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X-Ray Photoelectron Spectroscopy (XPS)

X-Ray Photoelectron Spectroscopy (XPS). Prof. Paul K. Chu. X-ray Photoelectron Spectroscopy. Introduction Qualitative analysis Quantitative analysis Charging compensation Small area analysis and XPS imaging Instrumentation Depth profiling Application examples. Photoelectric Effect.

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X-Ray Photoelectron Spectroscopy (XPS)

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

  2. X-ray Photoelectron Spectroscopy Introduction Qualitative analysis Quantitative analysis Charging compensation Small area analysis and XPS imaging Instrumentation Depth profiling Application examples

  3. Photoelectric Effect Einstein, Nobel Prize 1921 Photoemission as an analytical tool Kai Siegbahn, Nobel Prize 1981

  4. XPS is a widely used surface analysis technique because of its relative simplicity in use and data interpretation.

  5. KE = hn - BE - FSPECT BE = hn - KE - FSPECT hu: Al Ka(1486.6eV) P 2s P 2p1/2-3/2 Kinetic Energy

  6. Peak Notations

  7. For p, d and f peaks, two peaks are observed. The separation between the two peaks are named spin orbital splitting. The values of spin orbital splitting of a core level of an element in different compounds are nearly the same. The peak area ratios of a core level of an element in different compounds are also nearly the same. Au Spin orbital splitting and peak area ratios assist in elemental identification

  8. General methods in assisting peak identification (1)Check peak positions and relative peak intensities of 2 or more peaks (photoemission lines and Auger lines) of an element • Check spin orbital splitting and area ratios for p, d, f peaks A marine sediment sample from Victoria Harbor Si 2p Si 2s The following elements are found: O, C, Cl, Si, F, N, S, Al, Na, Fe, K, Cu, Mn, Ca, Cr, Ni, Sn, Zn, Ti, Pb, V Al 2s Al 2p

  9. Analysis Depth Inelastic mean free path (l) is the mean distance that an electron travels without energy loss For XPS,  is in the range of 0.5 to 3.5 nm Only the photoelectrons in the near surface region can escape the sample surface with identifiable energy Measures top 3 or 5-10 nm

  10. Redistribution of electron density B.E. provides information on chemical environment

  11. Example of Chemical Shift

  12. Example of Chemical Shift

  13. Chemical Shifts

  14. Chemical Shifts

  15. Factors Affecting Photoelectron Intensities For a homogenous sample, the measured photoelectron intensity is given by Ii,c: Photoelectron intensity for core level c of element i f: X-ray flux in photons per unit area per unit time Ni: Number of atoms of element i per unit volume si,c: Photoelectric cross-section for core level c of element i l: Inelastic mean free path of the photoelectron in the sample matrix q: Angle between the direction of photoelectron electron and the sample normal F: Analyzer solid angle of acceptance T: Analyzer transmission function D: Detector efficiency A: Area of sample from which photoelectrons are detected

  16. Quantitative Analysis Peak Area of element A Sensitivity factor of element A Peak Areas / Sensitivity factors of all other elements Au 4f Peak Area measurement Need background subtraction

  17. Empirical Approach Usually assume SF=1 For example, Teflon (-CF2-)

  18. Examples of Sensitivity Factors N = number of compounds tested

  19. X-ray damage Some samples can be damaged by x-rays For sensitive samples, repeat the measurement to check for x-ray damage.

  20. Charging Compensation Electron loss and compensation

  21. Note: for conducting samples, charging may also occur if there is a high resistance at the back contact.

  22. Differential (non-uniform) surface charging

  23. Charge Compensation Techniques Low Energy Electron Flood Gun

  24. Electron source with magnetic field Low energy electrons and Ar+ A single setting for all types of samples

  25. Shift in B.E. of a polymer surface

  26. Effects of Surface Charging

  27. Small area analysis and XPS Imaging

  28. Instrumentation • Electron energy analyzer • X-ray source • Ar ion gun • Neutralizer • Vacuum system • Electronic controls • Computer system Ultrahigh vacuum < 10-9 Torr (< 10-7 Pa) • Detection of electrons • Avoid surface reactions/ contamination

  29. XPS system suitable for industrial samples

  30. Vacuum Chamber Control Electronics Ion pump Turbopump Sample Introduction Chamber

  31. Dual Anode X-ray Source

  32. Commonly used

  33. X-ray monochromator Advantages of using x-ray monochromator • Narrow peak width • Reduced background • No satellite & ghost peaks

  34. Cylindrical Mirror Analyzer CMA: Relatively high signal and good resolution ~ 1 eV

  35. Concentric Hemispherical Analyzer (CHA) Resolution < 0.4 eV

  36. X-ray induced secondary electron imaging for precise location of the analysis area x-ray secondary electrons + 1 + 2 500 x 500mm

  37. Depth Profiling Sputtered materials Peak Area Sputtering Time

  38. Depth Scale Calibration • Sputtering rate determined from the time required to sputter through a layer of the same material of known thickness • After the sputtering analysis, the crater depth is measured using depth profilometry and a constant sputtering rate is assumed Peak Area Concentration Sputtering Time Depth

  39. Angle Resolved XPS

  40. Plasma Treated Polystyrene Angle-Resolved XPS Analysis High-resolution C 1s spectra

  41. Plasma Treated Polystyrene • O concentration is higher near the surface (10 degrees take off angle) • C is bonded to oxygen in many forms near the surface (10 degrees take off angle) • Plasma reactions are confined to the surface

  42. Angle-resolved XPS analysisOxide on silicon nitride surface

  43. Typical Applications

  44. Silicon Wafer Discoloration

  45. Depth Profiling Architectural Glass Coating • Architectural glass coating • ~100nm thick coating Sputtered crater Sample platen 75 X 75mm

  46. Depth profile of Architectural Glass Coating 100 80 O 1s O 1s O 1s 60 Ti 2p Atomic Concentration (%) 40 Nb 3d N 1s Ti 2p Si 2p Si 2p N 1s 20 Al 2p 0 0 200 Surface Sputter Depth (nm)

  47. 100 80 Atomic Concentration (%) 60 Ni 2p Cr 2p metal Cr 2p oxide Ni 2p Cr 2p metal Si 2p 40 O 1s 20 0 185 Sputter Depth (nm) 0 Nickel (30.3 nm) Depth profiling of a multilayer structure Chromium (31.7 nm) Chromium Oxide (31.6 nm) Nickel (29.9 nm) Chromium (30.1 nm) Silicon (substrate)

  48. Depth Profiling with Sample Rotation Ions: 4 keV Sample still Cr/Si interface width (80/20%) = 23.5nm Ions: 4 keV With Zalar rotation Cr/Si interface width (80/20%) = 11.5nm Ions: 500 eV With Zalar rotation Cr/Si interface width (80/20%) = 8.5nm

  49. Multi-layered Drug Package Optical photograph of encapsulated drug tablets SPS Photograph Cross-section of Drug Package Al foil Polymer Coating ‘A’ Polymer Coating ‘B’ Adhesion layer at interface ? 100 X 100mm 1072 X 812µm

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