-8423-2-e DE-627 ger DE-627 rakwb eng Xu, Yi verfasserin aut Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2014 Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. Resonance Peak (dpeaa)DE-He213 Shot Noise (dpeaa)DE-He213 Transmission Probability (dpeaa)DE-He213 Periodic Potential (dpeaa)DE-He213 Fano Factor (dpeaa)DE-He213 He, Ying aut Yang, Yanfang aut Enthalten in Applied physics Berlin : Springer, 1973 115(2014), 3 vom: 24. Apr., Seite 721-729 (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:115 year:2014 number:3 day:24 month:04 pages:721-729 https://dx.doi.org/10.1007/s00339-014-8423-2 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_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_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 115 2014 3 24 04 721-729
allfieldsGer	10.1007/s00339-014-8423-2 doi (DE-627)SPR004139844 (SPR)s00339-014-8423-2-e DE-627 ger DE-627 rakwb eng Xu, Yi verfasserin aut Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2014 Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. Resonance Peak (dpeaa)DE-He213 Shot Noise (dpeaa)DE-He213 Transmission Probability (dpeaa)DE-He213 Periodic Potential (dpeaa)DE-He213 Fano Factor (dpeaa)DE-He213 He, Ying aut Yang, Yanfang aut Enthalten in Applied physics Berlin : Springer, 1973 115(2014), 3 vom: 24. Apr., Seite 721-729 (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:115 year:2014 number:3 day:24 month:04 pages:721-729 https://dx.doi.org/10.1007/s00339-014-8423-2 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_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_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 115 2014 3 24 04 721-729
allfieldsSound	10.1007/s00339-014-8423-2 doi (DE-627)SPR004139844 (SPR)s00339-014-8423-2-e DE-627 ger DE-627 rakwb eng Xu, Yi verfasserin aut Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag Berlin Heidelberg 2014 Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. Resonance Peak (dpeaa)DE-He213 Shot Noise (dpeaa)DE-He213 Transmission Probability (dpeaa)DE-He213 Periodic Potential (dpeaa)DE-He213 Fano Factor (dpeaa)DE-He213 He, Ying aut Yang, Yanfang aut Enthalten in Applied physics Berlin : Springer, 1973 115(2014), 3 vom: 24. Apr., Seite 721-729 (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:115 year:2014 number:3 day:24 month:04 pages:721-729 https://dx.doi.org/10.1007/s00339-014-8423-2 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_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_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_2056 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 115 2014 3 24 04 721-729
language	English
source	Enthalten in Applied physics 115(2014), 3 vom: 24. Apr., Seite 721-729 volume:115 year:2014 number:3 day:24 month:04 pages:721-729
sourceStr	Enthalten in Applied physics 115(2014), 3 vom: 24. Apr., Seite 721-729 volume:115 year:2014 number:3 day:24 month:04 pages:721-729
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Resonance Peak Shot Noise Transmission Probability Periodic Potential Fano Factor
isfreeaccess_bool	false
container_title	Applied physics
authorswithroles_txt_mv	Xu, Yi @@aut@@ He, Ying @@aut@@ Yang, Yanfang @@aut@@
publishDateDaySort_date	2014-04-24T00:00:00Z
hierarchy_top_id	235503231
id	SPR004139844
language_de	englisch
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author	Xu, Yi
spellingShingle	Xu, Yi misc Resonance Peak misc Shot Noise misc Transmission Probability misc Periodic Potential misc Fano Factor Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials
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topic_title	Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials Resonance Peak (dpeaa)DE-He213 Shot Noise (dpeaa)DE-He213 Transmission Probability (dpeaa)DE-He213 Periodic Potential (dpeaa)DE-He213 Fano Factor (dpeaa)DE-He213
topic	misc Resonance Peak misc Shot Noise misc Transmission Probability misc Periodic Potential misc Fano Factor
topic_unstemmed	misc Resonance Peak misc Shot Noise misc Transmission Probability misc Periodic Potential misc Fano Factor
topic_browse	misc Resonance Peak misc Shot Noise misc Transmission Probability misc Periodic Potential misc Fano Factor
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials
ctrlnum	(DE-627)SPR004139844 (SPR)s00339-014-8423-2-e
title_full	Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials
author_sort	Xu, Yi
journal	Applied physics
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author_browse	Xu, Yi He, Ying Yang, Yanfang
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format_se	Elektronische Aufsätze
author-letter	Xu, Yi
doi_str_mv	10.1007/s00339-014-8423-2
title_sort	resonant peak splitting in graphene superlattices with one-dimensional periodic potentials
title_auth	Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials
abstract	Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. © Springer-Verlag Berlin Heidelberg 2014
abstractGer	Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. © Springer-Verlag Berlin Heidelberg 2014
abstract_unstemmed	Abstract We have investigated theoretically the resonant tunneling phenomenon of Dirac electrons through graphene superlattices with periodic potentials of square barriers. It is found that there are two resonance conditions for the graphene superlattices. Some of the resonance transmission peaks present N – 1-fold resonance splitting for %$ N{\text{-barriers}} %$, which is the analogy of the resonance splitting in semiconductor superlattices. The resonance splitting effect depends on the incidence angle rather than the height and width of the potential. However, there is no explicit splitting rule for the conductance and shot noise, which is different from the magnetic case. Furthermore, the resonant splitting rule of the transmission is not sensitive to the shape of the potential barrier. These properties in graphene superlattices may lead to potential applications in graphene-based electron devices. © Springer-Verlag Berlin Heidelberg 2014
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title_short	Resonant peak splitting in graphene superlattices with one-dimensional periodic potentials
url	https://dx.doi.org/10.1007/s00339-014-8423-2
remote_bool	true
author2	He, Ying Yang, Yanfang
author2Str	He, Ying Yang, Yanfang
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doi_str	10.1007/s00339-014-8423-2
up_date	2024-07-03T23:48:33.976Z
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