3 research outputs found
Origins of Charge Noise in Carbon Nanotube Field-Effect Transistor Biosensors
Determining the major noise sources in nanoscale field-effect
transistor
(nanoFET) biosensors is critical for improving bioelectronic interfaces.
We use the carbon nanotube (CNT) FET biosensor platform to examine
the noise generated by substrate interactions and surface adsorbates,
both of which are present in current nanoFET biosensors. The charge
noise model is used as a quantitative framework to show that insulating
substrates and surface adsorbates are both significant contributors
to the noise floor of CNT FET biosensors. Removing substrate interactions
and surface adsorbates reduces the power spectral density of background
voltage fluctuations by 19-fold
Single Electron Charge Sensitivity of Liquid-Gated Carbon Nanotube Transistors
Random
telegraph signals corresponding to activated charge traps
were observed with liquid-gated CNT FETs. The high signal-to-noise
ratio that we observe demonstrates that single electron charge sensing
is possible with CNT FETs in liquids at room temperature. We have
characterized the gate-voltage dependence of the random telegraph
signals and compared to theoretical predictions. The gate-voltage
dependence clearly identifies the sign of the activated trapped charge
Electrical Monitoring of sp<sup>3</sup> Defect Formation in Individual Carbon Nanotubes
Many carbon nanotube (CNT) applications
require precisely controlled
chemical functionalization that is minimally disruptive to electrical
performance. A promising approach is the generation of sp<sup>3</sup> hybridized carbon atoms in the sp<sup>2</sup>-bonded lattice. We
have investigated the possibility of using a carboxylic acid-functionalized
diazonium reagent to introduce a defined number of sp<sup>3</sup> defects
into electrically contacted CNTs. Having performed real-time measurements
on individually contacted CNTs, we show that the formation of an individual
defect is accompanied by an upward jump in resistance of approximately
6 kΩ. Additionally, we observe downward jumps in resistance
of the same size, indicating that some defects are unstable. Our results
are explained by a two-step reaction mechanism. Isolated aryl groups,
formed in the first step, are unstable and dissociate on the minute
time scale. Stable defect generation requires a second step: the coupling
of a second aryl group adjacent to the first. Additional mechanistic
understanding is provided by a systematic investigation of the gate
voltage dependence of the reaction, showing that defect formation
can be turned on and off. In summary, we demonstrate an unprecedented
level of control over sp<sup>3</sup> defect formation in electrically
contacted CNTs, and prove that sp<sup>3</sup> defects are minimally
disruptive to the electrical performance of CNTs