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. 2015 Jun 10;5:10941. doi: 10.1038/srep10941

Figure 4.

Figure 4

a) Dark count rate as a function of normalized bias current showing the major contributions to the experimentally measured dark count curves, i.e. false counts due to residual black body radiation and electronic noise. b) Dark count rate as a function of normalized bias current for nanowires of various nanowire widths. The orange dashed lines illustrate the growing contribution of black body radiation for narrower wires.