Fig. 6: Mathematical modelling and plasmon resonance energy transfer analysis for probing quantum tunnelling in bio-nanoantennae system. | Nature Nanotechnology

Fig. 6: Mathematical modelling and plasmon resonance energy transfer analysis for probing quantum tunnelling in bio-nanoantennae system.

From: Wireless electrical–molecular quantum signalling for cancer cell apoptosis

Fig. 6

a,b, Mathematic modelling to determine the rate of donor charging, rd, calculated using the metabolic activity, using equation (1), compared to the PEG linker length, L, for [email protected] c@Z (a) and [email protected] c@Z (b) in GIN 31 cell samples. The black lines show the exponential behaviour expected for quantum tunnelling with an inverse localization radius α and constant of proportionality β, shown in the figure legends. Error bars represent ±s.d. of the mean. The x-axis error bar represents the s.d. of the mean PEG linker length, and the y-axis error bar represents the s.d. of the mean rd (rate of Cyt c charging), which was obtained from equations (5)–(7) in the Methods. R2, coefficient of determination. c, Scattering spectra (I, intensity) and spectra difference (Δ) for QBET obtained for [email protected] c@Z bio-nanoantennae. The quantized peaks were obtained from the difference of scattering spectra between the samples functionalized with r.Cyt c and Z using a 2 kDa linker and GNP100. Solid curves are captured scattering spectra (linked to left axis) of [email protected] c@Z, and dashed curves are quantized peaks, that is, the corresponding spectra difference (linked to right axis). Blue arrows indicate a peak shift. LSPR, localized surface plasmon resonance. d, Quantized peaks of [email protected] c@Z within a 530–550 nm region (zoomed-in from c) confirming the presence of o.Cyt c in samples exposed to a.c. EFs.

Source data

Back to article page