ジャーナル論文 Near-field photocurrent nanoscopy on bare and encapsulated graphene
Achim Woessner (author) (この著者で検索)
;
Pablo Alonso-González (author) (この著者で検索)
;
Mark B. Lundeberg (author) (この著者で検索)
;
Yuanda Gao (author) (この著者で検索)
;
Jose E. Barrios-Vargas (author) (この著者で検索)
;
Gabriele Navickaite (author) (この著者で検索)
;
Qiong Ma (author) (この著者で検索)
;
Davide Janner (author) (この著者で検索)
;
Kenji Watanabe (author) (この著者で検索)
ORCID SAMURAI ;
Aron W. Cummings (author) (この著者で検索)
;
Takashi Taniguchi (author) (この著者で検索)
ORCID SAMURAI ;
Valerio Pruneri (author) (この著者で検索)
;
Stephan Roche (author) (この著者で検索)
;
Pablo Jarillo-Herrero (author) (この著者で検索)
;
James Hone (author) (この著者で検索)
;
Rainer Hillenbrand (author) (この著者で検索)
;
Frank H. L. Koppens (author) (この著者で検索)
コレクション

引用
Achim Woessner, Pablo Alonso-González, Mark B. Lundeberg, Yuanda Gao, Jose E. Barrios-Vargas, Gabriele Navickaite, Qiong Ma, Davide Janner, Kenji Watanabe, Aron W. Cummings, Takashi Taniguchi, Valerio Pruneri, Stephan Roche, Pablo Jarillo-Herrero, James Hone, Rainer Hillenbrand, Frank H. L. Koppens. Near-field photocurrent nanoscopy on bare and encapsulated graphene. Nature Communications. 2016, 7 (), 10783. https://doi.org/10.1038/ncomms10783
SAMURAI

説明:

(abstract)

We present and apply a new type of opto-electronic nanoscopy to measure locally both the optical and electronic properties of graphene devices. This is achieved by combining scanning near-field infrared nanoscopy with electrical device read-out, allowing infrared photocurrent mapping at length scales of tens of nanometers. We apply this technique to study the impact of edges and grain boundaries on spatial carrier density profiles and local thermoelectric properties.

権利情報:

キーワード: Optoelectronic devices, graphene, nanoscale variations

刊行年月日: 2016-02-26

出版者: Springer Science and Business Media LLC

掲載誌:

  • Nature Communications (ISSN: 20411723) vol. 7 10783

研究助成金:

原稿種別: 出版者版 (Version of record)

MDR DOI:

公開URL: https://doi.org/10.1038/ncomms10783

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更新時刻: 2025-02-27 12:30:51 +0900

MDRでの公開時刻: 2025-02-27 12:30:51 +0900

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