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10.1088/2399-1984/aa8f91

http://scihub22266oqcxt.onion/10.1088/2399-1984/aa8f91
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suck abstract from ncbi


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pmid29552645
      Nano+Futures 2017 ; 1 (3 ): ä
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  • Observation of Giant Conductance Fluctuations in a Protein #MMPMID29552645
  • Zhang B ; Song W ; Pang P ; Zhao Y ; Zhang P ; Csabai I ; Vattay G ; Lindsay S
  • Nano Futures 2017[]; 1 (3 ): ä PMID29552645 show ga
  • Proteins are insulating molecular solids, yet even those containing easily reduced or oxidized centers can have single-molecule electronic conductances that are too large to account for with conventional transport theories. Here, we report the observation of remarkably high electronic conductance states in an electrochemically-inactive protein, the ~200 kD ?(V)?(3) extracelluar domain of human integrin. Large current pulses (up to nA) were observed for long durations (many ms, corresponding to many pC of charge transfer) at large gap (>5nm) distances in an STM when the protein was bound specifically by a small peptide ligand attached to the electrodes. The effect is greatly reduced when a homologous, weakly-binding protein (?(4)?(1)) is used as a control. In order to overcome the limitations of the STM, the time- and voltage-dependence of the conductance were further explored using a fixed-gap (5 nm) tunneling junction device that was small enough to trap a single protein molecule at any one time. Transitions to a high conductance (~ nS) state were observed, the protein being "on" for times from ms to tenths of a second. The high-conductance states only occur above ~ 100mV applied bias, and thus are not an equilibrium property of the protein. Nanoamp two-level signals indicate the specific capture of a single molecule in an electrode gap functionalized with the ligand. This offers a new approach to label-free electronic detection of single protein molecules. Electronic structure calculations yield a distribution of energy level spacings that is consistent with a recently proposed quantum-critical state for proteins, in which small fluctuations can drive transitions between localized and band-like electronic states.
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