MXenes are a family of two-dimensional transition-metal carbides, nitrides, and carbonitrides first discovered in 2011, made by chemically stripping away the A-layers of a layered ceramic precursor called a MAX phase. The most studied member, Ti3C2Tx, is produced by etching aluminum out of Ti3AlC2 with hydrofluoric acid, leaving behind sheets of titanium carbide decorated with surface terminations such as hydroxyl, oxygen, and fluorine groups. Those terminations are the secret to the material’s compatibility with polymers: they form hydrogen bonds with the hydroxyl-rich backbones of PVA, anchoring the nanosheets into the matrix. Ti3C2Tx is also a superb electrical conductor, with reported conductivities between 2.0 and 2.4 times ten to the fourth siemens per centimeter, making it one of the most attractive fillers available for turning insulating plastics into functional electronic materials.

In the new work, the researchers began by making their own MXene. They slowly added 1.5 grams of Ti3AlC2 MAX phase powder to a 30 weight percent hydrofluoric acid solution, stirred the mixture at 50 degrees Celsius for twelve hours, and then filtered and washed the product until the supernatant reached a neutral pH of roughly seven. To split the resulting multilayered stacks into single and few-layer nanosheets, they intercalated dimethyl sulfoxide into the galleries between layers for a full day, washed out the solvent, and bath-sonicated the sediment in deionized water. The synthesis was verified by X-ray diffraction: the characteristic MAX phase peak near 39 degrees disappeared entirely, while the basal (002) reflection shifted from 9.59 degrees down to 7.19 degrees and broadened, the classic signature of successful etching.

The structural data also revealed a striking expansion of the MXene’s internal architecture. The interlayer spacing increased from 0.922 nanometers in the parent MAX phase to 1.228 nanometers in the MXene, an expansion of about 33 percent that the authors attribute to the removal of the aluminum layers and the attachment of oxygen, hydroxyl, and fluorine surface groups. The average crystallite size dropped slightly from 39.11 to 36.38 nanometers. Electron microscopy showed the transformation vividly: the dense, close-packed plate-like structure of the MAX phase gave way to an accordion-like arrangement of loosely stacked thin nanosheets. Energy-dispersive X-ray spectroscopy confirmed that aluminum content plunged from 9.39 to 1.52 weight percent, while oxygen at 29.76 percent and fluorine at 9.17 percent emerged, evidence of the new surface chemistry.

X-ray photoelectron spectroscopy provided an even finer-grained view of the surface. The team deconvoluted the core-level spectra into their constituent chemical states, identifying carbon-titanium-fluorine terminations, titanium fluoride species, and minor residual fluorinated byproducts in the fluorine 1s region. The carbon 1s spectrum contained the carbide carbon peak at 281.78 electron-volts that defines the intact MXene lattice, alongside adventitious carbon, ether-type carbon, and carboxyl groups. The titanium 2p envelope resolved into three spin-orbit doublet pairs corresponding to the carbide framework, partially oxidized titanium species, and titanium dioxide at the surface, with the expected spin-orbit splitting of about 5.7 electron-volts. Together these results map a complex but chemically coherent surface, rich in the functional groups that bond polymers.

The films themselves were made by a method simple enough to run in any laboratory. PVA and PEG were dissolved together in deionized water at a fixed 80:20 weight ratio, chosen because prior studies show this composition offers optimal miscibility and a good balance between crystallinity and chain mobility. Separately dispersed MXene was added at loadings of 0.5, 1.0, and 1.5 weight percent, the mixture was stirred, ultrasonicated, and drop-cast onto glass, then vacuum-dried. Infrared spectroscopy of the finished films showed the hydroxyl stretching band near 3,420 reciprocal centimeters broadening and shifting to lower wavenumbers as MXene content rose, a sign that hydrogen bonds between the polymer chains and the nanosheets’ surface groups were strengthening. Crucially, no new chemical bands appeared, indicating the composite is held together by physical hydrogen bonding rather than new covalent chemistry.

Perhaps the most subtle result concerns crystallinity. At the lowest loading of 0.5 weight percent, the crystallinity index of the polymer blend jumped from 34.60 to 48.01 percent as measured by X-ray diffraction, and from 42.45 to 49.87 percent by infrared analysis. The well-dispersed nanosheets act as heterogeneous nucleation sites, giving polymer chains additional surfaces on which to organize into ordered crystalline domains. But the effect is non-monotonic. At 1.0 and 1.5 weight percent, the crystallinity index fell back to 42.94 and 33.60 percent respectively, because the two-dimensional sheets begin to confine chain motion and, at higher loadings, partially aggregate, disrupting the regular packing needed for crystal growth. Microstrain and dislocation density rose in parallel, confirming that MXene introduces genuine structural disorder into the lattice even as it nucleates order at low doses.

The optical consequences were the study’s headline. Using ultraviolet-visible absorption spectroscopy and the Tauc method, the team extracted both direct and indirect band gap energies for each film. The pristine PVA/PEG blend, with its saturated, non-conjugated backbone, was a wide-gap insulator with direct and indirect gaps of 5.49 and 5.17 electron-volts. As MXene content increased, the absorption edge red-shifted steadily and the gaps fell monotonically: to 5.42 and 4.93 electron-volts at 0.5 weight percent, 5.17 and 3.88 at 1.0 weight percent, and finally 4.98 and 3.28 electron-volts at 1.5 weight percent. Remarkably, the indirect gap narrowed far more than the direct one, a 36.6 percent reduction versus 9.3 percent. The authors suggest this asymmetry arises because indirect transitions involve phonon-assisted excitation and therefore respond more sensitively to the localized electronic states and structural disorder that MXene introduces into the polymer’s electronic environment.

All the while, the films kept a useful optical property: they remained moderately transparent in the visible region even as their ultraviolet absorption intensified. That combination of enhanced ultraviolet shielding and preserved transparency is exactly what is sought for protective coatings, and the systematic gap tuning opens routes toward flexible optoelectronics, chemical sensors, and energy-related devices built from nothing more exotic than water-soluble polymers and a fraction of a percent of nanosheets. The study demonstrates that in the world of polymer nanocomposites, dosage is destiny: the same nanofiller can nucleate order at one concentration and disrupt it at another, while continuously rewriting the electronic band structure. As MXene research moves from laboratory curiosity toward practical devices, this work offers a clear, quantitative map of how to dial in the properties of a flexible plastic film with nothing more than careful control of filler loading.

Subject of Research: Tuning the structural properties and optical band gap of PVA/PEG polymer nanocomposite thin films with Ti3C2Tx MXene nanosheet loading

Article Title: Effect of Ti3C2Tx MXene content on the structural properties and optical band gap of PVA/PEG nanocomposite thin films

Article References: Effect of Ti3C2Tx MXene content on the structural properties and optical band gap of PVA/PEG nanocomposite thin films. (n.d.). https://doi.org/10.3389/fmats.2026.1934242

Image Credits: AI Generated

DOI: 10.3389/fmats.2026.1934242

Keywords: MXene, Ti3C2Tx, polymer nanocomposites, PVA, PEG, optical band gap, crystallinity index, thin films, X-ray diffraction, UV-Vis spectroscopy, XPS, flexible optoelectronics