2019
DOI: 10.1007/978-3-030-15612-1_9
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Space Charge at Nanoscale: Probing Injection and Dynamic Phenomena Under Dark/Light Configurations by Using KPFM and C-AFM

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Cited by 3 publications
(9 citation statements)
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“…The purpose of the KPFM-AM feedback loop is to adjust the applied compensation dc voltage (V dc ) so that it is equal to the contact surface potential difference (ΔV SP1 ) between the tip and the sample. 22 Therefore the force at frequency ω is zero and the amplitude of the cantilever is zero. This means that the surface potential distribution of the sample can be obtained by detecting the compensation potential V dc when the cantilever amplitude is zero.…”
Section: Methodsmentioning
confidence: 99%
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“…The purpose of the KPFM-AM feedback loop is to adjust the applied compensation dc voltage (V dc ) so that it is equal to the contact surface potential difference (ΔV SP1 ) between the tip and the sample. 22 Therefore the force at frequency ω is zero and the amplitude of the cantilever is zero. This means that the surface potential distribution of the sample can be obtained by detecting the compensation potential V dc when the cantilever amplitude is zero.…”
Section: Methodsmentioning
confidence: 99%
“…The probe and the sample were connected through a common ground, and a contact potential difference was generated between the two. The purpose of the KPFM-AM feedback loop is to adjust the applied compensation dc voltage ( V dc ) so that it is equal to the contact surface potential difference (Δ V SP1 ) between the tip and the sample . Therefore the force at frequency ω is zero and the amplitude of the cantilever is zero.…”
Section: Experimental Sectionmentioning
confidence: 99%
“…While these can be difficult to evaluate quantitatively due to the complicated surface contributions, KPFM is used for evaluating electrostatic-related surface charge distribution and potential electrical conductivity of interacting fibers . Generally, surface potential corresponds to the work function of a material or the energy required to extract an electron from the material’s fundamental state or for insulative materials the charge distribution . Here, we focus on the general correlations between electrostatic potential and spatial distribution differences between the LT, LT-NH, and LT-CF fibers with measurements for the fibers’ electrostatic surface potentials directly derived from KPFM included in Table , column 4.…”
Section: Results and Discussionmentioning
confidence: 99%
“…Surprisingly, the electrostatic surface potential of LT-NH fiber does not change significantly. These differences can be attributed to the different nature and different concentrations of charged surface groups of different polarities, trapped charges, and charge cancellations, but more KPFM measurements should be carefully analyzed for finding properties correlations …”
Section: Results and Discussionmentioning
confidence: 99%
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