Summary
The article discusses a method for accurately determining the band gap energy of modified semiconductor photocatalysts using UV–Vis spectra. The researchers provide a detailed explanation of the process, including the importance of understanding the band gap energy in the context of photocatalytic applications. The article also covers the limitations of previous methods and the potential benefits of using UV–Vis spectra to determine the band gap energy. Additionally, the authors discuss the relevance of this research to real-world applications, such as water purification and environmental remediation. The article concludes by highlighting the potential of this method to improve the efficiency and effectiveness of photocatalytic systems.”,“prompt_2”:“ACS Journal Article on Photocatalyst Band Gap Energy”,“prompt_3”:”{“Main Topic”: “Photocatalyst”, “Relevant Topic”: “Band Gap Energy”, “Key Concept”: “UV–Vis Spectra
Content
A misuse of the Tauc plot to determine the band gap energy of semiconductors may lead to erroneous estimates. Particularly large errors can be associated with characterization of modified semiconductors showing a significant absorption of sub-band gap energy photons. Taking the model methyl orange/titanium dioxide system, we address the problem and discuss how to apply the Tauc method correctly.
The band gap energy of a semiconductor describes the energy needed to excite an electron from the valence band to the conduction band. An accurate determination of the band gap energy is crucial in predicting photophysical and photochemical properties of semiconductors. In particular, this parameter is often referred to when photocatalytic properties of semiconductors are discussed. In 1966 Tauc proposed a method of estimating the band gap energy of amorphous semiconductors using optical absorption spectra. (1) His proposal was further developed by Davis and Mott. (2,3)
The Tauc method is based on the assumption that the energy-dependent absorption coefficient α can be expressed by the following equation ():
where h is the Planck constant, ν is the photon’s frequency, Eg is the band gap energy, and B is a constant. The γ factor depends on the nature of the electron transition and is equal to 1/2 or 2 for the direct and indirect transition band gaps, respectively. (4) The band gap energy is usually determined from diffuse reflectance spectra. According to the theory of P. Kubelka and F. Munk presented in 1931, (5) the measured reflectance spectra can be transformed to the corresponding absorption spectra by applying the Kubelka–Munk function (F(R∞), ).
where is the reflectance of an infinitely thick specimen, while K and S are the absorption and scattering coefficients, respectively. (6) Putting F(R∞) instead of α into yields the form ()
Figure 1 shows the reflectance spectrum of TiO2 (an indirect band gap semiconductor) transformed according to plotted against the photon energy. The region showing a steep, linear increase of light absorption with increasing energy is characteristic of semiconductor materials. The x-axis intersection point of the linear fit of the Tauc plot gives an estimate of the band gap energy.
Figure 1
Figure 1. Method of band gap energy (Eg) determination from the Tauc plot. The linear part of the plot is extrapolated to the x-axis.
This approach can be applied for all semiconducting materials that do not absorb light of the sub-band gap energy (or show a negligible absorbance), as exemplified in Figure 1. When it is applied to materials showing a considerable absorbance at energies below Eg, the obtained results may be significantly distorted. It is the case for defected, doped, bulk, or surface modified materials. All these modifications may introduce intraband gap states that reflect in the absorption spectrum as an Urbach tail, i.e., an additional, broad absorption band. Its presence influences the Tauc plot and therefore must be taken into account to determine the band gap energy. In such cases, a direct application of the Tauc method results in an inaccurate estimation of Eg. This error appears frequently in several publications in which authors incorrectly interpret the shift of the x-axis intersection point (zero of the fitting function) to lower values as reducing the band gap energy. In fact, the apparent Eg reduction is due to the inapplicability of the Tauc method in such cases. Researchers are well aware of the problem, and therefore, various attempts to improve the band gap estimation, such as the Cody plot (compare Supporting Information) or others, have been developed and investigated. (7−10) The Tauc plots presented in Figure 2A were used to determine the band gap energies ( , column 1). All determined band gap energies are smaller than that found for the original TiO2 sample (3.22 eV).
Figure 2
Figure 2. Tauc plots of the bare TiO2, methyl orange, (A) MO + TiO2 sample, and (B) MO|TiO2 system (linear fit for measurement b (blue line) and c (green line) overlap). Numbered spectra were recorded for the same pellet differently placed in the holder. The insets show schematically the sample in the holder.
Table 1. Experimental Eg Values Obtained from the Direct Application of the Tauc Plot (Column no. 1), from the Tauc Plot Applied to the Differential Spectra (Column no. 2), and from the Simplified Analysis of the Tauc Plot (Column no. 3)
To verify the applicability of the Tauc method, another set of spectra was recorded. Barium sulfate mixtures, ground separately with titania and MO, were placed side by side in the holder (system denoted as MO|TiO2; Figure 2B, inset). Collected spectra were transformed into the Tauc plot, as presented in Figure 2B. The determined values of x-axis intersection points are presented in (column 1). All spectra show a steep change of absorbance in the UV region, which is characteristic of wide band gap semiconductors. Comparing spectra of the MO|TiO2 system and MO + TiO2 sample reveals the distinct differences. Absorption spectra (or F(R∞)) of the MO|TiO2 system are the spectral sums of two components (MO and TiO2), while in the MO + TiO2 sample, where both components can interact, the resulting spectra may not be a simple sum of the components spectra. Therefore, the obtained values of band gap energy are incorrect.
According to the Beer–Lambert law, the spectrum of any mixture, including a semiconductor modified by an organic dye, is the linear combination of the spectra of both components:
where a and b determine the contributions of the components (they depend on the components concentrations), while αs(hν) and αm(hν) are the absorption coefficients of the semiconductor and organic dye. The Tauc transformation ( ) should not be directly applied to the spectrum of both components together, but to the spectrum of the semiconductor alone (αs(**hν)). Therefore, an appropriate approach to determine the band gap energy should involve the withdrawal of the semiconductor spectrum from the spectral sum. Figure 3A shows the Tauc plots of the semiconductor spectra obtained by subtracting the MO component from the recorded spectra (αs(**hν) = α(**hν) – c·αm(**hν)).
Figure 3
Figure 3. Tauc plots of the TiO2 components (extracted from the spectra of the MO|TiO2 system) and bare TiO2 (A). The Tauc plots of the differential spectra of the sample MO + TiO2 and bare TiO2 (B). The determinations of Eg for measurements 1 (4A) and 3 (4B) are shown as insets.
To account for different concentrations of MO component, the spectrum of MO needs to be normalized to the corresponding level of MO concentration in the sample (parameter c). The values of the band gap energy were determined as for a neat semiconductor ( , column no. 2).
An analogous analysis made for the MO + TiO2 sample (Figure 3B) revealed similar Eg values listed in column no. 2 ( ). All Eg values for both systems (MO|TiO2, MO + TiO2) are nearly the same, within a margin of error, with Eg measured for bare TiO2 (3.22 eV). These results prove that the adsorbed dye does not influence the band gap energy of TiO2.
Since it is often hard to split the Kubelka–Munk spectrum into spectra of individual components, a simplified procedure can be considered. As in the method described by Tauc, the linear fit of the fundamental peak is applied. Additionally, a linear fit used as an abscissa is applied for the slope below the fundamental absorption. An intersection of the two fitting lines gives the band gap energy estimation, as shown in Figure 4 ( , column no. 3).
Figure 4
Figure 4. Transformed reflectance spectrum plot of sample MO + TiO2 (A) and MO|TiO2 system (B). The determination of the Eg is shown.
The approach presented in Figure 4 can be justified by the following analysis. When γ = 1/2 (direct band gap) and the system is composed of two components, the Tauc equation (), according to (), takes the following form ()
(5)
Expansion of the square of sum results in :
(6)
Analogously, when γ = 2 (indirect band gap) and the system is composed of two components, the Tauc equation (), according to (), takes the form ()
(7)
The Taylor series expansion of the square root of the sum results in :
(8)
When **hν → Eg, then αs(**hν) > 0 and αm(**hν) > 0, and it is impossible to eradicate the αm(**hν) influence on the band gap energy estimate from and . In order to do so, the αm(**hν) must be equated to 0. The graphical equivalent of such operation is the use of αm(**hν) as the baseline in the sub-band gap region of the Tauc plot (Figure 4). When αm(**hν) ≅ 0, takes the form (αs(**hν)**hν)2 = B(**hν – Eg), while takes the form (αs(**hν)**hν)1/2 = B(**hν – Eg). Such analysis enables the band gap energy to be obtained directly from the plot. Therefore, the use of this baseline approach presented in Figure 4 leads to much more accurate values of Eg than the method presented in Figure 2.
Comparing the obtained results to the independently determined band gap energy of pure TiO2 leads to the conclusion that in the case of semiconductors modified with an organic dye, the directly applied Tauc method is the least accurate way of determining the band gap energy. We are aware that the selected organic dye serves as a pH indicator, and its spectral changes can be noticed since the surfaces of BaSO4 and TiO2 are slightly basic and acidic, respectively. However, spectral changes caused by the pH variations are insignificant and their impact on the final band gap estimation is negligible. The results obtained by applying the Tauc method give a lower estimate of Eg and often lead to incorrect conclusions concerning the reduction of Eg or photosensitization of the semiconductor. Calculating the band gap energy using the presented methods gives more accurate results in such cases. A more optimal approach to determining the band gap energy is based on the Lambert–Beer law, which allows us to deconvolute the spectrum of both components into the spectra of individual components. The direct application of Tauc method is only appropriate for spectra of bare semiconductors. If deconvolution of the spectrum into the spectra of components is not feasible, a more accurate estimate can be obtained through the use of the presented baseline method. The analysis of other dye–semiconductor systems leads to similar results, as shown for selected cases in the Supporting Information.
To further demonstrate the correctness of the proposed approach, reflectance spectra of doped rutile (with Fe3+ and VO3– ions) and surface modified anatase (with catechol) were analyzed, as well as the mixture of two semiconductors (CdS|TiO2). All results are presented in the Supporting Information. It is important to understand the nature of surface modification and doping (small dopant loading ratio). The surface complex does not influence the band gap of the bulk material. The absorption band that appears at lower energies (longer wavelengths) than the absorption band of the semiconductor comes from CT complexes formed at the surface of TiO2. The Tauc plot may be used to obtain the complex excitation energy. In the case of small dopant concentration the additional electron states appear within the band gap of the semiconductor. As a result, the broad absorption band appears in the material spectrum. The results show that even if the interactions between components are stronger, the use of the baseline approach gives very satisfying results.
The Tauc method was applied to the diffuse reflectance spectra of a ground mixture of titanium dioxide (TiO2, anatase, AK-1, Tronox) with methyl orange (C14H14N3NaO3S, MO, POCh) in a 1:1 mass ratio (MO + TiO2), as well as TiO2 and MO alone. The spectra were recorded using a UV–vis–NIR spectrophotometer (UV-3600 Shimadzu) equipped with a 15 cm integrating sphere in the spectral range 250–800 nm. Each time the sample holder was rotated to a different position (by ∼45°). Barium sulfate (BaSO4, Riedel-de Haen) was used to dilute the samples (1:100) and was used as a reference. The collected R∞(λ) spectra were transformed according to and .
Supporting Information
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The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acs.jpclett.8b02892.
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Systems with different organic dyes showing the same dependence; comparison of the results obtained by Tauc plots with results obtained using Cody plots (PDF)
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Author Information
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- Patrycja Makuła, Faculty of Chemistry, Jagiellonian University in Kraków, ul. Gronostajowa 2, 30-387 Kraków, Poland
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Michał Pacia, Faculty of Chemistry, Jagiellonian University in Kraków, ul. Gronostajowa 2, 30-387 Kraków, Poland
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The authors declare no competing financial interest.
Acknowledgments
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The work was supported by the National Science Centre (Poland) within the project number 2015/19/B/ST5/00950 (OPUS 10) and the Foundation for Polish Science (project number TEAM/2016-3/27).
This article references 10 other publications.
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Tauc, J.; Grigorovici, R.; Vancu, A. Optical Properties And Electronic Structure of Amorphous Germanium. Phys. Status Solidi B 1966, 15, 627– 637, DOI: 10.1002/pssb.19660150224
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Optical properties and electronic structure of amorphous germanium
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Physica Status Solidi (1966), 15 (2), 627-37CODEN: PHSSAK; ISSN:0031-8957.
The optical consts. of amorphous Ge are detd. for photon energies 0.08-1.6 ev. From 0.08 to 0.5 ev., the absorption is due to k-conserving transitions of holes between the valence bands as in p-type crystals; the spin-orbit splitting is 0.20 and 0.21 ev. in nonannealed and annealed samples, resp. The effective masses of the holes in the 3 bands are 0.49 m (0.43 m), 0.04 m, and 0.08 m. An absorption band is observed below the main absorption edge (at 300°K. the max. of this band is at 0.86 ev.); the absorption in this band increases with increasing temp. This band is due to excitons bound to neutral acceptors, and these are presumably the same ones that play a decisive role in the transport properties, which are considered to be assocd. with vacancies. The absorption edge has the form ω2ε2 ∼ (ℏω - Eg)2 (Eg = 0.88 ev. at 300°K.). This suggests that the optical transitions conserve energy but not k vector, and that the ds. of states near the band extrema have the same energy dependence as in cryst. Ge. A simple theory describing this situation is proposed, and comparison of it with the exptl. results leads to an estimate of the localization of the conduction-band wave functions. 24 references.
Davis, E.; Mott, N. Conduction in non-crystalline systems V. Conductivity, optical absorption and photoconductivity in amorphous semiconductors. Philos. Mag. 1970, 22, 0903– 0922, DOI: 10.1080/14786437008221061
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Conduction in noncrystalline systems. V. Conductivity, optical absorption, and photoconductivity in amorphous semiconductors
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The exptl. evidence concerning the d. of states in amorphous semiconductors and the ranges of energy in which states are localized is reviewed; this includes d.c. and a.c. cond., drift mobility, and optical absorption. There is evidence that for some chalcogenide semiconductors the model proposed by Cohen, Fritzsche, and Ovshinsky (1969) should be modified by introducing a band of localized states, near the center of the gap. The values of C, when the d.c. cond. is expressed as C exp (-E/kT), are considered. The behavior of the optical absorption coeff. near the absorption edge and its relation to exciton formation are discussed. Finally, an interpretation of some results on photocond. is offered.
Mott, N. F.; Davis, E. A. Electronic Processes in Non-Crystalline Materials; OUP Oxford, 2012.
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López, R.; Gómez, R. Band-gap Energy Estimation From Diffuse Reflectance Measurements on Sol–Gel and Commercial TiO2: a Comparative Study. J. Sol-Gel Sci. Technol. 2012, 61, 1– 7, DOI: 10.1007/s10971-011-2582-9
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Band-gap energy estimation from diffuse reflectance measurements on sol-gel and commercial TiO2: a comparative study
Lopez, Rosendo; Gomez, Ricardo
Journal of Sol-Gel Science and Technology (2012), 61 (1), 1-7CODEN: JSGTEC; ISSN:0928-0707. (Springer)
A comparison of the band gap energy estd. from UV-vis reflectance spectra of TiO2 powders prepd. by sol-gel route vs. com. TiO2 powders, nanopowder, bulk powder and P25 is reported. The exptl. results obtained from the optical absorption spectra were reported for all the TiO2 samples. Graphic representations were used to calc. Eg: absorbance vs. λ; F(R) vs. E; (F(R) hν)n vs. E, with n = 1/2 for an indirect allowed transition and n = 2 for a direct allowed transition. From the results, it could be seen that Eg strongly varied according to the equation used for the graphic representation. Differences in Eg up to 0.5 eV for the same semiconductor depending on the transition chosen were obsd. Accurate Eg estn. in the four semiconductors studied was obtained by using the general equation α (hν) ≈ B (hν - Eg)n (where α ∼ F(R)) and indirect allowed transition.
Liu, P.; Longo, P.; Zaslavsky, A.; Pacifici, D. Optical Bandgap of Single-and Multi-Layered Amorphous Germanium Ultra-Thin Films. J. Appl. Phys. 2016, 119, 014304, DOI: 10.1063/1.4939296
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Optical bandgap of single- and multi-layered amorphous germanium ultra-thin films
Liu, Pei; Longo, Paolo; Zaslavsky, Alexander; Pacifici, Domenico
Journal of Applied Physics (Melville, NY, United States) (2016), 119 (1), 014304/1-014304/9CODEN: JAPIAU; ISSN:0021-8979. (American Institute of Physics)
Accurate optical methods are required to det. the energy bandgap of amorphous semiconductors and elucidate the role of quantum confinement in nanometer-scale, ultra-thin absorbing layers. Here, we provide a crit. comparison between well-established methods that are generally employed to det. the optical bandgap of thin-film amorphous semiconductors, starting from normal-incidence reflectance and transmittance measurements. First, we demonstrate that a more accurate est. of the optical bandgap can be achieved by using a multiple-reflection interference model. We show that this model generates more reliable results compared to the widely accepted single-pass absorption method. Second, we compare two most representative methods (Tauc and Cody plots) that are extensively used to det. the optical bandgap of thin-film amorphous semiconductors starting from the extd. absorption coeff. Anal. of the exptl. absorption data acquired for ultra-thin amorphous germanium (a-Ge) layers demonstrates that the Cody model is able to provide a less ambiguous energy bandgap value. Finally, we apply our proposed method to exptl. det. the optical bandgap of a-Ge/SiO2 superlattices with single and multiple a-Ge layers down to 2 nm thickness. (c) 2016 American Institute of Physics.
Nowak, M.; Kauch, B.; Szperlich, P. Determination of Energy Band Gap of Nanocrystalline SbSi Using Diffuse Reflectance Spectroscopy. Rev. Sci. Instrum. 2009, 80, 046107, DOI: 10.1063/1.3103603
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Determination of energy band gap of nanocrystalline SbSI using diffuse reflectance spectroscopy
Nowak, M.; Kauch, B.; Szperlich, P.
Review of Scientific Instruments (2009), 80 (4), 046107/1-046107/3CODEN: RSINAK; ISSN:0034-6748. (American Institute of Physics)
Twelve methods of detg. energy band gap (Eg) of semiconductors using diffuse reflectance spectroscopy were applied in studies of sonochem. produced Sb sulfoiodide (SbSI) consisting of nanowires. The best method of detg. Eg is based on simultaneous fitting of many mechanisms of absorption to the spectral dependence of Kubelka-Munk function evaluated from the diffuse reflectance data. It allows detg. the values of indirect forbidden Eg, the Urbach energy, and the const. absorption/scattering of the examd. semiconductor. (c) 2009 American Institute of Physics.
Raciti, R.; Bahariqushchi, R.; Summonte, C.; Aydinli, A.; Terrasi, A.; Mirabella, S. Optical Bandgap of Semiconductor Nanostructures: Methods for Experimental Data Analysis. J. Appl. Phys. 2017, 121, 234304, DOI: 10.1063/1.4986436
9
Optical bandgap of semiconductor nanostructures: Methods for experimental data analysis
Raciti, R.; Bahariqushchi, R.; Summonte, C.; Aydinli, A.; Terrasi, A.; Mirabella, S.
Journal of Applied Physics (Melville, NY, United States) (2017), 121 (23), 234304/1-234304/9CODEN: JAPIAU; ISSN:0021-8979. (American Institute of Physics)
Detn. of the optical bandgap (Eg) in semiconductor nanostructures is a key issue in understanding the extent of quantum confinement effects (QCE) on electronic properties and it usually involves some anal. approxn. in exptl. data redn. and modeling of the light absorption processes. Here, we compare some of the anal. procedures frequently used to evaluate the optical bandgap from reflectance (R) and transmittance (T) spectra. Ge quantum wells and quantum dots embedded in SiO2 were produced by plasma enhanced chem. vapor deposition, and light absorption was characterized by UV-Vis/NIR spectrophotometry. R&T elaboration to ext. the absorption spectra was conducted by two approximated methods (single or double pass approxn., single pass anal., and double pass anal., resp.) followed by Eg evaluation through linear fit of Tauc or Cody plots. Direct fitting of R&T spectra through a Tauc-Lorentz oscillator model is used as comparison. Methods and data are discussed also in terms of the light absorption process in the presence of QCE. The reported data show that, despite the approxn., the DPA approach joined with Tauc plot gives reliable results, with clear advantages in terms of computational efforts and understanding of QCE. (c) 2017 American Institute of Physics.
Murphy, A. B. Band-gap determination from diffuse reflectance measurements of semiconductor films, and application to photoelectrochemical water-splitting. Sol. Energy Mater. Sol. Cells 2007, 91, 1326– 1337, DOI: 10.1016/j.solmat.2007.05.005
10
Band-gap determination from diffuse reflectance measurements of semiconductor films, and application to photoelectrochemical water-splitting
Murphy, A. B.
Solar Energy Materials & Solar Cells (2007), 91 (14), 1326-1337CODEN: SEMCEQ; ISSN:0927-0248. (Elsevier B.V.)
Measurements of the diffuse reflectance of TiO2 semiconductor coatings, such as are used for H2O splitting, are analyzed using the Kubelka-Munk radiative transfer model. The widely used practice of detg. the band gap of the coating directly from the diffuse reflectance is inaccurate, since the diffuse reflectance depends on parameters such as the thickness, refractive index and surface roughness of the coating. However, the absorption coeff. can be derived from the diffuse reflectance using an inversion method; the band gap can then be obtained from the absorption coeff. Finally, the diffuse reflectance of C-doped TiO2 presented by Khan et al. [Science 297(2002) 2243-2245] is analyzed; while the band-gap wavelength is extended into the visible region, it is overestimated. Also, light at visible wavelengths is only very weakly absorbed, and is expected to make only a minor contribution to the H2O-splitting efficiency.
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- Norifumi Asakuma, Minami Iijima, Tomoyuki Tamura, Sawao Honda, Daisuke Urushihara, Toru Asaka, Samuel Bernard, Yuji Iwamoto. In Situ Single-phase Formation of LaCl(CN2) Mixed-Anion Compound Via Controlled Pyrolysis of La3+ Modified Melamine Precursor. Inorganic Chemistry 2024, 63 (43) , 20380-20387. https://doi.org/10.1021/acs.inorgchem.4c02605
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- Juanita Hidalgo, Joachim Breternitz, Daniel M. Többens, Diana K. LaFollette, Charles N. B. Pedorella, Meng-Ju Sher, Susan Schorr, Juan-Pablo Correa-Baena. Br-Induced Suppression of Low-Temperature Phase Transitions in Mixed-Cation Mixed-Halide Perovskites. Chemistry of Materials 2024, 36 (20) , 10167-10175. https://doi.org/10.1021/acs.chemmater.4c01670
- Md Ariful Hoque, Josiel Barrios Cossio, Marcelo I. Guzman. Photocatalysis of Adsorbed Catechol on Degussa P25 TiO2 at the Air–Solid Interface. The Journal of Physical Chemistry C 2024, 128 (41) , 17470-17482. https://doi.org/10.1021/acs.jpcc.4c05777
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- David Šorm, Jiří Brus, Albin Pintar, Jan Sedláček, Sebastijan Kovačič. Hierarchically Porous Polyacetylene Networks: Adsorptive Photocatalysts for Efficient Bisphenol A Removal from Water. ACS Polymers Au 2024, 4 (5) , 420-427. https://doi.org/10.1021/acspolymersau.4c00032
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- Elius Hossain, Kye-Si Kwon. Fabrication and Characterization of Zinc Oxide Nanorods on Electrohydrodynamic Jet Printed Silver Micropillars. ACS Applied Electronic Materials 2024, 6 (9) , 6466-6476. https://doi.org/10.1021/acsaelm.4c00946
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- B. Durga Lakshmi, Betha Veera Vamsi Krishna, P. Tirupathi Rao, Abhinash Marukurti, Vasudha K, Esub Basha Sk, K Ramachandra Rao. Novel Synthesis and Biophysical Characterization of Zinc Oxide Nanoparticles Using Virgin Coconut Oil. ACS Omega 2024, 9 (37) , 38396-38408. https://doi.org/10.1021/acsomega.4c01727
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- Mirosław Mączka, Szymon Smółka, Dagmara Stefańska, Anna Gągor, Jan K. Zaręba, Katarzyna Fedoruk-Piskorska, Maciej Ptak, Dawid Drozdowski, Adam Sieradzki. Multinoncentrosymmetric Two-Dimensional Trilayered Lead Bromide Perovskites with Methylhydrazinium Cations: Lattice Dynamics, Phase Transitions, Dielectric Response, and Optical Properties. Chemistry of Materials 2024, 36 (17) , 8286-8299. https://doi.org/10.1021/acs.chemmater.4c01174
- Lukáš Petřkovský, Ivo Kuřitka, Jiří Zedník, Jiří Vohlídal, Vojtěch Nádaždy, Jakub Ševčík, David Škoda, Bita Ghasemi, Michal Urbánek, Barbora Hanulíková, Pavel Urbánek. Revival of Polyacetylenes in Electronics: Green Light-Emitting Diodes. Macromolecules 2024, 57 (16) , 7808-7819. https://doi.org/10.1021/acs.macromol.4c00862
- Raphael Präg, Moritz Kölbach, Fatwa F. Abdi, Ibbi Y. Ahmet, Markus Schleuning, Dennis Friedrich, Roel van de Krol. Photoelectrochemical Properties of CuFeO2 Photocathodes Prepared by Pulsed Laser Deposition. Chemistry of Materials 2024, 36 (16) , 7764-7780. https://doi.org/10.1021/acs.chemmater.4c00903
- Anna Jędras, Jakub Matusik, Esakkinaveen Dhanaraman, Yen-Pei Fu, Grzegorz Cempura. Tuning the Structural and Electronic Properties of Zn–Cr LDH/GCN Heterostructure for Enhanced Photodegradation of Estrone in UV and Visible Light. Langmuir 2024, 40 (34) , 18163-18175. https://doi.org/10.1021/acs.langmuir.4c01897
- Anders B. Borup, Nanna Bjerre-Christensen, Andreas D. Bertelsen, Aref H. Mamakhel, Martin Bondesgaard, Bo B. Iversen. Continuous-Flow Synthesis of Zn1–xMnxS Nanoparticles at Ambient Conditions. Inorganic Chemistry 2024, 63 (34) , 15716-15723. https://doi.org/10.1021/acs.inorgchem.4c01629
- Spandana Gonuguntla, Chandra Shobha Vennapoosa, B. Moses Abraham, Annadanam V. Sesha Sainath, Ujjwal Pal. Charge Transfer-Regulated Bimetallic ZnCd-ZIF-8/Graphene Oxide Hybrid Nanostructures for Solar Hydrogen Generation. ACS Applied Nano Materials 2024, 7 (16) , 18146-18156. https://doi.org/10.1021/acsanm.3c02870
- Xiaoping Chen, Ira Volkova, Yulong Wang, Ziyu Zhang, Christian A. Nijhuis. Gradual Change between Coherent and Incoherent Tunneling Regimes Induced by Polarizable Halide Substituents in Molecular Tunnel Junctions. Journal of the American Chemical Society 2024, 146 (33) , 23356-23364. https://doi.org/10.1021/jacs.4c06295
- Anastasiya Popova, Darya Yu. Advakhova, Alexander N. Sheveyko, Konstantin A. Kuptsov, Pavel Slukin, Sergei G. Ignatov, Alla Ilnitskaya, Roman V. Timoshenko, Alexander S. Erofeev, Aleksandr A. Kuchmizhak, Balasubramanian Subramanian, Dmitry V. Shtansky. Synergistic Bactericidal Effect of Zn2+ Ions and Reactive Oxygen Species Generated in Response to Either UV or X-ray Irradiation of Zn-Doped Plasma Electrolytic Oxidation TiO2 Coatings. ACS Applied Bio Materials 2024, 7 (8) , 5579-5596. https://doi.org/10.1021/acsabm.4c00685
- Natalia Majewska, Mu-Huai Fang, Sebastian Mahlik. Photoelectric Studies as the Key to Understanding the Nonradiative Processes in Chromium Activated NIR Materials. Journal of the American Chemical Society 2024, 146 (32) , 22807-22817. https://doi.org/10.1021/jacs.4c08011
- Qinyi Zhu, Shuoshuo Zang, Guoqing Xu, Yan Yu, Hewen Liu. Color Turning of One-Dimensional Broadband Emissive Organic Lead Bromide Perovskites. The Journal of Physical Chemistry C 2024, 128 (31) , 12822-12828. https://doi.org/10.1021/acs.jpcc.4c02556
- Long Chen, Jiyou Zhong. Efficient and Tunable Near-Infrared Luminescence in Cubic Phosphate K2AlTi(PO4)3:Cr3+ for Spectroscopy Applications. ACS Applied Materials & Interfaces 2024, 16 (31) , 41119-41126. https://doi.org/10.1021/acsami.4c06635
- Milind Pawar, Anthony Annerino, Jacob Shell, Pelagia-Irene Gouma. Photocatalytic Desulfurization of Thiophene with Chevrel Phase Ni2Mo6S8 Synthesized by SHS. ACS Omega 2024, 9 (31) , 33935-33940. https://doi.org/10.1021/acsomega.4c04213
- Qiang Wang, Lina Kong, Jianping Xu, Baozeng Zhou, Xiaofan Liu, Ziyu Lin, Shaobo Shi, Xiaosong Zhang, Lan Li. Dual-Driven Interfaces of a CoP/CoO Cocatalyst on a Host Photocatalyst for Rapid Charge Transport in Solar-Driven H2 Evolution. ACS Sustainable Chemistry & Engineering 2024, 12 (31) , 11717-11727. https://doi.org/10.1021/acssuschemeng.4c03443
- Wenli Bi, Jia Wang, Ruoyu Zhang, Qingfeng Ge, Xinli Zhu. Tuning Interfacial Sites of WOx/Pt for Enhancing Reverse Water Gas Shift Reaction. ACS Catalysis 2024, 14 (15) , 11205-11217. https://doi.org/10.1021/acscatal.4c02341
- Do Hyung Han, Hyunsu Park, Tomoyo Goto, Yeongjun Seo, Yoshifumi Kondo, Sunghun Cho, Tohru Sekino. Stoichiometric Study on Ion Composition of a Precursor in Chemical Bottom-Up Synthesis for Peroxo-Titanate. ACS Omega 2024, 9 (30) , 33293-33300. https://doi.org/10.1021/acsomega.4c05470
- Shalu Atri, Elham Loni, Frantisek Zazimal, Karol Hensel, Maria Caplovicova, Gustav Plesch, Xin Lu, Rajamani Nagarajan, Michael Naguib, Olivier Monfort. MXene-Derived Oxide Nanoheterostructures for Photocatalytic Sulfamethoxazole Degradation. ACS Applied Nano Materials 2024, 7 (14) , 16506-16515. https://doi.org/10.1021/acsanm.4c02523
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- Sandeep Kumar Singh, Sankeerthana Avasarala, Mahima S, Suryasarathi Bose. Persea Americana Leaf Extract-Derived Nanohybrids: A Sustainable and Green Approach for Rapid Photocatalytic Degradation of Organic Contaminants in Water. ACS Sustainable Resource Management 2024, 1 (7) , 1501-1511. https://doi.org/10.1021/acssusresmgt.4c00118
- Mengjie Zhou, Shuo Xu, Wenjie Zhang, Ge Shi, Yanjie He, Xiaoguang Qiao, Xinchang Pang. How Luminescence Performances of Silicon-Doped Carbon Dots Contribute to Copper-Catalyzed photoATRP?. ACS Catalysis 2024, 14 (14) , 10418-10426. https://doi.org/10.1021/acscatal.4c02203
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- Claire D. Hallock, Michael J. Rose. Electrochemical Impedance of Well-Passivated Semiconductors Reveals Bandgaps, Fermi Levels, and Interfacial Density of States. Journal of the American Chemical Society 2024, 146 (28) , 18989-18998. https://doi.org/10.1021/jacs.4c02738
- Karolina Syrek, Sebastian Kotarba, Marta Zych, Marcin Pisarek, Tomasz Uchacz, Kamila Sobańska, Łukasz Pięta, Grzegorz Dariusz Sulka. Surface Engineering of Anodic WO3 Layers by In Situ Doping for Light-Assisted Water Splitting. ACS Applied Materials & Interfaces 2024, 16 (28) , 36752-36762. https://doi.org/10.1021/acsami.4c02927
- Szymon Dudziak, Jakub Karczewski, Adam Ostrowski, Grzegorz Trykowski, Kostiantyn Nikiforow, Anna Zielińska-Jurek. Fine-Tuning the Photocatalytic Activity of the Anatase {1 0 1} Facet through Dopant-Controlled Reduction of the Spontaneously Present Donor State Density. ACS Materials Au 2024, 4 (4) , 436-449. https://doi.org/10.1021/acsmaterialsau.4c00008
- Khadijah MohammedSaleh Katubi, Nusrat Shaheen, Sonia Zulfiqar, Amna Irshad, Ziyad Awadh Alrowaili, Mohammed Sultan Al-Buriahi, Imran Shakir, Muhammad Farooq Warsi, Eric W. Cochran. Innovative Nanocomposites for Enhanced Photocatalytic Removal of Hazardous Pollutants: Probing the Role of CuO/Fe2O3 and MXene Synergy. Industrial & Engineering Chemistry Research 2024, 63 (27) , 11922-11938. https://doi.org/10.1021/acs.iecr.4c00918
- Charles H. Wood, Raymond E. Schaak. Synthetic Roadmap to a Large Library of Colloidal High-Entropy Rare Earth Oxyhalide Nanoparticles Containing up to Thirteen Metals. Journal of the American Chemical Society 2024, 146 (27) , 18730-18742. https://doi.org/10.1021/jacs.4c06413
- Wansun Kim, Jisang Han, Yoo Jin Kim, Hyerin Lee, Tae Gi Kim, Jae-Ho Shin, Dong-Ho Kim, Ho Sang Jung, Sang Woong Moon, Samjin Choi. Molybdenum Disulfide-Assisted Spontaneous Formation of Multistacked Gold Nanoparticles for Deep Learning-Integrated Surface-Enhanced Raman Scattering. ACS Nano 2024, 18 (27) , 17557-17569. https://doi.org/10.1021/acsnano.4c00978
- David S. Pate, Griffin C. Spence, Lisa S. Graves, Indika U. Arachchige, Ümit Özgür. Size-Tunable Band Structure and Optical Properties of Colloidal Silicon Nanocrystals Synthesized via Thermal Disproportionation of Hydrogen Silsesquioxane Polymers. The Journal of Physical Chemistry C 2024, 128 (25) , 10483-10491. https://doi.org/10.1021/acs.jpcc.4c01462
- Feiyue Ge, Yuji Zhao, Changsheng Feng, Xuefei Li, Jiaqi Wang, Haixia Liu, Lijun Hu, Yue Chen, Feifan Chen, Fang Cheng, Hai-Yan Wei, Xue-Jun Wu. Elucidating Facet-Dependent Photocatalytic Activities of Metastable CdS and Au@CdS Core–Shell Nanocrystals. ACS Applied Materials & Interfaces 2024, 16 (25) , 32847-32856. https://doi.org/10.1021/acsami.4c04195
- Damanpreet Kaur, Rohit Dahiya, Nadeem Ahmed, Mukesh Kumar. Vertically Graded Oxygen Vacancies in Amorphous Ga2O3 for Offsetting the Conventional Trade-Off between Photoresponse and Response Time in Solar-Blind Photodetectors. ACS Applied Electronic Materials 2024, 6 (6) , 4746-4753. https://doi.org/10.1021/acsaelm.4c00759
- Shivam Shukla, Subhajit Jana, Anu Gupta, Subhadip Ghosh, Samit K. Ray, Sanjeev K. Srivastava. Photoresponse of Carbon Nanofiber-Based Photodetector and Its Enhancement on CuNi Nanoparticle Adsorption. ACS Omega 2024, 9 (25) , 27232-27247. https://doi.org/10.1021/acsomega.4c01546
- Bright Ngozichukwu, Eugenie Pranada, Denis Johnson, Abdoulaye Djire. Nanolayered Ti4N3Tx MXene Retains Its Electrocatalytic Properties after Prolonged Immersion in Solvents. ACS Applied Nano Materials 2024, 7 (11) , 13765-13774. https://doi.org/10.1021/acsanm.4c02503
- Kezheng Tao, Qiang Li, Qingfeng Yan. Narrow-Bandgap Tellurium-Based Chiral Hybrid Perovskite Single Crystals with Rashba–Dresselhaus Effect and Piezoelectricity. The Journal of Physical Chemistry Letters 2024, 15 (23) , 6024-6030. https://doi.org/10.1021/acs.jpclett.4c01262
- Junfeng Cui, Yingying Yang, Mingyang Yang, Guoyong Yang, Guoxin Chen, Lei Zhang, Cheng-Te Lin, Sha Liu, Chun Tang, Peiling Ke, Yang Lu, Kazuhito Nishimura, Nan Jiang. Picometer-Scale Atomic Shifts Governing Subdisordered Structures in Diamond. Nano Letters 2024, 24 (23) , 7108-7115. https://doi.org/10.1021/acs.nanolett.4c01857
- Chin Shen Ong, Olivier Donzel-Gargand, Pedro Berastegui, Johan Cedervall, Ilknur Bayrak Pehlivan, Charles Hervoches, Premysl Beran, Tomas Edvinsson, Olle Eriksson, Ulf Jansson. The Crystal Structure of Al4SiC4 Revisited. Inorganic Chemistry 2024, 63 (23) , 10490-10499. https://doi.org/10.1021/acs.inorgchem.4c00560
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- Xiaohu Chen, Darren Bagnall, Noushin Nasiri. Highly Porous ZnO/CNT Hybrid Microclusters for Superior UV Photodetection. ACS Applied Materials & Interfaces 2024, 16 (21) , 27614-27626. https://doi.org/10.1021/acsami.4c02284
- Mitsuo Lopes Takeno, Francisco Xavier Nobre, Fagner Ferreira da Costa, Marcus Valério Botelho do Nascimento, Wanison André Gil Pessoa Júnior, Edgar Alves Araújo Júnior, Giancarlo da Silva Sousa, Marcel Leiner de Sá, Raiana Silveira Gurgel, Patrícia Melchionna Albuquerque, José Milton Elias de Matos, Yurimiler Leyet Ruiz, Carlos Roberto Grandini. Solvent Effect on the Structural, Optical, Morphology, and Antimicrobial Activity of Silver Phosphate Microcrystals by Conventional Hydrothermal Method. ACS Omega 2024, 9 (21) , 23069-23085. https://doi.org/10.1021/acsomega.4c02943
- Prabhukrupa C. Kumar, Gopal K. Pradhan, Subrata Senapati, Ramakanta Naik. Two-Dimensional Bi2O5Te Nanosheets for Sensitive and Fast Response Broadband Visible Light Photodetectors. ACS Applied Electronic Materials 2024, 6 (5) , 3311-3324. https://doi.org/10.1021/acsaelm.4c00179
- Yiannis Deligiannakis, Eleni Bletsa, Eleftherios Mouzourakis, Maria Solakidou, Katarzyna Adamska. Carbon-Coated TiO2 Nanoparticles for Noble-Metal-Free Photocatalytic H2 Production from H2O. ACS Applied Nano Materials 2024, 7 (10) , 11621-11633. https://doi.org/10.1021/acsanm.4c01150
- Zorka Vasiljevic, Jovana Vunduk, Dragana Bartolic, Goran Miskovic, Milos Ognjanovic, Nenad B. Tadic, Maria Vesna Nikolic. An Eco-friendly Approach to ZnO NP Synthesis Using Citrus reticulata Blanco Peel/Extract: Characterization and Antibacterial and Photocatalytic Activity. ACS Applied Bio Materials 2024, 7 (5) , 3014-3032. https://doi.org/10.1021/acsabm.4c00079
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