Cation vacancy stabilization of single-atomic-site Pt1/Ni(OH)x catalyst for diboration of alkynes and alkenes

Development of single-atomic-site catalysts with high metal loading is highly desirable but proved to be very challenging. Although utilizing defects on supports to stabilize independent metal atoms has become a powerful method to fabricate single-atomic-site catalysts, little attention has been devoted to cation vacancy defects. Here we report a nickel hydroxide nanoboard with abundant Ni2+ vacancy defects serving as the practical support to achieve a single-atomic-site Pt catalyst (Pt1/Ni(OH)x) containing Pt up to 2.3 wt% just by a simple wet impregnation method. The Ni2+ vacancies are found to have strong stabilizing effect of single-atomic Pt species, which is determined by X-ray absorption spectrometry analyses and density functional theory calculations. This Pt1/Ni(OH)x catalyst shows a high catalytic efficiency in diboration of a variety of alkynes and alkenes, yielding an overall turnover frequency value upon reaction completion for phenylacetylene of ~3000 h−1, which is much higher than other reported heterogeneous catalysts.

S ingle-atomic-site (SAS) heterogeneous catalysts have attracted much recent interest owing to their specific activity and maximum atom efficiency for low cost [1][2][3][4][5][6][7][8][9][10] . However, synthesis of such SAS catalysts is not trivial because isolated metal atoms are often very mobile and easy to sinter under realistic reaction conditions due to their high surface free energy 2,4 . For this reason, most available SAS catalysts must keep a low loading density of guest metals (usually <0.5 weight percent (wt%)) to resist their aggregation, and it remains a great challenge to improve the loading content in such catalysts for practical applications 5 . Exploiting defects on supports to enhance the interaction between individual metal atoms and the supports has been an effective strategy to fabricate SAS catalysts [11][12][13][14][15][16][17][18][19][20][21][22] . So far, much work has focused on oxygen vacancy defects on oxides and carbon vacancy defects on graphene [11][12][13][14][15][16][17][18] . Cation vacancies are another kind of classical defects but are comparatively little investigated in the research field of SAS catalysts [19][20][21][22] , probably because of their difficult characterization and scarce suitable support materials with such defects 23 . Hydroxides are a large class of functional, environmentally friendly, and inexpensive host materials 24 . As far as we know, the cation vacancies on hydroxides have never been reported, and utilizing the defect-rich hydroxide to achieve a high metal-loading SAS catalyst has not been realized yet.
Boronic acids and their derivatives are versatile and useful compounds for various applications in organic synthesis 25 , material science 26 , and biomedicine 27 . Over the past decades, a broad variety of transition-metal-catalyzed protocols have been developed for the preparation of these compounds 28 . Among them, the diboration of carbon-carbon multiple bonds represents a straightforward and atom-economic strategy 29 . Since the first discovery of the Pt-catalyzed diboration of alkynes by Suzuki and Miyaura et al. in 1993, various homogeneous transition-metal catalysts have been successfully applied into the diboration of alkynes or alkenes [29][30][31][32][33][34][35] . However, up to now, the development of heterogeneous catalysts for such diboration reactions lags far behind the homogeneous catalysts with limited reported cases that include Pd/C 36 , nanoporous-gold 37 , Pt/TiO 2 38 , and Pt/MgO 39 . To make matter worse, these heterogeneous catalysts are restricted in practical application for their low catalytic efficiency (overall turnover frequency (TOF overall ) upon reaction completion <50 h −1 ). There is thereby an urgent need to prepare a new heterogeneous catalyst with better catalytic efficiency for diboration reactions. Given that the catalytically active components in these reported catalysts are all metal nanoparticles and downsizing metal particles to single atoms is ordinarily a great impetus to improve the performance of a catalyst 4,5 , we expect that the rational design of SAS catalysts will offer exciting opportunities to achieve the ideal heterogeneous catalysts for diboration reactions.
Here we report that a defect-rich nickel hydroxide (Ni(OH) x ) nanoboards (NBs) supported SAS Pt catalyst (Pt 1 /Ni(OH) x ) fabricated by a simple wet impregnation method. Notably, although there have been a few reports on the combination of nickel hydroxides with Pt nanoparticles, the construction of SAS Pt species on nickel hydroxides has never been achieved [40][41][42] . In this work, a new polycrystalline Ni(OH) x NBs are synthesized on a large scale via a one-pot solvothermal procedure. The abundant Ni 2+ vacancy defects on the Ni(OH) x NBs are shown to be critical for preparing Pt 1 /Ni(OH) x with Pt loading up to 2.3 wt%. The as-prepared Pt 1 /Ni(OH) x catalyst exhibits a good performance for the diboration of alkynes and alkenes. A TOF overall upon reaction completion much greater than that of all reported heterogeneous catalysts is demonstrated on Pt 1 /Ni(OH) x in the diboration of alkynes.

Results
Synthesis and characterization of the Pt 1 /Ni(OH) x catalyst. To prepare the Pt 1 /Ni(OH) x catalyst, a polycrystalline Ni(OH) x NB material was first synthesized on a large scale through a solvothermal reaction between nickel nitrate (Ni(NO 3 ) 2 •6H 2 O), urea, sodium bicarbonate (NaHCO 3 ), and tetrabutylammonium hydroxide (TBAH) in water/triethylene glycol mixed solvent (for details, see the Methods section). The typical transmission electron microscopic (TEM) image clearly illustrates that the assynthesized samples display a uniformly NB morphology (Fig. 1a). Clear irregular crystal lattice fringes are observed on the NBs in the high-resolution TEM (HR-TEM) image (Fig. 1b), indicating the polycrystalline structure of the sample, which is further proved by the selected-area electron diffraction pattern and X-ray diffraction (XRD) pattern (Supplementary Figs. 1 and 2). X-ray photoelectron spectroscopy (XPS) and Fourier transform infrared spectroscopy (FT-IR) of this polycrystalline NBs both exhibit features that are typical nickel hydroxide ( Supplementary Fig. 3). To the best of our knowledge, this onedimensional polycrystalline nanostructures of nickel hydroxide are newly synthesized by our work, which are more challenging in synthesis compared with common nickel hydroxide nanosheets 43,44 .
The Pt 1 /Ni(OH) x catalyst was then prepared with the assynthesized Ni(OH) x NB material as a support by a wet impregnation method, which stands for an easy-handling, straightforward, and low-cost pathway to synthesize catalysts 45,46 . Hexachloroplatinic acid (H 2 PtCl 6 ) was introduced into an ethanol dispersion of Ni(OH) x NBs to allow the adsorption of Pt precursors. The mixture was then centrifuged and the recovered solid was reduced with hydrogen to provide the Pt 1 / Ni(OH) x catalyst (for details, see the Methods section). Scanning transmission electron microscopy (STEM) images and XRD detections of the obtained Pt 1 /Ni(OH) x reveal that no formation of Pt nanoparticles are observed on Ni(OH) x NBs, even with the   Fig. 4). Further energy-dispersive X-ray (EDX) elemental mapping analysis confirms that Pt species are evenly dispersed in Pt 1 /Ni(OH) x (Fig. 1c). To verify the SAS Pt species on the Ni(OH) x NBs, we performed the aberrationcorrected high-angle annular dark-field STEM (AC HAADF-STEM) measurements on Pt 1 /Ni(OH) x (Fig. 1d). It is clear that all the Pt species exist exclusively at isolated single atomic sites; neither subnanometer clusters nor nanoparticles are detected. The presence of SAS Pt can be further confirmed by X-ray absorption spectrometric (XAS) studies. Figure 2a represents the extended X-ray absorption fine structure (EXAFS) spectrum of Pt 1 /Ni(OH) x and the reference spectra of Pt foil and PtO 2 at the Pt L 3 -edge using a Fourier transform (for corresponding EXAFS in K-space, see Supplementary Fig. 5). There is one prominent peak at~1.6 Å from the Pt-O contribution and a relatively weak peak at~2.9 Å from the Pt-Ni contribution but no peak at~2.6 Å from the Pt-Pt contribution, confirming the sole presence of SAS Pt in the Pt 1 /Ni(OH) x catalyst. Moreover, the oxidation state of these SAS Pt is determined by the X-ray absorption near-edge structure (XANES) spectra, as shown in Fig. 2b. The white-line intensities in the spectra reflect the oxidation state of Pt in different samples, so the white-line intensity of Pt 1 /Ni(OH) x , which is close to that of PtO 2 , implies that the SAS Pt in the Pt 1 / Ni(OH) x catalyst still remain in a high oxidation state even after the reduction by hydrogen.
Catalytic performance evaluation for diboration reactions. We next investigated the catalytic activity of the as-prepared Pt 1 /Ni (OH) x for diboration reactions. Initially, the diboration of phenylacetylene (1a) with bis(pinacolato)diboron (B 2 pin 2 ) (2a) was chosen as a model reaction (Supplementary Table 1, entry 1). To our delight, the Pt 1 /Ni(OH) x displayed a high activity and selectivity for this reaction. The conversion of phenylacetylene attained 97% within 20 min at a molar ration of 1:10 3 (Pt: phenylacetylene), and bare of other by-products like hydroborylated product were observed by gas chromatography-mass spectrometer (GC-MS) analysis ( Supplementary Fig. 6). The calculated TOF overall value of Pt 1 /Ni(OH) x upon this reaction completion can reach a high level as~3000 h −1 , much higher than that of other heterogeneous catalysts reported previously. In contrast, no reaction occurred when using Ni(OH) x NBs as the catalyst without Pt (Supplementary Table 1, entry 2). The catalyst can be reused at least five times without any loss of selectivity although the activity has a slight decay ( Supplementary Fig. 7). STEM and AC HAADF-STEM characterizations reveal that no morphology changes and Pt components are still dispersed at isolated single atomic sites in the recovered catalyst ( Supplementary Fig. 8). Moreover, the expansion of the reaction scale has no effect on the catalytic efficiency of this Pt 1 /Ni(OH) x catalyst for such diboration reactions (Supplementary Fig. 9). We further investigated the substrate scope of the diboration reactions to study the influence of substrate categories on the catalytic efficiency of Pt 1 /Ni(OH) x . As shown in Fig. 3, the aryl alkynes bearing electron-donating groups (R = Me, OMe) can react smoothly with B 2 pin 2 over Pt 1 / Ni(OH) x at the same conversion rate of phenylacetylene, affording the corresponding products 3ba and 3ca in excellent yields. When the substituents are electron-withdrawing groups (R = Cl, Br, NO 2 ) on the aryl ring, however, a longer reaction time is required to give the target molecular 3da-3fa in high yields. Differently from substituent types, substituent positions have no influence on the catalytic efficiency of Pt 1 /Ni(OH) x , whether meta-methyl or ortho-methyl substituted phenylacetylene can completely transform into the products 3ga and 3ha without any loss in the reaction rate. As for diboration of internal aryl alkynes like diphenylacetylene, Pt 1 /Ni(OH) x suffers from a relatively low catalytic activity, although a complete conversion of the substrate and a quantitative selectivity of diborylated product 3ia can be also achieved. To our delight, different kinds of aliphatic alkynes are appropriate for the diboration reactions over Pt 1 /Ni(OH) x as well, furnishing the desired products 3ja-3la with the similar reaction efficiency to the terminal aryl alkynes. Besides the various alkynes, different boronate esters like bis(neopentylglycolate)diboron (B 2 neop 2 ) can also work well with phenylacetylene to provide the product 3ab in an excellent yield and selectivity at the same reaction rate of B 2 pin 2 . Even more, alkenes were also chosen as substrates to evaluate the catalytic performance of Pt 1 /Ni(OH) x for diboration reactions. It shows that the diboration of styrene and 1-octene catalyzed by Pt 1 /Ni(OH) x can proceed well and provide a selectivity to products 3ma and 3na of 99% at the conversion level of 90% and 86%, respectively, although the reaction rates are lower than that of alkynes with similar molecular structures.

Discussion
Apparently, the good catalytic performance of Pt 1 /Ni(OH) x derives from the high loading content of Pt at isolated single atomic sites. It is noteworthy that such a high loading density of SAS catalyst is quite difficult in fabrication through the wet impregnation method [47][48][49][50] . The impregnated metal precursors generally adsorb on the surface of supports and thus tend to aggregate to form clusters or nanoparticles easily during the posttreatment processes 1 . For comparison, a conventional perfect Ni (OH) 2 material was synthesized and impregnated with H 2 PtCl 6 with a lower Pt loading at 0.9 wt% (as determined by ICP-OES) 11 Supplementary Fig. 11), which results in a relatively low catalytic efficiency of Pt/Ni(OH) 2 for diboration reactions (Supplementary Table 1, entry 3 and 4). This visible difference indicates that Ni(OH) x NBs have a stronger interaction with isolated Pt atoms than the perfect Ni(OH) 2 to prevent the formation of Pt clusters or nanoparticles.
To explore the nature of this strong interaction, we first carried out the EXAFS spectrometry analysis to probe the atomic structure of these two different nickel hydroxides. As shown in Fig. 4a, the Ni K-edge Fourier-transformed EXAFS spectrum of Ni(OH) x NBs exhibit an apparent difference in spectral shape compared with that of the perfect Ni(OH) 2 , implying the different local atomic arrangement and a defective structure of Ni(OH) x NBs 51 . Further EXAFS fitting analysis revealed that the values of Debye-Waller factor (σ 2 ) for the first Ni-O and Ni-Ni shells of Ni(OH) x NBs are both higher than that of the perfect Ni(OH) 2 , suggesting a higher degree of disorder in Ni(OH) x NBs, which is in accord with the polycrystalline structure of Ni(OH) x NBs (Supplementary Table 2). More importantly, the coordination number (N) of the first Ni-Ni shell of Ni(OH) x NBs is about 4.8, which is lower than that of the perfect Ni(OH) 2 (~6.2), whereas their coordination numbers of the first Ni-O shell are nearly same (~6.0), indicating the formation of Ni 2+ vacancies in Ni(OH) x NBs. Many studies show that the formation of Ni 2+ vacancies will lead some Ni 2+ ions to transform into Ni 3+ ions due to the  52 . Hence, we carried out XPS measurements to detect the Ni 3+ ions in the Ni(OH) x NBs. Figure 4b displays the representative XPS spectrum in Ni 2p 3/2 region of Ni(OH) x NBs and the perfect Ni(OH) 2 , which can be deconvoluted into four peaks. The signal of Ni 3+ ions can be clearly distinguished from that of Ni 2+ ions (centered at 855.3 eV and 861.0 eV) with higher binding energies at 857.2 eV and 864.7 eV, respectively, which correspond with the data reported [53][54][55] . Distinctly, unlike the perfect Ni(OH) 2 , Ni(OH) x NBs display a stronger signal of Ni 3+ ions, manifesting the possession of more Ni 3+ ions in the Ni (OH) x NBs. The proof of Ni 3+ ions in Ni(OH) x NBs is garnered from the soft XAS (sXAS) analysis, too. As shown in Fig. 4c, the obviously increased intensity at 532.0 eV (Ni-O interaction) at O K-edge of Ni(OH) x NBs relative to that of the perfect Ni(OH) 2 suggests that electrons transfer intensively from oxygen to nickel, which is consistent with the presence of Ni 3+ ions [56][57][58] . In addition, the ultraviolet-visible diffuse reflectance spectroscopy (UV-Vis DRS) experiments also evidence the Ni 3+ ions in Ni (OH) x NBs. As can be seen from Fig. 4d, besides the two absorption bands of Ni 2+ ions at 388 nm and 679 nm in the both two samples, a unique absorption band of Ni(OH) x NBs appears at 314 nm and is characteristic of Ni 3+ ions 59,60 . On the basis of all above evidences, we conclude that abundant Ni 2+ vacancies exist on the Ni(OH) x NBs and induce the strong interaction with isolated Pt atoms.
To gain more insight into the interaction between Ni 2+ vacancies and isolated Pt atoms, density functional theory (DFT) calculations were conducted to verify the different formation energies of the isolated Pt atoms loaded on the Ni(OH) 2 with and without Ni 2+ vacancies (for details, see Supplementary Methods section). As can be seen from Fig. 5, the Pt atom adsorbed on the Ni(OH) 2 with Ni 2+ vacancies displays a formation energy at −3.89 eV, which is much lower than that of the Pt atom adsorbed on the Ni(OH) 2 without Ni 2+ vacancies (at −0.72 eV). For the Ni (OH) 2 with Ni 2+ vacancies, the most stable adsorption site for the Pt atom is found to be the Ni 2+ vacancy site as well as the three-fold hollow site of the oxygen atoms, and the Pt atom is fixed by the three top oxygen atoms near to the Ni 2+ vacancy according to the charge density difference (Fig. 5a). In contrast, the Pt atom on the Ni(OH) 2 without Ni 2+ vacancies tends to locate at the site slightly deviated from three-fold hollow site of oxygen atoms, which is caused by the competition between the strong interaction between the Pt atom and three top oxygen atoms and the electrostatic repulsion between positive charged Pt and Ni atoms (Fig. 5b). Furthermore, the oxidation states of isolated Pt atoms anchored on the Ni(OH) 2 with and without Ni 2+ vacancies were also estimated by evaluating Bader charges of the Pt atoms in the film and by normalizing them to Bader charges of PtO 2 (for details, see Supplementary Methods section). As a result, the oxidation state of the Pt atom on the Ni(OH) 2 with Ni 2+ vacancies is +3.55, which is higher than that on the Ni(OH) 2 without Ni 2+ vacancies (+2.70) and very compatible with the aforementioned XANES data of Pt 1 /Ni(OH) x in Fig. 2b. This higher oxidation state illustrates the increase of charge transfer from the support to the Pt atoms 4 . In terms of these DFT calculation results and the XANES data, it is convinced that the Ni 2 + vacancies play a vital role in the stabilization of isolated Pt atoms deposited on the Ni(OH) x by eliminating the spatial segregation between the Pt atoms and uncoordinated O atoms, as well as decreasing the formation energy of the Pt atoms through promoting charge transfer from Ni(OH) x to them. Further DFT calculations on the catalytic mechanism of the Pt 1 /Ni(OH) x catalyst for diboration reactions even disclosed that the Ni 2+ vacancies not only play an important role in locating isolated Pt atoms but also are conducive to the diboration reactions because the low-coordination oxygen atoms at the vacancy site around the located Pt atoms benefit the dissociation of B-B bonds (for details, see Supplementary Methods section).
In summary, we report that a defect-rich Ni(OH) x NBs supported SAS Pt catalyst with remarkable performance in diboration reactions. The Ni(OH) x NBs with a polycrystalline structure are newly synthesized and successfully loaded with SAS Pt to a high   After vigorous stirring for 15 min at ambient temperature, the mixture was transferred into a 50-mL Teflon-lined stainless-steel autoclave and heated at 120°C for 12 h. The green product was collected via centrifugation and further washed with deionized water and ethanol for two times, respectively. After drying in vacuum oven, the Ni(OH) x NBs were used for characterization and further preparation. Measurements of diboration reactions. All manipulations were carried out using standard Schlenk techniques. Unless otherwise noted, analytical grade solvents and commercially available reagents were used as received. In a typical procedure, alkynes or alkenes (0.5 mmol), B 2 pin 2 (0.5 mmol), and Pt 1 /Ni(OH) x (Pt/ substrate = 0.1%) were placed in a Shlenck tube equipped with a stir bar, and then mesitylene (2.0 mL) was injected and the mixture was stirred at 120°C for the corresponding reaction time. After the reaction was completed, the reaction mixture was analyzed by GC and GC-MS with dodecane as the internal standard. The overall TOF value was measured upon completion of reactions and the calculation of it was based on the total Pt loading in the catalyst.

Synthesis of the
Characterization. TEM images were taken from a Hitachi H-800 transmission electron microscope operated at 100 kV. HR-TEM, STEM, and EDX elemental mapping characterizations were carried out on a JEOL JEM-2100F field emission transmission electron microscope operated at 200 kV. The AC-HAADF STEM characterization was conducted on a Titan 80-300 scanning/transmission electron microscope operated at 300 kV, equipped with a probe spherical aberration corrector. XPS data were collected from a Thermo Fisher Scientific ESCALAB 250Xi XPS System, and the binding energy of the C1s peak at 284.8 eV was taken as an internal reference. The O K-edge sXAS spectra were collected at BL12B station of National Synchrotron Radiation Laboratory (NRSL) in Hefei, China. EXAFS spectra at Pt L 3 -edge and Ni K-edge and the XANES spectra at Pt L 3 -edge were all collected at the 1W1B station in Beijing Synchrotron Radiation Facility in transmission mode using a fixed-exit Si (111) double crystal monochromator. The incident X-ray beam was monitored by an ionization chamber filled with N 2 , and the acquired EXAFS data were processed according to the standard procedures using the ATHENA module implemented in the IFEFFIT software packages. XRD data were acquired from a Rigaku RU-200b X-ray powder diffractometer with Cu Kα radiation (λ = 1.5406 Å). ICP-OES measurements were conducted on a Thermo Fisher iCAP™ 7000 Series ICP-OES analyzer. FT-IR spectroscopy was performed on a Bruker V70 infrared spectrometer in the frequency of 600-4000 cm −1 . UV-Vis DRS spectra were acquired from a Hitachi U-3900 UV-vis spectrophotometer. The GC analysis was conducted on a Thermo Trace 1300 series GC with a FID detector using a capillary column (TR-5MS, from Thermo Scientific, length 30 m, i.d. 0.25 mm, film 0.25 μm). The GC-MS analysis was carried out on a ISQ GC-MS with a ECD detector (Thermo Trace GC Ultra) using a capillary column (TR-5MS, from Thermo Scientific, length 30 m, i.d. 0.25 mm, film 0.25 μm). 1 H nuclear magnetic resonance (NMR) and 13 C NMR data were recorded with a Bruker Advance III (400 MHz) spectrometer. High-resolution exact mass measurements were performed on Thermo Scientific Q Exactive mass spectrometer. The detailed characterization data of products in the article are present in the Supplementary Methods section, and for the corresponding NMR spectra, see Supplementary Figs. 14-43.
Data availability. The data supporting this study are available from the authors upon reasonable request. a b -3.89 eV -0.72 eV Fig. 5 Studies of the interaction between Ni 2+ vacancies and isolated Pt atoms. Top and side views of the most stable structure and charge density difference for the Pt atom adsorbed on the Ni(OH) 2 with Ni 2+ vacancies (a) and without Ni 2+ vacancies (b). The cyan, gray, red, and white balls refer to Pt, Ni, O, and H atoms, respectively. For charge density difference, yellow (blue) corresponds to charge accumulation (depletion) plotted with an isovalue of ±0.01 e Å −3