However, the identification of different species is discretionary. Computer programs are used to deconvolute the elemental peak.
The peaks may then be assigned to particular species, but the peaks may not correspond with species in the sample. As such, the data obtained must be used cautiously, and care should be taken to avoid over-analyzing data. Despite the aforementioned limitations, XPS is a powerful surface technique that can be used to accurately detect the presence and relative quantities of elements in a sample.
Further analysis can provide information about the state and environment of atoms in the sample, which can be used to infer information about the surface structure of the material. This is particularly useful for carbon nanomaterials, in which surface structure and composition greatly influence the properties of the material.
There is much research interest in modifying carbon nanomaterials to modulate their properties for use in many different applications. Carbon nanomaterials present certain issues in regard to sample preparation. The use of graphite tape is a poor option for carbon nanomaterials because the spectra will show peaks from the graphite tape, adding to the carbon peak and potentially skewing or overwhelming the data. Instead, a thin indium foil between 0. The sample is simply pressed onto a piece of the foil.
The XP survey scan is an effective way to determine the identity of elements present on the surface of a material, as well as the approximate relative ratios of the elements detected.
This has important implications for carbon nanomaterials, in which surface composition is of greatest importance in their uses. XPS may be used to determine the purity of a material. For example, nanodiamond powder is a created by detonation, which can leave nitrogenous groups and various oxygen containing groups attached to the surface. Based on the XPS data, the nanodiamond material is approximately XPS is a useful method to verify the efficacy of a purification process.
For this application, XPS is often done in conjunction with thermogravimetric analysis TGA , which measures the weight lost from a sample at increasing temperatures. TGA data serves to corroborate the changes observed with the XPS data by comparing the percentage of weight loss around the region of the impurity suspected based on the XP spectra.
Additionally, XPS can provide information about the nature of the impurity. In general, the atomic percentage of carbon obtained from the XPS spectrum is a measure of the purity of the carbon nanomaterials. XP spectra give evidence of functionalization and can provide insight into the identity of the functional groups. Carbon nanomaterials provide a versatile surface which can be functionalized to modulate their properties. For example, the sodium salt of phenyl sulfonated SWNTs is water soluble.
High resolution scans of each of the element peaks of interest can be obtained to give more information about the material. This is a way to determine with high accuracy the presence of elements as well as relative ratios of elements present in the sample.
This can be used to distinguish species of the same element in different chemical states and environments, such as through bonding and hybridization, present in the material. The distinct peaks may have binding energies that differ slightly from that of the convoluted elemental peak. The ratios of the intensities of these peaks can be used to determine the percentage of atoms in a particular state. Discrimination between and identity of elements in different states and environments is a strength of XPS that is of particular interest for carbon nanomaterials.
The hybridization of carbons influences the properties of a carbon nanomaterial and has implications in its structure.
XPS can be used to determine the hybridization of carbons on the surface of a material, such as graphite and nanodiamond. Graphite is a carbon material consisting of sp 2 carbons. Thus, theoretically the XPS of pure graphite would show a single C1s peak, with a binding energy characteristic of sp 2 carbon around On the other hand, nanodiamond consists of sp 3 bonded carbons. The XPS of nanodiamond should show a single C1s peak, with a binding energy characteristic of sp 3 carbon around eV.
The ratio of the sp 2 and sp 3 peaks in the C1s spectrum gives the ratio of sp 2 and sp 3 carbons in the nanomaterial. This ratio can be altered and compared by collecting the C1s spectra. For example, laser treatment of graphite creates diamond-like material, with more sp 3 character when a higher laser power is used. Alternatively, annealing nanodiamond thin films at very high temperatures creates graphitic layers on the nanodiamond surface, increasing sp 2 content.
Comparing the relative intensities of various C1s peaks can be powerful in verifying that a reaction has occurred. Fluorinated carbon materials are often used as precursors to a broad range of variously functionalized materials. XPS can also be applied to determine the nature and extent of functionalization.
In general, binding energy increases with decreasing electron density about the atom. Species with more positive oxidation states have higher binding energies, while more reduced species experience a greater degree of shielding, thus increasing the ease of electron removal.
The method of fluorination of carbon materials and such factors as temperature and length of fluorination affect the extent of fluoride addition as well as the types of carbon-fluorine bonds present. A survey scan can be used to determine the amount of fluorine compared to carbon. High resolution scans of the C1s and F1s peaks can also give information about the proportion and types of bonds.
A shift in the peaks, as well as changes in peak width and intensity, can be observed in spectra as an indication of fluorination of graphite. Krick , Tevis D. Jacobs , Subarna R. Khanal , Frank Streller , J. Prasad , Thomas W.
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Surface and Coatings Technology , , Pair your accounts. These reference pages contain tips and techniques that are designed to help both the novice and advanced XPS user. Hydrogen and Helium. Hydrogen and helium are essentially impossible to detect by a lab-based XPS. Helium is not normally present as a solid and even when present implanted in a solid its 1s orbital has a very small cross-section for photoemission.
Hydrogen also has an extremely small photoelectron cross-section and suffers from having to share its only electron in forming compounds, which then resides in a valence-like orbital.
Recent work [1] using a synchrotron based ambient pressure AP XPS has shown that it is possible to detect these elements with these specialized instruments. A lower energy, high flux X-ray source increases the cross-section for H and He dramatically, and ambient pressure apparatus are needed to handle these gas phase elements.
Note that lab based AP-XPS cannot detect these elements - the synchrotron source is essential for this type of work.
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