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A review on hydrogen production from ammonia borane: Experimental and theoretical studies
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Jinrong Huoa, c, Kai Zhanga, c, Haocong Weia, c, Ling Fue, Chenxu Zhaoc, d, Chaozheng Hec, d, *, Xincheng Hub, *
Chinese Chemical Letters | 2023, 34(12) : 108280
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Chinese Chemical Letters | 2023, 34(12): 108280
Review
A review on hydrogen production from ammonia borane: Experimental and theoretical studies
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Jinrong Huoa, c, Kai Zhanga, c, Haocong Weia, c, Ling Fue, Chenxu Zhaoc, d, Chaozheng Hec, d, *, Xincheng Hub, *
Affiliations
  • a School of Sciences, Xi'an Technological University, Xi'an 710021, China
  • b Henan Engineering Center of New Energy Battery Materials, College of Chemistry and Chemical Engineering, Shangqiu Normal University, Shangqiu 476000, China
  • c School of Materials Science and Chemical Engineering, Institute of Environmental and Energy Catalysis, Xi'an Technological University, Xi'an 710021, China
  • d Shaanxi Key Laboratory of Optoelectronic Functional Materials and Devices, School of Materials Science and Chemical Engineering, Xi'an Technological University, Xi'an 710021, China
  • e College of Resources and Environmental Engineering, Tianshui Normal University, Tianshui 741001, China
Published: 2023-12-15 doi: 10.1016/j.cclet.2023.108280
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Ammonia borane (NH3BH3, AB) is an ideal raw material of hydrogen production with higher hydrogen storage capacity. In this paper, the catalytic processes of AB dehydrogenation were described from different ways, including thermal dehydrogenation, hydrolysis, methanolysis, photocatalysis and photo-piezoelectric synergy catalysis with experimental research and theoretical calculations. Catalyst models include bulk materials, two-dimensional materials, nanocluster particles and single/diatomic structures. Among them, the proportion of H2 released is different, and the reaction conditions are also different, which are suitable for different application scenarios. Through this review, we could have a preliminary comprehensive understanding of AB dehydrogenation reaction.

Ammonia borane  /  Hydrogen production  /  Dehydrogenation catalyst  /  Hydrolysis  /  Methanolysis  /  Photo-piezoelectric synergy
Jinrong Huo, Kai Zhang, Haocong Wei, Ling Fu, Chenxu Zhao, Chaozheng He, Xincheng Hu. A review on hydrogen production from ammonia borane: Experimental and theoretical studies[J]. Chinese Chemical Letters, 2023 , 34 (12) : 108280 - . DOI: 10.1016/j.cclet.2023.108280
H2 is a clean and renewable fuel. So it will play a vital role in transition from conventional fossil fuels to renewable energy sources on the way towards a sustainable energy future. Like H2 production from ammonia borane, water splitting is also a promising startegy [1-3]. The safe storage and transportation of H2 has become the most important challenge. Ammonia borane (AB), the simplest type of B–N hydride, with a molecular weight of only 30.7 g/mol and a hydrogen storage capacity of up to 19.6 wt%, which was successfully synthesized in 1955 by Shore and Parry [4]. Ammonia borane become the most promising hydrogen carrier materials because it has some excellent physical and chemical properties, such as remain stable solid form at ambient conditions, high hydrogen content, eco-friendly, and high solubility in most solvents. AB coulde released ultrapure hydrogen via dehydrogenation reaction, hydrolysis reaction and methanolysis reaction.
In the 1950s, with the help of diethyl ether, Shore and Parry [4,5] synthesized AB through lithium borohydride and diammoniate of diborane. The reaction process is expressed as follows:
Yields of AB are only 45% of this process, which is far from enough for large-scale commerce applications of AB. Enhancing the yields of AB are one of the main goals. Heldebrant et al. [6] through metathesis of NH4X and MBH4 salts in liquid NH3 to synthesize AB and it is synthesized efficiency reach 99%. The reaction process is as follows:
So far, the high efficiency of AB has been achieved, which greatly promotes the wide application of AB.
Since 1995, the synthesis efficiency of aminoborane has increased from an initial 45% to 99% (prepared by the reaction of NH4X + MBH4 in liquid ammonia, where X represents halogen and M represents alkali metal). Ramachandran from Purdue University in the United States and his scientific research team have been committed to the study of the preparation reaction of aminoborane for many years. In 2015, they further optimized the reaction conditions, so that SBH (NaBH4) and (NH4)2SO4 could react to prepare aminoborane in an open environment in the presence of THF(C4H8O), and the reaction yield could reach more than 90%. This greatly reduces the price of commercial ammoniborane and improves the practicality of large-scale application of AB [7-9].
One method of releasing hydrogen from AB is thermal dehydrogenation [5-7]. The process of thermal dehydrogenation of AB as follows (Fig. 1a):
This indicates that AB is stable at a lower temperature (< 90 ℃), and the release of H2 requires a higher temperature, which limits the applicable of AB. So, looking for a catalyst material that catalyzes the ammonia borane dehydrogenation reaction at room temperature or about room temperature has been a major challenge. Experimental and theoretical efforts have been made to achieve this goal.
In order to make full use of H2, the dehydrogenation of ammonia borane should be realized in the near proton exchange membrane (PEM) fuel cell operating temperatures (−85 ℃) [10,11]. Co-P-B coating on Ni (Fig. 1a) [12] and silicon nanoparticles [13] catalysts were used as catalysts to study thermal decomposition of ammonia borane and can achieve the maximum hydrogen production rate at around 80 ℃. At the same time, for safety, we should ensure that the mixture of AB and catalyst is stable below 50 ℃ and does not produce H2. Therefore, it is very important to raise the triggering temperature of catalyst to about 60 ℃. By heating NH3BD3 to about 200 ℃ until two H2 molecules are released, hydrogen (HD) was released mainly from heteropolar hydrogen-deuterium interactions (N−Hδ+··· δ+D−B) and homopolar dihydrogen interactions (N−Hδ+···δ+H−N), and homopolar dideuterium interactions (B−Dδ···δ D−B) is negligible (Fig. 1b) [14]. As shown in Fig. 1c [15], using this configuration, a mixture of AB: MA = 1:1 was placed at the bottom, while another mixture of AB: BA = 1:1 was added at the top, the H2 equivalent was improved to 2.11 at 60 ℃. This also increases the H2 yield and lowers the temperature required for the reaction.
Cu metal has better catalytic activity for AB thermal catalytic process. As shown in Figs. 2a and b, the study have shown that CuCl2 has the highest catalytic activity at 85 ℃ among FeCl2, CoCl2, NiCl2, CuCl2, and ZnCl2 [16]. Moreover, Salinas-Torres et al. [17] added Cu atom in La0.7Sr0.3CoO3 and realized the highest catalytic activity among, when containing 2.72 wt% of Cu, turnover frequency (TOF) reaches 843 L H2/h. In this process, the closer interaction Cu-Co might be favoring the catalytic activity. The catalytic process is shown in Fig. 2c.
Tong et al. [18] construct two catalyst structures of AB-Pd2/MgO and AB-Pd4/MgO to investigated dehydrogenation mechanism of ammonia borane by DFT/UB3LYP method (Fig. 3a). The calculation results are shown in Fig. 3a and rate determining step (RDS) barrier reach 9.4 and 12.6 kcal/mol, respectively (Fig. 3b). Zhou et al. [19] calculated the catalysts of Fe2, FeCu, and Fe12Cu to catalyze dehydrogenation of AB through Gaussian 03 Program and for Fe12Cu catalyst, overall exothermic and barrierless were achieved, as shown in Fig. 3c. Kuang et al. [20] calculated various possible paths that pristine and defective h-BN sheets catalyst material catalyzed the dehydrogenation of AB to H2, indicating that defective was conducive to improving the catalytic activity. The defective h-BN sheets with VB and V3B+N vacancies are excellent metal-free catalysts for facilitating the hydrogen release of AB [20]. As shown in Figs. 3d and e, the energy barriers to release the H2 are 0.77 and 0.84 eV, respectively. This is a lower activation barrier than N-doped graphene catalysts. Wu et al. [21] showed that single Pt atoms supported on oxidized graphene (Pt1/Gr-O) catalyst can catalyze AB hydrolysis. The rate-limiting barrier is 16.1 kcal/mol, and the catalyst can spontaneously recover after H2 release. The production process of the first H2 molecule is shown in Fig. 3f. Based on the Kissinger method and isoconversional model-free fitting method of AB, and solid-state kinetics model-based method, Gangal and Sharma [22] obtained a new mechanism, based on the fundamental kinetic equations and isothermal experimental data.
We focus on the thermal decomposition of AB catalyzed by two-dimensional (2D) materials or nanoclusters (Fig. 4). Using 2D MgSiP2 structure [23] as the catalyst, we achieved the dissociation of 6 H atoms in AB, and 1 mol AB could generate 3 mol H2 without the participation of H2O molecules in the reaction. AB dehydrogenation is realized on the surface of Os/P3C monatomic structure [24] catalyst, and the calculation shows that the doping of O atom can greatly reduce the activation barrier. The reaction process of AB thermolysis dehydrogenation was simulated by Fe22@Co58 core-shell structure and Fe36Co44 bimetallic nanocluster catalyst [25,26].
The hydrolysis of AB is one of the safe and stable methods to prepare H2. The hydrolysis reaction path with break of B-N bond can be divided into four types (Eqs. 7–10) [25,27,28]. There is no difference in the formation process of the first H2, and the difference mainly comes from the formation of the second and three H2, as shown in the following formula:
In the other case that the B-N bond is not broken, the first H2 molecule is produced as follows [29]:
Taking Pt1Co1 as an example, the possible mechanism for the AB dehydrogenation reaction [30] is shown in Scheme 1.
Hydrolysis reaction is an effective catalytic process of AB dehydrogenation, and a variety of catalyst materials can show excellent catalytic activity (Table 1) [27-67]. Among them, Ru0.5Ni0.5/g-C3N4 catalyst has the lowest activation barrier energy (Ea), reaching 14.1 kJ/mol. It can be found that the presence of noble metal Ru can greatly improve the reactivity of the catalyst and the reaction rate. The RuP@NHMCs catalyst has the largest TOF of 4307 mL molcatal −1 min−1 in the presence of 0.2 mol/L NaOH. This enhancement effect confirms that NaOH can behave as the catalyst promoter to facilitate the hydrolysis of AB at room temperature.
From Table 1, it can be seen that element P plays an important role in the catalytic process. The comparison of catalytic TOF of CoNiP/GO and NiCo-NC shows that the catalytic rate is increased by nearly 4 times. With the addition of P element, the catalytic activity barrier of CoP nanoparticles and Co/C is decrease significantly. In addition, the transition metal Ni also has a good catalytic activity. Comparing Ru0.5Ni0.5/g-C3N4 and Ru/CS, it can be found that due to the addition of Ni, the reactivity activation barrier becomes 1/3 of the previous one. Therefore, non-metals and transition metals also play an important role in the design of catalysts.
Theoretical simulation can describe the structure and energy change of the reaction process more specifically. From the perspective of computational simulation, Peng and co-workers [27] described the formation process of the first H2 molecule in detail with Ni2P-catalyzed, as shown in Fig. 5. The remaining two H2 molecules are formed by dropping the H atom which attached to B atom. The step-by-step reaction process can be expressed as follows (Eqs. 12–15):
The total reaction can be expressed as Eq. 16, and the whole reaction requires the participation of 4 H2O molecules. After crossing the barrier of 0.12 eV (due to the binding of AB with the active atom of the catalyst), the whole reaction can occur spontaneously at room temperature.
The break of the B-N bond in AB can also be achieved by OH attack, which is known as the SN2 reaction mechanism. Hou et al. [28] simulated the formation of the first H2 molecule by SN2 reaction mechanism on Ni3P2(0001) and NiCo2P2(0001) surface catalysts.
As shown in Fig. 6, among the catalyst structures of Pt1/Co3O4, Pt1/CeO2, Pt1/ZrO2, and Pt1/ graphene, Pt1/Co3O4 has the largest TOF (1220 min−1) and the smallest Ea (37.4 kJ/mol) [68] and Pt1/Co3O4 still maintained good catalytic activity after 15 cycles. As shown in Fig. 6e, after the adsorption of AB by Pt1/Co3O4, the 5d electron of Pt atom interacts strongly with H atom, resulting in obvious elongation of B-H bond.
Using non-noble metal Fe and Co elements as main components, we completed the calculation of the catalytic hydrolysis reaction of AB catalyzed by Fe36Co44 bimetallic nanoclusters [26]. The path diagram is shown in Figs. 7a and b. Meanwhile, the different catalytic effects of different activation and coordination environments were analyzed in this work. We have completed the complete calculation process of AB hydrolysis to prepare 3 mol H2 using Fe22@Co58 core-shell as catalyst material (Fig. 7c), and it was found that there were new reaction paths (Eq. 17) beyond the paths shown in Eq. 16 (Fig. 5c) [25].
In the case that the B-N bond is not broken, Li et al. [29] gave the catalytic reaction process on the Pt/Ni surface catalyst from the perspective of calculation simulation (Fig. 8a). From the calculation, it can be found that the incorporation of Pt atom reduces the reaction rate-determination step activation barrier (0.75 vs. 0.88 eV). Wu and co-workers [34] calculated the first H2 formation process of Co(111), CoO(200), and CoO/CoP surfaces respectively from the perspective of calculation. And the high activity of CoP-CoO/surfaces was revealed (Fig. 8b). On the doped Ni(0001) surface, the rate-determining step of the AB hydrolysis reaction is the dissociation of H2O molecule. Therefore, by means of the first-principles calculation, Li et al. studied the dissociation process of H2O molecule [39] and the reaction path shown in Fig. 8c.
Therefore, the specific path of AB hydrolysis reaction is different for different catalysts, and this process needs to be further studied.
Liberation of NH3 and inefficacy in recycling the hydrolysis product, metaborate become the mianly problems for hydrolysis of AB. Using methanol instead of water is a better choice, since that Ammonia borane has high solubility in methanol (23 wt% at 23 ℃), methanolysis produces pure H2 gas with no ammonia contamination, and the methanolysis product, ammonium tetramethoxyborate, is recyclable. The technology of ammonia borane methanolysis is another prominent technology that suitable for application in on-board hydrogen production. The methanolysis product of NH4B(OCH3)4 can be converted back to AB by reaction with LiAlH4 in the presence of NH4Cl [69-72]. The process of Methanolysis of AB is shown in Eq. 18:
Methanolysis of AB occurs only in the presence of a suitable catalyst. Various catalytic systems consisting of homogeneous and heterogeneous metal catalysts, such as metal cations, monometallic nanoparticles (NPs), alloys, and core-shell catalysts have been studied for catalytic AB methanolysis. Among them, noble metal catalysts such as Pd [70,73-75], Pt [76], Ru [77-81], Rh [82-89] and Cu [90-92] nanoparticles have been determined to have superior catalytic activities for H2 release from AB methanolysis. The results are shown in Table 2. Ru/Immobilized in Montmorillonite catalyst had the lowest activation barrier, indicating that the noble metal has good catalytic activity. However, their high cost and less content hinder their widespread use for practical applications. Therefore, development of cost-saver, efficient, and reusable supported catalysts is very vital to overcome aforementioned problems for on-board applications. So far, there are few reports on computational simulation of methanolysis reaction, which needs to be supplemented by researchers in subsequent studies.
As shown in Table 2, TOF and Ea of methanolysis of AB are listed. It can be found that Ru/MMT [77] has the lowest Ea, indicating that noble metal catalyst has high catalytic activity. CuNi NPs [92] also has a low Ea, indicating that transition metal elements also can serve as a good methanolysis of AB catalyst.
Photocatalysis is a clean reaction process. It is an important research direction to realize the dehydrogenation process of AB under visible light (λ > 420 nm) by reducing the band gap of semiconductor catalyst.
Visible light is the most abundant and convenient clean energy, which is constantly available and very easy to obtain. Therefore, visible light catalysis is an important research direction. For example, Au and Ag [93] are excellent photocatalytic materials with excellent LSPR in the ultraviolet and near-infrared regions. Au nanoparticles deposited on TiO2 [94] catalysts can be used as electron traps to prevent electron-hole recombination, thus improving catalytic activity.
Oxides are often important photocatalytic materials. under visible light irradiation (λ > 420 nm), MoO3−x [95,96] and WO3−x nanowires [97] could catalyze ammonia borane to generate H2 (Figs. 9a and c), which opens up new prospects for efficient heterogeneous catalysis of plasma semiconductor nanostructures. Through the load of the noble metal Rh, the activity of Rh/WO3-x [98] catalysts were further improved with a TOF as high as 805.0 molH2 molRh−1 min−1 and an apparent activation energy of 45.2 kJ/mol (Fig. 9b).
As shown in Fig. 10, in Pd/H2Ti3O7 composite nanowires catalyst [99], excited electrons accumulate to Pd under light conditions, so the existence of Pd promotes the separation of electron-hole and prevents electron-hole recombination. This synergy enhanced the catalytic activity of Pd/H2Ti3O7 composite nanowires. Monometallic Co and bimetallic CuCo and FeCo catalysts supported by g-C3N4 are catalysts for transition metal nanoclusters [100]. After electrons are activated in g-C3N4 under light, they transfer to metal atoms. The metal atom becomes the center of catalytic activity. Taking CoAu/g-C3N4 catalyst [101] as an example, under the influence of the Mott-Schottky effect, electrons are transferred from the conduction band of g-C3N4 to metal and a potential barrier is formed to prevent electron countercurrent. Under the influence of light, more electrons are excited into the metal, increasing the separation of charge.
With favorable transfer properties, better dispersion, CdS-TiO2/carbon nanocomposite with high surface area [102] has become a good catalyst for ammonia borane dehydrogenation. Using non-noble metal nanoparticle supported on a chromium-based MOF (MIL-101) [103], such as Cu/MIL-101, can efficient catalysts H2 production in the hydrolysis of AB. The electrons generated by illumination concentrate on the surface of Cu atoms, making Cu atom become a good reduction catalytic site, and MIL-101 becomes a good oxidation active site. Co and Ni NPs supported by these C3N4 species [104], where TOF of Co/C3N4 reaches 93.8 min−1, which exceeded the values of all the reported heterogeneous noble metal-free catalysts, has excellent catalytic activity. Co and Ni NPs supported by seven photoactive and non-photoactive MOFs [105], Co-based catalysts had the highest activities among the reported noble-metal-free catalysts at 298 K. The TOF value is 117.7 min−1 and the activity almost as good as that of noble metal catalyst.
Under light conditions, NiCu alloy loaded carbon nitride nanosheets (NixCuy/CNS) [106] realized the hydrolysis process of AB (Figs. 11a and b). Under the effect of localized surface plasmon resonance (LSPR), charge accumulates from Cu to Ni, and the catalytic reaction with Ni as the active site achieves the break of B-H bond in AB and O-H bond in H2O. In Au-Co nanoparticles (Au-Co@CN), electrons flow from g-C3N4 and Co atoms to Au atoms, and thus Au act as active atoms (Figs. 11a and b). For Co/P3.59CN nanocluster catalyst [107], electrons accumulate towards Co atoms, which makes Co atoms behave more like noble metals with higher activity (Figs. 11c and d). At 298 K, TOF reaches to 67.09 mLH−1 minCo−1. The comparison between Ru/g-C3N4 and Ru/C/g-C3N4 shows that [108], when Ru/C(1.0)/g-C3N4, average Ru NP size is the smallest, and the maximum TOF reaches 196.4 h−1. The TOF of RuP2-/g-C3N4 [109] could reach 175 min−1 under light conditions (Fig. 11e). At the same time, the change of P atom ratio will greatly affect Schottky barriers and promote electron movement (Figs. 11c and d). Oxide based Co/V2O5 [110] and Ti2O3 [111] have a narrow band gap, which can realize the catalytic process of ammonia borane dehydrogenation under light conditions. In Co/V2O5, photogenerated electrons transfer from V2O5 to Co atoms. It is an important research direction to realize AB dehydrogenation at low temperature. Through a reduction transformation method, nanoscale Ti2O3 particles with high chemical stability and narrow band gap are prepared, realizing a rapid production of 2.0 equiv. of hydrogen from AB at ambient temperature (Fig. 12a) [105,111]. In NiCoP/TiO2 [112] catalyst, under visible light NiCoP work as sensitizer to absorb light and generate electron-hole pair while TiO2 work as electron trapper. So positively charged NiCoP surface and negatively charged TiO2 surface are achieved under visible light, and the H2 generation rate from hydrolysis of AB was increased to 2.0 folds, with Ea reduced from 52.76 kJ/mol to 25.89 kJ/mol. However, if 2.5%Pt is added to TiO2, the reaction rate will increase to 0.55 mL/s (Fig. 12b). In different proportions of CuNi/TiO2-CdS, Cu0.45Ni0.55/TiO2-CdS catalyst [113] had the fastest hydrogen evolution rate with a high conversion frequency (TOF) of 25.9 molH molcat−1 min−1 at 25 ℃ and low activation energy of 32.8 kJ/mol (Fig. 12c). The band gap of TiO2 structure modified by Fe3+ and graphene decreases [108,114], and the light absorption spectrum line has an obvious red shift (Fig. 12d). When added graphene concentration is 1% and Fe3+ concentration is 2%, H2 production efficiency is the highest, reaching 1235.32 µmol min−1 gcat−1 (Fig. 11d).
Au-Ru alloy [115] and Ag@Pd core-shell nanocubes [116] catalysts show significant light-boosting effect. Among them, the TOF of Au-Ru alloy catalyst reaches 240 molH molcat−1 min−1. Under the influence of light, electron transfer can be realized. For example, in Co-CeVO4/CeO2 catalyst [117], electrons are transferred from CeO2 to CeVO4 and then to Co atoms, thus forming electron-hole centers, respectively (Fig. 13).
TiN-Pt nanohybrid can catalyze the dehydrogenation of AB under light conditions [48]. The calculated study shows that the barrier of H2O dissociation in AB hydrolysis reaction is 0.3 and 0.5 eV under illumination and no illumination, respectively (Fig. 14a), indicating that illumination reduces the activation barrier.
Theoretical calculations show that the addition of Cu atoms greatly reduces the dissociation barrier of H2O, which is the RDS of AB hydrolysis, and the migration barrier of OH, which enables the reaction process to be carried out at lower temperatures. NiCu alloy loaded carbon nitride nanosheets (NixCuy/CNS) catalyst [106], under the influence of LSPR, electrons are transferred from Cu to Ni atoms, which makes Ni atoms activated and accelerated break of O−H bond from H2O and B−H bond from AB. Subsequently, the redox reactions separately proceed in the electron-rich metal and the hole-rich CNS. In this case, (1) M−H and M−H+ will combine with each other to release hydrogen molecules (HH+); (2) Two M−H+ intermediates will also get two electrons from electron-rich Ni sites to form hydrogen molecules (H+H+); (3) Two M−H will also get two holes from hole-rich CNS sites at the interface between the metal and the CNS carrier to form hydrogen molecules (HH). These intermediates M−BH2+NH3 react with the M−OH forming a H3NBH2OH species. Eventually, one molecule of AB and two molecules of H2O produce three H2 molecules and one molecule of NH4BO2 (Figs. 14b and c).
Whether single metal or binary metal clusters are attached to g-C3N4 surface (Cu/CNS, Ni/CNS and Cu0.5Ni0.5/CNS) [118], the band gap is greatly reduced and the transfer of photogenerated electrons and holes is increased, thus improving the photocatalytic activity. The calculated bandgap of pure CNS, Cu/CNS, Ni/CNS and Cu0.5Ni0.5/CNS were 1.18, 0.74, 0.54 and 0.36 eV respectively. β-SiC exhibits high catalytic activity when loaded with Pt and Ru clusters. By comparing the band structure of Pt/β-SiC and Ru/β-SiC with β-SiC [119]. Pure β-SiC is a wide band gap semiconductor catalyst, and the band gap of the Pt/β-SiC and Ru/β-SiC are less than the pure β-SiC. This is in good agreement with the experimental results (Fig. 15).
The electric field affects the distribution and transfer of charge, which is an important factor in catalytic reactions. A built-in electric field was formed on the surface of PtNi Alloy nanoparticles on Al2O3 (Al2O3-PtNi) catalyst, which promoted the process of AB dehydrogenation. As shown in Fig. 16a, the flow direction of electrons promotes the fracture of B-H bond and N-H bond, respectively [120].
With the help of the First-principles calculation simulation, activation of B-H bond in AB was achieved on BC3 surface [121] by applied axial electric field (Fig. 16b). The applied electric field can act as a switch for the activation of B-H and N-H bonds in AB, and the dehydrogenation of AB can be realized under the action of the applied axial electric field. For Pt-M /BC3N2 (M = Al, Zn, Hf, Y) diatomic catalysts, B-H bond and N-H bond break process have different switching electric field (Fig. 16c) [122].
Photopiezoelectric co-catalysis has been widely used in dye degradation and water splitting [123-128]. The photo-piezoelectric synergy effect can improve catalytic activity, and since the dehydrogenation of AB involves both oxidation and reduction, the separation of electrons and holes becomes critical. In Ag2O-BaTiO3 hybrid photocatalyst, the built-in electric field is formed through continuous ultrasonic excitation to continuously separate photocarriers and improve the catalytic activity [129]. In the case of NIPS compounds (Ni2P, Ni12P5 and Ni3P) [130], illumination promotes electron-hole separation and migration to two different surfaces to form oxidation and reduction active sites, respectively, catalyzing the dehydrogenation of AB.
MoS2 is superior piezocatalyst and Doped with metal atoms could changes the band gap of MoS2, allowing MoS2 to be activated by visible light to generate electron-hole pairs (Fig. 17) [131]. Co-doped [132] and Sr-doped [133] MoS2 two-dimensional materials can simultaneously form oxidation and reduction catalytic sites by forming a built-in electric field to promote electron-hole separation under the photo-piezoelectric co-catalytic action, and can catalyze the break of B-H bond and N-H bond in AB to generate H2 in the visible region.
AB regeneration is an important part of AB dehydrogenation reaction, which determines the promotion of application scope of AB dehydrogenation reaction. Up to now, AB regeneration and recycling are realized by means of intermediates and alcohols [69,72,134]. AB was regenerated from methanolysis intermediate by following borate → B(OH)3 → B(OMe)3 → NaBH4 → NH3BH3 (Fig. 18). The cost of regeneration is lower, and more environmentally friendly. And it could realize high yields (≥95%) and very high purity (≥98%).
Whether thermolysis, hydrolysis or methanolysis, AB can be regenerated by reaction byproducts. Sutton et al. [135] showed that the byproduct "BNH" after thermal decomposition of ammoniborane could react with N2H4 to regenerate BH3NH3 and realize the reaction cycle. Because the by-products of hydrolysis and alcoholysis have B-O bonds (NH4BO2 and NH4B(OCH3)4), and B-O bonds are more stable than B-N bonds, it is more difficult to prepare BH3NH3 from the byproducts of hydrolysis and alcoholysis than from the products of thermal decomposition. Hausdorf et al. showed that AB can be recycled from the by-product of "BNH" and the reaction material can be saved as much as possible [136]. Through the byproduct of thermal decomposition reaction "BNH" to achieve AB regeneration, the reaction process is further simplified as [135]:
AB can been regenerated by NH4BO2, a byproduct of the hydrolysis reaction, and the reaction process is as follows [137]:
Also, for methanolysis, AB can been regenerated by NH4B(OCH3)4, a byproduct of the methanolysis reaction, and the reaction process is as follows [69]:
The high hydrogen capacity of 19.6 wt% has made AB an attractive material for chemical hydrogen storage. In this paper, we describe AB dehydrogenation from the aspects of thermal decomposition, hydrolysis, methanolysis, photocatalysis and photo-piezoelectric synergy catalyzes. The adaptive relationship between different catalyst structures and catalytic reaction types was explored, which provided important theoretical support for the design of AB dehydrogenation catalyst. The convenient generation and transportation of H2 will expand the application scenarios of hydrogen energy and make important contributions to solving the energy crisis and environmental protection.
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
This study were funded by the Natural Science Basic Research Program of Shaanxi (Nos. 2022JQ-108 and 2022JQ-096) and the National Natural Science Foundation of China (No. 22104079).
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Year 2023 volume 34 Issue 12
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doi: 10.1016/j.cclet.2023.108280
  • Receive Date:2022-12-20
  • Online Date:2025-11-21
  • Published:2023-12-15
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  • Received:2022-12-20
  • Revised:2023-02-18
  • Accepted:2023-02-28
Affiliations
    a School of Sciences, Xi'an Technological University, Xi'an 710021, China
    b Henan Engineering Center of New Energy Battery Materials, College of Chemistry and Chemical Engineering, Shangqiu Normal University, Shangqiu 476000, China
    c School of Materials Science and Chemical Engineering, Institute of Environmental and Energy Catalysis, Xi'an Technological University, Xi'an 710021, China
    d Shaanxi Key Laboratory of Optoelectronic Functional Materials and Devices, School of Materials Science and Chemical Engineering, Xi'an Technological University, Xi'an 710021, China
    e College of Resources and Environmental Engineering, Tianshui Normal University, Tianshui 741001, China
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表12种不同金属材料的力学参数

Family
属数
Number of
genus
种数
Number of
species
占总种数比例
Percentage of
total species (%)

Genus
种数
Number of
species
占总种数比例
Percentage of total
species (%)
鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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