Lecture 8 Chemical/Electronic Structure of Glass

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Lecture 8 Chemical/Electronic Structure of Glass Syllabus Topic 6. Electronic spectroscopy studies of glass structure Fundamentals and Applications of X-ray Photoelectron Spectroscopy (XPS) a.k.a. Electron Spectroscopy for Chemical Analysis (ESCA) 1

Review of Lecture 7 XPS data come with Auger as by-product. XPS of solids consists of core levels and valence band. Intensity of core levels decreases with decreasing BE. BE of a given level is unique to the particular element. ARXPS allows depth profile by varying the angle between the detector and sample surface normal. XPS probes <10 nm of the surface region. The area under the peak of a core level peak is directly proportional to the concentration of that particular element. 2

Chemical Structure by XPS Charge potential model for bonds Free atoms Bonded atoms Consider valence electrons as hollow charged sphere. Neglecting relaxation effects: E i = E i0 + q i /r v + i=j q i /r ij E i = q i /r v + ( i=j q i /r ij ) q i for valence electrons => change in energy of all inner level by q i /r v where r v is the valence shell radius. http://ligand-depot.rcsb.org/marvin/chemaxon/marvin/help/charge.html 3

Chemical Shifts of Si oxide Si 2p Core Level Binding energy increases with increasing oxidation state of the cations. http://www.emsl.pnl.gov/new/emsl2002/tutorials/engelhard_xps.pdf 4

Sensitivity of core levels to local bonding Map the peaks for the four kinds of C in the molecule! 1 2 3 4 C 1s spectrum of ethyl trifluoroacetate 3 1 2 4 5

Polymethylmethacralate (PMMA) A deconvolution procedure may be needed when the components are not resolved. To obtain unique decomposition of spectrum, additional information may be required, including estimates from ab initio simulations. 6

Silica glass structure modification by alkali oxide addition N a S i B O n B O R a n d o m n e tw o r k str u c tu r e o f a s o d iu m s ilic a te g la s s in tw o -d im e n s io n (a fte r W a r r e n a n d B is c o e ) 7

Formation of NBO with the addition of M 2 O O 1s spectrum of sodium silicate glass?? Na Auger?? What do the two?? marked peaks represent? C. H. Hsieh et al. J. Non-cryst. Solids 168, 247-257 (1994). 8

O 1s Chemical shift ( NBO-BO ) in silicate glasses 9

O 1s spectra of sodium silicate, borate, germanate and tellurite glass series (a). xna 2 O-(1-x)SiO 2 (b). xna 2 O-(1-x)B 2 O 3 (c). xna 2 O-(1-x)GeO 2 (d). xna 2 O-(1-x)TeO 2 What question was raised earlier in the course with regard to the difference in the structure of alkali silicates and germanates? Nanba and Miura 10

Network modification in alkali germanate glasses Addition of alkali means two choices: Creation of NBO as in silicates or Change of Ge from tetrahedral to octahedral coordination Xu et al. Phys Chem Glass (1996) 11

NBOs vs Ge-octahedra? 12

O-1s BE for SiO 2 533.0 Polycrystalline powder of stishovite, natural mineral from meteor crater Arizona, the densest modification of SiO2 533.2 Alpha-quartz 532.9 pelletized, composition determined by XPS is SiO2.08 533.8 Thermal oxide - SiO2.1. 532.7 Thermaly grown SiO2 532.7 Fused quartz. 532.8 alpha phase, insulator, polycrystalline 533.2 Quartz (rock crystal). 532.0 Polycrystalline powder of stishovite from meteor crater, Arizona NIST X-ray Photoelectron Spectroscopy Database: http://srdata.nist.gov/xps/ 13

XPS instrument schematic 14

Complications of XPS on glass Charging of surface Error in BE Error in composition Damage by sputtering (if used in depth analysis) Alteration of structure 15

Charging of insulating sample Net build up of charge on the surface when e loss is not compensated by inward flow => Surface at unknown +V => All peaks shifted/broadened by ~ the same amount. Problem mostly corrected by flooding with low energy e. For precise b.e. values, need a reference: 1. Adventitious C-1s (may not be present on pristine surface) 2. Thin overlayer of Au 3. Internal reference e.g. Si-2p in silicate glasses. 4. Use Auger parameter 16

17

f NBO vs. time of XPS experiment Soda-Lime-Silicate Glass 13.30Na 2 O 11.62CaO 73.86SiO 2 (mole %) 18

Na/Si Na conc. vs time 0.55 0.5 0.45 0.4 0.35 0.3 0.25 0 10 20 30 Time (h) x-rays + e x-rays e X-irradiation is the primary cause for Na accumulation. Once liberated, Na can migrate to the surface very quickly, if e-field is present. 19

O/Si Total oxygen vs time 2.4 2.3 2.2 2.1 2 1.9 1.8 1.7 X-rays + e X-rays e 0 10 20 30 Time (h) The loss of oxygen is mostly determined by x-ray dose; electrons retard it. 20

Contrast of x-ray and e-gun effects e-gun X-rays e-gun + X-rays For experimental reasons, both e-gun and x-rays had to be used during analysis of all cases. 21

Summary: XPS capabilities Elements detected from Li to U. Nondestructive (x-ray beam damage in certain materials?) Quantitative. Chemical bonding (e-density) analysis. Surface sensitivity from 5 to 75 angstroms. Conducting and insulating materials. Detection limits that range form 0.01 to 0.5 atom percent. Spatial resolution for surface mapping from >10 m. Depth profiling (non-destructive as well as destructive). 23