SEMICONDUCTORS AS CATALYSTS FOR WATER SPLITTING. Chandramathy Surendran Praveen. Materials Research Laboratory UNIVERSITY OF NOVA GORICA

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SEMICONDUCTORS AS CATALYSTS FOR WATER SPLITTING Chandramathy Surendran Praveen Materials Research Laboratory UNIVERSITY OF NOVA GORICA

OUTLINE Introduction and history of the discovery of semiconductor photocatalysts Photocatalytic water splitting Semiconductors as photocatalysts and their properties Electrochemistry of semiconductors Photo electrochemical system Photocatalytic particles in suspension Enhancement of photocatalytic activity of semiconductors Summary

INTRODUCTION Hydrogen is the cleanest, sustainable and renewable energy carrier as well as an essential raw material in many chemical industries Mainly produced by steam reforming the hydro- carbons. If one consider the energy and the environmental issues, it must be produced from water using renewable energy sources such as solar light Photocatalytic water splitting is one of the candidates for solar hydrogen production

History of the discovery of Photocatalytic materials 1971 Dr. Akira Fujishima Dr. Kenichi Honda

Photocatalysis Photocatalysis catalyst reaction assisted by photons PHOTOCATALYSIS A conventional redox reaction The redox couple: both oxidation and reduction simultaneously Application to the improvement of living environment such as anti- stain, self cleaning, super hydrophylicity properties Light energy conversion as represented by water splitting TiO 2 based photocatalysts are widely used Perfect catalyst is still challenging

WATER SPLITTING Using standard conditions water can reversibly electrolyze at a potential of 1.23 ev, a value derived from the relationship The overall reaction G nf. E 0 0 1 H O h H O 2 Endothermic reaction 2 2 2 A two electron process with a Gibbs free energy change of 2.46eV -So electrochemical decomposition of water is possible when the cell emf is greater than or equal to 1.23eV

Concepts -why semiconductors are chosen as photocatalysts? For conventional redox reaction one is interested in either reduction or oxidation But for water splitting, both the reactions should be carried out simultaneously Reduction of hydrogen ions 2H 2e H 2 Oxygen evolution from hydroxyl ions 1 2OH 2h H O O 2 2 2 Band gap is important.

. Metals: No band gap, Only reduction or oxidation, Depends on the band position Insulators: High band gap So high energy is required to create the appropriate excitons for promoting both of the reactions. CB H + /H 2 CB CB VB Metals H 2 O/O 2 VB SC VB Insulators E Semiconductor is the best selection

OVERALL WATER SPLITTING V/NHE CB e - Active sites H + 0 +1.0 H + /H 2 1.23 V band gap H 2 O O 2 /H 2 O H 2 h O2 +2.0 VB h + H 2 O +3.0 h H 2 O H 2 +1/2O 2.

General properties of semiconductors Chemical properties - Semiconductors with high ionicity are stable against corrosion and passivation Optical properties- Threshold behavior is extremely important in photo electrochemistry Materials with band gap 1.1-1.7 ev are the best absorbers for solar energy conversion devices Visible light absorption is the most desirable property Ref: C H Henry, J. Appl. Phys.,51, 4494 (1980) : W. Shockley and H J Queisser, J. Appl.Phys., 32, 510 (1981)

Depth of light absorption in semiconductors Absorbance and transmittance of a material is given by Beer s law A l ln I I 0 T I exp( l) I l-optical path length I, I 0 transmitted and incident light intensity. α- absorption coefficient 0 Direct band gap semiconductors have large absorption coefficient (10 4-10 5 cm -1 ) A( h E ) m g h Here m is a constant which depends on the optical transition, m=2 for an indirect band gap semi conductor and ½ for a direct band gap semi conductor.

Carrier statistics Intrinsic carrier concentration in semiconductors is low Doping np i i Eg exp( ) kt increases the conductivity and able to control other electronic properties Crystal defects can also behaves as dopants Conductivity can be controlled by doping qn qp n Fermilevel Analogy to the Nernst equations-fermi level of a semiconductor phase p E E kt ln( n / N ) F Fi C E E kt ln( p / N ) F Fi V By doping electrical conductivity and Fermi level can be controlled!!

PRINCIPLE OF WATER SPLITTING ON SEMICONDUCTOR PHOTOCATALYSIS CB e- 0 V H / H 2 VB h+ +1.23V O / H O 2 2 Processes for photocatalytic reaction in electrode system Processes for photocatalytic reaction in powdered system

ELECTROCHEMISTRY OF SEMICONDUCTORS E C E F Band bending!!! + + + + + + + + E V - - - - - - - - E redox Concept of space charge region Electrochemical potential difference - charge movement n- type semiconductor upward bending of the band Metal oxide 1 Vfb E0 E 2 Mulliken electronegativity E 0 G free energy of electron in H 2 redox scale Flat band potential- no band bending For highly doped semiconductors, this equals the bottom of the conduction band Flat band potential must exceed the proton reduction potential 0.0 V at ph=0 and -0.41 t ph=7

Magnitude and direction of the band bending, varies with the applied potential Space charge region accumulation. E C EF E C E F E C EF EV E V EV semiconductorelectrode solution E > E fb E = E fb E < E fb Effect of varying the applied potential (E) on the band edges in the interior of an n type semiconductor

Effect of varying the applied potential (E) on the band edges in the interior of a p- type semiconductor accumulation. Space charge region EC EC E C EV EF E V E F EV EF E > E fb E = E fb E < E fb

The charge transfer abilities of a semiconductor electrode depends on whether there is an accumulation or depletion layer. If there is an accumulation layer behaves as metallic electrode-since excess of majority charge carriers available for charge transfer. If there is a depletion layer - there are few charge carriers available and the electron transfer reaction occur slowly However if the electrode is exposed to radiation of sufficient energy electron hole pairs are produced If the process occurs within the interior of the semiconductor recombinationheat If it occur in the space charge region, the electric field in this region will cause the separation of the charge

SEMICONDUCTORS AS PHOTO ANODE IN THE PHOTO ELECTROCHEMICAL CELL(PEC) PRODUCTION OF HYDROGEN

Width of the depletion layer W depends on donor concentration and the applied potential N Donor concentration 1 1 2 2 2 0 r kt fb end e W V V The flat band potential relates to the ph as PZC 2.3RT Vfb Vfb ( PZC ph ) F D V PZC V fb Applied potential ph at the net absorbed charge is zero At room temperature V fb changes with -59 mv per unit of ph

- The overall solar to- hydrogen conversion efficiency of the device can be determined from the electrical characteristics of the device STH j( Vredox VB ) P light P light V B Incident light intensity (W/m 2 ) Photocurrent density A/m 2 VB Bias voltage Activity of catalyst - rate of evolved gas per catalyst amount Apparent quantum efficiency QE =2[H 2 ] /I

SUITABLE PHOTO ELECTRODE MATERIALS IN PEC Required criteria's! Sufficiently high (visible) light absorption High stability in dark and under illumination (no photo corrosion) Suitable band edge positions to enable the reduction/oxidation of water by the photo generated holes /electrons Efficient charge transport in the semiconductor Low over potentials for the reduction/oxidation reaction(high catalytic activity)

Light absorption The spectral region depends on the band gap of the semi conductor Minimum band gap- 1.23 ev +(Thermodynamic losses (~0.4 ev)+ Over potentials required to ensure the fast reaction kinetics (~0.3-0.4eV)) So at least 1.9 ev, which corresponds to a wavelength of 650 nm Below 400 nm the intensity of sunlight falls rapidly, imposing an upper limit ~3.1eV Hence the optimum value ofthe band gap should be somewhere between 1.9-3.1 ev, which is in the visible range of the solar spectra!!

Stability against photo corrosion Most important property which imits the usefulness of many photo active materials Many non oxide semiconductors ( Si, Ga As, GaP, etc) either dissolve or form a thin oxide film which prevents the electron transfer across the interface Almost all M-O photo anodes are thermodynamically unstable! Eg; TiO 2 and SnO 2 show excellent stability over a wide range of ph and applied potential ZnO always decomposes, Fe 2 O 3 shows an intermediate case (ph and oxygen stochiometry)

Percentage ionic character of some semiconductors Semiconductor M-O Percentage ionic character TiO 2 SrTiO 3 Fe 2 O 3 ZnO WO 3 CdS CdSe LaRhO 3 LaRuO 3 PbO ZnTe ZnAs ZnSe ZnS GaP CuSe BaTiO 3 MoS 2 FeTiO 3 KTaO 3 MnTiO 3 SnO 2 Bi 2 O 3 Ti-O Ti-O-Sr Fe-O Zn-O W-O Cd-S Cd-S La-O-Rh La-O-Ru Pb-O Zn-Te Zn-As Zn-Se Zn-S Ga-P Cu-Se Ba-O-Ti Mo-S Fe-O-Ti K-O-Ti Mn-O-Ti Sn-O Bi-O 59.5 68.5 47.3 55.5 57.5 17.6 16.5 53.0 53.5 26.5 5.0 6.8 18.4 19.5 3.5 10.0 70.8 4.3 53.5 72.7 59.0 42.2 39.6 Percentage ionic character ( A B) 4 (1 e ) 100 Most of these have bond character 50-60% and modulating them will only lead to increased ionic character!! 20-30% ionic character with suitable band positions are suggested. 2

Requirement of band positions Conduction and valence band edges should straddle the reduction and oxidation potential of water Specifically E C should be above E RED and E V should be below E OX

Charge transport The exciton life time is a very important criteria The hole transfer across the n type semi conductor-electrolyte interface Should be fast enough 1) to compete with photocorrosion 2) to avoid accumulation Catalytically active surface species can be added Usually metals or hole trapping agents

Photocatalytic particle in suspension Most straight forward approach towards solar water splitting Oxidation and reduction takes place at the surface of the same particle GC H 2 O 2 CGS ACTIVITY = [H 2 ] QE = 2 [H 2 ] / I - Efficiency - Definition of quantum yield Driving force to seperatre is ELECTRIC FIELD AT INTERFACE SC/L

To enhance the kinetics and to avoid recombination of H 2 and O 2 co catalysts can be used The presence of sacrificial electron donor or acceptor ensure the stoichiometric conception of electrons or holes All metal sulfides including CdS and ZnS undergo photo chemical decomposition in the absence of sacrificial electron donors

More aspects An increase in either the recombination lifetime or interfacial charge transfer rate constant is expected to result in higher efficiencies The overall QE for interfacial charge transfer is determined by two critical processes Competition between charge carrier recombination and trapping Picoseconds nanoseconds Competition between trapped carrier recombination and interfacial charge transfer Microseconds-milliseconds A. Millis and S. L. Hunte J. Photochem. Photobiol. A: Chem 180 (1997) 1

Enhancement of photocatalytic activity Loading of metals like Cu, Ag, Au, Ni, Pd, Rh and Pt over a variety of metal oxide semiconductors results efficient charge separation! Pt is well known as an excellent co catalyst for hydrogen evolution The addition of carbonated salts or other electron mediators enhance the hydrogen production by preventing backward reaction Mixed metals oxide semiconductors NiO over SrTiO 3 NiO(H 2 ), SrTiO 3 (O 2 ) RuO 2 over TiO 2-30 times bigger activity than TiO 2 alone But if the concentration of RuO 2 exceeds a limit- act as electron hole recombination centers!!! In the presence of co -catalysts such as NiO highly active niobates, titanates and tandalates are reported (NiO/NaTaO 3 )

Visible light activity There are methods by which photocatalysts can be fabricated, by which they respond in the visible light Valence band formation using elements other than oxygen [ BiVO 4, AgNbO 3,Ag 3 VO 4,Ca 2 Bi 2 O 4...] Ion doping Cation doping - transition metals( V, Cr, Fe, Mo, Ru, Os, Re, Rh, V, etc.) -rare earth metals doped ion create new (impurity ) energy levels. metal ion dopants act as electron or hole traps

Anion doping Doping of anions such as N, F, C, Si in metal oxides or mixed metal oxides can shift in photo response into the visible region little tendency to form recombination centers-remarkable thing Z-scheme construction Dual semiconductor system Dye-sensitization Dye molecules absorb light with the transfer of an electron from the ground state to excited state. The excited electron goes to the conduction band of an appropriate metal oxide

SUMMARY Optimum value of band gap is 1.9-3.1eV Band edges should straddle the oxidation and reduction potential of H 2 O Photocatalyst should be stable against photo corrosion Metal oxide semiconductors with moderate ionicity are suggested Life time of the excitons should be high Cocatalyst is needed in most of the cases