2006
DOI: 10.1016/j.elspec.2005.11.006
|View full text |Cite
|
Sign up to set email alerts
|

Methods in carbon K-edge NEXAFS: Experiment and analysis

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
126
0

Year Published

2010
2010
2016
2016

Publication Types

Select...
7

Relationship

1
6

Authors

Journals

citations
Cited by 159 publications
(128 citation statements)
references
References 20 publications
2
126
0
Order By: Relevance
“…Normalization was performed using reference scans from a clean Si(100) surface together with the flux signal from a 50% transmissive gold grid placed upstream of the sample. 44 We note that at high photon intensity the triethylenediamine-dosed Si(100) surface was susceptible to beam-induced changes in surface composition. However, we were able to strongly limit the deleterious effects of the photon beam on our sample by reducing the intensity of the beam.…”
Section: Experimental and Computational Methodsmentioning
confidence: 99%
“…Normalization was performed using reference scans from a clean Si(100) surface together with the flux signal from a 50% transmissive gold grid placed upstream of the sample. 44 We note that at high photon intensity the triethylenediamine-dosed Si(100) surface was susceptible to beam-induced changes in surface composition. However, we were able to strongly limit the deleterious effects of the photon beam on our sample by reducing the intensity of the beam.…”
Section: Experimental and Computational Methodsmentioning
confidence: 99%
“…TEY was measured by monitoring the drain current to the sample, PEY was measured with a channeltron detector with a retarding voltage of ≈200 V, and FY was measured by a multichannel plate detector with a retarding field of 2600 V. Dark levels were measured and subtracted from the data, and double normalization was done using a gold mesh corrected by a www.afm-journal.de www.MaterialsViews.com photodiode. [83] Peak fitting and tilt angle calculations were done using the Quick AS NEXAFS Tool. [84] All tilt angles are calculated from a peak fit of structure at lower energies than 286 eV, which is in the π* manifold, corresponding to transition dipole moments normal to the face of a conjugated core, along the direction of the carbon π orbitals.…”
Section: Field-effect Transistor Fabrication and Characterizationmentioning
confidence: 99%
“…This can lead to significant errors when analyzing elements that are simultaneously present in multiple layers. In particular, for carbon-based materials previously exposed to air, their carbon K-edge NEXAFS spectra, even when corrected using any of the approaches outlined by Watts et al 52 , are a convolution of the spectrum of the sample of interest and the spectrum of the adventitious carbon contamination on its surface since the thickness of the latter (typically <2 nm 55 ) is smaller than the information depth at the carbon K-edge ( Figure 1). While the thickness of the adventitious carbon contamination has been shown to depend on the sample preparation procedure and history 55,56 , no comprehensive characterization of its composition and structure has yet been published.…”
Section: Introductionmentioning
confidence: 99%
“…While the approaches outlined by Watts et al are effective for addressing the issues commonly encountered in the evaluation of NEXAFS data 52 , the corrected spectra they yield represent the photo-absorption spectra of the specimens under the assumption of structural and compositional homogeneity within the nanometer-scale depth probed by NEXAFS spectroscopy. For electron yield NEXAFS spectroscopy of low-Z elements, the information depth (the specimen thickness measured normal to the surface from which a specified percentage of typically 95% of the detected signal originates) is usually less than 5 nm 1 .…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation