Technical description of photoelectron spectrometer Escalab 250Xi

Similar documents
A DIVISION OF ULVAC-PHI

MB Scientific AB Angular-Resolved Photoemission Spectroscopy System MBS A1SYS_V

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

Auger Electron Spectroscopy Overview

Surface Science Spectra

Vacuum Pumps. Two general classes exist: Gas transfer physical removal of matter. Mechanical, diffusion, turbomolecular

Characterization of Secondary Emission Materials for Micro-Channel Plates. S. Jokela, I. Veryovkin, A. Zinovev

Hiden SIMS Secondary Ion Mass Spectrometers. Analysers for surface, elemental and molecular analysis

Photoemission Spectroscopy

Thermo Scientific K-Alpha + XPS Spectrometer. Fast, powerful and accessible chemical analysis for surface and thin film characterization

Mass Spectrometers. for Surface Analysis SURFACE ANALYSIS

3. Experimental Methods and Instrumentation.

Methods of surface analysis

CIG B5. Capitolato Tecnico Technical requirements

A DIVISION OF ULVAC-PHI. Quantera II. Scanning XPS Microprobe

X-ray Photoelectron Spectroscopy/ Electron spectroscopy for chemical analysis (ESCA), By Francis Chindeka

Fall 2014 Mott Target Replacement and Ladder Position Re- Calibration JLAB- TN Joe Grames. September 17, 2014

SCANNING ELECTRON MICROSCOPE

CHARACTERIZATION of NANOMATERIALS KHP

Supporting Information. Re-Investigation of the Alleged Formation of CoSi Nanoparticles on Silica. Van An Du, Silvia Gross and Ulrich Schubert

SEY and Surface Analysis Measurements on FNAL Main Injector Ring S/S Beam Chamber Material

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

SNMS. SNMS Applications. Combined SIMS and SNMS

MODERN TECHNIQUES OF SURFACE SCIENCE

QUESTIONS AND ANSWERS

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

Surface Analysis - The Principal Techniques

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

Imaging Methods: Scanning Force Microscopy (SFM / AFM)

Electrochemical Deposition of Iron Nanoparticles on PPY and H terminated Si substrates. Karan Sukhija Co-op Term # 1 April 28 th, 2005

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

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

User Fees for the 4D LABS Characterization Facility

Cover Page. The handle holds various files of this Leiden University dissertation.

How to distinguish EUV photons from out-of-band photons

Gold nanothorns macroporous silicon hybrid structure: a simple and ultrasensitive platform for SERS

An Introduction to Auger Electron Spectroscopy

Ma5: Auger- and Electron Energy Loss Spectroscopy

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

Graphene films on silicon carbide (SiC) wafers supplied by Nitride Crystals, Inc.

Gaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition

Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD

UV Source Series. UVS 10/35 gas discharge, UVS 300 duoplasmatron. Key Features

EuCARD-2 Enhanced European Coordination for Accelerator Research & Development. Milestone Report

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high?

A fast, parallel acquisition, electron energy analyzer: The hyperbolic field analyzer

Dual Beam Helios Nanolab 600 and 650

CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD

AP5301/ Name the major parts of an optical microscope and state their functions.

Experimental 2.1 Introduction. Ultra high vacuum.

MSE 321 Structural Characterization

5.8 Auger Electron Spectroscopy (AES)

Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur

Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences

Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist

Thin Film Deposition

Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist

ToF-SIMS or XPS? Xinqi Chen Keck-II

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

Modern Optical Spectroscopy

Vacuum Chambers. Type DK /DK /DK

Lecture 5. X-ray Photoemission Spectroscopy (XPS)

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

8 Summary and outlook

The scanning microbeam PIXE analysis facility at NIRS

Auger Electron Spectroscopy (AES)

MSE 321 Structural Characterization

Iodine-Mediated Chemical Vapor Deposition Growth of Metastable Transition Metal

Fast, Effective XPS Point Analysis of Metal Components

Spin-resolved photoelectron spectroscopy

Highly efficient SERS test strips

JARA FIT Ferienprakticum Nanoelektronik Experiment: Resonant tunneling in quantum structures

Beetle UHV VT AFM / STM

Surface Analysis - The Principal Techniques

Lecture 4. Ultrahigh Vacuum Science and Technology

Chemistry Instrumental Analysis Lecture 19 Chapter 12. Chem 4631

.Fritjaf Capra, The Tao of Physics

arxiv: v1 [physics.acc-ph] 1 Apr 2015

Study on the Selective Hydrogenation of Nitroaromatics to N-aryl hydroxylamines using a Supported Pt nanoparticle Catalyst

and Environmental Science Centre

SOLID STATE PHYSICS PHY F341. Dr. Manjuladevi.V Associate Professor Department of Physics BITS Pilani

Final exam: take-home part

Selective aerobic oxidation of biomass-derived HMF to 2,5- diformylfuran using a MOF-derived magnetic hollow Fe-Co

Auger Analyses Using Low Angle Incident Electrons

Lecture 5-8 Instrumentation

Information from Every Angle

Analysis of Cadmium (Cd) in Plastic Using X-ray Fluorescence Spectroscopy

5) Surface photoelectron spectroscopy. For MChem, Spring, Dr. Qiao Chen (room 3R506) University of Sussex.

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

object objective lens eyepiece lens

Auger Electron Spectroscopy

Scanning Electron Microscopy

1 EX/P4-8. Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device

Electron beam scanning

Low Temperature (LT), Ultra High Vacuum (UHV LT) Scanning Probe Microscopy (SPM) Laboratory

PHI. Scanning XPS Microprobe

Outlines 3/12/2011. Vacuum Chamber. Inside the sample chamber. Nano-manipulator. Focused ion beam instrument. 1. Other components of FIB instrument

Multialkali photocathodes grown by MBE technique. General Physics Institute, USSR, Academy of Sciences, , Moscow, Vavilov street, 38.

Secondary Ion Mass Spectroscopy (SIMS)

Transcription:

Technical description of photoelectron spectrometer Escalab 250Xi Resource center Physical Methods of Surface Investigations 2014

Table of contents Common description 3 Analytical chamber 8 Preparation chamber 9 Load-lock 11 Requirements for samples. Sample holders. 11 Appendix A: main drawings of experimental station 15 Appendix B: drawings of analytical chamber 22 Appendix C: drawings of preparation chamber 28 2

Common description Figure 1: Common view of experimental station. Experimental station Escalab 250Xi (see fig. 1), designed by Thermo Fisher Scientific1, is designated for realization of elemental and chemical analysis of surface of samples. Next methods are realized in the station: 1. X-ray photoelectron spectroscopy (XPS) and X-Ray Photoelectron Imaging (XPi) 2. Ultraviolet photoelectron spectroscopy (UPS) 3. Auger electron spectroscopy (AES) and Scanning Auger Electron Mapping (SAM) 4. Scanning Electron Microscopy (SEM) 5. Ion Scattering Spectroscopy (ISS) 6. Electron Energy Loss Spectroscopy (EELS) 7. Raster ion etching 8. Low-energy Electron Diffraction (LEED) 9. Charge compensation system for insulating samples 10. Sample heating in controlled gas environment 1 see http://www.thermoscientific.com/en/product/escalab-250xi-x-ray-photoelectron-spectrometerxps-microprobe.html and http://xpssimplified.com/escalab 250xi.php 3

Control of gas lines, pump-down systems and process of measurement is realized in special software Avantage 2 (see fig. 2). Samples are assembled to standard sample holder kit Thermo Fisher Scientific SKIT20 (see section Requirements for samples. Sample holders. Figure 2: View of window of Avantage software. Possible objects of investigations: 1. monocrystals 2. polycrystalls 3. thin films 4. powders Available information about objects: 1. quantitative analysis 2. chemical shifts of core levels 2 see http://xpssimplified.com/avantage_data_system.php 4

(a) (b) Figure 3: XPS spectra of steel 09G2S: (a) before etching, (b) after ion etching Table 1: Determination of chemichal composition of steel 09G2S Elemental composition of the sample Initial state State after etching Element Energy (ev) Atomic fraction (%) Energy (ev) Atomic fraction (%) Fe2p 707.01 1.91 707.45 92.22 O1s 531.28 67.89 531.19 7.78 C1s 285.87 30.20 Figure 4: Core levels of palladium being in different states, shift - 0.7 ev. 3. electronic structure of valence band 5

(a) (b) Figure 5: Photoelectron spectra of valence band of polycrystalline gold: (a) HeI (21.2 ev), (b) HeII (40.8 ev) 4. depth profile of elements in near-surface area Figure 6: Layer-by-layer scheme TiO 2 /Si. Data about element distribution and value of film thicknesses are obtained from analysis of spectra, measured for different emission angles relative to normal of sample surface 5. map of chemical states of elements on surface 6

Figure 7: map of copper on surface of test sample 6. information about crystallographic structure and orientation in the surface Brillouin zone Figure 8: LEED image of Si(111)7 7. Beam energy - 50 ev. 7

Analytical chamber Figure 9: Analytical chamber. Experimental station consists of 3 chambers, which have independent pump-down systems: analytical chamber (see fig. 9), preparation chamber (see fig. 11) and load lock (see fig. 12). Base pressure in analytical chamber -1 10 10 mbar. Analytical chamber is equiped by the following devices (see fig. 10): 1. X-ray source Al-K α (1486.6 ev, with monochromator), spot size is adjusted from 200 microns to 900 microns. Minimal analysis area is less than 20 µm 2. ultraviolet source (HeI (21.2 ev), HeII (40.8 ev)) with differential pump-down system for investigations of valence band with angle resolution less than 1.5 3 3. system for XPS imaging with spatial resolution less than 3 microns 4. raster ion gun EX06 (energy of ions from 0.2 to 4 kev) 5. electron source build-in to lenses of analyser for neutralisation of positive charge and source of positive argon ions for neutralisation of negative charge (possibility of measuring of insulators) 6. hemispherical analyzer with 2 detectors: multi-channel detector, based on channel electron multipliers with wide dynamic rang and 2D-detector based on twin microchannel plate and coordinate detector 3 see http://www.datacompscientific.com/tvgs/uvl_an31058_ds.pdf 8

7. system of magnetic immersion lenses for increasing of sensivity (intensity) with saving of spatial resolution 8. raster ion gun based on effect of field emission FEG1000 with spot size less than 95 nm at current 5 na and energy 10 kev 4, Secondary Electron Detection (SED) system 9. digital camera The Imaging Source DFK 41AF02 5 10. 5-axis manipulator, which allows to hold the sample, save several points of measurements and restore position after moving to preparation chamber 11. system of heating of sample at manupulator (up to 1000 K) Figure 10: Devices in analytical chamber. Preparation chamber 4 see http://www.datacompscientific.com/tvgs/feg1000_an31059_ds.pdf 5 see http://www.theimagingsource.com/en_us/products/cameras/firewire-ccd-color/ dfk41af02/ 9

Figure 11: Preparation chamber. Preparation chamber chamber is equiped by the following devices: 1. ion gun EX03 6 2. diffractometer Omicron SPECTALEED with Auger electron optics 7 3. stage for heating of samples (up to 1000 K) 4. gas inlet system (it is possible to measure in gas environment with pressure 1 10 8-1 10 5 mbar) 5. storage for 3 sample holders 6 see http://www.datacompscientific.com/tvgs/ex03_an31062ds.pdf 7 see http://www.omicron.de/en/products/spectaleed-/instrument-concept 10

Load-lock (a) (b) Figure 12: Load-lock: (a) common view, (b) loading of sample holder to load lock Load-lock is a part of system, where sample holders are inserted from atmosphere and are taked out after measurements. Loading is realized through the door, closed with viton o-ring (see fig. 12(b). It is possible to take out from experimental station one sample holder, arranged at transfer probe, and install another one (or origin sample holder after change of samples) to its place during one cycle. Load-lock is not baked out after loading of samples, but pump-down system allows to get pressure about 1 10 9 mbar. Requirements for samples. Sample holders. Samples are installed to one of sample holders from kit Thermo Fisher Scientific SKIT20. It is possible to measure solid-state samples, which don t break ultrahigh vacuum conditions during measurements. Permissible length and width of samples vary from used sample holder, maximal height with using standard sample holder (Sample Carrier Block) equals 5 mm, maximal height with using sample holder for heating (Heated Sample Assembly) - 3 mm. It is allowed to install several samples at one sample holder. If samples are powders, users should preliminary install (press in) samples to appropriate substrate, for example, soft metal (copper, gold) or vacuum sticky tape. It is allowed to compress powders to tablets. If samples are conductive, substrates should be conductive too. It is allowed to measure dried suspension, which are carried on hard plain surface, for example, silicon. Preparation of samples and substrates (clipping, infliction of substances, drying etc.) is carried out by users, direct installing to sample holder - by stuff of resource center. Figure 13: Sample Carrier Block. 11

The Sample Carrier Block (see fig. 13) is a 25mm long by 14mm wide stainless steel by 6mm block. To attach samples to this Holder, the sample can either be attached directly to the Sample Carrier Block by using the M2 screws (see fig. 14) or clipped down using the molybdenum sample retainers with M2 screws. Alternatively for large samples tape or silver dag can be used (see fig. 15). Figure 14: Sample Carrier Blocks loaded using retainers. Figure 15: Sample Carrier Block loaded using silver DAG or double sided tape. The Multi-Sample Assembly comprises of a 50mm long by 20mm wide by 26SWG stainless steel plate mounted on a stainless steel Sample Carrier Block. To attach samples to this Holder, sample clips can be used either the type. Alternatively samples can be attached to this holder, using the 8 holes down the sided and clipped down by the M1.6 screws Figure 16: 50mm Multi-sample Assembly. 12

Figure 17: 50 mm Multi-Sample Assembly loaded using clips. Figure 18: 50mm Multi-Sample Assembly loaded using sample retainers. Improved depth resolution may be obtained for some materials if the sample is rotated during sputtering to reduce topography formation. Materials that tend to show improved depth resolution with rotation are polycrystalline metals on flat substrates, e.g. aluminium on silicon. Rotation can also be useful when profiling rough samples, as any shadowing of the ion beam by roughness on the sample is minimized. Rotation of the sample during sputtering is possible due to 5-axis manipulator and a rotatable sample holder, which consists of block, gear and metallic disc (see Fig. 19). (a) (b) Figure 19: Azimuthal Rotation Holder Assembly: (a) before installing a disc, (b) after installing a disc 13

Special sample holder (see Fig. 20) allows to heat the sample with temperature up to 600 K and cool down the sample by use of liquid nytrogen to temperature 170 K. System contains a thermocouple for feedback control. Figure 20: 600 deg K. Heated Sample Assembly. Sample holder for intensive heating (see Fig. 21) allows to heat the sample with temperatures up to 1000 K. Figure 21: 1000 K Heated Sample Assembly. 14

Appendix A: main drawings of experimental station Figure 22: Drawing of experimental station. 15

Figure 23: Drawing of experimental station. Top view. On the left: analytical chamber, on the bottom right - preparation chamber. on the top right - load lock chamber. 16

Figure 24: Common view of experimental station with bakeout tent. 17

Figure 25: Drawing of experimental station. View from the analytical chamber. 18

Figure 26: Drawing of experimental station. Front view. On the center - analytical chamber, on the right - preparation chamber. 19

Figure 27: Drawing of experimental station. View from the preparation chamber (right view). On the left - preparation chamber, on the right - load-lock chamber. 20

Table 2: Flanges and equpment of experimental station Escalab 250Xi No Description 4 UHV preparation chamber 8 bakeout tent 9 tent frame 23 LEED/Auger Omicron SPECTALEED 24 sample holder ZSHI 8 and XL09 sample receiver 25 coaxial feedthrough 26 Miniax translator ZXYZ1015 9 27 rotary motion drive RD2 10 8 see https://www.vgscienta.com/_resources/file/catalogue_sections/manipulation/ Manipulation-SampleHolders.pdf 9 see http://www.vgscienta.com/_resources/file/catalogue_sections/manipulation/ Manipulation-Miniax.pdf 10 see http://www.vgscienta.com/_resources/file/catalogue_sections/vgscienta_rotary_ Drives.pdf 21

Appendix B: drawings of analytical chamber Figure 28: Drawing of analytical chamber. Top view (on the right - preparation chamber). 22

Figure 29: Drawing of analytical chamber. Front view (on the right - preparation chamber). 23

Figure 30: Drawing of analytical chamber. View from the preparation chamber (right view). 24

Figure 31: Drawing of analytical chamber. Back view (on the left - preparation chamber). 25

Figure 32: Drawing of analytical chamber. Left view. 26

Table 3: Flanges and equpment of analytical chamber No Tube size Flange type angle β angle γ Designation 1 - DN100 0 0 lens assembly 2 71.65mm OD x 2.5mm DN63 57 0 raster electron gun FEG1000 3 3/4 O/D 16 SWG DN63 58 180 monochromator and X-Ray source assembly (XR6) 4 3/4 O/D 16 SWG DN35 55 135 vacuum gauge 5 3/4 O/D 2.5mm DN63 90 270 preparation chamber 6 O/D O/D 16 SWG DN100 65 315 viewport 7 3/4 O/D x 16 SWG DN35 40 50 scintiallator 8 3/4 O/D x 16 SWG DN35 50 227 flood gun 9 4 O/D x 16 SWG DN100 70 40 view port 10 3/4 O/D x 16 DN45 33 90 microscope camera 11 4 O/D x 2.5mm DN100 90 90 motorised manipulator 12 3/4 O/D x 18 SWG DN16 38 313 viewport for light source adaptor 13 3/4 O/D x 18 SWG DN16 30 330 iris shutter drive (Field of View) 11 14 3/4 O/D x 2.5mm DN63 40 270 raster ion gun EX06 15 1/2 O/D x 18 SWG DN35 34 204 11-pin feedthrough for flood gun 16 8 I/D x 14 SWG DN200 - - turbomolecular pump 17 4 O/D x 16 SWG DN100 90 221 magnetic lens assembly 18 1/2 O/D x 18 SWG DN35 34 149 ultraviolet source 11 iris shutter drive (Angle) is located upper 27

Appendix C: drawings of preparation chamber (a) (b) Figure 33: Preparation chamber: (a) top view, (b) side view Table 4: Flanges and equipment of preparation chamber No Flange Designation 1 DN63 analytical chamber 2 DN35 ion gun accessory 3 DN35 spare flange 4 DN35 ion gun EX03 5 DN35 heating state 6 DN35 vacuum-gauge sensor 7 DN35 differential pump-down 8 DN35 spare flange 9 DN63 viewport 10 DN35 gas line 11 DN63 spare flange 12 DN63 load lock chamber 13 DN16 viewport for light source adaptor 14 DN35 carrier of platform for placement of 3 sample holders 15 DN63 viewport 16 DN150 diffractometer Omicron SPECTALEED 17 DN63 VG Scienta 4-axis manipulator 18 DN63 viewport 19 DN35 manipulator 20 DN100 pump-down 21 DN35 spare flange 28