1. Introduction
Metal corrosion poses a severe challenge to the industries, resulting in huge economic losses worldwide each year. The application of surface treatment technologies can not only relieve material degradation and maintain structural integrity, but also ensure the long-term stable operation of mechanical equipment by improving both corrosion and wear resistance. Among various surface modification technologies, electroless nickel–boron (Ni-B) alloy coatings have garnered significant interest in both academic and industrial circles over the past few decades [
1,
2], owing to their excellent weldability [
3], hardness, wear [
4] resistance, and chemical stability [
5]. Electroless plating is based on a redox reaction in which metal ions in solution are reduced to metallic nickel by a strong reducing agent [
6,
7], yielding a coating that is both well-distributed and compact across the substrate surface [
8,
9]. This process is particularly suitable for surface treatment of components with complex geometries [
10].
The boron content is the key factor in determining the microstructure and performance of Ni-B alloy coatings [
11,
12]. Coatings with low boron content typically exhibit a nano-crystalline structure, while increasing the boron content will cause the coating to gradually transition to an amorphous structure [
13]. This evolution of structure is ascribed to lattice distortion and grain refinement caused by the solid solution of boron atoms in the nickel lattice [
14,
15]. Amorphous or nano-crystalline Ni-B alloys often demonstrate superior corrosion resistance owing to their significantly reduced grain-boundary density. However, engineering components in actual usage environments are often subjected to harsh conditions of corrosion and wear [
16,
17]. Under such circumstances, single-phase Ni-B coatings may fail to meet the comprehensive performance requirements for specific applications [
18]. Consequently, the development of novel surface materials with structural and functional stability has become a major research hotspot in the area of surface engineering [
19,
20].
Composite coating technology, which involves the co-deposition of particles into a metal matrix [
21], offers an effective approach to enhance the performance of coatings. Studies have shown that introducing micro- or nano-sized ceramic or rare-earth oxide particles (such as α-ZrP [
22], SiC [
12], Y
2O
3 [
23], Si
3N
4 [
24], MMT [
25], Al
2O
3 [
26], CeO
2 [
13]) into nickel-based alloy coatings can significantly improve their hardness, abrasive resistance, and anti-corrosion properties [
26,
27]. The strengthening mechanisms mainly include the dislocation pinning by the dispersed reinforcing particles [
28], the filling of microscopic defects, leading to optimization of the coating microstructure, and the formation of a barrier that hinders the penetration of corrosive media [
29]. In particular, rare-earth oxides exhibit considerable potential in metal-matrix composite coatings owing to their unique electronic structures and chemical activity.
Although techniques such as heat treatment can improve coating performance by promoting crystallization and the precipitation hardening, they often simultaneously intensify corrosion and wear, and may lead to uneven treatment of components with complex geometries. In contrast, composite co-deposition technology allows direct microstructural control during the plating process, offering a more promising route for the synergistic enhancement of properties. La2O3, as a typical rare-earth oxide, possesses excellent chemical stability, thermal resistance, and distinctive solubility properties under acidic conditions, and has been widely used in catalysis, ceramics and the electronics industry. While the strengthening effect of La2O3 in Ni-P, Ni-W and other alloy coatings has been reported, systematic studies on the co-deposition behavior of nano-sized La2O3 particles in electroless Ni-B systems and their synergistic impact on the microstructural characteristics and corrosion behavior of the coatings remain scarce. Given the importance of Ni-B-based composite coatings in surface engineering, a systematic investigation into the effect of La2O3 in modifying the microstructure and anti-corrosion properties of Ni-B matrix coatings carries clear scientific significance and engineering value.
This study aims to synthesize Ni-B/La2O3 composite coatings through co-depositing nano-La2O3 particles into an electroless Ni-B alloy matrix. The distribution characteristics of La2O3 nanoparticles in the coating and their influence on the phase constituents and grain refinement mechanism of Ni-B alloy matrix were mainly studied, thereby revealing the intrinsic correlation between the composite coating’s anti-corrosion properties and its microstructure. The clear novelty of this work is that it fills the key research gap: systematic studies on the co-deposition behavior, grain refinement mechanism and corrosion resistance enhancement mechanism of nano-La2O3 in electroless Ni-B systems are extremely scarce, while the strengthening effect of La2O3 has only been reported in Ni-P, Ni-W and other alloy systems. This work clarifies the synergistic strengthening mechanism of nano-La2O3 in electroless Ni-B coatings, including grain boundary pinning, grain refinement and passive film stabilization. The findings offer both theoretical insights and technical guidance for fabricating advanced Ni-B based composite coatings.
3. Results
The morphology of the Ni-B coating is displayed in
Figure 2a, and the morphological characteristics of the Ni-B/La
2O
3 composite coating surface deposited under different concentrations of nano-La
2O
3 is shown in
Figure 2b–e, and the loading of nano-La
2O
3 in the electroless plating bath ranges from 0 g·L
−1 to 10 g·L
−1. The magnification from
Figure 2a–e is 5000×. It is evident from
Figure 2a that the outer layer of Ni-B alloy coating has a densely arranged spherical structure. Observing
Figure 2b–e, it is apparent that the surface of Ni-B/La
2O
3 composite coating does not have pinholes, cracks or other defects that affect the wholeness of the deposited layer, and the surface is compact and well-distributed. With the increase in nano-La
2O
3 particle content, a gradual increase in surface material is observed, accompanied by a change in surface morphology. This observation could be explained by the progressive enhancement of surface deposit coverage with increasing nano-La
2O
3 particle concentration in the plating bath. Among them, when the addition of nano-La
2O
3 reached 8 g·L
−1 (
Figure 2d), the composite coating demonstrates enhanced surface quality, with a more compact and homogeneous morphology.
However, when the addition of nano-La
2O
3 reached 4 g·L
−1 (
Figure 2b), the clustering of nano-La
2O
3 resulted in the development of distinct clusters on the composite coating surface. Excessive agglomeration of nano-La
2O
3 particles may lead them to fall off. This detachment, combined with the formation of large inter-nodular gaps, leads to an increase in surface defects on the coating, as shown in
Figure 2e. In addition, hydrogen production can also promote defect formation on the coating surface during electroless plating at higher nanoparticle concentrations. These factors can lead to a deterioration in coating properties.
Figure 2f illustrates the results of the Ni-B/La
2O
3 composite coating at the nano-La
2O
3 concentration (8 g·L
−1) to investigate the coating/substrate interface, as well as the coating thickness. The thickness of composite coating is about 10.3 μm. The composite coating-metal matrix interface is free from structural imperfections, including micro-cracks, cracks, and delamination. This defect-free interface suggests a compact bonding and superior adhesion between the coating and the substrate.
To better visualize the distribution of nano-La
2O
3 within the composite coating, we performed an EDS mapping on the surface region of Ni-B/La
2O
3 composite coating at the nano-La
2O
3 concentration (8 g·L
−1) as shown in
Figure 3. From the region selected in the scan, the coating is found to contain predominantly Ni, B, and La. A nano-La
2O
3 composite coating was successfully fabricated, as evidenced by the results. Additionally, it was found that the nano-La
2O
3 particles are homogeneously distributed throughout the coating. However, due to the relatively shallow scanning depth of the scanning electron microscope, the detected content of La in the coating is low. As B is a light element, its signal may be overshadowed by that of Ni, leading to an underestimation of its content.
Table 3 provides a detailed EDS element distribution of Ni-B/La
2O
3 composite coating. The B content is 1.20 wt.%, which is basically consistent with Ni-B coating prepared using DMAB as the boron precursor, which typically contain 0.1–2 wt.% B.
In order to gain insight into the performance-related crystallographic features, the Ni-B/La
2O
3 composite coating was characterized by XRD to determine its crystal planes and crystallite size. The obtained diffraction patterns are presented in
Figure 4. In
Figure 4a, we found Ni characteristic peaks at 44.496° and 51.849°, assigned to the Ni (111) and Ni (200), respectively. The Ni-B/La
2O
3 composite coatings exhibit broad and poorly defined Ni diffraction peaks, which are characteristic of nanocrystalline or partially amorphous structures. The significant peak broadening arises from two main factors: (
i) the fine crystallite size (12–20 nm, as calculated in
Figure 4b) and (
ii) lattice microstrain induced by the solid solution of boron atoms into the nickel lattice. Notably, only the Ni (111) peak is clearly distinguished, while the Ni (200) peak appears much weaker and broader. This phenomenon is commonly observed in nanocrystalline Ni-based coatings and can be explained by a preferred (111) crystallographic orientation and significant anisotropic microstrain, which preferentially broadens the (200) reflection.
At the same time, the incorporation of nano-La2O3 led to changes in the relative peak intensities; however, this had no effect on the crystalline phase formation. Upon increasing the nano-La2O3 content in the electrolyte (0 g·L−1 to 4 g·L−1), a reduction in the relative peak intensities was observed, emphasizing that the coating has smaller crystalline sizes. This may be due to the pinning effect of nano-La2O3, which suppresses the movement of grain boundaries, thus inhibiting grain growth and reducing the crystalline size of the coating. When the nano-La2O3 content reached 6 g·L−1 and 10 g·L−1, the Ni (111) peak became more intense and its shape sharpened considerably. This may be attributed to agglomeration, which reduces nucleation sites and consequently increases crystallite size. Furthermore, no characteristic diffraction peaks of nano-La2O3 were observed in the XRD patterns, this phenomenon possibly arising from the fact that the amount of nano-La2O3 present at the composite coating surface falls below the detection threshold of XRD.
The average crystalline size is used to further verify the function of nano-La
2O
3 on the coating crystalline size. The crystallite size was calculated using Scherrer’s equation:
In Scherrer’s equation,
D corresponds to the mean crystallite size,
K denotes the Scherrer constant (typically 0.89),
λ represents the X-ray wavelength (1.54056 Å),
β represents the peak broadening at half maximum intensity (FWHM), and
θ corresponds to the Bragg angle. The peak broadening (FWHM) values were obtained by fitting the Ni (111) and Ni (200) diffraction peaks using a pseudo-Voigt function after background subtraction in X’Pert HighScore Plus software 2.2a. The instrumental broadening was calibrated using a standard LaB
6 sample. The corrected FWHM was then used in the Scherrer equation.
Figure 4b demonstrates that the average grain size of the Ni-B/La
2O
3 composite coating decreases up to a certain nano-La
2O
3 concentration, beyond which it increases. The Ni-B/La
2O
3 (8 g·L
−1) composite coating has the minimum grain size (12.943 nm). However, adding excessive nano-La
2O
3 to the deposition solution leads to increased accumulation, and the agglomeration of nanoparticles hinders the development of the coating’s surface microstructure. This further confirms that uniformly dispersed nano-La
2O
3 is beneficial for grain refinement of the coating, forming a relatively dense microstructure, which is one of the factors responsible for the enhanced coating performance.
To further demonstrate that nano-La
2O
3 has been successfully mixed into the Ni-B coating, we analyzed the bond energy of the compound using XPS as displayed in
Figure 5, which demonstrates the XPS test diagram of the Ni-B/La
2O
3 composite coating, which contains four elements: C, B, Ni and La. It should be noted that energy-dispersive X-ray spectroscopy (EDS) has inherent limitations in accurately quantifying light elements such as boron (B) due to the low fluorescence yield of light elements and the strong spectral overlap between B-Kα (≈183 eV) and Ni-Mζ (≈186 eV) lines. Therefore, the B contents reported in
Table 3 are semi-quantitative and serve primarily for comparative purposes rather than as absolute values. As shown in
Figure 5a, the high-resolution C 1s spectrum can be fitted with three components centered at binding energies of 284.83, 286.28, and 288.18 eV, which are attributed to C–C, C–OH, and O–C=O species, respectively.
Figure 5b shows the 1s spectra of element B, with peaks at 187.18, 187.43 and 192.13 eV, which can be assigned to B
4C, Ni
XB and boron oxide, respectively. As presented in
Figure 5c, the high-resolution Ni 2p spectrum can be resolved into three components. The peaks at 852.03, 855.53, and 861.38 eV correspond to metallic Ni (Ni0), NiO/Ni(OH)
2 species, and the corresponding shake-up satellite, respectively, all of which belong to Ni 2p3/2. Meanwhile, the features observed at 869.18, 873.28, and 879.93 eV are attributed to metallic Ni (Ni0), NiO/Ni(OH)
2 species, and the corresponding shake-up satellite, respectively, which belongs to Ni 2p1/2. The presence of Ni(OH)
2 suggests that metallic Ni on the Ni-B/La
2O
3 composite coating surface has undergone oxidation, forming a nickel oxide film. Studies have shown that this nickel oxide film is preferentially formed as a passivation product at the grain boundary and forms an adherent barrier layer on the coating surface, thereby enhancing corrosion protection.
Figure 5d shows the 3d spectra of the element La, where the La 3d spectrum displays two distinct peaks at 835.13 eV and 838.48 eV, corresponding to the La 3d
5/2 core level. The presence of these characteristic La signals verifies that nano-La
2O
3 has been successfully embedded within the Ni-B coating, confirming the successful fabrication of the Ni-B/La
2O
3 nanocomposite.
Figure 6 shows the EIS results. It is obvious that the impedance of all Ni-B/La
2O
3 composite coatings with added nano-La
2O
3 surpass that of the unmodified Ni-B coating (
Figure 6a), indicating that incorporation of nano-La
2O
3 effectively enhances the coating’s corrosion resistance. Among them, the composite coating containing 8 g·L
−1 nano-La
2O
3 displays the greatest impedance semicircle diameter, signifying superior corrosion protection. The rest are ranked in descending order of impedance as Ni-B/La
2O
3 (10 g·L
−1) composite coating, Ni-B/La
2O
3 (6 g·L
−1) composite coating, Ni-B/La
2O
3 (4 g·L
−1) composite coating, and Ni-B coating.
Figure 6b is the Bode plot of the Ni-B/La
2O
3 (0 g·L
−1–10 g·L
−1) composite coatings. The results show that in the low-frequency region, the Ni-B/La
2O
3 composite coatings exhibit excellent performance and maintain a prominent trend. Furthermore, the impedance modulus (|
Z|) at 0.01 Hz for each Ni-B/La
2O
3 composite coating is consistently higher than the unmodified Ni-B coating, and the |
Z| value at 0.01 Hz of the Ni-B/La
2O
3 (8 g·L
−1) composite coating is the highest. This is consistent with the impedance plot results, providing additional evidence that incorporating nano-La
2O
3 into the coating leads to improved corrosion protection, and among all formulations, the composite coating containing 8 g·L
−1 nano-La
2O
3 demonstrates the highest corrosion protection.
As revealed in
Figure 6c, the phase angle response of the Ni-B/La
2O
3 coatings varies with La
2O
3 content. The broadest and most elevated phase angle peak is observed at 8 g·L
−1, signifying the most compact and uniform surface structure, which correlates well with the enhanced corrosion resistance and the SEM microstructural findings.
In the case of a single time constant response, the widely used Randles equivalent circuit (
Figure 6d) is used for quantitative analysis. An equivalent circuit model is used for fitting the EIS data:
Rs(
CPEc(
Rc(
CPEtRt))).
Rc and
CPEc represent the resistance and constant phase element of the outer porous coating layer, and
Rt and
CPEt correspond to the inner barrier layer charge transfer process, which represents the resistance and constant phase element of the inner coating layer, the data of which are shown in
Table 4. Pitting corrosion in mild steel is mainly attributed to oxygen and chloride ions. Therefore, corrosion resistance can be substantially improved by introducing agents that either impede the transport of these ions or decrease the chloride ion content via chemical reactions. Within the
Rs(
CPEc(
Rc(
CPEtRt))) equivalent circuit,
CPEc corresponds to the double-layer capacitance at the electrode–electrolyte interface, which rises as the electrolyte permeates toward the substrate. Therefore, starting from the value of
CPEc, we can also analyze the erosion effect of the electrolyte solution on the coating. In the table, the data confirm that the coating with 8 g·L
−1 La
2O
3 exhibits the lowest
CPEc; it is suggested that the adsorption of chloride ions by the electrical double layer is significantly reduced by the presence of nanoparticles, making it more difficult for these ions to reach the coating surface and thus lowering the corrosion rate. Meanwhile the data confirm that the coating with 8 g·L
−1 La
2O
3 exhibits the highest inner layer resistance, consistent with its superior corrosion resistance.
To quantify and verify the rationality of the selected equivalent circuit, we have supplemented the chi-square goodness of fit values (
χ2) for each sample. The smaller the chi-square value, the higher the consistency between the fitting results and the experimental data. Generally, for EIS fitting, if the
χ2 value is on the order of 10
−3, the fitting results are considered reliable. As shown in
Table 4, the fitted chi-square values of all samples are at relatively low levels, indicating that fitting this composite coating system with a single-time-constant Randles circuit not only meets the requirements of physical model simplification but also has high mathematical fitting accuracy.
Figure 7 illustrates the polarization curves of Ni-B/La
2O
3 composite coating. The dynamic potential polarization was performed at a scan rate of 1 mV/s, from cathode to anode (from OCP − 200 mV to OCP + 200 mV). Based on these curves, the Tafel parameters (
βa,
βc,
Ecorr,
Icorr) were obtained by Tafel extrapolation, as shown in
Table 5. In polarization curve analysis, the corrosion potential (
Ecorr) is the open-circuit potential of the metal measured without external current.
Ecorr serves as an indicator of corrosion susceptibility: a higher (more noble)
Ecorr value typically corresponds to better corrosion resistance, whereas a lower (more active)
Ecorr indicates a greater tendency for the material to lose electrons and undergo oxidation, thereby increasing its corrosion susceptibility. From the polarization curves, it is apparent that the addition of nano-La
2O
3 shifts the Ni-B/La
2O
3 composite coating’s polarization curve to more positive corrosion potential values.
Table 5 also shows that with increasing nano-La
2O
3 concentration in the Ni-B/La
2O
3 composite coating,
Ecorr displaces to more positive potentials, while
Icorr decreases. This suggests that the coating exhibits enhanced inertness and superior corrosion resistance. Meanwhile, the Ni-B/La
2O
3 (8 g·L
−1) composite coating achieves the most positive
Ecorr (
Ecorr = −0.37189 V) coupled with the minimum
Icorr (
Icorr = 3.7524 μA/cm
2). Upon further increasing the nano-La
2O
3 content, the
Ecorr of the composite coating shifts to more negative values, accompanied by an increase in
Icorr, implying a reduction in the coating’s inertness and a decline in corrosion resistance. The more positive corrosion potential coupled with low corrosion current sufficiently demonstrate that the Ni-B/La
2O
3 (8 g·L
−1) composite coating has optimal corrosion resistance.