Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions

We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induce...
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Autor*in:	Zhou, Xingfei [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2020

Schlagwörter:	Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions

Übergeordnetes Werk:	Enthalten in: Physics letters / A - Amsterdam : North-Holland Publ., 1967, 384
Übergeordnetes Werk:	volume:384

DOI / URN:	10.1016/j.physleta.2020.126612

Katalog-ID:	ELV004383982

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520			\|a We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling.
650		4	\|a Valley splitting
650		4	\|a Anomalous Klein tunneling
650		4	\|a Borophane
650		4	\|a n-p and n-p-n junctions
773	0	8	\|i Enthalten in \|t Physics letters / A \|d Amsterdam : North-Holland Publ., 1967 \|g 384 \|h Online-Ressource \|w (DE-627)266015298 \|w (DE-600)1466603-0 \|w (DE-576)074959905 \|x 1873-2429 \|7 nnns
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author_variant	x z xz
matchkey_str	article:18732429:2020----::alypitnadnmlukenunlnibrpaea
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publishDate	2020
allfields	10.1016/j.physleta.2020.126612 doi (DE-627)ELV004383982 (ELSEVIER)S0375-9601(20)30479-5 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Zhou, Xingfei verfasserin (orcid)0000-0002-1856-4969 aut Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling. Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 384 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:384 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 384
spelling	10.1016/j.physleta.2020.126612 doi (DE-627)ELV004383982 (ELSEVIER)S0375-9601(20)30479-5 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Zhou, Xingfei verfasserin (orcid)0000-0002-1856-4969 aut Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling. Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 384 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:384 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 384
allfields_unstemmed	10.1016/j.physleta.2020.126612 doi (DE-627)ELV004383982 (ELSEVIER)S0375-9601(20)30479-5 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Zhou, Xingfei verfasserin (orcid)0000-0002-1856-4969 aut Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling. Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 384 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:384 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 384
allfieldsGer	10.1016/j.physleta.2020.126612 doi (DE-627)ELV004383982 (ELSEVIER)S0375-9601(20)30479-5 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Zhou, Xingfei verfasserin (orcid)0000-0002-1856-4969 aut Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling. Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 384 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:384 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 384
allfieldsSound	10.1016/j.physleta.2020.126612 doi (DE-627)ELV004383982 (ELSEVIER)S0375-9601(20)30479-5 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Zhou, Xingfei verfasserin (orcid)0000-0002-1856-4969 aut Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling. Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 384 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:384 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 384
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author	Zhou, Xingfei
spellingShingle	Zhou, Xingfei ddc 530 bkl 33.00 misc Valley splitting misc Anomalous Klein tunneling misc Borophane misc n-p and n-p-n junctions Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions
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topic_title	530 DE-600 33.00 bkl Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions Valley splitting Anomalous Klein tunneling Borophane n-p and n-p-n junctions
topic	ddc 530 bkl 33.00 misc Valley splitting misc Anomalous Klein tunneling misc Borophane misc n-p and n-p-n junctions
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title	Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions
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title_full	Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions
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title_sort	valley splitting and anomalous klein tunneling in borophane-based n-p and n-p-n junctions
title_auth	Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions
abstract	We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling.
abstractGer	We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling.
abstract_unstemmed	We analytically investigate the transport properties of electron in borophane-based n-p and n-p-n junctions. When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. Our work designs an alternative valley splitter and provides an insight into the understanding of the Klein tunneling.
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title_short	Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions
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up_date	2024-07-06T22:48:29.543Z
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When the electron beam in n region go through the n-p junction, the beam will be split into two valley-dependent beam in p region. This comes from the valley-dependent refraction angle induced by the anisotropic band structure of borophane. Interestingly, the behavior of valley splitting can be generated in a borophane-based n-p junction naturally without any external modulation methods. Generally, the Klein tunneling is described as the perfect transmission at a zero incident angle of electron regardless of the width and height of potential barrier. However, in a borophane-based n-p-n junction, the anomalous Klein tunneling, i.e., the perfect transmission exists at a nonzero incident angle, is found due to the anisotropic band structure of borophane. 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Valley splitting and anomalous Klein tunneling in borophane-based n-p and n-p-n junctions

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