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Photodiode
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==Materials== The material used to make a photodiode is critical to defining its properties, because only [[photon]]s with sufficient energy to excite [[electron]]s across the material's [[bandgap]] will produce significant photocurrents. Materials commonly used to produce photodiodes are listed in the table below.<ref>Held. G, Introduction to Light Emitting Diode Technology and Applications, CRC Press, (Worldwide, 2008). Ch. 5 p. 116. {{ISBN|1-4200-7662-0}}</ref> {| class="wikitable" ! Material ! [[Electromagnetic spectrum]]<br />[[wavelength]] range (nm) |- | [[Silicon]] || 190β1100 |- | [[Germanium]] || 400β1700 |- | [[Indium gallium arsenide]] || 800β2600 |- | [[Lead(II) sulfide]] || <1000β3500 |- | [[Mercury cadmium telluride]] || 400β14000 |} Because of their greater bandgap, silicon-based photodiodes generate less noise than germanium-based photodiodes. Binary materials, such as MoS<sub>2</sub>, and graphene emerged as new materials for the production of photodiodes.<ref>{{cite journal |last1=Yin |first1=Zongyou |last2=Li |first2=Hai |last3=Li |first3=Hong |last4=Jiang |first4=Lin |last5=Shi |first5=Yumeng |last6=Sun |first6=Yinghui |last7=Lu |first7=Gang |last8=Zhang |first8=Qing |last9=Chen |first9=Xiaodong |last10=Zhang |first10=Hua |title=Single-Layer MoS Phototransistors |journal=ACS Nano |date=21 December 2011 |volume=6 |issue=1 |pages=74β80 |doi=10.1021/nn2024557|pmid=22165908 |arxiv=1310.8066 |s2cid=27038582 }}</ref>
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