Large amplitude charge noise and random telegraph fluctuations in room-temperature graphene single-electron transistors

Fried, Jasper P.; Bian, Xinya; Swett, Jacob L.; Kravchenko, Ivan I.; Briggs, G. Andrew D.; Mol, Jan A.

doi:10.1039/c9nr08574b

Cited by 15 publications

(16 citation statements)

References 33 publications

(49 reference statements)

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“…Nanopores integrated with complementary nanostructures have received interest in recent years as they have the ability to overcome issues associated with ionic current based nanopore sensing including limited device density [59,60] and low bandwidths. [61][62][63] Such complementary nanostructures include field-effect sensors, [59,[64][65][66] tunneling nanogaps, [67,68] plasmonic nanostructures, [69,70] radiofrequency antennas, [62] and dielectrophoretic electrodes. [9] To date, the development of these devices has been limited by the difficult fabrication processes that are required to integrate pores with complementary nanostructures.…”

Section: Cbd With Microelectrodes On the Membrane Surfacementioning

confidence: 99%

Understanding Electrical Conduction and Nanopore Formation During Controlled Breakdown

Fried

Swett

Nadappuram

et al. 2021

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ionic current therefore provides a simple single-molecule biosensing technique. [1][2][3][4] Indeed, over the past several decades, nanopores have proven to be versatile single-molecule sensing devices with applications ranging from DNA [5,6] and protein sequencing, [7,8] to ultra-dilute analyte detection, [9][10][11][12] polymer data storage, [13,14] and enzymology. [15] Nanopore sensors can be classified as either biological [16] or solid-state. [17] Biological nanopores generally consist of barrel shaped proteins that self-insert into lipid or synthetic membranes. Solid-state nanopores, however, are typically formed in thin (<50 nm) dielectrics such as SiN x , [18] TiO 2 , [19] and HfO 2 [20] or 2D materials such as graphene, [21][22][23] MoS 2 , [6] and hBN. [24] The ability to fabricate solid-state nanopores of different diameters and operate them in a wide range of environmental conditions makes them particularly attractive for many of the applications discussed above. [1,17] In the past, solid-state nanopores were typically fabricated using focused charged particle beams to locally sputter material from the membrane. [25][26][27][28] However, this requires specialized equipment, trained operators, and is a labor intensive process thus limiting the availability of this technique to the wider research community.To overcome these issues, a technique called controlled breakdown (CBD) has been developed to fabricate nanopores in solid-state membranes. [29][30][31] In this method, an electric Controlled breakdown has recently emerged as a highly appealing technique to fabricate solid-state nanopores for a wide range of biosensing applications. This technique relies on applying an electric field of approximately 0.4-1 V nm −1 across the membrane to induce a current, and eventually, breakdown of the dielectric. Although previous studies have performed controlled breakdown under a range of different conditions, the mechanism of conduction and breakdown has not been fully explored. Here, electrical conduction and nanopore formation in SiN x membranes during controlled breakdown is studied. It is demonstrated that for Si-rich SiN x , oxidation reactions that occur at the membrane-electrolyte interface limit conduction across the dielectric. However, for stoichiometric Si 3 N 4 the effect of oxidation reactions becomes relatively small and conduction is predominately limited by charge transport across the dielectric. Several important implications resulting from understanding this process are provided which will aid in further developing controlled breakdown in the coming years, particularly for extending this technique to integrate nanopores with on-chip nanostructures.

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Section: Cbd With Microelectrodes On the Membrane Surfacementioning

confidence: 99%

Understanding Electrical Conduction and Nanopore Formation During Controlled Breakdown

Fried

Swett

Nadappuram

et al. 2021

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“…Recently, Fried et al, investigated the noise characteristics of a graphene quantum dot at room temperature in liquid environments. 67 Unlike reported studies, 68 they observed that the noise was significantly independent of the liquid environment and the substrate. In this study, the noise was attributed to charge trapping and detrapping at the disordered graphene edges.…”

Section: Discussionmentioning

confidence: 70%

Single molecule electronic devices with carbon-based materials: status and opportunity

Ghasemi

Moth‐Poulsen

2021

Nanoscale

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“…This may simplify the complex signal decovolution processes currently required to sequence DNA using biological nanopores where multiple bases reside within the pore at a given time. Graphene and MoS 2 can also be used as field-effect sensors 56,69,167,174 that when integrated with nanopores offer larger detection bandwidths and increased device densities compared to what is possible using ionic current measurements.…”

Section: Electrochemical Reactionmentioning

confidence: 99%

In situsolid-state nanopore fabrication

et al. 2021

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Large amplitude charge noise and random telegraph fluctuations in room-temperature graphene single-electron transistors

Abstract: We analyze the noise in room-temperature liquid-gated quantum dots. We demonstrate large amplitude charge noise and two-level fluctuations in the current level which we attribute to charge trapping at the disordered graphene edges.

Cited by 15 publications

References 33 publications

Understanding Electrical Conduction and Nanopore Formation During Controlled Breakdown

Understanding Electrical Conduction and Nanopore Formation During Controlled Breakdown

Single molecule electronic devices with carbon-based materials: status and opportunity

In situsolid-state nanopore fabrication

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