catalysts
Review Boosting the Characterization of Heterogeneous Catalysts for H2O2 Direct Synthesis by Infrared Spectroscopy
Maela Manzoli
Department of Drug Science and Technology, University of Turin, Via Pietro Giuria 9, 10125 Turin, Italy; [email protected]; Tel.: +39-011-670-6663 Received: 30 November 2018; Accepted: 19 December 2018; Published: 2 January 2019
Abstract: Infrared (IR) spectroscopy is among the most powerful spectroscopic techniques available for the morphological and physico-chemical characterization of catalytic systems, since it provides information on (i) the surface sites at an atomic level, (ii) the nature and structure of the surface or adsorbed species, as well as (iii) the strength of the chemical bonds and (iv) the reaction mechanism. In this review, an overview of the main contributions that have been determined, starting from IR absorption spectroscopy studies of catalytic systems for H2O2 direct synthesis, is given. Which kind of information can be extracted from IR data? IR spectroscopy detects the vibrational transitions induced in a material by interaction with an electromagnetic field in the IR range. To be IR active, a change in the dipole moment of the species must occur, according to well-defined selection rules. The discussion will be focused on the advancing research in the use of probe molecules to identify (and possibly, quantify) specific catalytic sites. The experiments that will be presented and discussed have been carried out mainly in the mid-IR frequency range, between approximately 700 and 4000 cm−1, in which most of the molecular vibrations absorb light. Some challenging possibilities of utilizing IR spectroscopy for future characterization have also been envisaged.
Keywords: H2O2 direct synthesis; IR spectroscopy; FTIR characterization; Diffuse Reflectance Fourier Transform IR characterization; catalyst characterization; Pd catalysts; AuPd catalysts; bimetallic catalysts
1. The Direct Synthesis of Hydrogen Peroxide from Molecular Hydrogen and Oxygen Hydrogen peroxide is a benign and environmentally friendly oxidising reagent extensively employed in the production of both fine and bulk chemicals. Moreover, it finds application in water treatment, paper and pulp bleaching, textiles, and in large-scale selective oxidation processes, such as the epoxidation of olefins, the hydroxylation of aromatics, and the synthesis of cyclohexanone oxime, which is strategic for nylon-6 production (Figure1)[ 1]. These applications would greatly benefit from on-site, moderate-scale production facilities in order to reduce transport costs. However, H2O2 is produced worldwide on a multi-million ton scale annually by the energy intensive Riedl−Pfleiderer anthraquinone oxidation process [2]. Significant amounts of organic waste due to the anthraquinone, along with several energy consuming separation and concentration steps, and the use of benzene as the solvent are the main drawbacks of the process, which is economically feasible only in large-scale plants. In this frame, the research is devoted to the development of new economic scalable methods for the direct synthesis of H2O2 starting from hydrogen and oxygen and to the optimization of efficient oxidation catalysts able to work in the presence of H2O2 for sustainable production.
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44 Figure 1. Main applications of H2O2. Figure 1. Main applications of H2O2.
45 The direct synthesis reaction can be considered as a dream reaction involving molecular H2 and The46 direct O2, synthesisin which the reaction formationcan of H be2O2 consideredtakes place upon as aproton dream−electron reaction transfer involving to O2 and molecular*OOH H2 and 47 intermediates. Conversely, the formation of H2O implies the O–O bond cleavage of the surface O2, in which43 the formation of H2O2 takes place upon proton−electron transfer to O2 and *OOH 48 *OOH species [3]. As a matter of fact, H2O2 selectivity is ruled by the competitive O–H bond intermediates.4449 formation Conversely, and O–O the bond formation cleavage.Figure of 1. H Main2O applications implies theof H2 O–OO2. bond cleavage of the surface *OOH species [503]. As aH matter2O2 direct of fact,synthesis H2 Ocan2 selectivity potentially halve is ruled the bycost thewith competitive respect to the O–H anthraquinone bond formation and 45 The direct synthesis reaction can be considered as a dream reaction involving molecular H2 and O–O bond51 cleavage.commercial process, resulting in a much lower environmental impact, also due to the possibility to 4652 Oavoid2, in whichchlorine the for formation oxidation of chemistry H2O2 takes [1,4]. place In uponaddition, proton the−electron direct synthesistransfer toreaction O2 and has *OOH the H 47O directintermediates. synthesis Conversely, can potentially the formation halve of H the2O costimplies with the respectO–O bond to cleavage the anthraquinone of the surface commercial 2 532 potential to produce inexpensive H2O2 at the mid-scale in geographically distributed facilities, process,4854 resulting *OOHbecause inspecies such a much facilities[3]. As lower awould matter environmental have of fact,much H lower2O2 selectivity impact,capital and is also ruledoperating due by tothe costs thecompetitive than possibility Riedl-Pfleiderer O–H tobond avoid chlorine 49 formation and O–O bond cleavage. for oxidation55 plants chemistry with comparable [1,4]. In dimension addition, [5,6]. the Nevertheless, direct synthesis no alternative reaction process has for the H potential2O2 direct to produce 5056 synthesisH2O2 hasdirect yet synthesisbeen marketed, can potentially despite several halve published the cost patentswith respect [2,7–11] to and the literature anthraquinone papers inexpensive5157 commercial[10,12–25]. H2O2 at Indeed, process, the mid-scale selectivity resulting inisin stilla much geographically far fromlower bein environmentalg high distributed and mustimpact, be alsosignificantly facilities, due to the improved becausepossibility for to sucha facilities 52 would have58 avoid muchsuccessful chlorine lower industrial for capital oxidation exploitation. and chemistry operating Indeed, [1,4]. wate costsInr is addition, thethan most thethermodynamically Riedl-Pfleiderer direct synthesis favouredreaction plants producthas with the comparable 53 potential to produce inexpensive H2O2 at the mid-scale in geographically distributed facilities, 59 (as shown in 2) and the H2-O2 gas mixtures are explosive in a very broad range of compositions (4– dimension [5,6]. Nevertheless, no alternative process for H2O2 direct synthesis has yet been marketed, 5460 because96%), posing such severefacilities limitations would have to the much practi lowercability cap ofital the andprocess operating under safecosts conditions. than Riedl-Pfleiderer despite5561 several plants published with comparable patents dimension [2,7–11 ][5,6]. and Nevertheless, literature papersno alternative [10,12 process–25]. Indeed,for H2O2 direct selectivity is still far from56 being synthesis high and has yet must been be marketed, significantly despite improvedseveral published for a patents successful [2,7–11] industrial and literature exploitation. papers Indeed, 57 [10,12–25]. Indeed, selectivity is still far from being high and must be significantly improved for a water is58 the mostsuccessful thermodynamically industrial exploitation. Indeed, favoured water product is the most (as thermodynamically shown in Figure favoured2) and product the H 2-O2 gas mixtures59 are (as explosive shown in in2) and a very the H broad2-O2 gas rangemixtures of are compositions explosive in a very (4–96%), broad range posing of compositions severe limitations (4– to the practicability60 96%), of the posing process severe underlimitations safe to the conditions. practicability of the process under safe conditions. 61
62
63 Figure 2. Reactions involved in the direct synthesis of H2O2.
64 Palladium, either alone [26–37] or associated with gold [17,22,25,38–44], with platinum [45–48], 65 with tin [49,50], with nickel [51], with tellurium [52], and with zinc [53,54], has been extensively 66 studied and it is considered as the best catalyst in terms of both activity and selectivity, the latter 62 67 being fundamental for commercial applications [19,55]. Rh and Ru additives have detrimental 63 Figure 2. Reactions involved in the direct synthesis of H2O2. 68 effects on theFigure H2O2 yields 2. Reactions because they involved promote in H the2O2 directdecomposition synthesis and/or of H enhance2O2. H2 to H2O 69 activity [19]. 64 Palladium, either alone [26–37] or associated with gold [17,22,25,38–44], with platinum [45–48], Palladium,65 with eithertin [49,50], alone with [nickel26–37 [51],] or with associated tellurium with[52], and gold with [ 17zinc,22 [53,54],,25,38 has–44 been], with extensively platinum [45–48], with tin66 [ 49,50studied ], with and it nickel is considered [51], as with the best tellurium catalyst in [ 52terms],and of both with activity zinc and [ 53selectivity,,54], has the beenlatter extensively studied67 and itbeing is considered fundamental asfor thecommercial best catalyst applications in terms [19,55]. of Rh both and activity Ru additives and have selectivity, detrimental the latter being 68 effects on the H2O2 yields because they promote H2O2 decomposition and/or enhance H2 to H2O fundamental69 activity for commercial [19]. applications [19,55]. Rh and Ru additives have detrimental effects on the H2O2 yields because they promote H2O2 decomposition and/or enhance H2 to H2O activity [19].
The effect of the nature of the support (ZrO2, Ga2O3, CeO2, SiO2, ThO2, CeO2–ZrO2, Al2O3, carbon etc.) on the catalytic activity and selectivity was extensively investigated [19,32,56]. Carbon porosity and surface structure play a key role to achieve high chemoselectivity [38]. Unluckily, the catalysts employed to perform the direct synthesis of H2O2 are also active for its decomposition. It was shown that an acid pretreatment of the carbon support of AuPd alloy catalysts turned off the H2O2 decomposition [21]. In particular, the acid treatment induced a decrease in the size of the bimetallic nanoparticles, which were supposed to decorate the sites, hence inhibiting the Catalysts 2019, 9, 30 3 of 34 decomposition reaction, and hydrogen selectivity >95% were achieved. It was also demonstrated that H2O2 can be produced over metallic Pd sites which have been geometrically and electronically modified by additives, such as Cl−, Br−, oxygen, and/or nitrogen atoms of the support [21,57–59]. In this frame, it has also been shown that the modification with ligands of Pd nanoparticles supported on carbon created a hybrid nanostructure with unique catalytic performance [60]. Acids and halides have been commonly added in order to improve the H2O2 selectivity [1,12,58,61,62]. Indeed, acid additives are able to impede the H2O2 decomposition, whereas halide additives hinder water formation [1,14,61]. Nevertheless, both corrosion of the reactor and dissolution of the catalytically-active metal occur in the presence of acid additives. Alternative acid 2− − supports, such as solid acid supports like SO3H- functionalized mesoporous silicas [24], SO4 -, Cl -, F−-, and Br−-doped zirconia [63], insoluble heteropolyacids [64–66], and insoluble heteropolyacids supported mesoporous silica [66,67], cesium-containing CsH3−PW12O40/MCF [68,69], and have been reported to act as acid sources. Cs-exchanged phosphotungstic acid was employed as an acid additive to an Au-Pd/TiO2 catalyst with significant improvement of the H2O2 synthesis rate and selectivity with respect to the promotional effect of common oxides and non-halo acids [70]. It has also been reported that acidity of the catalysts played a crucial role in determining the catalytic performance in the direct synthesis of hydrogen peroxide [66,67]. Approaches, such as the catalyst wet pre-treatment method (CWPM), involving the post-modification of commercially available Pd catalysts with aqueous solutions of Br− with different concentrations, have been shown to enhance the selectivity [30].
2. Infrared Absorption Spectroscopy as a Tool for Catalyst Characterization Infrared (IR) absorption spectroscopy is one of the most popular characterization tools to describe heterogeneous catalysts [71]. In FTIR analysis, a molecule is excited to a higher vibrational energy state upon absorption of the IR radiation. Only the molecules that undergo to a variation of the dipole moment during the vibrational transition are IR active [72]. It should be, therefore, remembered that both O2 and H2 molecules, i.e., the reactants involved in the direct synthesis of hydrogen peroxide, owing to their symmetry, are IR inactive (no change of the dipole moment). The energy associated to the excited states is related to the molecular bond vibrations, such as stretching, bending, rocking, twisting, wagging, as well as out-of-plane deformations, which take place at different frequencies or wavenumbers (cm−1) in the IR spectroscopic region [72]. The position of a band is defined by Equation (1), which describes the behaviour of an anharmonic oscillator:
ν = 1/2πc·(k/µ)1/2 (1) where ν is the frequency, c is the light speed, k is the force constant related to the bond between the two atoms which constitute the oscillator, and µ represents the reduced mass of the oscillator. As a consequence, the position of an IR band depends either on the strength of the bond or on the mass (isomeric effect). This implies that the specific physicochemical properties of the molecule or adsorbate (i.e., when performing a FTIR experiment of adsorbed probe molecules), i.e., the bonds involved and the local environment, affect the position of the IR absorbance peak, making the technique diagnostic, since the corresponding IR spectrum represents a fingerprint of that particular functional group, such as C–H, O–H, C=O, C≡O, N=N, and so on. Moreover, similar vibrational modes possess similar energetics, meaning that the interpretation of the IR spectra of unknown species is useful to identify the specific moieties that constitute the sample. In particular, the position of the absorption bands of the adsorbed species gives a measure of the strength of the bond between the adsorbate and the adsorbing site [73]. Moreover, the specific frequencies of individual vibrational modes can probe the chemical nature of the surrounding catalytic environment. Catalysts 2019, 9, 30 4 of 34
The energy related to most of the molecular vibrations falls in the mid-infrared (MIR) region of the electromagnetic spectrum, and this is the reason for which the largest amount published papers reports spectra in this region, which ranges between 4000 and 400 cm−1. Another point is that the absorbance related to each molecular vibration is proportional to the abundance of the corresponding functional groups, hence the concentration of the species can be derived by the Beer-Lambert Law, Equation (2):
A = −log10 I/I0 = ε·l·c (2) where A stands for the absorbance (dimensionless), and I and I0 represent the intensity of the transmitted and incident light, respectively. The molar absorptivity ε parameter is expressed as L·mol−1·cm−1), the thickness of the sample l is reported in cm, and the molar concentration c is in mol·cm−1.
2.1. FTIR Spectroscopy of Adsorbed Probe Molecules The surface sites in catalysts can be efficiently characterized by FTIR spectroscopy of probe molecules. FTIR spectroscopy is ideal for this approach, due to the specificity of the spectra for each adsorbate and to the high sensitivity to the kind of surface bonding to the local environment. The choice of the most appropriate probe molecule is therefore strategic: some probes are able to adsorb on specific sites, which can be detected and quantified, based on the intensity of the absorption. Other probes display different bonding on different sites, which can be identified by the corresponding changes in the IR spectra. Generally, the use of opportune molecular probes combined with FTIR absorption spectroscopy can provide information on: (i) Acidic sites, in particular Brønsted sites, such as OH surface groups, and Lewis cationic sites. In this case, basic probe molecules as for example pyridine or other amines, NH3, and acetonitrile are typically employed [74,75]. Moreover, the acid strength can also be determined by the shift observed in the O–H stretching region upon interaction by hydrogen bonding with weak basic probes, such as CO and NO [76,77]. (ii) Basic sites, normally surface oxygen atoms in oxides, CO2 is usually employed, along with other probes less commonly used such as methanol [78], and also CO. CO2 adsorption gives rise to the formation of mono- and bidentate carbonate species, hydrogen carbonates, and linearly-coordinated 2− x+ 2− x+ CO2, providing detailed knowledge on the basic O sites and M –O pairs (M = metallic cation) [74].
Carbon Monoxide A separate paragraph is dedicated to carbon monoxide because this molecular probe can be considered as the most versatile and clever probe [79]. Only vibrational modes with high cross-sections can be readily detected by FTIR spectroscopy, and this is among the reasons for which a large fraction of spectroscopic investigations concerns the adsorption of carbon monoxide (or other molecules containing C–O bonds). Indeed, besides providing information on the acidic and basic sites, the use of the CO probe offers knowledge on the nature of the metal catalytic sites, their oxidation state, and coordination mode [77,80,81]. In addition, CO can also be employed to determine the amount of sites with coordinative vacancies and available for catalysis. The CO molar absorptivity is commonly high, giving rise to strong IR signals for the C–O stretching mode in a frequency range almost without interference due to other species. The bands due to linear bonded CO can be observed in the 2000–2170 cm−1 range, whereas the position of those related to doubly bridged species is in the 1880–2000 cm−1 region, and multiply-bridged CO species give rise to bands below 1880 cm−1. Moreover, the C–O stretching frequency is strongly dependant from the nature of the bond with the surface, i.e., from the electronic properties of the adsorbent site. Due to the small size, the CO molecule adsorption is ruled by steric hindrance effects. The frequency of the free molecule (2143 cm−1) changes Catalysts 2018, 8, x FOR PEER REVIEW 5 of 36
166 size, the CO molecule adsorption is ruled by steric hindrance effects. The frequency of the free 167 molecule (2143 cm–1) changes when CO is adsorbed and such a shift is explained by the Bhyholder 168 Model [82], in which the bond between the adsorbent site (a metal site) and CO is the result coming Catalysts1692019 , 9from, 30 two main contributions, which are shown in Figure 3. The first contribution is the donation 5 of 34 170 that arises from the overlapping of the 5 full orbital of the carbon atom (C, with weak anti-bonding 171 nature) and of the empty d orbital of the metal site (M), which possesses dz2 symmetry. The result of 172 when CO isthis adsorbed overlapping and is suchan electron a shift density is explained transfer from by the the CO Bhyholder molecule (lone Model pair on [C82 atom)], in to which M the bond 173 with an increase of the C–O bond strength. As a consequence, according to Equation (1), the CO blue between174 theshift adsorbents with respect site to (athe metal position site) of the and free molecule. CO is the result coming from two main contributions, which175 are shownThe in second Figure contribution3. The first is the contribution back donation is (d the→pσ) withdonation bonding that character, arises resulting from from the overlapping of the176 5σ fullthe orbital overlapping of the among carbon two atomfull d orbitals (C, with of M weak and the anti-bonding anti-bonding 2 nature)* degenerate and CO of molecular the empty d orbital 177 orbitals. Such overlapping brings electron density in the anti-bonding CO orbital and the bond 2 of the178 metal strength site (M), is decreased. which possesses Therefore, the dz positionsymmetry. of the CO The band result red-shift ofs this with overlapping respect to the free is an electron Catalysts 2018, 8, x FOR PEER REVIEW 5 of 36 density179 transfer molecule. from These the two CO factors molecule can predo (loneminate pair on oneach C other atom) based to Mon the with nature an increaseof the adsorbent: of the C–O bond 180 generally, donation is prevalent for metal ions with high oxidation state, on the contrary back strength.166 As asize, consequence, the CO molecule according adsorption to is Equationruled by ster (1),ic hindrance the νCO effects.blue shiftsThe frequency with respect of the free to the position 181 donation control the adsorption by neutral or partially negatively-charged metal atoms. of the free167 molecule.molecule (2143 cm–1) changes when CO is adsorbed and such a shift is explained by the Bhyholder 182168 Model [82], in which the bond between the adsorbent site (a metal site) and CO is the result coming 169 from two main contributions, which are shown in Figure 3. The first contribution is the σ donation 170 that arises from the overlapping M C bond of the 5σ full orbital of the carbon atom (C, with weak anti-bonding _ _ _ 2 171 nature) and of the empty dM orbital+ of the+ metal+ siteC_O (M),: whichM possessesC_ dzO: symmetry. The result of 172 this overlapping is an electron density transfer from the CO molecule (lone pair on C atom) to M 173 with an increase of the C–O bond strength. As a consequence, according to Equation (1), the νCO blue 174 shifts with respect to the Mposition → C bond of the free molecule. 175 The second contribution is the π back donation (dπ→pπ) with bonding character, resulting from + _ + _ + + _ _ _ π 176 the overlapping among twoM full d+ orbitalsC _O of: M and the anti-bondingM : _2 :* degenerate CO molecular _ _ C O 177 orbitals. Such overlapping_ brings+ electron density+ in the anti-bonding_ CO+ orbital and the bond 183178 strength is decreased. Therefore, the position of the CO band red-shifts with respect to the free 179 molecule. These two factors can predominate on each other based on the nature of the adsorbent: 184 Figure 3. MetalFigure atomic3. Metal atomic (M) orbitals (M) orbitals and and CO CO molecular orbitals orbitals involved involved in the adsorption. in the adsorption. 180 generally, σ donation is prevalent for metal ions with high oxidation state, on the contrary π back 185181 2donation.2. Experimental control Setup the adsorption by neutral or partially negatively-charged metal atoms. The182 second contribution is the π back donation (dπ→pπ) with bonding character, resulting from 186 The experiments that are presented and discussed in this review have beenπ carried out mainly the overlapping187 in the among mid IR frequency two full range, d orbitals between of approximately M and the 700 anti-bonding and 4000 cm–1 2, in* which degenerate most of the CO molecular orbitals.188 Suchmolecular overlapping vibrations absorbbrings light. electron Currently, density Fourier intransform the anti-bonding infrared spectrometers CO orbital (FTIR) are and the bond strength189 is decreased.employed, and Therefore,such instruments the are position fairly cheap of and the widespread CO band in red-shiftsmost analytical with and respectresearch to the free 190 laboratories. In FTIR instruments a Michelson interferometer processes the collimated IR light before molecule.191 Thesefocusing two it onto factors the sample can and predominate further collects on and each detect others the resulting based beam on. the According nature to Figure of the adsorbent: generally,192 σ4donation, the IR beam is is prevalentsplit into two forequal metal beams, ions the former with ishigh refracted oxidation in the direction state, of ona fixed the mirror contrary, π back donation193 controlwhereas the the adsorption latter is transmitted by neutral to a movable or partially mirror. negatively-charged metal atoms.
fixed mirror 2.2. Experimental183 Setup 184 Figure 3. Metal atomic (M) orbitals and CO molecular orbitals involved in the adsorption. The experiments that are presented and discussed in thistranslating review have been carried out mainly mirror in the mid185 IR2.2. frequency Experimental Setup range, between approximately 700 and 4000 cm−1, in which most of the molecular186 vibrationsThe experiments absorb light.thatIR source are presented Currently, and Fourierdiscussed in transform this review have infrared been carried spectrometers out mainly (FTIR) are 187 in the mid IR frequency range, between approximately 700 and 4000 cm–1, in which most of the employed, and such instruments are fairlybeamsplitter cheap and widespread in most analytical and research 188 molecular vibrations absorb light. Currently, Fourier transform infrared spectrometers (FTIR) are laboratories.189 employed, In FTIR instrumentsand such instruments a Michelson are fairly cheap interferometersample and position widespread processes in most analytical the collimated and research IR light before focusing190 it ontolaboratories. the sample In FTIR and instruments further a Michelson collects andinterf detectserometer processes the resulting the collimated beam. IR According light before to Figure4, 191 the IR beamfocusing is split it into onto twothe sample equal and beams, further collects the former anddetector detects is refractedthe resulting inbeam. the According direction to Figure of a fixed mirror, 194192 4, the IR beam is split into two equal beams, the former is refracted in the direction of a fixed mirror, whereas195193the latterwhereas is the transmitted latter isFigure transmitted 4 to. Schematic a movableto a movable representation mirror. mirror. of a Michelson interferometer.
194 195 Figure 4.FigureSchematic 4. Schematic representation representation of of a aMichelson Michelson interferometer. interferometer.
Then, these beams are recombined by the beam splitter and further directed toward the sample. The difference in optical path between the two beams is called retardation, and is varied over time by scanning the movable mirror. As a consequence, an interferogram is obtained by recording the signal Catalysts 2019, 9, 30 6 of 34 from the detector as a function of the retardation. The Fourier transformation of that signal provides the IR spectrum, which is reported as a function of the frequency. Modern FTIR instruments are usually equipped by glow-bar IR lamps as the source and by Catalysts 2018, 8, x FOR PEER REVIEW 6 of 36 mercury–cadmium–telluride (MCT) detectors for signal detection, due to the high sensitivity and to the196 capability Then, to detectthese beams most are recombined of the mid by IRthe beam frequency splitter and range. further Due directed to toward the opportunity the sample. to collect 197 simultaneouslyThe difference all wavelengths, in optical path higher between signal-to-noise the two beams is ratio called can retardation, be achieved and is varied at a givenover time scanning time. 198 by scanning the movable mirror. As a consequence, an interferogram is obtained by recording the Moreover,199 thesignal throughput from the detector is determined as a function onlyof the byretardation. the diameter The Fourier of thetransformation collimated of that IR signal beam. However, being200 a non-zero-background provides the IR spectrum, technique, which is reported FTIR as a instruments function of the frequency. have limited sensitivity and glow-bar 201 lamps should beModern replaced FTIR by instruments synchrotron are usu radiationally equipped or by by glow tunable-bar IR IR lamp laserss as the [71 source]. and by 202 mercury–cadmium–telluride (MCT) detectors for signal detection, due to the high sensitivity and to Nevertheless,203 the capability the widespread to detect most acceptance of the mid IR of frequency IR absorption range. Due spectroscopy to the opportunity to efficiently to collect characterize solid catalysts204 simultaneously is mainly all due wavelengths, to the availability higher signal-to of-noise several ratio can experimental be achieved at setups, a given scanning which render the 205 technique adaptabletime. Moreover, to a the number throughput of experiments is determined only that by can the be diameter tailored of the on collimated the nature IR beam of the. sample to 206 However, being a non-zero-background technique, FTIR instruments have limited sensitivity and be investigated.207 glow-bar lamps should be replaced by synchrotron radiation or by tunable IR lasers [71]. The208 most commonNevertheless, experimental the widespread setups acceptance employed of forIR absorptioncatalyst characterization spectroscopy to efficiently using IR absorption spectroscopy209 characterize are (i) transmission solid catalysts is FTIR mainly mode, due to (ii)the diffuseavailability reflectance of several experimental (DRIFTS) setups, mode, which (iii) attenuated 210 render the technique adaptable to a number of experiments that can be tailored on the nature of the total reflection211 sample (ATR) to be mode,investigated. in which the sample is placed in tight contact with a flat surface of the prism212 used to directThe most the IR common beam, experimental and (iv) reflection–absorption setups employed for catalyst (RAIRS) characterization mode, in using which IR the IR beam is recoiled213 fromabsorption a flat spectroscopy reflective surfaceare (i) transmission before collection. FTIR mode, (ii) This diffuse last reflectance setup is usually(DRIFTS) mode, employed (iii) for model 214 attenuated total reflection (ATR) mode, in which the sample is placed in tight contact with a flat systems215 in surface-sciencesurface of the prism studies. used to Indirect this the review, IR beam, we and will (iv) reflectionmainly– focusabsorption on the(RAIRS) transmission mode, in FTIR and diffuse216 reflectance which the (DRIFTS) IR beam is recoiled common from setups. a flat reflective surface before collection. This last setup is usually 217 employed for model systems in surface-science studies. In this review, we will mainly focus on the 2.2.1. Transmission218 transmission FTIR FTIR Mode and diffuse reflectance (DRIFTS) common setups. Most219 of2.2 the.1. Transmission spectroscopic FTIR studies Mode reported in the literature have been performed in transmission mode.220 Generally Most the of setup the sconsistspectroscopic in a studies self-sustaining reported in pellet the literature of the havepowered been catalyst performed orin of a mixture 221 with IR transparenttransmission KBr, mode placed. Generally inside the setup a cell consists allowing in a self to-sustaining work in pellet controlled of the powered atmosphere, catalyst or and collect in 222 of a mixture with IR transparent KBr, placed inside a cell allowing to work in controlled atmosphere, situ IR223 spectra and [39 collect,40 ].in Asitu schematic IR spectra [39, picture40]. A ofschematic an example picture of an transmission example of transmission mode is mode shown is in Figure5. There224 is also shown the possibility in Figure 5. There to follow is also the spectroscopically possibility to follow thespectroscopically catalytic reaction the catalytic and reaction to collect and operando 225 IR spectra. to collect operando IR spectra. 226
sample pellet IR beam
KBr windows 227 Figure228 5. TransmissionFigure 5. Transmission (TIR) mode,(TIR) mode, where where the the IRIR beam is isdirected directed through through a self-sustained a self-sustained sample sample 229 placed inside the catalytic reactor and collected after exiting for analysis. placed inside the catalytic reactor and collected after exiting for analysis. 230 Despite being quite popular, transmission mode setups undergo to the following constraints: Despite231 the being catalyst quite must be popular, transparent transmission to IR radiation in mode order setupsto obtain undergospectra withto reasonable the following intensity, constraints: the catalyst232 the must catalyst be transparenthas to give the possibility to IR radiation to make thin in self order-sustaining to obtain pellets, spectra and the intrinsic with reasonable nature of intensity, the catalyst has to give the possibility to make thin self-sustaining pellets, and the intrinsic nature of the catalyst and the final sample form, such as pellets, depositions, and monoliths, can give serious problems for mass transport. Catalysts 2019, 9, 30 7 of 34
Catalysts 2018, 8, x FOR PEER REVIEW 7 of 36 2.2.2. Diffuse-Reflectance (DRIFTS) Mode 233 the catalyst and the final sample form, such as pellets, depositions, and monoliths, can give serious To234 successfully problems for overcome mass transport. the problems arising from poorly transparent catalysts, or from samples not adequate to prepare a pellet, the diffuse-reflectance (DRIFTS) mode can be alternatively adopted. 235 2.2.2. Diffuse-Reflectance (DRIFTS) Mode Here, the powdered sample is placed in a cell, where the interaction with the IR beam gives 236 raise to scatteredTo light,successfully which overcome is collected the problems with arising appropriate from poorly optics transparent (Figure catalysts6). With, or from this approach, 237 samples not adequate to prepare a pellet, the diffuse-reflectance (DRIFTS) mode can be alternatively the preparation238 adopted of. theHere, sample the powdered is simpler sample is than placed that in a withcell, where transmission the interaction FTIR. with the Due IR beam to this gives experimental setup,239 the intensityraise to scattered of DRIFT light, which signal is collected tends with to be appropriate low and optics collecting (Figure 6). good With this quality approach, spectra the becomes 240 difficult. However,preparation the of intensity the sample isof simpler the bands than that can with be transmissionquite more FTIR. enhanced Due to this when experimental working in DRIFT 241 setup, the intensity of DRIFT signal tends to be low and collecting good quality spectra becomes mode242 with respectdifficult. toHowever, the acquisition the intensity in of transmissionthe bands can be mode, quite more due enhanced to the lightwhen multipleworking in internalDRIFT reflection close to243 the samplemode with surface, respect toresulting the acquisition also in in improved transmission sensitivity mode, due to towards the light multiplethe surface internal species rather than towards244 reflection the gas close phase to the species. sample surface, On the resulting contrary, also in the improved major sensitivity drawbacks towards are the related surface to the poor 245 species rather than towards the gas phase species. On the contrary, the major drawbacks are related reproducibility246 to the due poor to reproducibility the variations due of to scattering the variations coefficients of scattering depending coefficients depending on the cellon the geometry, cell on the sample247 insertion geometry procedure, on the sample and insertion on the procedure occurrence and on the of occur temperaturerence of temperature gradient gradient within within the powdered sample248 with the respect powdered to thesample surface. with respect to the surface. 249
Mirror IR source
sample powder Detector
250 Figure251 6. DiffuseFigure reflectance6. Diffuse reflectance (DRIFTS) (DRIFTS) mode, mode, where where an an IR IR beam beam is focused is focused on the p onowder theedpowdered samples samples 252 and the scattered light is collected by a parabolic mirror. and the scattered light is collected by a parabolic mirror. 253 3. FTIR Spectroscopic Characterization: What Can Be Learned? 3. FTIR Spectroscopic Characterization: What Can Be Learned? 254 Usually, the use of FTIR spectroscopy is dedicated to the identification of the surface exposed Usually,255 sites the of usethe catalyst of FTIR to establish spectroscopy structure- isactivity dedicated relationships. to the Another identification application deals of the with surface the exposed 256 identification of the adsorbed species, and sometimes to their quantification and evolution during sites of257 the catalystthe reaction. to In establish this review structure-activity, we will try to center relationships.on some meaningful Another examples applicationthat shed light dealson with the identification258 open of the questions adsorbed and improved species, the and knowledge sometimes on the to theiractive quantification sites involved in and the H evolution2O2 direct during the reaction.259 Insynth thise review,sis and on we the willparameters try to that center have aon beneficial some effect meaningful on both conversion examples and selectivity. that shed light on open questions260 and3.1.improved Nature of the Active the knowledge Sites on Pd Cataly onsts the active sites involved in the H2O2 direct synthesis and on the261 parameters Many that studies have focused a beneficial on the identification effect on of both the nature conversion and the androle of selectivity. Pd sites in promoting 262 the direct synthesis of hydrogen peroxide from hydrogen and oxygen. In a very recent and 3.1. Nature263 ofinteresting the Active paper, Sites Han on et Pd al.Catalysts deduced that the active sites should not be properly represented by 264 metallic or oxidized Pd species and elegantly pointed out that the active sites for the reaction Many265 studiesoriginated focused from the oninterfaces the identification among Pd and PdO ofthe domains nature on Pd/TiO and the2 catalysts, role of as Pdshown sites in F inigure promoting the direct266 synthesis 7a [59] of. The hydrogen combined peroxide use of high from resolution hydrogen transmission and electron oxygen. microscopy In a very (HRTEM) recent, X and-ray interesting paper,267 Han Diffraction et al. deduced (XRD), in thatsitu diffuse the activereflectance sites Fourier should Transform not IR be spectroscopy properly (DRIFT) represented of adsorbed by metallic or 268 CO, X-ray photoelectron spectroscopy (XPS), X-ray absorption near edge structure (XANES), and oxidized269 PdExtended species andX-ray elegantly Absorption pointed Fine Structure out (EXAFS) that the allowed active to sites demonstrate for the thatreaction the structure originated of from the interfaces among Pd and PdO domains on Pd/TiO2 catalysts, as shown in Figure7a [ 59]. The combined use of high resolution transmission electron microscopy (HRTEM), X-ray Diffraction (XRD), in situ diffuse reflectance Fourier Transform IR spectroscopy (DRIFT) of adsorbed CO, X-ray photoelectron spectroscopy (XPS), X-ray absorption near edge structure (XANES), and Extended X-ray Absorption Fine Structure (EXAFS) allowed to demonstrate that the structure of such Pd ensembles can be finely tuned by varying the Pd loading, while keeping constant the particle size. Indeed, the surface configuration of Pd atoms changed significantly for 1.0–5.0 wt% Pd loadings, whereas the size and the crystallinity of Pd particles remains unchanged. In situ DRIFTS spectra of adsorbed CO were collected on the Pd/TiO2 catalysts with different Pd loadings to determine the surface structure and the results are shown Figure7b. Catalysts 2018, 8, x FOR PEER REVIEW 8 of 36
270 such Pd ensembles can be finely tuned by varying the Pd loading, while keeping constant the 271 particle size. Indeed, the surface configuration of Pd atoms changed significantly for 1.0–5.0 wt% Pd 272 loadings, whereas the size and the crystallinity of Pd particles remains unchanged. In situ DRIFTS 273 spectra of adsorbed CO were collected on the Pd/TiO2 catalysts with different Pd loadings to 274 determine the surface structure and the results are shown Figure 7b. 275 The sharp peak at 2094 cm–1 is due to CO linearly adsorbed on low coordinated metallic Pd 276 atoms located at the corners or at the edges of the nanoparticles. Moreover, the bands at 1978, 1932, 277 and 1876 cm–1 are related to CO adsorbed on bridge and hollow sites of the Pd ensembles [83]. Such 278 absorptions decreased in intensity by decreasing the Pd loading, however, the linear species/bridged 279 and multibonded species ratio increases regularly. The intensity of the CO band at 1876 cm–1 was 280 almost nil in the case of 1.0% Pd/TiO2, which means that the increase of the Pd content induced the 281 formation of continuous Pd ensembles exposing flat sites, thus lowering the amount of Pd corners or Catalysts 2019, 9, 30 8 of 34 282 edges. 283
a b
284
285 Figure 7. (a) Structural model of the Pd/TiO2 catalyst. (b) In situ DRIFTS of CO adsorption over Formatted: Not Highlight Figure 7. (a) Structural model of the Pd/TiO2 catalyst. (b) In situ DRIFTS of CO adsorption over 286 different catalysts at room temperature in an Ar flow (50 mL/min): A: 1.0% Pd, B: 2.0% Pd, C: 3.0% Pd, different287 catalystsand D: 5.0% at room Pd. Reprinted temperature from J. Catal in an., 321, Ar L. flow Ouyang, (50 P. mL/min): Tian, G. Da, A:X. Xu, 1.0% C. Ao, Pd, T. B:Chen, 2.0% R. Si, Pd, J. C: 3.0% Pd, and288 D: 5.0%Xu, Pd. Y. Reprinted Han , The origin from of J.active Catal., sites 321,for direct L.Ouyang, synthesis of P. H Tian,2O2 on G.Pd/TiO Da,2 catalysts: X. Xu, C.Interfaces Ao, T. of Chen, R. Si,Formatted: J. Subscript 289 Pd and PdO domains, 70–80, Copyright (2018), with permission from Elsevier. Formatted: Subscript Xu, Y. Han, The origin of active sites for direct synthesis of H2O2 on Pd/TiO2 catalysts: Interfaces of Pd and PdO domains, 70–80, Copyright (2018), with permission from Elsevier. Formatted: Subscript 290 A rate in TOF of 630 h–1 along with 61% selectivity to H2O2 were obtained for the 1.0 wt% Pd 291 catalyst at 283 K and 1 atm in a semibatch reactor. The reasons for the good catalytic performance −1 The292 sharpwere peak disentangled at 2094 with cm the contributionis due toof spectroscopic CO linearly experiments adsorbed focused on onlow the coordinated Pd surface metallic Pd atoms293 locatedsites’ reactivity at the that corners will be discussed or at in the Section edges 3.3. of the nanoparticles. Moreover, the bands at 294 The origin of −Pd1 particle size effects on H2O2 synthesis was rarely investigated [25,57]. It was 1978,295 1932, reported and 1876 that high cm metalare dispersion related of Pd to nanoparticles CO adsorbed supported on on bridge silica has and a detrimental hollow effect sites of the Pd ensembles296 [on83 ]. the Such catalytic absorptions activity and selectivity decreased towards in intensity H2O2 [31]. byMoreover, decreasing shape-dependent the Pd catalyticloading, however, the linear297 species/bridgedactivity of Pd nano andcubes multibondedwith {1 0 0} facets, species and octahedrons ratio increases with {1 1 regularly.1} facets was Thedemonstrated intensity of the CO 298 2 2 band at 1876[84 cm]. The−1 Pdwas octahedron almost shape nil in gave the rise case to higher of 1.0% H O Pd/TiO selectivity ,and which productivity means than that the thecatalyst increase of the 299 with Pd cubes, therefore, suggesting that the Pd {1 1 1} facet is more2 active than the Pd {1 0 0} one. In Pd content300 inducedanother paper, the formation{1 0 0} facet-enclosed of continuous Pd nanocubes Pd ensemblesof uniform shape, exposing size, and flat crystallinity sites, thus were lowering the amount301 of Pdprepared corners and or supported edges. on silica. It was found that the {1 0 0} Pd facet efficiently catalyzed H2O2 302 A rate information, TOF of however 630 h,− it1 promotedalong with side reactions, 61% selectivity thus decreasing to H theO selectivitywere obtained[85]. for the 1.0 wt% Pd 303 In this frame, a series of size-controlled Pd/hydroxyapatite (HAp)2 2 catalysts ranging from single catalyst304 at 283sites K (Pd and clusters) 1 atm to innanoparticles a semibatch (∼30 nm) reactor. were synthesized The reasons and tested for the in H good2O2 direct catalytic synthesis, performance were disentangled305 showing withup to 94 the% selectivity contribution toward of H spectroscopic2O2 formation when experiments the Pd particlefocused size is in the on range the Pd2.5– surface sites’ 306 reactivity that1.4 willnm [57] be. Extensive discussed characterization in Section by3.3 multi. -technique approach was performed with the aim to 307 obtain detailed information on the role played by crystal phase, morphology, surface electronic The308 originstates of, and Pd coordination particle sizenumber effects of Pd particles on H2O (from2 synthesis atomic level was to nano rarelymeters) investigated and to establish [25 a ,57]. It was reported that high metal dispersion of Pd nanoparticles supported on silica has a detrimental effect on the catalytic activity and selectivity towards H2O2 [31]. Moreover, shape-dependent catalytic activity of Pd nanocubes with {1 0 0} facets, and octahedrons with {1 1 1} facets was demonstrated [84]. The Pd octahedron shape gave rise to higher H2O2 selectivity and productivity than the catalyst with Pd cubes, therefore, suggesting that the Pd {1 1 1} facet is more active than the Pd {1 0 0} one. In another paper, {1 0 0} facet-enclosed Pd nanocubes of uniform shape, size, and crystallinity were prepared and supported on silica. It was found that the {1 0 0} Pd facet efficiently catalyzed H2O2 formation, however, it promoted side reactions, thus decreasing the selectivity [85]. In this frame, a series of size-controlled Pd/hydroxyapatite (HAp) catalysts ranging from single sites (Pd clusters) to nanoparticles (∼30 nm) were synthesized and tested in H2O2 direct synthesis, showing up to 94% selectivity toward H2O2 formation when the Pd particle size is in the range 2.5–1.4 nm [57]. Extensive characterization by multi-technique approach was performed with the aim to obtain detailed information on the role played by crystal phase, morphology, surface electronic states, and coordination number of Pd particles (from atomic level to nanometers) and to establish a proper size range to obtain the best catalytic performances in the H2O2 direct synthesis. In particular, in situ CO DRIFT measurements were carried out to define the electronic structure of the surface Pd atoms and the spectra are shown in Figure8a. Firstly, no vibrational band related to the HAp support was observed. The intensity of the peak at 2091 cm−1 related to CO linearly adsorbed on atop sites increased with decreasing the Pd particle size. Conversely, a gradual decrease in intensity of the absorption bands associated with CO adsorbed on bridged (1988–1964 cm−1) and three-fold (1913–1873 cm−1) sites was detected [83]. More in detail, the presence of the band at 2091 cm−1, attributed to linear adsorbed CO, signalled the presence of highly dispersed Pd atoms and clusters Catalysts 2018, 8, x FOR PEER REVIEW 9 of 36
309 proper size range to obtain the best catalytic performances in the H2O2 direct synthesis. In particular, 310 in situ CO DRIFT measurements were carried out to define the electronic structure of the surface Pd 311 atoms and the spectra are shown in Figure 8a. Firstly, no vibrational band related to the HAp Catalysts 2019, 9, 30 9 of 34 312 support was observed. The intensity of the peak at 2091 cm−1 related to CO linearly adsorbed on atop 313 sites increased with decreasing the Pd particle size. Conversely, a gradual decrease in intensity of the 314 absorption bands associated with CO adsorbed on bridged (1988–1964 cm−1) and three-fold (1913– (0D and315 2D 1873 particles) cm−1) sites on was the detected 0.5–2.0 [83] wt%. More Pdin detail, catalyst. the presence In addition, of the band suchat 2091 acm band−1, attributed did not to change in intensity316by increasinglinear adsorbed the CO, Pd signalled content. the Thepresence authors of highly inferred dispersed that Pd theatoms surface and clusters local (0D environment and 2D of the 317 HAp supportparticles) strongly on influencedthe 0.5–2.0 wt% the Pd formation catalyst. In ofaddition, these such particles. a band Bandsdid not relatedchange in to intensity CO bridged by species, 318 increasing the Pd content. The authors inferred that the surface local environment of the HAp growing319 in intensitysupport strongly withthe influenced Pd content, the formation were detectedof these particles. on the Bands 0.5 wt% related Pd to catalyst.CO bridged These species, spectroscopic features,320 i.e., growing the bands in intensity observed with in the the Pd 1913–1873 content, were cm detected−1 range, on the due 0.5 to wt% CO Pd adsorbed catalyst. Theseon Pd to hollow 321 −1 sites, pointedspectro out thescopic presence features, ofi.e.,Pd the clusters,bands observed composed in the 1913 of– high-density1873 cm range, due sites, to CO or largeradsorbed 3D on Pd particles. 322 Pd to hollow sites, pointed out the presence of Pd clusters, composed of high-density sites, or larger In addition,323 3D the Pd band particles due. In toaddition, linear the carbonyls band due to totally linear carbonyls disappeared totally disappeared in the case in the of case the of 3.0 the and 5.0 wt% Pd catalysts,324 3.0 suggesting and 5.0 wt% thatPd catalysts neither, suggest 0D noring that 2D neither particles 0D nor are 2D particles present are at present the surface at the surface of these of catalysts, due to325 Pd coalescencethese catalysts, phenomena due to Pd coalescence during phenomena the preparation. during the preparation. 326
a b
c
327 328 Figure 8. (a) In situ DRIFTS of CO adsorption over different catalysts at 283 K in an Ar flow (50 Formatted: Not Highlight Figure 8. (a) In situ DRIFTS of CO adsorption over different catalysts at 283 K in an Ar flow 329 mL/min): a: HAp, b: 0.5 wt% Pd, c: 1.0 wt% Pd, d: 2.0 wt% Pd, e: 3.0 wt% Pd, and f: 5.0 wt% Pd. (b) (50330 mL/min): Size a: dependence HAp, b: 0.5of H wt%2O2 selectivity Pd, c: 1.0over wt% Pd/HAp Pd, catalysts: d: 2.0 a wt%–e: catalysts Pd, e: calcined 3.0 wt% at 673 Pd, K andwith Pd f: 5.0 wt% Pd. (b331) Size dependenceloadings of of 0.5, H 1.0,2O 2.0,2 selectivity 3.0, and 5.0 wt% over, respectively; Pd/HAp f: catalysts:3.0 wt% Pd calcined a–e: catalysts at 773 K; g) calcined 3.0 wt% Pd at 673 K with Pd332 loadings calcined of 0.5, 1.0, at 873 2.0, K; 3.0,(c) Structures and 5.0 ofwt%, catalysts respectively; corresponding f: 3.0 to three wt% scales Pd calcined of particle at sizes 773 and K; g) 3.0 wt% 333 proposed mechanism for H2O2 synthesis. Blue, red, white, purple, and green spheres are palladium, Pd334 calcined oxygen, at 873 hydrogen, K; (c) Structures phosphorus, of and catalysts calcium atoms, corresponding respectively. Reprinted to three from scales J. Catal., of particle 349, P. sizes and proposed335 mechanismTian, L. Ouyang, for HX .2 Xu,O2 C.synthesis. Ao, X. Xu, R. Blue, Si, X. Shen, red, M. white, Lin, J. purple,Xu, Y.-F. Han, and The green origin spheres of palladium are palladium, oxygen,hydrogen, phosphorus, and calcium atoms, respectively. Reprinted from J. Catal., 349, P. Tian, L. Ouyang, X. Xu, C. Ao, X. Xu, R. Si, X. Shen, M. Lin, J. Xu, Y.-F. Han, The origin of palladium particle
size effects in the direct synthesis of H2O2: is smaller better? 30–40, Copyright (2017), with permission from Elsevier.
Based on the experimental findings in combination with DFT calculations, a structure–activity relationship by varying the Pd particle size was established (Figure8b). Particularly, based on the Pd particle sizes and on the catalytic performance, three types of catalysts were identified: the first type is the single site catalyst (Pd(IE)), which is composed of atomically dispersed Pd species, and is almost inactive due to the lack of active sites (Figure8c). The catalysts with 0.5–2.0 wt% Pd belong to type II, and are mainly made up by 2D and 3D Pd sub-nanoparticles with average size ranging from 1.4 to 2.5 nm (Figure8c). According to the experimental results and the DFT calculations, these species are active in the H2O2 synthesis (Figure8b), proving that the surface arrangement of Pd atoms plays a decisive role in the catalytic activity [86]. The 3.0–5.0 wt% Pd catalysts can be classified as the third type (Figure8b,c), which is composed by large nanoparticles with size >2.5 nm, exposing mainly the Catalysts 2018, 8, x FOR PEER REVIEW 10 of 36
336 particle size effects in the direct synthesis of H2O2: is smaller better?, 30–40, Copyright (2017), with Formatted: Subscript 337 permission from Elsevier. Formatted: Subscript
Catalysts 2019338, 9, 30 Based on the experimental findings in combination with DFT calculations, a structure–activity 10 of 34 339 relationship by varying the Pd particle size was established (Figure 8b). Particularly, based on the Pd 340 particle sizes and on the catalytic performance, three types of catalysts were identified: the first type 341 is the single site catalyst (Pd(IE)), which is composed of atomically dispersed Pd species, and is Pd(1 1 1)342 facets. almost The inactive H2O due2 formation to the lack of is active inhibited sites (Figure on 8c these). The sites,catalysts due with to 0.5 the–2.0 wt% activity Pd belong of metallicto Pd towards343 O2 dissociation,type II, and are thus mainly decreasing made up by the2D and selectivity. 3D Pd sub-nanoparticles with average size ranging from The344 HAp 1.4 support to 2.5 nm helped (Figure 8 inc). According keeping to the the size experimental distribution results and of the the DFT Pd calculations, particles these ina defined 345 species are active in the H2O2 synthesis (Figure 8b), proving that the surface arrangement of Pd range, resulting346 atoms in theplays formation a decisive role of in Pdthe catalytic particles activity with [86 different]. The 3.0–5.0 geometric wt% Pd catalysts and can electronic be classified structures. In particular,347 as the the interactionthird type (Figure between 8b,c), which Pd is composed and OH by groups large nanoparticles of HAp with favoured size >2.5 nm, the exposing generation of δ Formatted: Not Highlight sub-nanometer348 mainly Pd speciesthe Pd(1 1 with 1) facets. a high The H Pd2O2 formation+/Pd0 ratio. is inhibited This on thesewas sites, ascribed due to tothe be activity responsible of of 349 metallic Pd towards O2 dissociation, thus decreasing the selectivity. δ+ the remarkable350 improvementThe HAp support of helped H2O in2 keepingselectivity the size because distribution the of the presence Pd particles of in Pd a definedspecies range, lower the dissociative351 O2resultingactivation in the along formation with of Pd the particles H2O2 withdecomposition different geometric [59 ]. and Hence, electronic the structures. Pd particles In with sub-nanometer352 particular, size are the strongly interaction interacting between Pdwith and the OH support groups ofand HAp act favoured as primary the g activeeneration sites. of 353 sub-nanometer Pd species with a high Pdδ+/Pd0 ratio. This was ascribed to be responsible of the 354 2 2 δ+ 3.2. Site Isolationremarkable and Electronic improvement Effects of H O selectivity because the presence of Pd species lower the 355 dissociative O2 activation along with the H2O2 decomposition [59]. Hence, the Pd particles with High356 dispersion sub-nanometer of Pd size sites are strongly as well interacting as incremented with the support Pd 0andcontent act as primary can boost active sites the. hydrogenation rate of hydrogen357 3.2. Site peroxide, Isolation and however Electronic Effects lowering H2O2 selectivity. Theoretical studies revealed the beneficial358 effect ofH Pdigh dispersion monomers, of Pd whichsites as well favour as incremented H2O2 formation Pd0 content can and, boost at the the hydrogenation same time, rate avoid the O–O bond359 dissociation of hydrogen [ 87peroxide]. Ouyang, however et lowering al. studied H2O2 bothselectivity. H2O Theoretical2 direct synthesisstudies revealed and the side beneficial reactions over 360 effect of Pd monomers, which favour H2O2 formation and, at the same time, avoid the O–O bond different Pd–Au/TiO2 catalysts and discovered that the productivity of hydrogen peroxide increased 361 dissociation [87]. Ouyang et al. studied both H2O2 direct synthesis and side reactions over different by decreasing the Pd/Au ratio [86]. The in situ DRIFT spectra of CO adsorbed on Pd and Pd–Au 362 Pd–Au/TiO2 catalysts and discovered that the productivity of hydrogen peroxide increased by catalysts,363 are reporteddecreasing in the Figure Pd/Au 9 ratioa. Different[86]. The in metallic situ DRIFT Pd spectra sites of were CO adsorbed observed on onPd and the Pd monometallic–Au catalyst,364 and assignedcatalysts, are to reported linear COin Figure adsorbed 9a. Different on low metallic coordination Pd sites were Pdobserved atoms, on the presumably monometallic corners or 365 catalyst, and assigned to linear CO adsorbed− on1 low coordination Pd atoms, presumably corners or edges of366 the nanoparticlesedges of the nanoparticles (the band (the at band 2096 at cm2096 cm)[–1)88 [88],],and and to to bridged bridged and andmultibonded multibonded CO on Pd CO on Pd −1 ensembles367 formed ensembles by two formed or by three two or adjacent three adjacent atoms atoms (the (the bands bands at 1977, 1977, 1910 1910,, and and1851 cm 1851–1) [8 cm3]. )[83]. 368 a b
369 370 Figure 9. (a) In situ DRIFTS of CO adsorption over different catalysts at room temperature in streams Figure 9. (a) In situ DRIFTS of CO adsorption over different catalysts at room temperature in streams of 371 of Ar with a flow rate of 50 ml/min. A: Pd, B: Pd2.5Au0.5, C: Pd2.0Au1.0, D: Pd1.5Au1.5, E: Ar with372 a flowPd1.0Au2.0, rate of 50 ml/min.F: Pd0.5Au2.5. A: Pd,(b) Mechanism B: Pd2.5Au0.5, of H2O2C: synthesis Pd2.0Au1.0, directly D:from Pd1.5Au1.5, H2 and O2 on E: a Pd1.0Au2.0,Pd F: Pd0.5Au2.5.373 monomer (b) Mechanism catalyst. Reprinted of H2O from2 synthesis J. Catal., 311, directly L. Ouyang, from G. H Da2 and , P. Tian, O2 on T. Chen, a Pd G. monomer Liang, J. catalyst. Reprinted374 fromXu,Y. J. Catal.,-F. Han, 311, Insight L. Ouyang, into active G. sites Da, of P. Pd Tian,–Au/TiO T.2 Chen, catalysts G. in Liang, hydrogen J. Xu, peroxide Y.-F. Han, synthesis Insight into Formatted: Subscript 375 directly from H2 and O2, 129–136, Copyright (2014), with permission from Elsevier. active sites of Pd–Au/TiO2 catalysts in hydrogen peroxide synthesis directly from H2 and O2, 129–136,
Copyright (2014), with permission from Elsevier.
Moreover, the intensity of these bands diminished dramatically by decreasing the Pd/Au ratio. Conversely, the ratio of the linear CO bands vs. bridged- and multi-bonded CO bands grew from 0.4 (monometallic Pd catalyst) to 1.0 (bimetallic Pd1.0Au2.0 catalyst). Based on these observations, the amount of surface Pd ensembles was lowered upon Au addition, whereas isolated Pd sites were increased (geometric effect occurring between Pd and Au), due to a dilution by gold. A small red-shift of the band related to the linear carbonyls, and a shift of the absorption of bridged carbonyls from 1977 to 1969 cm−1 were observed after Au addition. These shifts are possibly a consequence of the charge-transfer from gold to palladium, which enhanced the electron density of the involved d orbitals, resulting in a stronger back-donation to the 2π CO molecular orbitals. The authors suggested that molecularly adsorbed O2 is activated without suppressing the O–O bond on Pd monomers embedded in low-coordinated Au sites to form H2O2 (Figure9b). These Pd isolated sites are present at the surface of the homogeneous Pd–Au alloy observed by High Angle Annular Dark Field (HAADF)-TEM analyses. Conversely, the Pd ensembles favoured H2O2 hydrogenation. It was also proposed that the Catalysts 2018, 8, x FOR PEER REVIEW 11 of 36
376 Moreover, the intensity of these bands diminished dramatically by decreasing the Pd/Au ratio. 377 Conversely, the ratio of the linear CO bands vs. bridged- and multi-bonded CO bands grew from 0.4 378 (monometallic Pd catalyst) to 1.0 (bimetallic Pd1.0Au2.0 catalyst). Based on these observations, the 379 amount of surface Pd ensembles was lowered upon Au addition, whereas isolated Pd sites were 380 increased (geometric effect occurring between Pd and Au), due to a dilution by gold. A small 381 Catalysts 2019, 9,red 30-shift of the band related to the linear carbonyls, and a shift of the absorption of bridged 11 of 34 382 carbonyls from 1977 to 1969 cm–1 were observed after Au addition. These shifts are possibly a 383 consequence of the charge-transfer from gold to palladium, which enhanced the electron density of 384 the involved d orbitals, resulting in a stronger back-donation to the 2 CO molecular orbitals. The sites at385 the interfaceauthors suggested between that Au molecularly and TiO adsorbed2 are active O2 is activated in the without H2O formation suppressing directlythe O–O bond from on H2 and O2, because386 of thePd lowest monomers selectivity embedded andin low the-coordinated absence Au of sites contiguous to form H2 PdO2 (Figure ensembles. 9b). These Pd isolated 387 sites are present at the surface of the homogeneous Pd–Au alloy observed by High Angle Annular The promotional effect of gold was previously reported for Pd–Au/SiO2 catalysts by XPS 388 Dark Field (HAADF)-TEM analyses. Conversely, the Pd ensembles favoured H2O2 hydrogenation. It measurements389 was combined also proposed with that the in sites situ at DRIFTthe interface spectroscopy between Au and of TiO adsorbed2 are active in CO. the H These2O formation studies proved the occurrence390 directly of surface from H2 and and electronic O2, because modifications of the lowest selectivity of Pd and when the alloyed absence of with contiguous Au atoms, Pd leading 391 ensembles. to enhanced reactivity and selectivity for the H2O2 direct synthesis [89]. Very recently, Flaherty et al. 392 The promotional effect of gold was previously reported for Pd–Au/SiO2 catalysts by XPS investigated393 measurements Pd and Au xcombinedPd1 nanoparticles with in situ DRIFT with spectroscopy similar of size adsorbed (7–11 CO. nm) These to studies understand proved the the effect of alloying394 Pd withoccurrence Au [of90 surface]. In particular,and electronic themodifications aim was of toPd findwhen betteralloyed explanationswith Au atoms, leading for the to high H2O2 395 enhanced reactivity and selectivity for the H2O2 direct synthesis [89]. Very recently, Flaherty et al. selectivity of these bimetallic catalysts by measuring the steady-state formation rates of both H2O2 and 396 investigated Pd and AuxPd1 nanoparticles with similar size (7–11 nm) to understand the effect of H2O with397 respectalloying to Pd the with pressure, Au [90]. theIn particular, temperature, the aim and was theto find nature better ofexplanations the solvent. for the The high authors H2O2 indicated that H2398O2 is producedselectivity of bythese sequential bimetallic catalysts surface by proton-electron measuring the steady transfers.-state formation Interestingly, rates of both an H increase2O2 of the Au:Pd399 ratio correspondsand H2O with respect to different to the pressure, and simultaneous the temperature, increasesand the nature in theof the activation solvent. The enthalpies authors related 400 indicated that H2O2 is produced by sequential surface proton-electron transfers. Interestingly, an to the H4012O 2 increaseand H 2ofO the production. Au:Pd ratio co Theserresponds changes to different are and due simultaneous to the occurrence increases in the of electronicactivation changes induced402 by theenthalpies addition related of gold to the to H palladium2O2 and H2O andproduction. are responsible These changes for are the due improved to the occurrence selectivity of towards 403 electronic changes induced by the addition of gold to palladium and are responsible for the H2O2 reported for AuPd bimetallic catalysts. The Pd and AuxPd1 were characterized also by FTIR 404 improved selectivity towards H2O2 reported for AuPd bimetallic catalysts. The Pd and AuxPd1 were spectroscopy,405 characterized and the results also by areFTIR reported spectroscopy, in and Figure the results 10a. are reported in Figure 10a. 406 a b
407
408 Figure 10. (a) Infrared spectra of CO adsorbed on Pd (black; 0.5 wt% Pd), Au1Pd1 (red; 0.5 wt% Pd), Figure 10. (a) Infrared spectra of CO adsorbed on Pd (black; 0.5 wt% Pd), Au1Pd1 (red; 0.5 wt% Pd), 409 and Au7Pd1 (blue; 0.014 wt% Pd) obtained after saturating surfaces under flowing CO (~15 min in 5 and410 Au 7Pd1 (blue;kPa CO, 0.01496 kPa wt%He, 303 Pd) K) obtainedand purging after gas-phase saturating CO with surfacesHe (101 kPa, under 47.5 cm3 flowing min–1, 303 CO K). (~15 min in − 5 kPa411 CO, 96Spectra kPa He, are the 303 average K) and of 128 purging scans with gas-phase a 4 cm–1 resolution. CO with Peak He heights (101 were kPa, normalized 47.5 cm 3bymin the 1, 303 K). Spectra412 are theatop average bound CO of feature 128 scansat 2090– with2000 cm a– 41. ( cmb) Steady−1 resolution.-state H2O2 (black) Peak and heights H2O formation were normalizedrates (red) by the 413 and selectivity towards H2O2 (blue) on catalysts with different ratios of Au to Pd (55 kPa H2, 60 kPa atop bound CO feature at 2090–2000 cm−1.(b) Steady-state H O (black) and H O formation rates (red) 414 O2, 305 K, 30 cm3 min–1 20% v/v methanol). Dashed bars indicate2 2 that rates were2 undetectable. and415 selectivity Reprinted towards from H2 OJ. 2 Catal.,(blue) 357, on N. catalysts M. Wilson, with P. Priyadarshini, different ratios S. Kunz, of Au D. to W. Pd Flaherty, (55 kPa Direct H2 , 60 kPa O2, 305 K, 30 cm3 min−1 20% v/v methanol). Dashed bars indicate that rates were undetectable. Reprinted
from J. Catal., 357, N. M. Wilson, P. Priyadarshini, S. Kunz, D. W. Flaherty, Direct synthesis of H2O2 on Pd and AuxPd1 clusters: Understanding the effects of alloying Pd with Au, 163–175, Copyright (2018), with permission from Elsevier.
The absorption bands in the 2090–2000 cm−1 range are assigned to atop CO species adsorbed on Pd, whereas those between 1960 and 1940 cm−1 are due to the formation of bridge bounded CO on Pd [83]. Upon gold addition to Pd, the peaks related to the atop carbonyl species are significantly red-shifted of about 90 cm−1 [91]. The ratio between the integrated areas of the bridge bounded/atop bands was taken as an indication of the relative amount of Pd ensembles with respect to Pd monomers [86], and decreased by adding Au to Pd, indicating the simultaneous presence of Pd and Au atoms within the same nanoparticle. The formation turnover rates of H2O2 and H2O are dependent on the Au content of the bimetallic −1 AuxPd1 nanoparticles (Figure7b). In particular, the formation rates of 0.11 mol H 2O2 (mol Pds s) −1 and 0.08 mol H2O (mol Pds s) over the Au12Pd1 catalyst are lower than those obtained for the −1 −1 Pd catalyst (0.40 mol H2O2 (mol Pds s) and 1.4 mol H2O (mol Pds s) . Bare Au nanoparticles catalysed neither H2O2 nor H2O formation, meaning that Pd is needed for the H2O2 direct synthesis and that Pd atoms are probably the active sites. Moreover, an enhancement of the selectivity towards H2O2 from 23% (bare Pd) up to 60% (Au12Pd1) was observed, since the decrease in H2O formation at Catalysts 2018, 8, x FOR PEER REVIEW 12 of 36
416 synthesis of H2O2 on Pd and AuxPd1 clusters: Understanding the effects of alloying Pd with Au, 163– Formatted: Subscript 417 175, Copyright (2018), with permission from Elsevier. Formatted: Subscript Formatted: Subscript 418 The absorption bands in the 2090–2000 cm–1 range are assigned to atop CO species adsorbed on Subscript 419 Pd, whereas those between 1960 and 1940 cm–1 are due to the formation of bridge bounded CO on Pd Formatted: 420 [83]. Upon gold addition to Pd, the peaks related to the atop carbonyl species are significantly 421 red-shifted of about 90 cm–1 [91]. The ratio between the integrated areas of the bridge bounded/atop 422 bands was taken as an indication of the relative amount of Pd ensembles with respect to Pd Catalysts4232019 , 9,monomers 30 [86], and decreased by adding Au to Pd, indicating the simultaneous presence of Pd and 12 of 34 424 Au atoms within the same nanoparticle. 425 The formation turnover rates of H2O2 and H2O are dependent on the Au content of the 426 bimetallic AuxPd1 nanoparticles (Figure 7b). In particular, the formation rates of 0.11 mol H2O2 (mol increasing Au amount was larger than that of H2O2 at the experimental conditions reported in the 427 Pds s)–1 and 0.08 mol H2O (mol Pds s)–1 over the Au12Pd1 catalyst are lower than those obtained for the paper (55 kPa H , 60 kPa O , 305 K). These observations were in agreement with the observed decrease 428 Pd catalyst2 (0.40 mol2 H2O2 (mol Pds s)–1 and 1.4 mol H2O (mol Pds s)–1. Bare Au nanoparticles of the bridge/atop429 catalysed CO neither ratio H2 (FigureO2 nor H72Oa), formation, and with meaning literature that Pd findings is needed for on the AuPd H2O2 nanoparticlesdirect synthesis supported 430 and that Pd atoms are probably the active sites. Moreover, an enhancement of the selectivity towards on carbon [92], TiO2 [27], and SiO2 [89]. The increase in selectivity at increasing Au amounts was 431 H2O2 from 23% (bare Pd) up to 60% (Au12Pd1) was observed, since the decrease in H2O formation at associated with greater activation enthalpies for H O and H O production on isolated Pd atoms than 432 increasing Au amount was larger than that of H22O2 2at the experimental2 conditions reported in the on ensembles433 paper of Pd (55 atoms kPa H2, [ 8760 ].kPa O2, 305 K). These observations were in agreement with the observed 434 decrease of the bridge/atop CO ratio (Figure 7a), and with literature findings on AuPd nanoparticles With the aim of obtaining catalysts enriched with surface isolated Pd active sites for H2O2 435 supported on carbon [92], TiO2 [27], and SiO2 [89]. The increase in selectivity at increasing Au synthesis,436 Zhangamounts et was al. associated [54] synthesized with greater Pd-Znactivation bimetallic enthalpies for catalysts H2O2 and H supported2O production onon isolated alumina and with −1 −1 different437 Pd/ZnPd atoms metal than ratios.on ensembles The of Pd 1Pd5Zn atoms [87]. bimetallic catalyst reached 25,431 mol kgPd h of 438 With the aim of obtaining catalysts enriched with surface isolated Pd active sites for H2O2 produced H2O2, which was superior than the productivity achieved in the presence of monometallic 439 synthesis, Zhang et− al.1 [54]− 1synthesized Pd-Zn bimetallic catalysts supported on alumina and with 1Pd catalyst440 (8533different mol Pd/Zn kg Pdmetal hratios.). The 1Pd5Zn bimetallic catalyst reached 25,431 mol kgPd−1 h−1 of The441 authors produced bestowed H2O2, which the was marked superior improvement than the productivity of catalyticachieved inactivity the presence to of geometric monometallic and electronic effects442 induced 1Pd bycatalyst Zn (8533 addition. mol kgPd XPS−1 h−1).results indicated that at increasing Zn loadings the number of 443 The authors bestowed the marked improvement of catalytic activity to geometric and electronic surface444 contiguous effects induced Pd sites by Zn decreased addition. XPS and, results at the indicated same that time, at increasing an increase Zn loadings of the the number number of of isolated Pd sites was445 observed.surface contiguous Indeed, Pd Zn sites is decreased able to and, disassemble at the same time, the an surface increase Pdof the agglomerates, number of isolated thus Pd enhancing the amount446 ofsites Pd was islands observed. and Indeed, single Zn is atomsable to disass [53].emble The the catalysts surface Pd wereagglomerates, reduced thus atenhancing 300 ◦C by using a 447 the amount of Pd islands and single atoms [53]. The catalysts were reduced at 300 °C by using a 10% ◦ 10% H2448/N 2 mixtureH2/N2 mixture for 60for min,60 min, and and then cooled cooled in ain N2a atmosphere N2 atmosphere before CO before interaction CO at interaction 30 °C for 15 at 30 C for 15 min.449 The DRIFTmin. The spectraDRIFT spectra collected collected on on monometallic monometallic Pd and Pd on and bimetallic on bimetallic PdZn catalysts PdZn are shown catalysts in are shown in Figure450 11 . Figure 11. 451
452
Figure 11. In situ DRIFTS of CO adsorption over different catalysts. Reprinted from Appl. Catal. A: General, 531, S. Wang, K. Gao, W. Li, J. Zhang, Effect of Zn addition on the direct synthesis of hydrogen peroxide over supported palladium catalysts, 89–95, Copyright (2017), with permission from Elsevier.
Bands at 2089 (linear CO adsorbed on isolated surface Pd sites [51]), 1994 (bridged CO species on Pd edges [93]), and 1941 cm−1 (bridged CO species on Pd atoms exposed at the surface of either (100) or (111) facets [39]) due to CO on different Pd sites were observed on the monometallic 1Pd catalyst [88]. Upon Zn addition, a red-shift of these peaks along with a gradual decrease in intensity of the peak at 1941 cm−1, related to bridged carbonyls on Pd atoms on either (100) or (111) facets, was observed (red and blue curves), which almost completely disappeared in the case of the 1Pd5Zn catalyst (pink curve). These spectroscopic features put in evidence a strong Pd surface modification induced by the presence of Zn. In agreement with Ouyang et al. [86], the authors ascribed the observed red-shift to an increase of the electron density of the d-orbital due to the charge transfer from Zn to Pd species [86], resulting in an increase of the isolated Pd0 sites amount. Indeed, the Pd-Zn electronic interaction positively promoted both H2 conversion and H2O2 productivity. Changes in surface composition and structure of bimetallic PdZn catalysts supported on silica were also already elegantly evaluated by Miller et al. using DRIFTS of CO adsorption combined with electron microscopy, X-ray absorption spectroscopy, CO chemisorption, and calorimetric analysis [53]. They observed the surface changes induced by varying the pre-reduction temperature from 225 up to 500 ◦C and reported the linear-to-bridge-bound ratio obtained by comparing the areas of the Catalysts 2019, 9, 30 13 of 34 peaks observed on two PdZn samples with different Pd:Zn molar ratios. The results are reported in Table1. A significant increase in linear-bound CO was observed upon Zn addition, moreover the addition of a Zn excess zinc (2%Pd–10%Zn catalyst) resulted in a contained enhancement of the linear-to-bridge-bound CO ratio (2.5:1) with respect to the 3%Pd–1.8%Zn catalyst (2.1:1).
Table 1. Initial heat of CO adsorption values (±5 kJ/mol) in the presence of chemisorbed hydrogen and linear-to-bridge ratios from DRIFTS. Reprinted from J. Catal., 318, D. J. Childers, N. M. Schweitzer, S. Mehdi Kamali Shahari, R. M. Rioux, J. T. Miller, R. J. Meyer, Modifying structure-sensitive reactions by addition of Zn to Pd, 75–84, Copyright (2014), with permission from Elsevier.
CO (Initial) Heat of Reduction Sample 1 Adsorption with Chemisorbed Linear-to-Bridge Ratio Temperature (◦C) H (kJ/mol CO) 2 3 2Pd/SiO2 225 92 0.2:1 2Pd–10Zn/SiO2 300 102 2.5:1 3Pd–1.8Zn/SiO2 300 99 2.1:1 550 93 1.8:1 1 Catalysts were initially reduced under 5.11% H2/Ar (both gases, 99.999% UHP) for 2 h at the specified reduction 2 temperature,Catalysts followed 2018, 8, byx FOR subsequent PEER REVIEW cooling in H2. Initial heat of CO adsorption determined by microcalorimetry14 of 36 on a reduced Pd or PdZn surface containing chemisorbed hydrogen. 3 Monometallic Pd catalyst from previous work495 studied usingBased theon modifiedthe characterization procedure. results, the authors proposed simplified models of the catalyst 496 structure, which are shown in Figure 12b. In particular, the bimetallic nanoparticles of the 3%Pd– 497 1.8%Zn catalyst have a Pd core with surface Zn atoms upon reduction at 275 °C, and the surface The498 comparison PdZn film possesses of the DRIFT an intermetallic spectra alloy of COstructure, adsorbed based on on the the high 3%Pd–1.8%Zn intensity of the band catalyst related pre-reduced at 300499 and 550to linear-bound◦C (Figure CO 12 bands.a) put An increase in evidence in the surface a shift PdZn from intermetallic 2075 toalloy, 2070 with cm few− residual1 of the Pd peak due to 500 linear CO peakensembles, by increasing occurs at 550 the °C, reductionwhile the nanoparticle temperature core is Pd-rich. at 500 This◦C, is indicating due to the limited a small amount increase of the 501 of Zn atoms interacting with Pd, resulting in the impossibility to form a fully intermetallic PdZn population502 ofalloy linear nanoparticle carbonyls at such located temperature at the [94]. Pd edge sites. Analogously, the absorption band related to bridge-bounded503 Conversely, CO species in the case showed of the 3%Pd–1.8%Zn a broadening catalyst, and a ashell shift made from up by 1975 PdZn to alloy, 1965 totally cm −1 upon the 504 covering the Pd-rich core was proposed already at 275 °C. For both catalysts, the PdZn metallic increase505 of the reduction temperature. However, the linear-to-bridge ratio did not change significantly: surface◦ consists of an ordered◦ alloy structure, and a random distribution of metallic Pd and Zn from 2.1:1506 atsurface 275 C atoms to 1.8:1 is very at unlikely. 550 C. At 550 °C, there is almost complete formation of the PdZn alloy shell.
507 Figure508 12. (a)Figure Normalized 12. (a) Normalized DRIFT DRIFT spectra spectra of the of the 3%Pd–1.8%Zn 3%Pd–1.8%Zn catalyst catalyst pre-reduced pre-reduced at 300 °C at (red) 300 ◦C (red) and 509 ◦ and at 550 °C (blue). (b) Cross-section of Pd and PdZn catalysts showing structure change as at510 550 C (blue).reduction (b) temperature Cross-section increased. of Pd Reprinted and PdZn from J. catalystsCatal., 318, showingD. J. Childers, structure N. M. Schweitzer, change S. as reduction temperature511 increased.Mehdi Kamali Reprinted Shahari, R. M. from Rioux, J. J. Catal., T. Miller, 318, R. J. D. Meyer, J. Childers, Modifying N.structure-sensitive M. Schweitzer, reactions S. Mehdi Kamali Shahari,512 R. M.byRioux, addition J.of T.Zn Miller, to Pd, 75–84, R. J. Copyrigh Meyer,t Modifying(2014), with permission structure-sensitive from Elsevier. reactions by addition of Zn to513 Pd, 75–84,However, Copyright isolated (2014), Pd withatoms permissionwere responsible from for Elsevier. the enhancement of the catalytic activity and 514 the authors ascribed this improvement to geometric effects rather than an electronic effect due to Based515 onalloy the formation. characterization results, the authors proposed simplified models of the catalyst structure,516 whichAn areexcellent shown Pd–Te/TiO in Figure2 catalyst with12b. almost In 100% particular, H2O2 selectivity the under bimetallic mild conditions nanoparticles (283 of the 517 K, 0.1 MPa, using a semi-batch continuous flow reactor) was recently investigated [52]. Upon ◦ 3%Pd–1.8%Zn518 addition catalyst of tellurium, have Pd a Pdnanoparticles core with with surface smaller size Zn were atoms obtained, upon and reduction such Te-modified at 275 Pd C, and the surface519 PdZn surfaces film possesses hindered the anO2 dissociative intermetallic activation, alloy favouring structure, at the based same time on the the non-dissociative high intensity O2 of the band related520 to linear-boundhydrogenation. CO In bands.order to Anfind increasestructure–activity in the surfacerelationships, PdZn DRIFT intermetallic spectroscopy alloy, of adsorbed with few residual 521 CO was employed in combination◦ with STEM-EDS, EXAFS, O2-TPD, XPS, and DFT calculations to Pd ensembles,522 shed occurs light on atthe 550electronicC, structure while theof the nanoparticle surface Pd atoms. core is Pd-rich. This is due to the limited amount523 of Zn atomsAs shown interacting in Figure 13a, with the band Pd, ascribed resulting to CO in linearly the impossibility adsorbed on Pd sites to formred-shifted a fully from intermetallic –1 PdZn alloy524 nanoparticle2079 to 2051 cm at upon such addition temperature of Te. Moreover, [94]. according to DFT calculations, the binding energy 525 of CO adsorbed on low-coordinated Pd sites exposed at the surface of smaller particles was 526 noticeably higher than that related to CO adsorbed on the Pd terrace sites of extended surfaces. 527 Particularly, the amount of smaller Pd nanoparticles increased at increasing Te loading, resulting in 528 an increase of the low-coordinated Pd corners and edges, as indicated by the enhancement of the 529 intensity of the band related to linearly carbonyls and by the gradual decrease of the absorption 530 centred at 1982–1902 cm–1 ascribed to CO on bridge and hollow sites [83]. Indeed, only the band 531 related to CO linearly bounded was present in the case of the Pd17Te4 and Pd3Te2 catalysts, 532 confirming the presence of highly dispersed clusters or isolated Pd atoms. 533 A mechanism explaining the role of Te in improving the catalytic activity was proposed based 534 on STEM-EDS, EXAFS, and CO-DRIFTS results. In particular, the reason for the noticeable catalytic
Catalysts 2019, 9, 30 14 of 34
Conversely, in the case of the 3%Pd–1.8%Zn catalyst, a shell made up by PdZn alloy, totally covering the Pd-rich core was proposed already at 275 ◦C. For both catalysts, the PdZn metallic surface consists of an ordered alloy structure, and a random distribution of metallic Pd and Zn surface atoms is very unlikely. At 550 ◦C, there is almost complete formation of the PdZn alloy shell. However, isolated Pd atoms were responsible for the enhancement of the catalytic activity and the authors ascribed this improvement to geometric effects rather than an electronic effect due to alloy formation. An excellent Pd–Te/TiO2 catalyst with almost 100% H2O2 selectivity under mild conditions (283 K, 0.1 MPa, using a semi-batch continuous flow reactor) was recently investigated [52]. Upon addition of tellurium, Pd nanoparticles with smaller size were obtained, and such Te-modified Pd surfaces hindered the O2 dissociative activation, favouring at the same time the non-dissociative O2 hydrogenation. In order to find structure–activity relationships, DRIFT spectroscopy of adsorbed CO was employed in combination with STEM-EDS, EXAFS, O2-TPD, XPS, and DFT calculations to shed light on the electronic structure of the surface Pd atoms. As shown in Figure 13a, the band ascribed to CO linearly adsorbed on Pd sites red-shifted from 2079 to 2051 cm−1 upon addition of Te. Moreover, according to DFT calculations, the binding energy of CO adsorbed on low-coordinated Pd sites exposed at the surface of smaller particles was noticeably higher than that related to CO adsorbed on the Pd terrace sites of extended surfaces. Particularly, Catalysts 2018, 8, x FOR PEER REVIEW 15 of 36 the amount of smaller Pd nanoparticles increased at increasing Te loading, resulting in an increase of the low-coordinated535 performance Pd corners was ascribed and to edges, the presence as indicated of selectively by active the enhancementsites bimetallic Pd–Te, of the in which intensity the Te of the band 536 2 2 inertness toward O adsorption significantly inhibited the dissociative O activation as revealed by −1 related to537 linearly XPS carbonylsand O2-TPD andanalyses. by theAs agradual matter of decreasefact, the Pd of150Te the1 catalyst absorption containing centred poor Te at amount 1982–1902 cm ascribed538 to COshowed on bridge higher and selectivity hollow than sites the [ 83monometallic]. Indeed, Pd only catalyst. the band Side reactions related towere CO noticeably linearly bounded 539 inhibited and a selectivity of almost 100% was achieved by increasing the Te/Pd atomic ratio to 1:100, was present in the case of the Pd17Te4 and Pd3Te2 catalysts, confirming the presence of highly dispersed 540 because of the increased number of surface Pd–Te sites. Indeed, a much contained increase of the clusters or541 isolated Te/Pd Pdratio atoms. to 1:50 and 1:17 resulted to lower selectivity (78.8% and 67.3%, respectively). 542
543
Figure544 13. (a) InFigure situ 13. DRIFTS (a) In situ measurement DRIFTS measurement of CO of adsorptionCO adsorption over over the the Pd–Te/TiO Pd–Te/TiO2 catalysts2 catalysts at 283 K at 283 K in 545 in an Ar flow. (b) Proposed mechanism for the direct synthesis of H2O2 over Pd–Te/TiO2 catalysts. an Ar flow. (b) Proposed mechanism for the direct synthesis of H2O2 over Pd–Te/TiO2 catalysts. Blue 546 Blue and brown spheres are Pd and Te atoms, respectively. Reprinted from P. Tian, X. Xu, C. Ao, D. and547 brown spheresDing, areW. Li, Pd R. andSi, W. Te Tu, atoms, J. Xu, Y.-F. respectively. Han, ChemSusChem, Reprinted 10, from3342–3346, P. Tian, Copyright X. Xu, (2017), C.Ao, John D. Ding, W. Li, R.548 Si, W. Tu,Wiley J. Xu, and Y.-F. Sons. Han, ChemSusChem, 10, 3342–3346, Copyright (2017), John Wiley and Sons. 549 At the same time, as indicated by XRD, TEM, and CO-DRIFTS findings, the Pd particle size was A mechanism550 diminished explaining at increasing the Te/Pd role ratios, of Te and in improvinglow-coordinated the active catalytic edges and activity corners were was formed. proposed based on STEM-EDS,551 Such EXAFS, low-coordinated and CO-DRIFTS sites are much results. more active In particular,to bind and dissociate the reason molecular for theO2, with noticeable respect catalytic 552 to terrace sites [95]. As a result, the selectivity to H2O2 of the Pd50Te1 and Pd17Te1 catalysts is lower performance was ascribed to the presence of selectively active sites bimetallic Pd–Te, in which the 553 than that observed in the case of Pd100Te1. Thus, a high amount of surface Te sites would inhibit both Te inertness554 towardH2 and O O2 2reactantadsorption molecules significantly adsorption, resulting inhibited in inert thePd17Te dissociative4 and Pd3Te2 materials. O2 activation Indeed, the as revealed 555 surface Pd atoms of these catalysts are isolated by Te atoms, as revealed by EXAFS and CO-DRIFTS. by XPS and O2-TPD analyses. As a matter of fact, the Pd150Te1 catalyst containing poor Te amount 556 The results indicate that only by finely tuning the Pd/Te ratio it is possible to control the amount of showed higher557 terrace selectivity Pd-Te sites, than as thewell monometallicas the particle size Pdto obtain catalyst. highly-performing Side reactions catalysts. were noticeably inhibited and a selectivity558 ofVery almost recently 100% Flaherty was et achievedal. reported that by increasingthe steady-state the selectivity Te/Pd to atomic H2O2 of AgPt ratio octahedra to 1:100, because of the increased559 supported number on ofsilica surface (50%) is Pd–Te 10-fold sites.greater Indeed,than observed a much with containedPt/SiO2 nanoparticles increase with of similar the Te/Pd ratio 560 size (6%) [45]. In addition, the abundance and location of Pt atoms on the AgPt octahedra surface to 1:50 and 1:17 resulted to lower selectivity (78.8% and 67.3%, respectively). 561 play a role on the initial formation rates selectivity to H2O2. The population of these sites can be At the562 samemodulated time, aseither indicated by CO exposure by XRD, at TEM,373 K to and obtain CO-DRIFTS a Pt-rich surface findings, (with 16% the initial Pd particle H2O2 size was diminished563 atselectivity) increasing or by Te/Pd inert gases ratios, exposure and at low-coordinated the same temperature activeto achieve edges a Pt-poor and surface corners (withwere 36% formed. 564 initial H2O2 selectivity). Such low-coordinated565 FTIR experiments sites are muchof adsorbed more 12CO active were then to bindperformed and on dissociate the monometallic molecular Pt catalyst O2 and, with respect 566 on the AgPt catalyst pretreated in 12CO or He (Figure 14a). Firstly, it has to be recalled that 12CO does 567 not adsorb on the Ag sites under the adopted experimental conditions. The bands of adsorbed 12CO 568 on AgPtCO (black curve) and AgPtHe (red curve) octahedra differ significantly in both position and 569 intensity, due to modifications of surface structure of the AgPt octahedral, because the FTIR spectra 570 were obtained by submitting the same sample pellet to in situ CO and He pre-treatments. 571 Conversely, the band at 2098 cm–1 was assigned linear carbonyl species adsorbed on single Pt atoms 572 exposed at the surface of the nanoparticles [96] and on Pt(111) [81]. The positions of the bands 573 related to linearly adsorbed 12CO are significantly red-shifted at 2051 cm–1 for AgPtCO and at 2033 cm– 574 1 in the case of AgPtHe, revealing different extents of electron exchange between the 12CO probe. Such 575 a feature can be ascribed to lower dipole–dipole coupling between the 12CO molecules due to the
Catalysts 2019, 9, 30 15 of 34
to terrace sites [95]. As a result, the selectivity to H2O2 of the Pd50Te1 and Pd17Te1 catalysts is lower than that observed in the case of Pd100Te1. Thus, a high amount of surface Te sites would inhibit both H2 and O2 reactant molecules adsorption, resulting in inert Pd17Te4 and Pd3Te2 materials. Indeed, the surface Pd atoms of these catalysts are isolated by Te atoms, as revealed by EXAFS and CO-DRIFTS. The results indicate that only by finely tuning the Pd/Te ratio it is possible to control the amount of terrace Pd-Te sites, as well as the particle size to obtain highly-performing catalysts. Very recently Flaherty et al. reported that the steady-state selectivity to H2O2 of AgPt octahedra supported on silica (50%) is 10-fold greater than observed with Pt/SiO2 nanoparticles with similar size (6%) [45]. In addition, the abundance and location of Pt atoms on the AgPt octahedra surface play a role on the initial formation rates selectivity to H2O2. The population of these sites can be modulated either by CO exposure at 373 K to obtain a Pt-rich surface (with 16% initial H2O2 selectivity) or by inert gases exposure at the same temperature to achieve a Pt-poor surface (with 36% initial H2O2 selectivity). FTIR experiments of adsorbed 12CO were then performed on the monometallic Pt catalyst and on the AgPt catalyst pretreated in 12CO or He (Figure 14a). Firstly, it has to be recalled that 12CO does not adsorb on the Ag sites under the adopted experimental conditions. The bands of adsorbed 12CO on AgPtCO (black curve) and AgPtHe (red curve) octahedra differ significantly in both position and intensity, due to modifications of surface structure of the AgPt octahedral, because the FTIR spectra were obtained by submitting the same sample pellet to in situ CO and He pre-treatments. Conversely, the band at 2098 cm−1 was assigned linear carbonyl species adsorbed on single Pt atoms exposed at the surface of the nanoparticles [96] and on Pt(111) [81]. The positions of the bands related to linearly 12 −1 −1 adsorbed CO are significantly red-shifted at 2051 cm for AgPtCO and at 2033 cm in the case of 12 AgPtHe, revealing different extents of electron exchange between the CO probe. Such a feature can be ascribed to lower dipole–dipole coupling between the 12CO molecules due to the lower coverage of linear carbonyls, which results in a red-shift of the 12CO band [81]. In addition, the intensity of the peaks related to the AgPt octahedra pre-treated with CO was about six times the intensity observed 12 for AgPtHe, which pointed out that the CO pre-treatment was able to extract a much bigger amount of exposed Pt sites at the surface of the AgPt octahedra with respect to the treatment in He. Moreover, −1 the difference in position of about 20 cm for AgPtCO and AgPtHe was in agreement with the literature on CO adsorbed on well-coordinated Pt terraces and on under-coordinated Pt edges [96]. In order to verify the occurrence of different electronic effects on the catalysts, the singleton frequency can be evaluated by using 13CO–12CO isotopic mixture to dilute the adsorbed 12CO molecules and by evaluating of exchange rates between adsorbed 13CO and 12CO. The changes in the singleton frequency of adsorbed 13CO clearly pointed out the electronic changes in Pt atoms as shown in section b of Figure 14. In particular, a red-shift of the band related to adsorbed 13CO was 13 13 observed by decreasing the CO coverage (θ CO), signifying the occurrence of dipole–dipole coupling. The 13CO singleton frequency was calculated by extrapolation of the spectra (shown in section a) to a zero coverage, and obtaining 2016 ± 6 cm−1 for the monometallic Pt catalyst, 1974 ± 8 cm−1 for −1 AgPtCO, and 1979 ± 12 cm for AgPtHe. The last two values were much lower than on the Pt catalyst, which indicates a greater extent of electron back-donation from the Pt atoms to the CO 2π* orbitals on the AgPt octahedra. The above findings were unexpected, since the AgPt octahedra gave higher selectivity to H2O2 than Pt nanoparticles. 13 12 The isosteric CO desorption under CO flow on AgPtHe, AgPtCO and on Pt nanoparticles are reported in Figure 14, section c. It can be observed that the 13CO desorption and exchange with 12 13 CO take 400 s on Pt, whereas only about 50% and 15% CO exchange occurs in 800 s on AgPtHe 13 and AgPtCO, respectively. The CO desorption rates were described by Equation (3), a first-order desorption process for surfaces containing n adsorbing sites:
n dθ13CO − = ∑ ki·θ13CO,i (3) dt i Catalysts 2018, 8, x FOR PEER REVIEW 16 of 36
576 lower coverage of linear carbonyls, which results in a red-shift of the 12CO band [81]. In addition, the 577 intensity of the peaks related to the AgPt octahedra pre-treated with CO was about six times the 578 intensity observed for AgPtHe, which pointed out that the 12CO pre-treatment was able to extract a 579 much bigger amount of exposed Pt sites at the surface of the AgPt octahedra with respect to the 580 treatment in He. Moreover, the difference in position of about 20 cm–1 for AgPtCO and AgPtHe was in 581 agreement with the literature on CO adsorbed on well-coordinated Pt terraces and on Catalysts 2019, 9, 30 16 of 34 582 under-coordinated Pt edges [96]. 583 In order to verify the occurrence of different electronic effects on the catalysts, the singleton 584 frequency can be evaluated by using 13CO–12CO isotopic mixture to dilute the adsorbed 12CO −1 where 585ki is themolecules rate constant and by evaluating for CO of desorption exchange rates from between site adsorbedi expressed 13CO and in 12CO. s The. The changes sum in ofthe all coverages 13 586 singleton frequency of adsorbed 13CO clearly pointed out the electronic13 changes in Pt atoms as θ CO,I = 1 at the exchange onset. The desorption rates for >95% of CO molecules from the surfaces 587 shown in section b of Figure 14. In particular, a red-shift of the band related to adsorbed 13CO was of the Pt nanoparticles were accurately delineated by a model that describes a uniform surface for 588 observed by decreasing the 13CO coverage (θ13CO), signifying the occurrence of dipole–dipole which 589n = 1.coupling. This was The not13CO truesingleton in the frequency case ofwas AgPt calculatedHe and by extrapolation AgPtCO octahedral, of the spectra because(shown in two distinct sites have590 tosection be considered a) to a zero coverage, to explain and obtaining the desorption 2016 ± 6 cm kinetics–1 for the monometallic and the significant Pt catalyst, 197413CO ± 8 amount that 591 cm–1 for AgPtCO, and 1979 ± 12 cm–1 for AgPtHe. The last two values were much lower than on the Pt remain592 adsorbed catalyst, during which indicates the experiment. a greater extent H of2 Oelectron2 and back-donation H2O form from on distinctthe Pt atoms active to the CO sites 2π* and the ratio between593 those orbitals on whichon the AgPt H2 Ooctahedra.2 is formed The above and findings those were on whichunexpected, H2 Osince formation the AgPt octahedra occurs gave increased upon Ag addition.594 higher selectivity to H2O2 than Pt nanoparticles. 595
596 597 Figure 14. (a) infrared spectra of adsorbed 12CO following the purge of gas-phase 12CO with He (101 Figure 14. (a) infrared spectra of adsorbed 12CO following the purge of gas-phase 12CO with He 598 kPa, 30 cm3 min–1, 303 K) on Pt (blue), AgPtCO (black), and AgPtHe (red). Spectra are the average of 128 3 −1 (101599 kPa, 30 cmscansmin with a 4, cm 303–1 resolution. K) on Pt Dotted (blue), lines AgPt are intendedCO (black), to show and the peak AgPt positionHe (red). for each Spectra spectrum. are the average −1 13 13 13 of600 128 scans with(b and ac) 4Peak cm positionresolution. of ν(C=O) for DottedCO as a function lines are of the intended coverage of to adsorbed show theCO peak(θ CO) position(total for each 601 of 1 kPa CO, 100 kPa He, 100 cm3 min–1, 298 K) and change in the coverage of θ13CO as a function of spectrum. (b,c) Peak position of ν for 13CO as a function of the coverage of adsorbed 13CO (θ13 ) 602 time during exchange with (C=O)12CO on Pt (blue triangles) and CO-treated (black squares) and He-treated CO 3 −1 13 (total603 of 1 kPa(red CO, circles) 100 AgPt kPa octahedral He, 100 particles cm (0.2min kPa 12CO,, 298 100 cm K)3 min and–1, change298 K; surfaces in the pre-saturated coverage with of θ CO as a function604 of time13CO). duringSolid lines exchange in (b) represent with a linear12CO fit to on the Pt data, (blue and da triangles)shed lines in and panel CO-treated c represent the (black fit squares) 605 of θ13CO as a function of time. Adapted with permission from ACS Catalysis, N. M. Wilson, Y.-T. Pan, and He-treated (red circles) AgPt octahedral particles (0.2 kPa 12CO, 100 cm3 min−1, 298 K; surfaces 606 Y.-T. Shao, J.-M. Zuo, H. Yang, D. W. Flaherty, Direct Synthesis of H2O2 on AgPt Octahedra: The Formatted: Subscript pre-saturated with 13CO). Solid lines in (b) represent a linear fit to the data, and dashed lines in panel c 607 Importance of Ag–Pt Coordination for High H2O2 Selectivity, 8, 2880–2889. Copyright (2018) Formatted: Subscript 13 represent608 theAmerican fit of θ ChemicalCO as Society. a function of time. Adapted with permission from ACS Catalysis, N. M. Wilson, Y.-T. Pan, Y.-T. Shao, J.-M. Zuo, H. Yang, D. W. Flaherty, Direct Synthesis of H2O2 on AgPt 609 The isosteric 13CO desorption under 12CO flow on AgPtHe, AgPtCO and on Pt nanoparticles are Octahedra:610 reported The Importancein Figure 14, section of Ag–Pt c. It Coordinationcan be observed forthat Highthe 13CO H2 desorptionO2 Selectivity, and exchange 8, 2880–2889. with 12CO Copyright (2018)611 Americantake 400 s Chemical on Pt, whereas Society. only about 50% and 15% 13CO exchange occurs in 800 s on AgPtHe and 612 AgPtCO, respectively. The 13CO desorption rates were described by Equation (3), a first-order 3.3. Reactivity613 desorption of the Exposed process for Metal surfaces Sites containing n adsorbing sites: Only few studies proposed in situ approaches to investigate by FTIR spectroscopy of adsorbed probes the reactivity of the metallic active sites upon interactions with the reagents, i.e., molecular hydrogen and oxygen or mixtures of the two. It is worth noting that the reagents involved in the H2O2 direct synthesis are IR inactive, because there is no change in the dipole moment of the molecules upon interaction with the IR radiation. One very recent example on this approach is reported in the study by Han et al. [58], which has been already discussed in Section 3.1 as for the nature of the Pd sites on Pd/TiO2 catalysts. In addition to the common investigation carried out by adsorbing the CO probe, the authors characterized the catalysts submitted to subsequent adsorption of molecular oxygen and hydrogen, before the inlet of the CO probe. Indeed, the surface of the freshly reduced catalyst dramatically changed −1 upon O2 preadsorption: the narrow peak at 2094 cm due to the linear carbonyls (see Figure7b) was transformed into two weak peaks at 2090 and 2064 cm−1 (Figure 15). Moreover, bridged and multibonded CO species on Pd ensembles red-shifted to 1986, 1914, and 1874 cm−1, and also the relative intensities were modified, due to the geometric and electronic modification of Pd atoms induced by oxygen adsorption. Such changes were accompanied by an increase in intensity of the band at 1646 cm−1 due to the formation of carbonate species. Catalysts 2018, 8, x FOR PEER REVIEW 17 of 36