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- (395b) Detection of Ions and DNA Hybridization Using Diamond Solution Gate Fets
2. Variation of Ion Sensitivity by Surface Modification and Biomolecule Immobilization. The surface chemical modification can be realized from the H-terminated surface which is a starting diamond surface after the chemical vapour deposition of diamond in the hydrogen atom rich condition. The surface has highly p-type semiconductivity after the adsorption of negatively charged ions in air. The H-terminated surface can attract negative charges because the surface dipoles caused by the electronegativity difference between hydrogen (2.1 in Pauling unit) and carbon (2.5). The charge density of H -C dipoles is about 1E14 e/cm2. This effect is valid in air or in electrolyte solution where negative charged particles are effectively physisorbed on the H-terminated diamond. Using the properties halogen ions such as Cl-, Br-, and I- are detected by the SGFETs down to 1E-7 M [2,3]. Negatively charged biomolecules such as DNA might be also detected if they present in the Helmholtz layer.
3. Sensing of DNA molecules in Helmholtz Layer. The surface carrier density has been affected by the change in electric charge in the Helmholtz layer. When probe DNAs are in the Helmholtz layer hybridise with target DNAs with the equivalent length of charge, the surface holes can be induced by the increase of surface negative charge in the hybridised DNAs and can be detected as the drain current increase or the positive shift of the threshold voltage in the p channel SGFET. It is clearly and reproducibly observed in the diamond SGFET where the surface has been partially aminated (NH2 terminated) and the probe DNAs have been immobilized [7]. The difference between complementary and non complementary target DNA has been detected by the real time shift of gate voltage to keep the constant drain current. The surface density of probe (immobilized) DNA and effective charge of DNA are discussed in our presentation considering the thickness of Debye length.
[1] H.Kawarada et al., Phys. Status Solidi A 185 (2001) 79. [2] H.Kanazawa et al., Diamond Relat. Mater., 12 (2003) 618. [3] K.S. Song, et al., Biosens. Bioelectron. 19(2003) 137. [4] K.S. Song, et al., Jpn. J. Appl. Phys., 43 (2004) L814. [5] J.Garrido, et al., Appl. Phys. Lett. 86 (2005) 073504. [6] W.Yang, et al. Appl. Phys. Lett. 85 (2004) 3626. [7] K.S. Song , H.Kawarada et al. (submitted).