1988
DOI: 10.1103/physrevb.37.5845
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Structure of the high-TcsuperconductorBa2et al.

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Cited by 3 publications
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“…[ 10,11 ] The p–n junction is a building block for most self‐powered optoelectronic and photovoltaic devices. [ 12 ] Several methods, such as chemical doping, [ 13 ] double electrostatic gating, [ 14 ] and vertical 2D‐based heterostructures, [ 15,16 ] have been utilized to form p–n diodes in 2D materials. However, creating p–n diodes with high stability is particularly difficult in atomically thin TMDs due to challenges in selectively doping them into p‐ or n‐type semiconductors [ 13 ] or the 2D material transfer processes.…”
Section: Introductionmentioning
confidence: 99%
“…[ 10,11 ] The p–n junction is a building block for most self‐powered optoelectronic and photovoltaic devices. [ 12 ] Several methods, such as chemical doping, [ 13 ] double electrostatic gating, [ 14 ] and vertical 2D‐based heterostructures, [ 15,16 ] have been utilized to form p–n diodes in 2D materials. However, creating p–n diodes with high stability is particularly difficult in atomically thin TMDs due to challenges in selectively doping them into p‐ or n‐type semiconductors [ 13 ] or the 2D material transfer processes.…”
Section: Introductionmentioning
confidence: 99%