Spectroscopic Study of Local Interactions of Platinum in

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Spectroscopic Study of Local Interactions of Platinum in Small [Cex. Oy]Ptx ‾ Clusters Manisha

Spectroscopic Study of Local Interactions of Platinum in Small [Cex. Oy]Ptx ‾ Clusters Manisha Ray Prof. Caroline C. Jarrold group Department of Chemistry International Symposium on Molecular Spectroscopy June 20 -24, 2016, Champaign-Urbana, Illinois

Importance of Ceria (Ce. O 2) • Catalytic activity of ceria is directly related

Importance of Ceria (Ce. O 2) • Catalytic activity of ceria is directly related to the number of oxygen vacancies in the crystal • Cerium dioxide is a good ionic conductor • High Reducibility of Ce+4 state Importance of Pt-supported Ceria in Water-Gas-Shift Reaction coordinate Phys. Chem. Phys. , 2011, 13, 19393– 19400 2

Background Water-Gas-Shift Reaction mechanism in Pt-supported Ceria structures CO + H 2 O →

Background Water-Gas-Shift Reaction mechanism in Pt-supported Ceria structures CO + H 2 O → CO 2 + H 2 J. Am. Chem. Soc. 2012, 134, 8968− 8974 ACS Catal. 2014, 4, 2088− 2096 § Role of oxygen vacancy on ceria surface § What are the reaction intermediates form (e. g. , HCOO ˉ, CO 3ˉ, HCO 3 ˉ and HOCO ˉ)? § Is H 2 O dissociation a rate determining step ? 3

Bulk to Small Cerium Oxide Cluster Knowledge of the structure and composition of the

Bulk to Small Cerium Oxide Cluster Knowledge of the structure and composition of the active sites is crucial for understanding and optimizing the properties of catalysts Highlighted pyramidal Ce 3 O 4 unit in 111 surface Ce 2 O 2 structure • Small cerium oxide clusters exhibit structural features similar to the bulk • The purpose of studying model catalysts is to gain understanding that ultimately can lead to design. Phys. Chem. Phys. , 2011, 13, 19393– 19400 4

Experimental Apparatus TOF mass spectrometry combined with Anion Photoelectron Spectroscopy TOF Mass Spectrometer GENERAT

Experimental Apparatus TOF mass spectrometry combined with Anion Photoelectron Spectroscopy TOF Mass Spectrometer GENERAT Reactant E Carrier gas CLUSTER lines S Ablation laser hits metal target Electron detector ANION MASS SPEC PES interaction region PES Ion detector 5

Method Principle of Anion Photoelectron Spectroscopy and Significance of β parameter Spectra are collected

Method Principle of Anion Photoelectron Spectroscopy and Significance of β parameter Spectra are collected with the laser polarization perpendicular and parallel to the electron drift direction. Depending on orbital types, β varies as -1<β˂2 Selection Rule, 6

Mass Spectrum 194 Pt. O 194 Pt 2 O Ce 3 O 2 Ce

Mass Spectrum 194 Pt. O 194 Pt 2 O Ce 3 O 2 Ce 3 O 3 Ce 2194 Pt Ce 2 O 4 194 Pt. O 2 Ce. O 194 Pt Ce 2 O 2 Ce. O 4 H 4 Ce. O 3 194 Pt Ce. O 2 H 2 Ion Intensity (au) Ce. O 3 H 2 194 Pt–Ce pressed target with 75 mol% 194 Pt to 25 mol% Ce 2 O 194 Pt Ce. O 194 Pt 2 × 20 Mass/charge (amu/e ) • Ptˉ atomic anion dominates the mass spectrum • Presence of Cex. Oyˉ clusters, Ptx. Oyˉ clusters with limited distribution of Ce–Pt heteronuclear oxides 7

Electron counts (a. u. ) Measured PE Spectra Photon Energy, hv = 3. 49

Electron counts (a. u. ) Measured PE Spectra Photon Energy, hv = 3. 49 e. V [Ce. O]Pt 2 [Ce. O 2]Pt [Ce. O 2 H 2]Pt 2 Electron Binding energy (e. V) = 0 o = 90 o Electron Binding energy (e. V) • M. Ray, J. Kafader, J. Topolski and C. C. Jarrold, J. Chem. Phys. (submitted) 8

Ce. OPtˉ vs Ce. Oˉ hv = 2. 33 e. V [Ce. O]Pt 825

Ce. OPtˉ vs Ce. Oˉ hv = 2. 33 e. V [Ce. O]Pt 825 cm 1 Eo= 0. 57 ± 0. 10 e. V • Presence of partially resolved 825± 20 cm-1 vibrational progression β = 1. 0 ± 0. 1 • Bond dissociation energies, Do (Ce-O)=790 k. J/mol and Do (Pt-O)=418 k. J/mol Ce. O Eo= 0. 936 ± 0. 007 e. V 4 f 6 s 2 825 cm 1 β = 1. 0 ± 0. 1 Pt 5 d 96 s 2 hv = 3. 49 e. V β = 1. 85 ± 0. 15 for Pt Eo= 2. 128± 0. 002 e. V 0 0. 5 1 1. 5 2 2. 5 3 Electron Binding energy (e. V) • Preference of Ce–O bonding rather Pt–O, with Pt– Ce. O type structure, not Ce–Pt–O or Ce–O–Pt type structures. • Bond would be partially ionic and more localized on Pt M. Ray, J. Felton, J. Kafader, J. Topolski and C. C. Jarrold, J. Chem. Phys. 142, 064305 (2015). 9

Computational Details • GAUSSIAN 09 suite of electronic structure programs • B 3 LYP

Computational Details • GAUSSIAN 09 suite of electronic structure programs • B 3 LYP hybrid density functional method • For Cerium, 28 electron quasirelativistic pseudopotential and atomic natural basis for valence electrons named ECP 28 MWB_ANO, consists of (14 s 13 p 10 d 8 f 6 g)/ [6 s 6 p 5 d 4 f 3 g] functions • For Pt, 60 electron ECP 60 MWB quasirelativistic pseudopotential with valence electron basis set consists of (8 s 7 p 6 d 2 f 1 g)/[6 s 5 p 3 d 2 f 1 g] functions • aug-cc-pv-tz basis set was used for O-atom • No spin orbit coupling is considered in the calculations • M. Ray, J. Felton, J. Kafader, J. Topolski and C. C. Jarrold, J. Chem. Phys. 142, 064305 (2015). • J. O. Kafader, M. Ray, and C. C. Jarrold, J. Chem. Phys. 142, 034305 (2015). • J. O. Kafader, M. Ray, and C. C. Jarrold, J. Chem. Phys. , 143, (2015) http: //www. uni-stuttgart. de/theochem/ University of Stuttgart Institute for theoretical chemistry 10

σ* 0 e. V Neutral: 4 f Anion: 4 f 6 s -1. 2

σ* 0 e. V Neutral: 4 f Anion: 4 f 6 s -1. 2 e. V 6 s [Ce. O]Pt hv = 2. 33 e. V Ce. O Pt -2. 7 e. V Simulated Intensity Computational Results using DFT σ [Ce. O]Pt ca. 1 e. V [Ce. O]Ptˉ Neutral ← Anion Relative Pt 7 doubly-occupied orbitals 5 d 9 6 s 2 (four Pt 4 d-local, three O 2 p -local) -4. 2 e. V e counts (a. u. ) … 6 s [Ce. O]Pt hv = 2. 33 e. V Electron Binding energy (e. V) [4 f Ce. O+][5 d 9 6 s 2 Ptˉ ] ←[4 f 6 s. Ce. O][5 d 9 6 s 2 Ptˉ ] • Ionic bonding interactions in the neutral and charge dipole interaction in anion • Bent structure 0. 3 e. V more stable than the linear structure 11

Photodissociation and Photodetachment [Ce. O]Pt 2 and [Ce(OH)2]Pt 2 Clusters = 0 o =

Photodissociation and Photodetachment [Ce. O]Pt 2 and [Ce(OH)2]Pt 2 Clusters = 0 o = 90 o [Ce. O]Pt 2 hv = 3. 49 e. V [Ce(OH)2]Pt 2 hv = 3. 49 e. V β = 0. 25 ± 0. 1 β = 0. 60 ± 0. 05 0 0. 5 1. 0 1. 5 2. 0 2. 5 3. 0 • Presence of sharp peaks at energies correspond to PE spectrum of Ptˉ • Low signal to noise ratio in the PE spectrum of [Ce(OH)2]Pt 2 , except the presence of two sharp peaks • Anisotropy parameter spikes at energies around Ptˉ detachment peaks 12

Computational Results using DFT [Ce. O]Pt 2 • The detachment transition is from a

Computational Results using DFT [Ce. O]Pt 2 • The detachment transition is from a π*5 d-5 d orbital [4 f Ce. O+]∙ [5 d 10]σ2 g, 6 s. Pt 22ˉ Ce. OPt + Ptˉ Singly occupied Ce 4 f 0 e. V Singly occupied in neutral, doubly occupied in anion Pt 2 * 1. 5 e. V Doubly occupied Ce-O 3. 0 e. V Electron Binding energy (e. V) • … [Ce. O]Pt 2 = 90 o; hv = 3. 49 e. V Simulation … • Photodissociation Simulated and e Intensity • The negative charge is shifted from 6 s- (LUMO) into the 5 d based Pt 2 local orbitals Unoccupied Pt 2 * 1 e. V Promotion of an e- to LUMO will weaken the Pt-Pt bond and facilitate overlap between Pt atoms and Ce. O Doubly occupied Pt 2 4. 0 e. V … [4 f Ce. O+]∙[…(π5 d-5 d *)3]σ2 g, 6 s. Pt 2ˉ Unoccupied Ce. O 6 s 2. 7 e. V 13

Electron counts (a. u. ) PE Spectrum of [Ce. O 2]Pt hv = 3.

Electron counts (a. u. ) PE Spectrum of [Ce. O 2]Pt hv = 3. 49 e. V 0 0. 5 1 1. 5 2 2. 5 3 Electron Binding energy (e. V) Structure of 3 A neutral Structure of 2 A anion 1 Anion spin density • Neutral [Ce. O 2]Pt is a low symmetry structure lacking charge-dipole interaction … • Anion structure exhibits charge-dipole type of interaction, [Ce. O 2]∙Ptˉ … • Similar presence of sharp peaks correspond to Ptˉ Pt-local 6 s and 5 d AOs interleaved with Ce. O 2 MOs within 2 e. V energy window • High electron affinity in the [Ce. O 2]Pt←[Ce. O 2]∙Ptˉ transition compared to Pt← Ptˉ 14

Conclusions and Potential Application of the Interactions Studied • Preference of distinct Ce–O bonding

Conclusions and Potential Application of the Interactions Studied • Preference of distinct Ce–O bonding interactions in [Cex. Oy]Ptx ˉ heteronuclear clusters. • The resulting neutral complexes from [Ce. O]Ptˉ, [Ce. O]Pt 22ˉ or [Ce(OH)2]Pt 22ˉ anions are ionic neutral complexes Ø Oxygen vacancies facilitate dissociative adsorption of H 2 O to form hydroxyl groups Ø Negative charge accumulation on Pt is important to facilitate reduction of 2 H+ to H 2 • Charge transfer from Pt in [Ce. O 2]Ptˉ anion complex (where Ce is in +4 oxidation state) to neutral involves a profound structural change Ø The possibility of substantial structural arrangement with the oxygen atoms in Pt–Ce. O 2 environment in ceria (Ce. O 2) surface, if charge transfer is a component of any catalytic activation 15

Acknowledgment Caroline Chick Jarrold Jared Kafader Josey Topolski Kellyn Patros Brett Williams Vicmarie Marrero-Colon

Acknowledgment Caroline Chick Jarrold Jared Kafader Josey Topolski Kellyn Patros Brett Williams Vicmarie Marrero-Colon Big Red II Supercomputer at Indiana University Previous Group Members NSF Grant CHE-1265991 Dr. Jeremy Felton Dr. Sarah Waller 16

October 30, 2020

October 30, 2020

Principle of Anion Photoelectron Spectroscopy and Significance of β parameter Expected Possible anion to

Principle of Anion Photoelectron Spectroscopy and Significance of β parameter Expected Possible anion to neutral transition in [Ce. O]Pt 2 system [5 d 9]σ2 g, 6 s ← [5 d 9]σ2 g, 6 s σu, 6 s (Triplet Neutral state) (Quartet anionic state) October 30, 2020

Photodissociation and Photodetachment October 30, 2020 [Ce. O]Pt 2 and [Ce(OH)2]Pt 2 Clusters [Ce.

Photodissociation and Photodetachment October 30, 2020 [Ce. O]Pt 2 and [Ce(OH)2]Pt 2 Clusters [Ce. O]Pt 2 hv = 3. 49 e. V β = 0. 25 ± 0. 1 β = 0. 60 ± 0. 05 [Ce(OH)2]Pt 2 hv = 3. 49 e. V = 0 o = 90 o 0 0. 5 1. 5 2. 5 3 Pt hv = 3. 49 e. V 0 0. 5 1. 5 2. 5 3 12

Photodissociation and Photodetachment October 30, 2020 [Ce. O]Pt 2 and [Ce(OH)2]Pt 2 Clusters 0

Photodissociation and Photodetachment October 30, 2020 [Ce. O]Pt 2 and [Ce(OH)2]Pt 2 Clusters 0 0. 5 1. 0 1. 5 0 2. 0 0. 5 1 1. 5 2 1. 5 1 0. 5 0 3. 0 2. 5 2 2. 5 3 3 13