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Titania - Supported transition metals sulfides as photocatalysts for hydrogen production from

propan-2-ol and methanol

C. Maheu, Eric Puzenat, Christophe Geantet, Luis Cardenas, Pavel Afanasiev

To cite this version:

C. Maheu, Eric Puzenat, Christophe Geantet, Luis Cardenas, Pavel Afanasiev. Titania - Supported transition metals sulfides as photocatalysts for hydrogen production from propan-2-ol and methanol.

International Journal of Hydrogen Energy, Elsevier, 2019, �10.1016/j.ijhydene.2019.05.080�. �hal- 02935057�

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1 Titania - supported transition metals sulfides as photocatalysts for hydrogen production 1

from propan-2-ol and methanol 2

Clement Maheu*, Eric Puzenat, Christophe Geantet, Luis Cardenas, Pavel Afanasiev*

3

Institut de Recherches sur la Catalyse et l’Environnement de Lyon IRCELYON, UMR 5256, 4

CNRS – Université Lyon 1, 2 av A. Einstein 69626 Villeurbanne Cedex (France); Fax: 33 04 5

7244 5399; Tel: 33 04 72 44 5466;

6 7 8

E-mail: [email protected] 9

[email protected] 10

11 12

Abstract 13

A series of transition metals sulfides deposited on anatase titania (MSx/TiO2) were prepared 14

by precipitation of transition metals salts with thioacetamide in aqueous medium under reflux.

15

The solids were characterized by XRD, XPS, temperature programmed reduction and 16

transmission electron microscopy. The properties of as obtained catalysts were compared for 17

the photocatalytic hydrogen evolution reaction (PHER) in pure methanol and water- 18

isopropanol mixture. The sequences of PHER activity were compared with electrochemical 19

HER and thiophene hydrodesulfurization (HDS) activity of the corresponding sulfides 20

prepared by the same technique. For PHER, in both alcohols the most active photocatalysts 21

contain hydrogenating sulfides of Co and Ru. However the PHER activity does not follow the 22

same trend as electrocatalytic HER and thiophene HDS. Some sulfides, such as HgS or CuS, 23

show poor activity in HDS and electrocatalytic HER, but have the PHER activity comparable 24

with that of the best samples. This difference suggests that the PHER rate is not merely 25

related to the hydrogen activating properties of the co-catalyst, but is enhanced by the transfer 26

of photogenerated electrons from TiO2 towards the sulfide. The ranking of the co-catalysts 27

and the PHER activity depend also on the nature of the alcohol molecule, the overall PHER 28

rates in water-isopropanol mixture being lower than in methanol.

29 30

Keywords:

31

Hydrogen evolution reaction; transition metal sulfides; photocatalysts; titanium oxide 32

33

© 2019 published by Elsevier. This manuscript is made available under the Elsevier user license https://www.elsevier.com/open-access/userlicense/1.0/

Version of Record: https://www.sciencedirect.com/science/article/pii/S0360319919319366 Manuscript_e2d3289b89e0d9fb215783198a4bf081

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2 1. Introduction

1

Direct conversion of solar energy to chemical energy of hydrogen is considered to be a very 2

promising strategy to mitigate the global warming and to address the problem of alternative 3

energy sources [1,2]. Titanium dioxide TiO2 is by far the most studied semiconductor for the 4

artificial photosynthesis design [3,4]. Versatile aspects of surface chemistry and bulk 5

properties are important for photocatalytic hydrogen evolution reaction (PHER) using titania, 6

such as surface hydroxylation, type of exposed crystallographic facets [5], or carrier dynamics 7

[6,7]. Intense current research efforts are directed to the design of efficient co-catalysts, 8

present on the surface of TiO2 in order to enhance the utilization of photogenerated electrons 9

and holes in redox processes involved in the targeted reactions. PHER catalysts are widely 10

studied that include proton reduction by photogenerated electrons and oxidation of organic 11

molecules by photogenerated holes. Association of titania with electron accepting and/or 12

hydrogenating materials, such as noble metals, proves favorable for PHER, one of the best 13

benchmark reference PHER catalyst being Pt/TiO2. The relationships between the PHER 14

performance and the properties of co-catalysts are widely studied but not fully understood.

15

The improvement of PHER performance in composite catalysts vs. bare titania was attributed 16

to increased charge separation [8], plasmonic effects and increased rate of hydrogen atoms 17

recombination [9]. The impact of a co-catalyst is complex as it might simultaneously 18

influence several thermodynamic or kinetic parameters in the system, including the lifetimes 19

of charge carriers or adsorbed intermediates, which are usually unknown. Beside the efforts of 20

fundamental understanding, great number of research works report on the empirical studies of 21

novel catalysts combining titania and nanoparticles of various co-catalysts, aiming to enhance 22

PHER performance. Much attention has been recently paid to the studies of layered sulfides 23

on titania, particularly to the MoS2/TiO2 composites [10], which has been recently reviewed 24

[11]. MoS2 is considered as a cheap alternative to platinum, both for electrochemical HER 25

and PHER. However the specific PHER rates even for the best MoS2/TiO2 systems are still 26

lover than for Pt/TiO2. 27

Other sulfides were also investigated as co-catalysts with TiO2, though less extensively 28

studied than MoS2. Tungsten sulfide WS2 demonstrated PHER performance comparable to 29

MoS2 [12,13]. Copper sulfide on Aeroxide® P25 titania (0.5-15% wt. CuS) has been prepared 30

hydrothermally using thiourea and showed good activity for methanol reforming, the best 31

catalyst containing 1wt%. CuS [14]. Core-shell composite of NiS and anatase TiO2 was 32

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3 applied for PHER using methanol as an organic substrate and demonstrate promising activity 1

[15]. Cobalt sulfide quantum dots on TiO2 nanoparticles prepared with a precipitation- 2

deposition method were tested using ethanol as a sacrificial reagent and showed PHER rate 3

exceeding that of the pure TiO2 by more than 35 times [16]. Cadmium sulfide CdS had been 4

widely studied for PHER, but rather as a semiconductor than as a co-catalyst [17]. Moreover 5

CdS as a semiconductor could be promoted by other TM sulfide and non-sulfide co-catalysts 6

[18,19]. However CdS value for photocatalytic applications is limited because of its 7

solubilisation by photocorrosion, releasing toxic cadmium ions. Composite materials 8

containing bismuth [20], zinc [21] and indium [22] sulfides in combination with TiO2 showed 9

promising HER activities, as well as bimetallic and trimetallic sulfide materials as CuS/ZnS 10

[23] or ZnS–In2S3–CuS [24]. Multi-metal titania–based composite materials have been 11

applied as photocatalysts, containing up to four metals chalcogenides such as, for instance, 12

ZnS/CdS-Mn/MoS2/CdTe/TiO2 [25]. Comparison of PHER efficiency measured in different 13

laboratories is always difficult because the conditions of the experiments (preparation 14

methods, reactor geometry, light source, oxidized molecule, support...) are strongly varied.

15

Despite a great number of publications on the sulfide-containing photocatalysts, systematic 16

comparison of PHER performance for a series of sulfides on titania prepared by a uniform 17

technique have never been reported. The present work aims to study an extended series of 18

sulfides prepared by means of thioacetamide precipitation technique, in an attempt to provide 19

a qualitative insight into the key properties defining their relative PHER performance.

20 21

2. Experimental 22

2.1 Preparation of catalysts 23

The series of MSx/TiO2 supported catalysts (M= Ag, Co, Cu, Hg, Mo, Ni, Ru) were prepared 24

with the aqueous deposition method under the conditions similar to those reported by Girel et 25

al. [26] and with the same molar amount of co-catalyst metals (1.3 at % of metal). Typically, 26

2.0 g of commercial TiO2 (CristalACTiVTM PC500) and 900 mg of thioacetamide were 27

suspended in 100 mL of deionized water. For each synthesis, transition metal precursor salt 28

was added, in an amount containing 350 µmol equivalent of metal. Then, aqueous suspension 29

was refluxed under stirring for 1 h. In the synthesis using ammonium heptamolybdate, 2.0 ml 30

of 2.5 M HCl was added to accelerate precipitation. The solid materials were isolated by 31

centrifugation, washed and dried under N2. 32

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4 Bulk transition metal sulfides were prepared in the same conditions as titania-deposited 1

catalysts, but with a tenfold increase of the precursor amount and without addition of TiO2. 2

They were used as reference samples for characterization and phase identification of sulfide 3

phases as well as for comparison of the electrochemical HER activity. A reference catalyst 4

containing 1 wt.% Pt on P25 TiO2 was prepared by impregnation, drying and reduction with 5

H2, as described earlier [27].

6 7

2.2. Characterizations 8

Temperature-programmed reduction (TPR) was carried out in a quartz reactor. The samples of 9

sulfides (0.05–0.1 g) were heated under H2 flow (50 ml min−1) from room temperature to 10

1050 °C at a rate 5° min−1. The H2S produced in the reduction reaction was detected by a 11

Thermo Prolab quadrupole mass-spectrometer. The amount of H2S released from the solid 12

was quantified after calibration of the quadrupole detector with a known H2S content gas 13

mixture. Transmission electron microscopy (TEM) was carried out on a JEOL 2010 device 14

with an accelerating voltage 200 keV. The samples were dispersed in ethanol by ultrasound, 15

and then put onto a lacey carbon on a copper grid. In order to protect them from oxidation by 16

air, the samples still covered with liquid hexane were immediately introduced into the TEM 17

vacuum chamber. The X-ray diffraction (XRD) patterns were obtained on a Bruker D8 18

Advance diffractometer with Cu-Kα emission and identified using standard JCPDS files. The 19

metal content in the solids was determined by plasma-coupled atomic emission spectroscopy 20

(ICP-OES Activa Jobin Yvon) after dissolution in a HNO3/H2SO4 mixture. Elemental analysis 21

of light elements (CHNS) was performed on an analyzer Thermo Fisher Flash 2000. X-ray 22

photoelectron spectroscopy (XPS) measurements were performed using a commercial Axis 23

Ultra DLD spectrometer (Kratos Analytical). A monochromatic Al-Kα X-ray source at 24

1486.6 eV was used and a flood electron gun to minimize surface charging. Energy 25

calibration was made fixing both the binding energy of the C 1s intense peak assigned to C-C 26

or C-H bonds at 284.5 eV and the binding energy of the Ti 2p3/2 state at 458.5 eV. Data 27

analysis was performed using CasaXPS, after a Shirley background subtraction. The C 1s and 28

S 2p signals were decomposed into a combination of Voigt functions. For Ru 3d an 29

asymmetric lineshape was used: product of a Doniach Sunjic with a Gaussian/Lorentzian 30

function. UV-Vis diffuse reflectance was measured at room temperature with an optical fiber 31

set-up. Six optical fibers illuminate the powder sample with a Deuterium-Halogen light source 32

(AvaLight-DHS, Avantes). A seventh fiber collects the diffused light which is then analyzed 33

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5 by a CCD dectector. Pure BaSO4 was used as a reference and to dilute TiO2-based powders.

1

Kubleka-Munk (KM) function was applied to interpret spectra. Note that KM theory is valid 2

only for thick samples (here 2 mm) with weak absorption ( > 0.6). To do so we diluted the 3

samples in BaSO4 (0.1 wt.% MSx/TiO2 in BaSO4) [28].

4 5

2.3 Photocatalytic tests 6

Photocatalytic reaction was conducted in liquid phase, in a double-wall semi-batch slurry 7

reactor. Most of the catalytic tests involved 50 mg of catalyst dispersed either in pure 8

methanol or in 50 mL of 50 vol. % mixture of propan-2-ol (IPA) and distilled water. Before 9

irradiation, the reactor was purged under an argon flow for 30 min to conduct the test under 10

anaerobic conditions. Gases were analyzed by micro gas chromatography with thermal 11

conductivity detectors (Agilent Technologies, 300 A). It quantified several gases including 12

oxygen, hydrogen, hydrogen sulphide, propene and propane. Photoreactor temperature was 13

regulated at 20°C by thermostated water recirculation in the double-wall.

14

A 125 W high-pressure mercury lamp (Philips HPK 125) was used to illuminate the reactor 15

through a 20 cm2 area optical window. The reactor Pyrex glassware cut light below 290 nm 16

wavelength. The number of incident photons, likely to be absorbed by anatase, was measured 17

between 290 and 390 nm with a radiometer device, a spectrometer (AvaSpec-2018, Avantes) 18

coupled with one fiber optic probe (AvaSpec, FCR-7UV-400-2-ME) equipped with a cosinus 19

corrector. The intensity value was 1370 µE/h for the screening test in water-IPA mixture and 20

1550 µE/h for the methanol PHER test. Irradiance spectrum is provided in the Supplementary 21

Information (SI), Fig. S1. The photonic efficiency (PE) has been calculated as hydrogen 22

production rate divided by this photonic intensity, following IUPAC recommendations [29].

23

Because of the uncertainty on the amount of hydrogen produced and on the incident amount 24

of photons determination, the error on the PE was estimated to be close to 10%. As the PE 25

depends on the slurry concentration, reference curve of normalized PHER rate as a function of 26

catalyst mass (slurry concentration) was measured (Fig. S2). This curve was applied to 27

compare PHER rates measure in this work with literature data.

28 29

2.4. Electrochemical measurements 30

To prepare the electrodes, 5 mg of a solid were dispersed by ultrasound in a solvent 31

containing 800 µl of ethanol and 400 µl of 0.5% Nafion solution, optionally containing 1 mg 32

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6 of acetylene black carbon. Then, 10 µl of suspension was dropped onto rotating glassy carbon 1

electrode (0.0706 cm2) and then dried in argon. The catalyst loading was 0.65 mg/cm2. The 2

electrochemical measurements were performed on a Voltalab three-electrode potentiostat 3

using a Pt counter electrode and SCE reference electrode at 25 °C in purged solutions of 4

0.1 M H2SO4, by bubbling argon. Cyclic voltammograms were obtained in the potential range 5

from 0.5 to −0.1 V vs. SCE at scan rates ranging from 20 to 200 mV s−1. Linear Sweep 6

Voltammetry (LSV) scans were carried out at 2 mV/s rate.

7 8

2.5. Thiophene hydrodesulfurization (HDS).

9

Catalytic activity in thiophene HDS (Scheme 1) was measured at atmospheric pressure in a 10

fixed-bed flow microreactor. Prior to catalytic tests, all samples were re-activated under the 11

standard conditions by means of treatment under a flow of 10% H2S/H2 at 350°C, for 2h.

12

13

Scheme 1. Thiophene HDS pathways 14

Reaction was carried out in the temperature range 280–340 °C, under 50 ml/min gas flow, 15

using 100–200 mg of catalyst and partial pressure of thiophene 2.7 kPa. The plug-flow reactor 16

model was used to calculate the specific reaction rate, Vs, according to the equation 17

Vs = − (F/m)ln(1 − x) 18

where F is thiophene molar flow (mol/s), m is the catalyst mass (g), and x is thiophene 19

conversion. Catalytic activity was estimated at steady state conversion, after at least 16 h on- 20

stream.

21

22

3. Results and discussion 23

S

S

HYD

DDS

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7 3.1. Synthesis and characterizations of solid materials (TEM, XRD, TPR)

1

The primary goal in this work was to study the PHER activity for a series of titania-supported 2

sulfides obtained with the same preparation technique, as a function of the nature of transition 3

metal (TM) sulfide. First, the composition and the morphology of sulfides deposited with this 4

technique were investigated. To this aim, the samples of supported catalysts and/or the 5

corresponding reference bulk sulfides have been characterized using elemental analysis, 6

TEM, XRD, XPS and TPR.

7

The set of available sulfides is limited by the possibilities of the preparation technique.

8

Stability of TM sulfides vs. the corresponding oxides increases from the left to the right of the 9

periodic table. Sulfides of oxophilic early TM (Ti, Nb or Zr) could not be precipitated using 10

aqueous thioacetamide reaction. We studied the reactions of 3d metals from Mn to Zn.

11

Additionally we tried several 4d and 5d TMs (Mo, W, Ru, Pt, Ag, Hg).

12

Thioacetamide has been widely used as sulfur source for synthetic and analytic purposes. In 13

various conditions, reaction of metals precursors with thioacetamide has been applied to 14

prepare sulfides of Mo [30], Co and Ni [31], Cd [32], Sn [33] and other metals. Here we use 15

uniform aqueous reflux synthesis conditions. Already by visual observation we could identify 16

the cases where TM sulfides were probably not formed. An inspection of the color change 17

after the reaction suggested that for Mn, Fe, W and Pt the corresponding (yellow or dark 18

brown) sulfides were not formed, but the reactants probably remained in the oxide form.

19

Platinum-containing product remained yellow as is the parent hexachloroplatinate. Zinc 20

nitrate if put into the reaction with thioacetamide does not give any precipitate under the 21

conditions applied (though ZnS could be prepared using thioacetamide in different conditions, 22

[34]). Therefore, W, Pt, Mn, Fe and Zn- containing solids were discarded. From twelve metals 23

precursors initially tried, seven sulfides were obtained and retained for further 24

characterizations and catalytic tests. The TM sulfides for which the thioacetamide technique 25

failed could be prepared using different methods, such as hydrothermal or microwave 26

assisted, but in this work we follow a uniform preparation protocol.

27

Chemical analysis of the solids after reaction shows quantitative deposition of the transition 28

metals species onto titania (Table S1). For four metals, the chemical form of supported 29

species might be inferred from the XRD of the reaction products of individual precursors.

30

Indeed, Ag2S, CuS, NiS2 and HgS crystalline sulfides are formed upon reflux (Fig. 1-4). Other 31

three sulfides (Mo, Ru, Co) form sulfur-rich amorphous precipitates with no crystalline 32

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8 phases detectable by XRD. Secondary reaction of slow oxidation of thioacetamide upon 1

reflux leads to the formation of crystalline sulfur impurities in CoSx, MoSx and RuSx (Fig. 5).

2

As discussed in [26], molybdenum precipitates as amorphous MoSx phase with composition 3

close to MoS3. Ruthenium and cobalt give dark XRD-amorphous precipitates but due to 4

considerable sulfur impurity the exact composition of amorphous metal sulfides is unclear.

5

6

Figure 1. XRD pattern of bulk AgSx (black) and the matching pattern of β-Ag2S (PDF 01- 7

080-5476) (blue).

8

9

Figure 2: XRD pattern of bulk CuSx (black) and the matching pattern of CuS (PDF 00-006- 10

0464) (blue).

11

10 20 30 40 50 60 70 80

(-104)

(-210) (-104)

(210) (133)

(102) (013) (-122) (-113)

(111)

(-102) & (110)(-111)

angle (2θ)

(211) & (220)

(-114) & (122)

(-202)(031)

(022)

(120)(-121)

(100) (-112)(012)

AgSx

β−Ag2S: PDF 01-080-5476

10 20 30 40 50 60 70 80

(006)

CuSx

CuS: PDF 00-006-0464

angle (2θ)

(108) (116) (213)

(105) (208)

(103) (1011)

(100) (110)

(002) (101) (102)

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9 1

Figure3: XRD pattern of bulk NiSx (black) and the matching pattern of NiS2 (PDF 04-003- 2

1992) (blue); elemental orthorhombic sulfur (04-012-7311) is also observed.

3 4

5

Figure 4. XRD pattern of bulk HgSx (black) and the matching pattern of HgS (PDF 04-002- 6

6787) (blue).

7

8

10 20 30 40 50 60 70 80

(313)

(026)(222)

(113)

NiSx

NiS2: PDF 04-003-1992 S: PDF 04-012-7311

(311)

(220)

angle (2θ)

(331)

(210) (211)

(111) (200) (222) (023) (321)

10 20 30 40 50 60 70 80

(111) (113) (202) & (015)(021)(104)(110) (114) & (203)

angle (2θ) HgSx

HgS: PDF 04-002-6787

(116)(122) & (205)

(006)

(103)

(012)

(101)(100) (211)(024)

(003)

0 10 20 30 40 50 60 70 80

CoSx RuSx MoSx

angle (2θ)

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10 Figure 5. XRD patterns of CoSx, RuSx and MoSx amorphous phases. Narrow peaks 1

correspond to the common impurity of elemental rhombohedral sulfur (00-024-1206) and 2

elemental monoclinic sulfure (04-007-3019) only observed for CoSx. 3

4

Fig. 6 depicts TEM images of the supported sulfide catalysts under study. TEM reveals that 5

sulfides dispersion varies depending on its nature. For Ag and Ni, 100 nm - range particles of 6

Ag2S and NiS2 were observed, so the dispersion is rather poor. Hg and Mo give relatively 7

well-dispersed 10 nm - range particles. MoSx amorphous phase is fragile and rapidly 8

transforms under the electron beam into the MoS2 fringes. For the supported Co and Cu 9

sulfides, we could not identify the sulfide species by means of HREM and STEM. The TM 10

species are ultradispersed, of subnanometer size and are homogeneously smeared over the 11

titania, as attested by the EDS scans. For both cobalt and copper (Cu sample is shown in Fig.

12

S3) only titania grains were observed. Similarly, ruthenium sulfide while detected by EDS 13

forms highly dispersed sulfide species not detectable by HREM (Fig. S4). However, due to 14

the relatively high mass of Ru, STEM contrast was sufficient to detect 1-1.5 nm size clusters 15

of RuSx (Fig. 6).

16

Additional characterization has been carried out using temperature programmed reduction 17

(TPR), in which we detected hydrogen sulfide released upon linear heating of the samples up 18

to 1050°C (Fig. S5-S11). TPR study allows correlating the amount of sulfur released and the 19

temperature of TPR peaks with the chemical nature of sulfide species. In particular the TPR 20

characterization is important to give evidence of the sulfides formation in the case of 21

amorphous species, not detectable by TEM.

22

For the metals that form large sulfide particles (Ag, Ni), TPR of supported catalysts gives the 23

main reduction peaks in the same temperature range as for the corresponding bulk sulfides 24

(Fig. S5, S6). The shape of the ascending part in the high temperature TPR curve region is 25

related to the sulfide formation enthalpy, and therefore is specific for the corresponding metal 26

sulfide phase, as discussed earlier [35]. Beside the sulfide core reduction, additional peaks are 27

observed at low temperatures due to the weakly bonded sulfur species located at the surface of 28

TiO2 and/or at the surface of sulfide particles. The higher is sulfide dispersion, the higher is 29

the area of low-temperature peak. For highly dispersed supported species TPR proves the 30

presence of sulfides not detectable by TEM (Cu, Co, Fig. S7, S8). Beside the low-temperature 31

peaks, TPR attests formation of transition metal sulfides due to systematic presence of 32

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11 relatively high temperature feature, related to the core reduction (Fig. S8, Fig. S9). Thus, 1

supported ruthenium sulfide TPR shows a large pic of weakly bonded sulfur at low 2

temperature but also the high temperature core reduction peak, which attests the presence of 3

RuS2 particles, having size of the order of 1 nm (Fig. S9).

4

The presence of RuSx clusters (x≈2) was also confirmed by XPS measurement, as shown in 5

Fig. S12. Ru 3d, Ru 3p and S 2p signals were analyzed for supported and bulk RuSx. The Ru 6

3p and Ti 2p signals overlap, which makes the interpretation difficult. The state at 279.9 eV 7

(Fig. S12 C) can be either metallic Ru or its sulfide [36,37]. A second state, probably an 8

oxide, is also observed in low surface concentration. The contribution located at 161.9 eV 9

(Fig. S12 D) is attributable to pyrite type sulfur (S-S)2-. It confirms that RuSx is deposited at 10

the surface of TiO2. The molar ratio / Ru was found close to 1.4 for the supported 11

sulfides. We wanted to study sulfides-based material in realistic conditions, as it is present in 12

the catalytic tests. Therefore, no particular precaution was taken to load the photoreactor 13

without air exposure. It explains why some sulfate is observed by XPS (167 eV, Fig. S12 B 14

and D) [38].

15

Finally, BET surface areas of the supported catalysts are high and remain similar to that of 16

bare titania (350 m2/g) and are all greater than 300 m2/g. For example specific surface area is 17

of 321 m2/g for MoSx/TiO2 and 328 m2/g for CoSx/TiO2. The morphology of supported 18

catalysts is dominated by TiO2 support because the TM sulfides loadings are relatively small, 19

whereas no thermal treatments were involved during preparation, which could lead to TiO2 20

sintering.

21

Overall, for seven metals under study, sulfide species deposited on the PC500 anatase TiO2 22

were prepared by thioacetamide method. However the crystallinity and the dispersion of the 23

sulfides as obtained are different.

24 25

3.2. Photocatalytic HER activity 26

The two studied reactions are:

27

- CH3OH HCHO + H2 (1)

28

- CH3CHOHCH3 CH3COCH3 + H2 (2) 29

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12 The initial values of PHER activity were compared after several hours of test, in order to 1

characterize the intrinsic ability of TM sulfides to co-catalyze the reactions (1, 2). In all cases, 2

a short induction period (15-20 min) was observed. Then, for the duration of the experiment 3

(3-6 hours) the PHER rate was stable.

4

The PHER rate evolution was also checked on a longer time scale. We studied stability for 5

several days on-stream for the semi-continuous flow IPA test, or for several repetitive runs for 6

the batch methanol test (in the last case - with refreshing the methanol and carrying out purge 7

with argon between the runs). In the water-IPA test we measured PHER rate at the 8

temperatures stepwisely changed between 10 and 45 °C, in order to determine the apparent 9

activation energy (which is beyond the scope of the present work and will be discussed 10

elsewhere).

11

After the initial stabilization period, during several hours on-stream in isothermal conditions 12

the relative variations of PHER rate were less than 5%; an apparent steady state was achieved.

13

However the PHER rates slowly evolved on the several-days scale for the continuous flow 14

test (Fig. S13, S14). In most cases (Co, Cu, Hg, Mo, Ni, Ru) slow activation occurred, 15

probably due to the cleaning of TiO2 surface from the residuals of thioacetamide used in the 16

preparation. In the case of Ag2S slow deactivation occurs, which might be attributed to photo 17

corrosion. The steady state rate measured at 20 °C in the first or in the second temperature 18

cycle was taken to compare the PHER activity (Fig. S13). Batch PHER test in the methanol 19

medium provides good stability for several (4-5) repetitive 3h runs (Fig. S15). In bothcases, 20

the variations of activity with time are lesser than the differences between various TM 21

sulfides and do not influence the conclusions of this work.

22

Post-mortem XPS analysis of the solids after water-IPA tests showed that both metal species 23

and sulfur species are partially transformed to the higher oxidation states (Fig. S16). In 24

agreement with the PHER test results, the most important degree of corrosion was observed 25

for Ag2S/TiO2 sample. After 70 hours of test, surface layers were tatally transformed to 26

sulfate. Note that the stability study was not in the focus of this work, because we are 27

interested in the understanding of titania combined with fresh sulfides.

28

The PHER photon efficiency measured in pure methanol and water-IPA 50/50 vol. mixture is 29

presented in Fig. 7. The absolute and mass - specific PHER rates are given in Table S2. For 30

the water–IPA mixture, the performance changes in the sequence Ru > Ni > Co > Hg > Ag>

31

Mo > Cu. In methanol the sequence is Co > Ni > Ru = Mo = Cu > Ag > Hg. In methanol even 32

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13 the least active HgS/TiO2 produced 5 times more hydrogen than bare TiO2. In IPA the PHER 1

activity of the least active CuS/TiO2 was 12 times higher than of bare titania which undergone 2

the thioacetamide reflux procedure.

3

The photocatalytic properties of HgS, Ag2S and RuSx supported on TiO2 are reported for the 4

first time. Moreover, no transition metal sulfides-based photocatalysts were studied 5

previously for IPA dehydrogenation. Therefore no literature references exist for these cases.

6

In methanol, the PHER performance of our most active catalysts (Co and Ru sulfides) is at the 7

level of the best sulfide catalysts reported in the literature (Table S2). As far as comparison is 8

possible, our absolute PHER values are lower than the literature values for copper and nickel 9

sulfides [14,39]. Our values for molybdenum sulfide are lower than for amorphous MoSx

10

reported in [10] but higher than observed earlier for the MoS2 nanosheets [40]. However if 11

approximately re-calculated for the same conditions (lamp power and slurry concentration, 12

Table S2, Fig. S2), the best values reported in the literature for Co, Cu and Mo sulfides are in 13

a remarkable agreement with our data (Table S2). Finally, our values measured in methanol 14

for cobalt and nickel co-catalysts are higher than observed in ethanol for CoSx and in lactic 15

acid for NiS, but since the organic molecules are not the same, such comparison makes lesser 16

sense [39,40,16,41].

17

Comparison with the existing literature is only approximate as the conditions applied from 18

one study to another are never the same and recommendations for reporting the activities 19

[42,43] are not always followed. Hence a more reliable activity assessment might be achieved 20

by comparison with a well-known Pt/TiO2 benchmark reference (Table S2). The overall 21

activity in methanol is much higher than in water-IPA, showing the importance of organic 22

substrate for this type of studies. In methanol, the best cobalt sulfide promoted catalyst shows 23

approximately 30 % PHER rate of the 1% Pt/TiO2 reference (Table S2). In water-IPA the 24

relative activity of TM sulfides attains, in the best case of RuSx, only 16 % of activity of the 25

Pt/TiO2 reference. The observed PHER activity changes depending on the alcohol, in 26

agreement with previous works [44]. With metal supported on TiO2 the activity is often 27

higher in methanol than in IPA [45,46].

28

The observed PHER trends show both expected and unexplained features. The best catalysts 29

in methanol and water-IPA media are, respectively, Co and Ru sulfides, which are known as 30

active hydrogen production catalysts [47,48]. On the other hand, MoSx, which is by far the 31

most studied sulfide for PHER, is not among the best co-catalysts in both media. We closely 32

(15)

14 reproduce the PHER activity in methanol of MoSx/TiO2, observed in the previous work, which 1

used similar thioacetamide preparation [26]. However MoSx/TiO2 activity in methanol is 2

almost the same as for CuS/TiO2, which is not among the front-running PHER catalysts.

3

Moreover, MoSx/TiO2 shows poor performance in water-IPA, where it appears less active 4

than HgS/TiO2. Surprisingly, HgS is a reasonably good co-catalyst for PHER, 5

To understand the observed trends of PHER, various properties of the systems under study 6

were compared such as the morphology, the electrocatalytic HER activity and their thiophene 7

Hydrodesulfurization (HDS) activity. Deposition of sulfides at the surface of TiO2 does not 8

alter the light absorption properties, important for PHER. The observed color change is due to 9

light absorption by sulfides in visible region, which does not interfere with electron-hole 10

generation in titania. Indeed, Kubelka-Munk transforms of UV-vis spectra (Fig. S17) are 11

similar between 5.5 and 3.2 eV. The band gap (Eg) was determined as the intersection 12

between the x-axis in the Tauc plots. The Eg for seven samples under study is included within 13

the region between 3.2 and 3.35 eV. The Eg of seven catalysts and pure PC500 titania is the 14

same within the accuracy of the experimental method and corresponds to the literature value 15

for PC500 anatase [49]. Therefore the amount of (useful) photons absorbed by the samples is 16

similar, so other properties are responsible for the differences of observed PHER activity.

17

The dispersion degree of the co-catalyst species seems to be less important than the nature of 18

the TM sulfide. Indeed, two most active co-catalysts in the methanol medium are CoSx and 19

NiS2. However, CoSx species are too finely dispersed to be observed by conventional TEM, 20

whereas the NiS2 particles are large (near 100 nm). On the other hand, poorly dispersed Ag2S 21

shows better activity in water-IPA than well - dispersed MoSx. We already noted in the 22

previous works that for PHER in methanol, the dispersion of sulfide co-catalyst on titania 23

does not seem to be a crucial parameter [26].

24

We are compelled to conclude that the differences of PHER rates are related to the intrinsic 25

properties of sulfides deposited onto titania. The property of a co-catalyst obviously relevant 26

to the PHER performance should be its ability to reversibly activate hydrogen. This ability is 27

revealed in the heterogeneous catalysis or in the electrochemical HER. Seven TM sulfides 28

considered here are known to possess very different ability to activate hydrogen and to 29

catalyze hydrogenation or hydrogenolysis of organic substrates. Ru and Mo sulfides are well- 30

known highly active hydrogenating catalysts [36,38,50]. Co and Ni are used as promoters in 31

sulfide heterogeneous catalysts but the activity of Co and Ni binary sulfides is low, though 32

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15 non-negligible. Finally, CuS, HgS and Ag2S have never been shown to act as hydrogen 1

activators or hydrogenating heterogeneous catalysts. To check in what extent the hydrogen 2

activation ability of TM sulfides is important, we compare the trends in HDS and in the 3

electrochemical HER with the observed PHER trend. The corresponding literature data are 4

dispersed; the preparation techniques and the reaction conditions are very different from one 5

work to another. To provide a reliable series of activity, we measured the electrochemical 6

HER performances and HDS activity for the catalysts studied above in PHER, as follows.

7

8

Figure 6 TEM and STEM HAADF images of selected solids. The transition metals forming co- 9

catalyst sulfides are indicated on the images. White spots in the STEM images correspond to the 10

TM sulfides particles.

11

(17)

16 0

1 2 3 4

CuS MoSx Ag2S HgS CoSx NiS2 RuS2

Photon Efficiency (%) isopropanol - water methanol

1

Figure 7. PHER activity of titania-deposited sulfides in methanol and in water-IPA mixture.

2 3

3.3. Electrocatalytic HER and thiophene HDS activity 4

PHER via alcohols dehydrogenation certainly follows a complex mechanism. To get a better 5

insight, we used model HER and HDS reactions, in order to disentangle the intrinsic 6

hydrogen-activating properties of TM sulfides from their influence on the titania 7

semiconductor. HER and thiophene HDS reactions include respectively the H-H bond 8

formation and breaking on the sulfide surface. These properties are correlated, because of the 9

microreversibility principle. So HDS and HER both estimate the ability of a catalyst to 10

activate H2 and as such they mimic the last PHER step, where molecular H2 is formed.

11

However, these reactions occur under different conditions and may involve different species.

12

Thus, HER proceeds with a participation of hydrated protons, whereas HDS obviously cannot 13

involve such species.

14

TM sulfides and in particular MoS2 recently emerged as HER electro catalysts with high 15

activity and good stability in acidic medium [51]. The HER performance of sulfides strongly 16

depends on the nature of TM metal and on the preparation technique. To understand how the 17

nature of TM sulfides obtained by thioacetamide technique impacts its electrochemical HER 18

performance, we compared the initial activities of seven sulfides as prepared. Such initial 19

HER activities are provided by steady–state characteristics which are achieved after several 20

LSV cycles. Since pure titania is inactive, the electrocatalytic properties of diluted sulfides 21

species supported on inert PC500 are difficult to measure. By this reason we proceeded with 22

(18)

17 the HER measurements for bulk TM sulfides obtained from the thioacetamide reaction. Here 1

we assume that similar TM sulfide species are formed with and without TiO2 and they have 2

similar electrochemical properties.

3

The Tafel plots and LSV curves are presented in Fig 8a, b. The numeric values of Tafel slopes 4

and η10 are summarized in Table 1. Low Tafel slope and low values of η10 (overpotential 5

necessary to attain the 10 mA/cm2 current) are characteristics of high HER performance. The 6

overall ranking of sulfides HER performance as a function of metal is Mo > Ru ≈ Ag > Cu >

7

Co > Ni > Hg. Worth emphasizing that we do not claim this ranking to be a general trend, 8

transposable to any sulfides of these metals, but merely a particular sequence for the materials 9

prepared using thioacetamide method.

10

The specific rate of thiophene HDS reaction (Scheme 1) could be considered as another 11

descriptor of hydrogen-activation and hydrogenating activity. With the exception of Ag, we 12

see that highly hydrogenating sulfides (Ru, Mo) demonstrate the highest HER activity and 13

overall correlation between the electrocatalytic HER and HDS performances is good (Table 14

1). The activities per mole of sulfided metal of Cu, Co and Ni sulfides are usually found to be 15

low, whereas the activities of Ru and Mo sulfides are high. This is true for both hydrogenation 16

and HDS reactions [52] and for binary [53] or ternary sulfides including these elements [54].

17

Silver sulfide Ag2S was recently studied as HER electrocatalyst and shown moderate but non- 18

negligible performance [55]. However, its HDS activity appeared negligible, probably 19

because relatively harsh HDS conditions modify the initial sulfide. Finally, mercury sulfide 20

HgS was never studied in HDS/HER and here we attest its zero HDS activity as well as poor 21

electrochemical performance.

22

Confronting the results of photocatalytic HER, electrocatalytic HER and thiophene HDS, we 23

see that if the two latter activities are well correlated, there is no clear relationship between 24

any of them and observed PHER. Therefore, photocatalytic performance depends more 25

strongly on other parameters influenced by the co-catalysts (charges separation, lifetimes etc.) 26

than by their hydrogen-activating ability.

27

(19)

18

-600 -500 -400 -300 -200 -100

-0,8 -0,3 0,2

Overmpotential vs. RHE (mV)

Log J (mA/cm2) HgS 209

NiS2240 CuS 134 CoSx 170

MoSx87 RuSx124

Ag2S 127

(a)

-20 -16 -12 -8 -4 0

-600 -400 -200 0

J (mA/cm2)

Overmpotential vs. RHE (mV) HgS

CoSx

Ag2S RuSx NiS2

CuS

MoSx

(b)

1

Figure 8. Electrochemical HER activity of TM sulfides: Tafel plots (a) and LSV curves (b).

2

Table 1 Overall performance in the PHER, thiophene HDS and electrochemical HER.

3

property\sulfide Ag2S CoSx CuS HgS MoSx NiS2 RuS2

Thiophene HDSa 0.1 2.1 0.3 0.0 16 0.5 91

Electro HER Tafel b 127 170 134 209 87 240 124

Electro HER η10c 460 670f 580 910f 433 770f 445 Photo HER, methanold 1.50 4.25 2.50 0.50 2.45 4.00 2.70 Photo HER, IPA-H2Oe 0.30 0.40 0.01 0.35 0.10 0.50 1.90

a reaction rate,10-8 mol.g-1.s-1 measured at 300 °C (per gram of metal sulfide); b mV/decade; c 4

-mV; d,e photon efficiency, %; f extrapolation.

5

3.4. Mechanisctic considerations 6

The observed HDS and HER trends have many common points, which could be expected. In 7

the most general case, the overall (HER, HDS) performance of a sulfide material is a product 8

of two terms. The first term is the intrinsic chemical performance and the second is 9

morphology –related term describing the availability of a sulfide surface to the reactants.

10

Beside these factors, the electric conductivity of sulfide plays an important role for the 11

electrochemical HER, though in some extent it is leveled off by applying conductor binders 12

(usually Nafion and carbon). While morphology of sulfides can be extremely versatile 13

depending on the preparation ways, the intrinsic chemical trends are relatively well 14

understood on the basis of generalized Sabatier principle [56–58].The energies of S - vacancy 15

creation and those of hydrogen dissociative adsorption and desorption govern both the HDS 16

and HER trends. Thus, M-S bond energy and hydrogen adsorption energy are recognized to 17

be useful descriptors for HDS activity. So-called volcano plots allow predicting which 18

sulfides could be potentially active HDS (HER) catalysts [59,60].

19

(20)

19 With this respect Mo and Ru sulfides have the M-S bond energies are close to the optimal 1

value [60], whereas Ag2S and HgS have it too weak (∆Hf0 values are −31.8 and −58.2.

2

KJ/mol , respectively [61]. The observed HDS trend is therefore in agreement with the 3

existing volcano plots.

4

The HDS and HER properties are probably related to the electronic band structures of the 5

corresponding sulfides via the M-S bond energy. However there are neither clear rules for 6

such relationship, nor any features of the band structure could be potential descriptors for the 7

HDS and/or HER activity. The HDS and HER rates for the sulfides having similar electronic 8

bands vary by many orders or magnitude. Thus, semiconducting sulfides with Eg between 1 9

and 2 eV can be both highly active (MoS2, RuS2) and very poor (HgS) HDS catalysts.

10

On the other hand the PHER rate sequence vs. the nature of sulfide and its dispersion has 11

much lesser variations. All tested sulfides induce a significant increase of the PHER rate on 12

titania, even if the ranking is not the same for two alcohols. This observation suggests that the 13

action of different sulfides might be explained on a common basis. For PHER, not the 14

hydrogen-activating power but the electronic structure of transition metal sulfide is the most 15

important property.

16

Consideration of relative positions of electronic bands shows that similar alignment between 17

TiO2 and all sulfides should occur. The electron affinity of all sulfides under study is higher 18

than for titania. The Fermi levels are slightly higher than Fermi level of TiO2. Position of VB 19

slightly varies from one sulfide to another, but in all cases the top of VB is due to the states 20

dominated by S 3p electrons. After the band alignment the bottom of CB for semiconductor 21

sulfides (Ef for metallic sulfides) will be always below the bottom of CB for TiO2 (Scheme 2).

22

23

Scheme 2. Relative bands positions of titania and seven sulfides studied in this work; values 24

adopted from [62].

25

(21)

20 Therefore the photo generated electrons from the bottom CB of titania (or shallow trapped 1

electrons) wouldtransferred to the sulfides CB. That means, photo generated electrons will be 2

attracted towards the interface between sulfide and TiO2. If a sulfide possess strong hydrogen 3

- activating power then the overall PHER rate might be additionally increased due to the 4

catalytic action of sulfide surface (similarly to the well-known Pt/TiO2 reference case).

5

However, even if the sulfide possesses no hydrogen-activating properties at all, the PHER rate 6

is still higher than for bare titania, due to an enhance charge carrier separation. In that case, 7

TiO2 is the active site for both oxidation and reduction half reactions.

8

The second important finding to be explained is that the dispersion of TM sulfide particles 9

does not play a crucial role. We suppose that due to polarization of TiO2 agglomerate by 10

adjacent sulfide particle, the photo generated electrons which have high mobility and 11

relatively long lifetime, might be collected towards the interface between TiO2 and sulfide via 12

an antenna-like mechanism [63], as depicted in Scheme 3.

13

14

Scheme 3 Harvesting of photo generated electrons from distant regions of a TiO2 agglomerate by 15

a TM sulfide particle.

16

Finally there are two distinct groups of co-catalysts with respect to their relative activity in 17

water-IPA and in methanol media. In the first group, water-IPA and methanol tests give the 18

PHER rates ratio close to 1. This group includes Ru, Hg sulfides and Pt metal co-catalysts 19

(Table S2). For the second group including five of seven tested sulfides (Co, Cu, Mo, Ag and 20

Ni), the PHER rate in methanol is at least an order of magnitude greater than in water-IPA.

21

Both groups include relatively poor and highly active catalysts in PHER as well as in HER 22

and HDS. Both groups include relatively poorly dispersed and highly dispersed sulfides. No 23

(22)

21 property descriptor correlated with this activity difference could be identified for the time 1

being. However such a striking difference of behavior suggests that some fundamental 2

mechanistic difference exists between two types of co-catalysts, though it remains yet 3

unexplained.

4

4. Conclusions 5

In this work we prepared a series of transition metals sulfides on PC500 titania using 6

thioacetamide solution reaction. The properties of obtained catalysts were compared in PHER 7

in methanol and water-isopropanol media, as well as electrocatalytic HER in 0.5 M H2SO4 8

and heterogeneous gas-phase thiophene HDS reaction. The following conclusions can be 9

drawn from our work.

10

(i) Several transition metals sulfides of the first and the second raw show high PHER activity 11

in the methanol and water-isopropanol media, superior to that of frequently studied MoS2. 12

(ii) Commonly known hydrogen-activating sulfides (Ru, Co, Ni) show the best photocatalytic 13

HER performance. However, other metals sulfides such as Hg or Cu have a poor activity for 14

HDS but show a PE many times higher than bare titania. Similarly, the trends established for 15

the seven sulfides differ in photocatalytic and electrocatalytic HER. Therefore proton 16

reduction or hydrogen activation by the co-catalyst, albeit favorable, is not a critical parameter 17

in the PHER.

18

(iii) Dispersion of the sulfide species has no determining effect on the PHER performance.

19

Porly dispersed NiS2 and highly dispersed CoSx species show comparable high PHER 20

activity. In agreement with previous observations, sulfide particles, even moderately 21

dispersed, can efficiently harvest electrons from extended areas of adjacent titania.

22

(iv) The observed PHER rates strongly depend on both the nature of sulfide and that of the 23

organic substrate. However, this observation does not allow concluding on which step in the 24

multistep PHER scheme is rate limiting, because the organic molecule might interfere with 25

both electron and hole evolution. In order to understand this issue, integrated models should 26

be developed with rate equation including all the essential steps of the process. A better 27

insight can be obtained further measuring apparent activation energy of the process.

28

Supplementary data 29

(23)

22 Supplementary material is available including experimental conditions, samples

1

compositions, photocatalytic results, EDS analyses,TPR patterns, XPS spectra and UV-Vis 2

absorption spectra.

3

(24)

23 References

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