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. 2019 May 18;20(10):2461. doi: 10.3390/ijms20102461

Figure 3.

Figure 3

(a) The structure of surface plasmon resonance (SPR) sensor and its working principle. (b) Simulated transmittance of light at λ0 = 633 nm (crosses) and measured transmittance of white light (squares) as a function of the number of graphene layers. (c) The SPR curves for the conventional biosensor (L = 0) and the monolayer graphene biosensor (L = 1) for He-Ne laser light. (d) The sensitivity enhancement ΔSRIL/SRI0 as a function of the number of graphene layers L. Reproduced from [68] with permission of the Optical Society of America.