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Article

Chemical Modification of B4C Films and B4C/Pd Layers Stored in Different Environments

by
Yufei Feng
1,
Runze Qi
1,*,
Li Jiang
1,
Qiushi Huang
1,
Tongzhou Li
1,
Genchang Liu
1,
Wenbin Li
1,
Wensheng Yan
2,
Zhong Zhang
1 and
Zhanshan Wang
1
1
MOE Key Laboratory of Advanced Micro-Structured Materials, Institute of Precision Optical Engineering (IPOE), School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
2
National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230029, China
*
Author to whom correspondence should be addressed.
Materials 2021, 14(5), 1319; https://doi.org/10.3390/ma14051319
Submission received: 2 February 2021 / Revised: 27 February 2021 / Accepted: 3 March 2021 / Published: 9 March 2021
(This article belongs to the Section Materials Physics)
Browse Figures
Versions Notes

Abstract

:
B4C/Pd multilayers with small d-spacing can easily degrade in the air, and the exact degradation process is not clear. In this work, we studied the chemical modification of B4C films and B4C/Pd double layers stored in four different environments: a dry nitrogen environment, the atmosphere, a dry oxygen-rich environment, and a wet nitrogen environment. The XANES spectra of the B4C/Pd layers placed in a dry oxygen-rich environment showed the most significant decrease in the σ* states of the B–C bonds and an increase in the π* states of the B–O bonds compared with the other samples. X-ray photoelectron spectroscopy (XPS) measurements of the samples placed in a dry oxygen-rich environment showed more intensive B-O binding signals in the B4C/Pd layers than in the single B4C film. The results of the Fourier-transform infrared spectroscopy (FTIR) showed a similar decrease in the B–C bonds and an increase in the B–O bonds in the B4C/Pd layers in contrast to the single B4C film placed in a dry oxygen-rich environment. We concluded that the combination of palladium catalysis and the high content of oxygen in the environment promoted the oxidization of boron, deteriorated the B4C composition.

1. Introduction

The photon flux of multilayer monochromators on synchrotron beamlines is approximately two orders of magnitude larger than that of crystal monochromators [1,2]. The most distinct advantage of these techniques is that they do not require high energy resolution, such as X-ray fluorescence spectroscopy (XRF) [3,4], small-angle X-ray scattering (SAXS) [5,6], and X-ray micro-imaging [7,8]. There are many typical multilayer material combinations for monochromators, for example, Si/W [9,10], B4C/W [4,11,12], and B4C/Pd [8,13,14]. B4C/Pd multilayers, which have high reflectivity and good energy resolution at approximately 7–15 keV, have been used in synchrotron beamlines, such as TopoTomo (ANKA light source) [14]. Recently, Ni et al. have fabricated the ultrathin B4C/Pd multilayers with d-spacing of 2.5 nm by magnetron sputtering using the heavy noble gas Kr to improve the layer structure [15]. The excellent performance of B4C/Pd multilayers are suitable to be used as a monochromator.
However, small d-spacing B4C/Pd multilayers are unstable under an atmospheric environment. Morawe et al. reported that B4C/Pd multilayers with d-spacing of approximately 3 nm degraded in the air after only a few days without protective layers [16,17]. The first peak of measured X-ray reflectivity curve broadened and shoulders appeared at higher angles indicating the compaction of the B4C layers and destruction of the periodic structure. With larger d-spacing, multilayers deposited by reactive sputtering using an Ar and N2 gas mixture were also unstable compared to other nitridated multilayers, like B4C+N/Ru [18,19] and B4C+N/W multilayers [20]. Wang et al. reported that nitridated B4C/Pd multilayers with d-spacing of approximately 5 nm decayed after the samples were stored in an air environment for 6–17 months [21].
We found that many layers near the surface deteriorated with severe interdiffusion and compaction of the layers. This is a significant issue for applications, as most multilayers for hard X-ray monochromator have d-spacing less than 3 nm, and the conditions for preparation, storage, and installation become critical. Although certain protective layers have been developed to elongate the lifetime of B4C/Pd multilayers [16], there is no further investigation of the effects of different environmental factors, the contribution from different materials, and the composition changes of films in the degradation process, which is essential for the future development and applications of B4C/Pd multilayer monochromators.
The oxidation of B4C as an important subject has been studied in many literatures. Zehringer et al. [22] reported that exposure of sputter-cleaned surfaces of boron-carbide to molecular oxygen at room temperature did not cause a measurable surface oxidation. Li et al. [23] found Gibbs energy of the reaction between B4C and oxygen was great than that of the reaction between B4C and water vapor at the same temperature. Viricelle et al. [24] reported that the oxidation rate of B4C increases and is enhanced by water vapor at 700 and 800 °C. To sum up, B4C is very stable at room temperature, and will oxidize with oxygen and water at a high temperature.
Palladium is typically used as a catalyst in chemistry. Nicolaou et al. reported that palladium catalyzed carbon–carbon bond formation in most common synthesis reactions [25]. Tat Thang Vo Doan et al. [26] and Li et al. [27] found that B–Pd nanocrystals reduced O=O bond reaction barriers and strengthened oxygen reduction reactions. Palladium catalysis promotes the dissociation of oxygen and reduces the oxidation reaction potential. Therefore, we can assume that the presence of Pd promotes B4C oxidation.
In this paper, we first confirm the hypothesis of the catalytic effect of Pd on B4C/Pd layered systems and further explore the degradation process by investigating the stability of B4C films and B4C/Pd double layers stored in different environments. We fabricated two groups of samples of a single B4C film and a B4C layer with a Pd layer underneath. Both groups of samples were placed in different environments for 50 days. The samples were then measured using X-ray absorption near-edge structure (XANES) spectroscopy, X-ray photoelectron spectroscopy (XPS), and Fourier-transform infrared spectroscopy (FTIR) to analyze the changes in the chemical state after film degradation. The results indicated that boron combined with oxygen and boron carbide degraded under the action of palladium in the oxygen environment. The work is a useful guide for exploring the oxidation process of B4C materials with nano-film state, and for the protection and application of ultrathin B4C/Pd multilayers in synchrotron monochromators.

2. Experimental Techniques

2.1. Sample Preparation

The direct current (DC) magnetron sputtering technique was developed to prepare samples. Each magnetron cathode was operated at 100 W and 15 W for the B4C and Pd targets, respectively. The samples were deposited at Ar gas pressures of 1 mTorr at room temperature and the background pressure was lower than 5.5 × 10−5 Pa to avoid the incorporation of oxygen into the sputtering process. Firstly, the deposition rate of B4C and Pd was calibrated by measuring and fitting the X-ray reflectivity curve of single B4C and Pd films. Known from our previous investigation [28], the stoichiometric ratio of B:C was around 4:1 as the B4C layer sputtered at Ar gas pressures of 1 mTorr. The thin B4C film obtained under this sputtering condition is very dense, with a density (2.39 g/cm3) equivalent to 95% of the bulk B4C material (2.52 g/cm3). Then two groups of samples were fabricated. In the first group of samples, a 10 nm B4C film was deposited directly on a Si substrate. In the second group, a 1 nm Pd layer was added between a 10 nm B4C layer and a Si substrate to prove the function of Pd. After preparation, the samples were immediately transferred to the corresponding storage environment.

2.2. Storage Environment Conditions

To explore the factors that degrade films, the B4C films and B4C/Pd layers were sealed in boxes and stored in four different environments for 50 days: (A) A dry nitrogen environment (pumped down and filled with nitrogen), which is isolated from O2 and H2O and can be used as a reference. (B) The atmosphere, which is the assumed working environment of the optics. (C) A dry oxygen-rich environment (pumped down and filled with oxygen), where oxygen is the impact factor. (D) A wet nitrogen environment (pumped down, humidified, and filled with nitrogen), where H2O is the impact factor. Detailed parameters of the storage environments are listed in Table 1. The samples stored in a dry nitrogen environment, isolated from O2 and H2O, can be used as a reference.

2.3. The X-ray Absorption Near-Edge Structure (XANES)

X-ray absorption near-edge structure (XANES) spectroscopy is commonly used to probe the local atomic structure around specific elements in films and often used as a fingerprint of the changes in the coordination numbers of elements [29,30,31,32,33]. XANES measurements were conducted 50 days after fabrication at the Beamline U12b at the National Synchrotron Radiation Laboratory (NSRL) in the total electron yield (TEY) mode by collecting sample drain currents under a vacuum at greater than 5 × 10−8 Pa. The beam from a bending magnet was monochromatized with a varied line-spacing plane grating and refocused using a toroidal mirror. An energy range from 100 to 1000 eV was used with an energy resolution of approximately 0.2 eV [34].
All XANES spectra were measured using the process of background subtraction and normalization by considering the low and high photon energy parts of the spectra far from the threshold [32].

2.4. X-ray Photoelectron Spectroscopy (XPS)

To study the changes in the electronic structures of the films’ elements after degradation, the XPS measurements were conducted using a Thermo Fisher Scientific K-Alpha+ spectrometer (Thermo Fisher Scientific, Waltham, MA, USA) with an Al-Kα characteristic emission line (photon energy E = 1486 eV) [35]. The B 1s, C 1s, and O 1s core-level spectra were investigated after the single B4C films and B4C/Pd layers were placed in the dry oxygen-rich environment. The Pd 3d core-level spectra at the interface of the Pd and B4C layers were also investigated to explore the chemical state of Pd.

2.5. Fourier-Transform Infrared Spectroscopy (FTIR)

Fourier-transform infrared spectroscopy was recorded on a Fourier-transform infrared spectrometer (FTIR, Tensor 27). First, a spectrum of the Si substrate was collected as the background spectrum. The spectra of the single B4C films and B4C/Pd layers placed in the dry oxygen-rich environment were then obtained under the same test conditions. The data processing consisted of two steps: Background subtraction and position correction based on the peaks of the Si–Si bonds [36].

3. Experimental Results

3.1. XANES Measurements

3.1.1. B K-Edge XANES

The B K-edge X-ray absorption near-edge structure spectra of the samples placed in the different storage environments are shown in Figure 1. The spectra had three features: One peak at 191.6 eV, one minor sharp oscillation at 193 eV, and one broad slope from 196.0 eV to 208.0 eV that were marked as a, b, and c, respectively. The spectral features at the different energy positions represented different chemical states and the local atomic structure of boron. Peak a at 191.6 eV was due to the transition of B 1s electrons to unoccupied B 2p states of B4C [37]. Feature b at 193 eV was attributed to the localized π* states of B2O3 [37,38,39], and the broad feature c from 196.0 eV to 208.0 eV was due to the σ* states of the B-C bonds [38,39,40,41]. As shown in Figure 1a, the three spectral features of the B1, C1, and D1 samples of the single B4C films underwent no significant changes compared with the A1 sample placed in the dry nitrogen environment.
The results indicate that the local atomic structure around the boron experienced almost no changes in the single B4C films even in the different environments. Figure 1b shows that the three spectral features of the B4C/Pd layers placed in the dry oxygen-rich environment (C2 sample) changed significantly compared with the A2 sample placed in the dry nitrogen environment. Peak a at 191.6 eV in the C2 sample’s spectrum was more intense and sharper than the other samples, indicating that some boron atoms became unstable in the B4C/Pd layers placed in the dry oxygen-rich environment.
The peak position of feature b was related to the π* states of the B2O3, suggesting that some of the boron combined with oxygen. This change agreed with the results of the O K-edge XANES presented in Figure 4, with peaks at 536.1 eV [39,42,43]. The decline in feature c, assigned to the σ* states of the B–C bonds, indicated that some B–C chains were breaking in the film [38,39]. The corresponding change also appeared in the C K-edge XANES signal with a peak at 284.5 eV and a slope from 291 to 298 eV [40,41] as shown in Figure 3. These spectral features demonstrated that, in the B4C/Pd layers placed in the oxygen-rich environment, the local atomic structure and chemical states of the boron changed.
The spectral features of the B4C/Pd layers placed in the atmosphere and wet nitrogen environment (the B2 and D2 samples, respectively) changed little compared with the B4C/Pd layers placed in the dry nitrogen environment (A2 sample). There was almost no increase in the B2 sample’s spectrum due to the low concentration of oxygen in the atmosphere. As no obvious changes were observed in the D2 sample’s spectrum, H2O appeared to have less effect on the degradation of the layers compared to O2.
To further prove the effects of palladium and oxygen on the degradation of the films, the spectra of different films in the same storage environments are demonstrated in Figure 2. Figure 2a shows the spectra of the single B4C film and B4C/Pd layers placed in the dry nitrogen environment. There was no obvious difference in the spectral features between the two samples, proving that the B4C/Pd layers were stable without the action of oxygen. Figure 2b shows the spectra of the single B4C film and the B4C/Pd layers placed in the dry oxygen-rich environment. The spectral features, as previously mentioned, of the B4C/Pd layers showed obvious changes, indicating that the presence of palladium degraded the film in the dry oxygen-rich environment.

3.1.2. C K-Edge XANES

The C K-edge X-ray absorption near-edge structure spectra were measured to analyze the change of local atomic structure around the carbon element. Figure 3 shows the C K-edge X-ray absorption near-edge structure spectra of the different films placed in the dry oxygen-rich environment. The C 1s absorption edge of the B4C film was characterized by the antibonding π* state of the C–B bonds at 284.5 eV and the σ* states of the C–B bonds from 291 to 298 eV, symbolized by d and e, respectively [40,41]. The most significant change in the C 1s spectrum of the B4C/Pd layers was the decrease in the intensity of the antibonding π* state and the σ* state compared with the spectrum of the B4C film. The decrease proved that the part of C–B chain was breaking due to the presence of Pd in the oxygen-rich environment and as a result, part of the B4C composition was destroyed.

3.1.3. O K-Edge XANES

To prove the effect of oxygen on the film, the O K-edge X-ray absorption near-edge structure spectra were also measured. Figure 4 displays the O K-edge X-ray absorption near-edge structure spectra of the different films placed in the dry oxygen-rich environment. The spectra had two significant features: one small bump due to the π* state of the O2 molecule at 529.5 eV [42,43,44,45], labeled f, and another broad feature attributed to the σ* state of the B–O bonds at 536.1 eV [43,44,45], labeled g. There was a significant increase in the σ* states of the B–O bonds in the spectrum of the B4C/Pd layers compared with the spectrum of the B4C film, which indicated that some of the oxygen was excited and combined with boron under palladium catalysis. The same O2 peak occurred in the spectra because the samples were placed in a dry oxygen-rich environment.
Summarizing the XANES results, there was a reasonable explanation of the degradation of the B4C/Pd layers: Under palladium catalysis, some of oxygen was excited [27], replacing some of the carbon atoms around the boron and combining with the boron, which caused the deterioration of the B4C composition.

3.2. XPS Measurements

Examinations of the XPS spectra around the B 1s, O 1s, C 1s, and Pd 3d regions provided more details about the electronic structures of the film elements. Figure 5 presents the B 1s, O 1s, and C 1s spectra of the single B4C film and B4C/Pd layers placed in the dry oxygen-rich environment. Both test positions were approximately 5 nm from the surface of the B4C layer to avoid surface contamination. All photoelectron peaks were fitted by a weighted least-squares fitting method using Lorentzian–Gaussian line shapes after background subtraction according to the Shirley method. The peak width of the fitted spectra of B4C film was consistent with the B4C/Pd layers.
Figure 5a presents the B 1s spectra of the single B4C film and B4C/Pd layers. In the spectrum of the B4C/Pd layers, there was a weak slope at a binding energy of 192.5 eV due to the B–O component [27,46,47], which indicated that some of the boron (~9% in atomic fraction) combined with oxygen under the action of palladium. A small B–O component (~2% in atomic fraction) was also found by fitting the B 1s spectra of the single B4C film. The B 1s spectra also show the reduction of B–B bonds (from about 48% down to 45% in the atomic fraction) and B–C bonds (from about 50% down to 46% in the atomic fraction) at binding energies of 188 and 189 eV, respectively [46,47,48].
Figure 5b shows the O 1s spectra of the single B4C film and B4C/Pd layers. The signal peak was due to the O–B bonds at 531.7 eV [49] and the O–H bonds at 533.2 eV [50] from the adsorbed water molecules. The amount of O–B bonds in the spectrum of the B4C/Pd layers (~58% in the atomic fraction) were higher than in the spectrum of the single B4C film (~54% in the atomic fraction). The results indicate that a larger ratio of oxygen reacted with boron under the presence of palladium, which is consistent with the results of the B 1s spectra. The stoichiometric ratio of O:B was around 1:9.8 in the B4C/Pd layers, which was larger than in the single B4C films (1:18.8). This shows that the content of oxygen in the B4C/Pd layers significantly increased under the catalysis of palladium. The results also indicate that the amount of oxidized boron in the B4C/Pd layers increased significantly.
Figure 5c demonstrates the XPS spectra of C 1s in the single B4C film and B4C/Pd layers. The C 1s spectra had peaks at binding energies of 283.0 eV and 284.5 eV due to the C–B bonds and C–C bonds, respectively [46,47,48]. There was a reduction in the C–B bonds in the spectrum of the B4C/Pd layers (~66% in atomic fraction) compared with those in the spectrum of the B4C film (~71% in atomic fraction), indicating that some of the C–B bonds broke due to the reaction of B with O in the B4C/Pd layers. This result was consistent with the C K-edge XANES analysis.
To further explore the changes of palladium, the XPS spectra of Pd 3d were also measured. Figure 6a shows the XPS spectrum of the Pd 3d at the interface of the B4C/Pd layers placed in the dry oxygen-rich environment. The spectrum of the Pd 3d at the position approximately 5 nm from the surface of single Pd layer, as reference, is also shown in Figure 6b. All photoelectron peaks were fitted by a weighted least-squares fitting method using Lorentzian–Gaussian line shapes after background subtraction according to the Shirley method. In the spectrum of the pure Pd layer, the peak was fitted as the 3d 5/2 and 3d 3/2 levels of the Pd-Pd bonds located at 335.3 eV and 340.6 eV [27,51,52], and a small portion of the 3d 5/2 and 3d 3/2 levels of the Pd–O bonds located at 335.9 eV and 341.3 eV [27,51,52]. The atomic fraction of the Pd–O bonds was about 21%.
For the spectrum of the Pd 3d at the interface of the B4C/Pd layers placed in the dry oxygen-rich environment, the peaks were slightly shifted to a higher energy position due to the enhancement of the Pd–O bonds signal. The atomic fraction of the Pd–O bonds was about 39%. The increase of the Pd–O bonds indicates that more Pd atoms were excited. Therefore, Pd will be more involved in the reaction in the B4C/Pd layers placed in the dry oxygen-rich environment. The same result also appeared in other Pd catalytic experiments [26,27], demonstrating that, when Pd, B, and O coexist, Pd donates electrons to O and B transfers electrons to O, indicating that Pd and B are involved in the decomposition of O and promotes oxygen reduction reactions.

3.3. FTIR Absorption Spectra

To further investigate the vibration of bonds, the FTIR absorption spectra were recorded. Figure 7 shows the FTIR absorption spectra of the single B4C film and B4C/Pd layers placed in the dry oxygen-rich environment. The spectrum of the B4C film had a strong absorption peak near 1100 cm−1 that was due to the B–C bonds in the B4C composition [53,54,55,56]. In the spectrum of the B4C/Pd layers, the peak of the B–C bonds decreased significantly, indicating that some of B–C chains were breaking due to the presence of the Pd in the oxygen-rich environment. In addition, there were two new peaks in the spectrum of the B4C/Pd layers, minor features in the regions of 950–1000 cm−1, and absorption bands in the regions of 1200–1300 cm−1 due to the B–O modes [54,55,56], indicating that some of the boron was oxidized. The FTIR absorption spectra confirmed that part of B4C composition was destroyed and that boron combined with oxygen in the dry oxygen-rich environment under palladium catalysis.

4. Discussion

The three measurements showed the same results indicating that the B4C composition tended to degrade under palladium catalysis in the oxygen environment. Considering that the film is only a few nanometers, these characterizations are enough to clearly prove the effect of Pd and O on this degradation process. A simple degradation process could be assumed as follows:
  • First oxygen diffused into the film. Known from the previous calculation of density functional theory (DFT), O2 dissociation proceeds on a Pd layer with reaction barriers of 0.72 eV [26]. The energy of the reaction barriers decreases to 0.63 eV when B and Pd exist simultaneously [26], indicating B and Pd enhance the decomposition of O and promote the oxidation reaction. In our work, the most obvious structural change occurs in the B4C/Pd layers placed in a dry oxygen-rich environment. In this case, it is essential that numerous O2 will decompose into O with the participation of B and Pd.
  • Then, dissociated oxygen replaced the carbon around boron and combined with boron. The formation of B2O3 (ΔfH° = −1194 kJ/mol) releases a larger amount of energy than B4C (ΔfH° = −71 kJ/mol) [16], indicating that boron prefers to combine with oxygen. In other B4C oxidation experiments [23], at elevated temperatures, carbon atoms will form carbon dioxide. While in our experiment, at room temperature, carbon atoms can only be in a non-excited state [17]. Thus, we could assume that the reaction product prefers boron oxide and carbon.
  • Finally, if water vapor exists, B2O3 will react to form H3BO3, and then volatilize [24], leading to the reduction in the B content in the film.
As a result, the B4C layer is deteriorated and degraded. As for the B4C/Pd multilayers, the reduction of B atoms leads to the destruction of the periodic structure and the degradation of the optical performance [16,17].
More theoretical and experimental research are required to explore the evolution of the chemical modifications in films. The sample in this study was only a double-layer structure with a thick B4C top layer. These structures can be more stable compared with nanoscale multilayer structures in which each layer is only ~1 nm thick [16]. In future, we will investigate the effect of environmental factors, including oxygen and H2O, on real B4C/Pd multilayers.

5. Conclusions

In summary, we explored the stability of B4C films and B4C/Pd layers placed in a dry nitrogen environment, the atmosphere, a dry oxygen-rich environment, and a wet nitrogen environment. The chemical state of the films was analyzed using XANES, XPS, and FTIR. There was no significant change in the XANES spectra of the single B4C films, suggesting that the single B4C film was stable even under different environments. In the sample with B4C/Pd layers placed in the dry oxygen-rich environment, the XANES spectra demonstrated a significant increase in the π* states of the B–O bonds and a decrease in the σ* states in the B–C bonds, indicating that the boron was oxidized and that the B4C composition was destroyed under the action of both palladium and oxygen. The XPS results also proved that the amount of oxidized boron in the B4C/Pd layers increased due to Pd catalysis. The FTIR results provided the same conclusions as XANES and XPS. These analyses reasonably explain the degradation of the B4C/Pd layers in a high-oxygen environment, which should be avoided during storage. This study provides useful guidance for the further development and applications of B4C/Pd multilayers.

Author Contributions

Conceptualization, Y.F.; methodology, W.L.; software, Y.F.; validation, L.J. and Q.H.; formal analysis, Y.F.; investigation, T.L., G.L. and W.Y.; resources, Z.W.; data curation, R.Q.; writing—original draft preparation, Y.F.; writing—review and editing, L.J., Q.H., Z.Z. and Z.W.; visualization, Y.F.; supervision, R.Q.; project administration, R.Q.; funding acquisition, Z.Z. and Z.W. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the National Key R&D Program of China (2016YFA0401304), National Natural Science Foundation of China (61621001), Shanghai Rising-Star Program (19QA1409200), Shanghai Municipal Science and Technology Major Project (2017SHZDZX02), and the Major projects of Science and Technology Commission of Shanghai (No. 17JC1400800). And the APC was funded by National Natural Science Foundation of China (61621001).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

No new data were created or analyzed in this study. Data sharing is not applicable to this article.

Conflicts of Interest

The authors declare no conflict of interest.

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Materials 14 01319 g001 550
Figure 1. The B K-edge X-ray absorption near-edge structure (XANES) spectra of the B4C films (a) and B4C/Pd layers (b) in the different storage environments. Samples A1 and A2 were placed in a dry nitrogen environment; samples B1 and B2 were placed in the atmosphere; samples C1 and C2 were placed in a dry oxygen-rich environment; and samples D1 and D2 were placed in a wet nitrogen environment. The insert in Figure 1b is an enlarged view of feature b in the B4C/Pd layers.
Figure 1. The B K-edge X-ray absorption near-edge structure (XANES) spectra of the B4C films (a) and B4C/Pd layers (b) in the different storage environments. Samples A1 and A2 were placed in a dry nitrogen environment; samples B1 and B2 were placed in the atmosphere; samples C1 and C2 were placed in a dry oxygen-rich environment; and samples D1 and D2 were placed in a wet nitrogen environment. The insert in Figure 1b is an enlarged view of feature b in the B4C/Pd layers.
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Figure 2. The B K-edge XANES spectra of the B4C films (A1 and C1) and B4C/Pd layers (A2 and C2) placed in the dry nitrogen environment (a) and in the dry oxygen-rich environment (b).
Figure 2. The B K-edge XANES spectra of the B4C films (A1 and C1) and B4C/Pd layers (A2 and C2) placed in the dry nitrogen environment (a) and in the dry oxygen-rich environment (b).
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Figure 3. The C K-edge XANES spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment.
Figure 3. The C K-edge XANES spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment.
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Figure 4. The O K-edge XANES spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment.
Figure 4. The O K-edge XANES spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment.
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Figure 5. The X-ray photoelectron spectroscopy (XPS) spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment. (a) B 1s, (b) O 1s, and (c) C 1s.
Figure 5. The X-ray photoelectron spectroscopy (XPS) spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment. (a) B 1s, (b) O 1s, and (c) C 1s.
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Figure 6. The XPS spectra of the Pd 3d: (a) at the interface of the Pd layer and B4C layer placed in the dry oxygen-rich environment; and (b) pure Pd layer.
Figure 6. The XPS spectra of the Pd 3d: (a) at the interface of the Pd layer and B4C layer placed in the dry oxygen-rich environment; and (b) pure Pd layer.
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Figure 7. The Fourier-transform infrared spectroscopy (FTIR) absorption spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment.
Figure 7. The Fourier-transform infrared spectroscopy (FTIR) absorption spectra of the B4C film and B4C/Pd layers placed in the dry oxygen-rich environment.
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Table
Table 1. Detailed parameters of the storage environments.
Table 1. Detailed parameters of the storage environments.
EnvironmentsTemperature/°CHumidity/%rh
A: Dry nitrogen environment20 °C~25%rh
B: Atmosphere20 °C~35%rh
C: Dry oxygen-rich environment20 °C~25%rh
D: Wet nitrogen environment20 °C~85%rh
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Feng, Y.; Qi, R.; Jiang, L.; Huang, Q.; Li, T.; Liu, G.; Li, W.; Yan, W.; Zhang, Z.; Wang, Z. Chemical Modification of B4C Films and B4C/Pd Layers Stored in Different Environments. Materials 2021, 14, 1319. https://doi.org/10.3390/ma14051319

AMA Style

Feng Y, Qi R, Jiang L, Huang Q, Li T, Liu G, Li W, Yan W, Zhang Z, Wang Z. Chemical Modification of B4C Films and B4C/Pd Layers Stored in Different Environments. Materials. 2021; 14(5):1319. https://doi.org/10.3390/ma14051319

Chicago/Turabian Style

Feng, Yufei, Runze Qi, Li Jiang, Qiushi Huang, Tongzhou Li, Genchang Liu, Wenbin Li, Wensheng Yan, Zhong Zhang, and Zhanshan Wang. 2021. "Chemical Modification of B4C Films and B4C/Pd Layers Stored in Different Environments" Materials 14, no. 5: 1319. https://doi.org/10.3390/ma14051319

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