structure and paramagnetic character R. Kakavandi, S-A. Savu, A. Caneschi, T. Chassé, M. B. Casu Electronic Supporting Information

Similar documents
Spin-resolved photoelectron spectroscopy

Ultra-High Vacuum Synthesis of Strain-Controlled Model. Pt(111)-Shell Layers: Surface Strain and Oxygen Reduction

Supporting Information. for. Advanced Materials, adma Wiley-VCH 2005

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960

The Use of Synchrotron Radiation in Modern Research

On surface synthesis of a 2D boroxine framework: a route to a novel 2D material?

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu

Photoemission Spectroscopy

Photocatalysis: semiconductor physics

X-ray Photoelectron Spectroscopy (XPS)

Reduced preferential sputtering of TiO 2 (and Ta 2 O 5 ) thin films through argon cluster ion bombardment.

Spectro-microscopic photoemission evidence of surface dissociation and charge uncompensated areas in Pb(Zr,Ti)O 3 (001) layers

Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies.

Supplementary Figures

Electron Rutherford Backscattering, a versatile tool for the study of thin films

NanoEngineering of Hybrid Carbon Nanotube Metal Composite Materials for Hydrogen Storage Anders Nilsson

Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging

SUPPLEMENTARY INFORMATION

Introduction of XPS Absolute binding energies of core states Applications to silicene

Understanding electron energy loss mechanisms in EUV resists using EELS and first-principles calculations

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7

X- ray Photoelectron Spectroscopy and its application in phase- switching device study

Special Properties of Au Nanoparticles

Electronics Supplementary Information for. Manab Kundu, Cheuk Chi Albert Ng, Dmitri Y. Petrovykh and Lifeng Liu*

SUPPLEMENTARY INFORMATION

Supporting Information

CsK 2 Sb PHOTOCATHODE DEVELOPMENT FOR. Martin Schmeißer, Julius Kühn, Thorsten Kamps, Andreas Jankowiak Helmholtz-Zentrum Berlin

Photoelectron spectroscopy Instrumentation. Nanomaterials characterization 2

Energy Spectroscopy. Ex.: Fe/MgO

Supporting information High density monodispersed cobalt nanoparticles filled into multi-walled carbon nanotubes

Covalent assembly of a two-dimensional molecular sponge on a Cu(111) surface: Confined electronic surface states in open and closed pores

The Benefit of Wide Energy Range Spectrum Acquisition During Sputter Depth Profile Measurements

Introduction of XPS Absolute binding energies of core states Applications to silicone Outlook

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy

Supplementary Information

Role of the substrate in electronic structure, molecular orientation, and morphology of organic thin films: diindenoperylene on rutile TiO 2 (110)

Synchrotron radiation study of free and adsorbed organic molecules

A DIVISION OF ULVAC-PHI

Modern Methods in Heterogeneous Catalysis Research: Preparation of Model Systems by Physical Methods

A Novel Electroless Method for the Deposition of Single-Crystalline Platinum Nanoparticle Films On

Visible-light Driven Plasmonic Photocatalyst Helical Chiral TiO 2 Nanofibers

High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni

Electronic Supporting Information for

Supporting Information. Oxygen reduction and methanol oxidation behaviour of SiC based Pt. nanocatalysts for proton exchange membrane fuel cells

XPS/UPS and EFM. Brent Gila. XPS/UPS Ryan Davies EFM Andy Gerger

FUNDAMENTAL PARAMETER METHOD FOR THE LOW ENERGY REGION INCLUDING CASCADE EFFECT AND PHOTOELECTRON EXCITATION

A Plasmonic Photocatalyst Consisting of Silver Nanoparticles Embedded in Titanium Dioxide. Ryan Huschka LANP Seminar February 19, 2008

Supplementary Figure 1 Result from XRD measurements. Synchrotron radiation XRD patterns of the as-prepared gold-ceria samples.

Table S1. Structural parameters of shell-by-shell fitting of the EXAFS spectrum for reduced and oxidized samples at room temperature (RT)

Graphene field effect transistor as a probe of electronic structure and charge transfer at organic molecule-graphene interfaces

Engineering electronic structure of Two-Dimensional Subnanopore. nanosheet by Molecular Titanium-oxide Incorporation for Enhanced

Thin and Ultrathin Plasma Polymer Films and Their Characterization

Atmospheric pressure Plasma Enhanced CVD for large area deposition of TiO 2-x electron transport layers for PV. Heather M. Yates

The Diffusion of H in Mg and the Nucleation and Growth of MgH2 in Thin Films*

Segregated chemistry and structure on (001) and (100) surfaces of

Supporting Information. for. Angew. Chem. Int. Ed. Z Wiley-VCH 2003

Water clustering on nanostructured iron oxide films

arxiv: v1 [cond-mat.mtrl-sci] 24 Apr 2008

Supporting Information. Surface-Enhanced Polymerization via Schiff-base Coupling. at the Solid-Water Interface under ph-control. and Claudio Goletti d

Lecture 12 Multiplet splitting

Magnetism of TbPc 2 SMMs on ferromagnetic electrodes used in organic spintronics

AN XPS STUDY OF THE INTERACTION OF MODEL Ba/TiO 2 AND Ba/ZrO 2 NSR CATALYSTS WITH NO 2 INTRODUCTION

Near-surface regions of chalcopyrite (CuFeS 2 ) studied using XPS, HAXPES, XANES and DFT

Internal Heterostructure of Anion-Exchanged Cesium Lead Halide. Nanocubes

Surface and Electronic Structure Study of Substrate-dependent Pyrite Thin Films

Supplementary Figure 1 PtLuSb RHEED and sample structure before and after capping layer

X-ray Standing-Wave Investigation of (1X2)Rb/ Cu(110)

PHOTOELECTRON SPECTROSCOPY (PES)

Application of Surface Analysis for Root Cause Failure Analysis

An extraordinarily stable catalyst: Pt NPs supported on two-dimensional Ti 3 C 2 X 2 (X=OH, F) nanosheets for Oxygen Reduction Reaction

Soft X-ray Physics DELNOR-WIGGINS PASS STATE PARK

Name: (a) What core levels are responsible for the three photoelectron peaks in Fig. 1?

Photon Interaction. Spectroscopy

Stability of Organic Cations in Solution-Processed CH3NH3PbI3 Perovskites: Formation of Modified Surface Layers

Temperature-dependent templated growth of porphine thin films on the (111) facets of copper and silver Supporting Information

Probing the Chemical Structure of Monolayer Covalent-Organic Frameworks Grown via Schiff-Base Condensation Reactions

a b c Supplementary Figure S1

Thermal decomposition of ethylene on Si(111): formation of the Si(111) 3

Defense Technical Information Center Compilation Part Notice

Electronic and chemical structure of the H 2 O/GaN(0001) interface under ambient conditions

Report of the Electronic Structure- and Adsorption Group

Surface Characte i r i zat on LEED Photoemission Phot Linear optics

MODERN TECHNIQUES OF SURFACE SCIENCE

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD

Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline

X-ray photoelectron spectroscopic characterization of molybdenum nitride thin films

Energy Spectroscopy. Excitation by means of a probe

Formation of Halogen Bond-Based 2D Supramolecular Assemblies by Electric Manipulation

Formation of interface and surface oxides on supported Pd nanoparticles

Electrochemical investigation of covalently post-synthetic modified SURGEL coatings

Synchrotron Methods in Nanomaterials Research

Low pressure CO 2 hydrogenation to methanol over gold nanoparticles activated on a CeO x /TiO 2 interface

Organic semiconductor heterointerfaces containing bathocuproine

conversion reactions

Sub-10-nm Au-Pt-Pd Alloy Trimetallic Nanoparticles with. High Oxidation-Resistant Property as Efficient and Durable

Controllable Growth of Bulk Cubic-Phase CH 3 NH 3 PbI 3 Single Crystal with Exciting Room-Temperature Stability

Electronic Supplementary Information

Supporting Information s for

Experiment Section Fig. S1 Fig. S2

Probing Matter: Diffraction, Spectroscopy and Photoemission

Transcription:

At the interface between organic radicals and TiO 2 (110) single crystals: electronic structure and paramagnetic character R. Kakavandi, S-A. Savu, A. Caneschi, T. Chassé, M. B. Casu Electronic Supporting Information This Electronic Supplementary Information provides 1) Experimental details. 2) Tables 1-3 with all fit parameters for XPS C1s core level spectra. 3) Tables 4-6 with all fit parameters for XPS N1s core level spectra. 4) The XPS spectra after film annealing at 790 K. 5) The XPS Ti2p core level of two surfaces with different densities of Ti 3+ 3d states and the relative tables with all fit parameters. 6) Relevant pk a /ph values in solution. 1

Further experimental details. Sample preparation and XPS investigations where performed both in our laboratory and at the BESSY II synchrotron source (Berlin, Germany) at the UE52-PGM-PES. Our system consists of a preparation chamber, and an analysis chamber (base pressure = 1x10-10 mbar) equipped with a concentric hemispherical Specs Phoibos 150 analyser and a monochromatized Al Kα X-ray source. The measuring chamber (base pressure = 4x10-10 mbar) at the UE52-PGM-PES undulator beamline is equipped with a standard twin anode X-ray source, and a SCIENTA R4000 electron energy analyzer. The measurements were carried out in low-alpha and single bunch (ring current at injection = 13/20 ma (mode B/mode A), cff = 2.5, analyser resolution= 0.1 ev). We found that these operation modes minimise the radiation damage. The C1s photoelectron spectra at BESSY were taken with 1000 ev photon energy. As the substrate already contains oxygen, we concentrate only on carbon and nitrogen species. Clean TiO 2 (110) single crystals were prepared using multiple cycles of argon ion sputtering and UHV annealing. 1 The surface preparation was monitored by XPS and X-ray absorption spectroscopy. The change in colour of the crystals from transparent to light blue/gray indicated the oxygen deficient surface. The molecules were deposited by OMBD under UHV conditions keeping the substrate at room temperature (evaporation rate =1 Å /min, determined with a quartz microbalance). No degradation of the samples was observed on the time scale of all presented experiments. 1. F. Allegretti, S. O'Brien, M. Polcik, D. I. Sayago and D. P. Woodruff, Phys. Rev. Lett., 2005, 95, 226104. 2

Table 1: NitPyn fit results for energy position and relative areas of the photoemission lines in the C1s spectra for a 0.3 nm nominally thick film: C-C 284.04 0.08 1.32 31.45 C-H 284.32 0.08 1.32 38.94 CH 3 284.60 0.08 1.32 17.13 C-N 286.27 0.08 1.32 9.98 Table 2: NitPyn fit results for energy position and relative areas of the photoemission lines in the C1s spectra for a 0.5 nm nominally thick film. C-C 284.02 0.08 1.32 31.30 C-H 284.30 0.08 1.32 39.10 CH 3 284.58 0.08 1.32 17.20 C-N 286.01 0.08 1.68 12.40 Table 3: NitPyn fit results for energy position and relative areas of the photoemission lines in the C1s spectra for a 1.0 nm nominally thick film. C-C 284.02 0.08 1.32 31.20 C-H 284.30 0.08 1.32 36.50 CH 3 284.58 0.08 1.32 16.45 C-N 286.01 0.08 1.68 14.21 3

Table 4: NitPyn fit results for energy position and relative areas of the photoemission and satellite lines in the N1s spectra for a 0.3 nm nominally thick film: (~ 17% of Ti 3+ 3d states) Decomposed 400.03 0.1 2.35 83.37 radical (N-H) Ti -N 397.75 0.1 1.33 13.47 Satellite 402.93 0.1 2.03 3.16 (~ 3% of Ti 3+ 3d states) Intact radical 402.04 0.1 1.72 47.02 Decomposed 399.76 0.1 1.72 33.73 radical (N-H) Ti-N 398. 14 0.1 1.72 11.63 Satellite 403.44 0.1 1.72 7.62 Table 5: NitPyn fit results for energy position and relative areas of the photoemission and satellite lines in the N1s spectra for a 0.5 nm nominally thick film: Intact radical 401.92 0.1 1.32 47.58 Decomposed 400.03 0.1 2.35 33.40 radical (N-H) Ti-N 398.02 0.1 1.32 10.60 Satellite 403.32 0.1 1.32 4.48 Satellite 405.15 0.1 1.32 3.88 Table 6: NitPyn fit results for energy position and relative areas of the photoemission and satellite lines in the N1s spectra for a 1.0 nm nominally thick film: Intact radical 401.92 0.1 1.32 56.14 Decomposed 400.03 0.1 1.98 28.58 radical (N-H) Ti-N 398.02 0.1 1.32 5.86 Satellite 403.32 0.1 1.32 9.41 4

annealed at ~ 790 K O 1s C 1s [a.u.] Ti 2p N 1s 1200 1000 800 600 400 200 0 Binding [ev] Figure 1S: XPS survey spectra after annealing @ 790 K of a 2 nm nominally thick NitPyn film. 5

Ti 4+ 2P 3/2 Ti 3+ 2P 3/2 [a.u.] Ti 3+ 2P 1/2 Ti 2+ 2P 1/2 s Ti 4+ 2P 1/2 s Ti 2 O 3 Ti 2+ 2P 3/2 468 464 460 456 Binding energy [ev] Ti 4+ (2p 3/2 ) 458.50 0.70 1.45 44.71 Ti 4+ (2p 1/2 ) 464.20 0.70 2.52 23.18 Ti 3+ (2p 3/2 ) 456.60 0.70 1.41 14.29 Ti 3+ (2p 1/2 ) 462.50 0.70 1.66 3.05 Ti 2+ (2p 3/2 ) Ti 2+ (2p 1/2 ) 455.83 0.70 1.35 2.46 461.93 0.70 1.22 1.08 Ti 2 O 3 460.05 0.70 1.13 6.30 Satellite 461.68 0.70 1.45 2.73 Satellite 468.68 0.70 1.45 2.18 Figure 2S: Ti2p core level spectra of the surface before deposition of a 0.3 nm thick film as in Figure 2a, together with the Table containing the fitting parameters. 6

Ti 4+ 2p 3/2 [a.u.] Ti 4+ 2p 1/2 Ti 3+ 2p 1/2 Ti 3+ S 2p 3/2 468 464 460 456 Binding energy [ev] Ti 4+ (2p 3/2 ) 458.50 0.70 1.48 68.17 Ti 4+ (2p 1/2 ) 464.20 0.70 2.00 27.11 Ti 3+ (2p 3/2 ) 456.65 0.70 1.06 2.25 Ti 3+ (2p 1/2 ) 462.55 0.70 1.60 1.63 Satellite 1 461.02 0.70 1.48 0.84 Figure 3S: Ti2p core level spectra of the surface before deposition of a 0.3 nm thick film as in Figure 2b, together with the Table containing the fitting parameters. 7

Relevant pk a /ph values in solution from Ref. 25. The nitronyl nitroxide radical derivatives in benzene with triphenylphosphine spontaneously lose an oxygen atom. The compounds are weak bases and they may be reversibly protonated without decomposition. The compound with substituent = C 6 H 5 has a pk a =1.9. The unsubstituted derivative with substituent =H undergoes deuterium exchange at the central carbon atom at ph 7, within 6 hours. The formation of a compound as in Figure 4S occurs, after decomposition without degradation, when the solid with substituent =H, is kept at room temperature. Figure 4S: One of the possible derivatives of the nitronyl nitroxide radical as from Ref. 25. 8