lecture 7 chemical/electronic structure of glass fundamentals and

20
1 Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide Lecture 7 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)

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Page 1: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

1Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Lecture 7Chemical/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)

Page 2: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

2Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Bibliography

1. D. Briggs and M.P. Seah, Practical surface analysis, vol 1. Auger

and XPS. Wiley, 1990.

2. M.A. Sherwood in Surface imaging and visualization, A.T. Hubbard,

ed. Ch 63. CRC Press.

3. D.A. Skoog, F.J. Holler, T.A. Nieman, Principles of Instrumental

Analysis, Brooks/Cole. Ch. 21.

4. NIST X-ray Photoelectron Spectroscopy Database:

http://srdata.nist.gov/xps/

5. http://www.emsl.pnl.gov/new/emsl2002/tutorials/engelhard_xps.pdf

6. www.courses.vcu.edu/PHYS661/pdf/08TechSpectroscopy041.ppt

Page 3: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

3Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Outline

Introduction – chemical structure, electron spectroscopy

XPS as a tool for composition analysis

Surface limitation of XPS

Chemical structure

Spectrometer

Video tour of Scienta instrumenthttp://rm1.cc.lehigh.edu:8080/asxgen/dept/IMI/VirtualGl

assCourse/Video/XPS_miller150.wmv

Charging issues - special to glass

Page 4: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

4Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Different Aspects of the Static Structure

Physical structurePhysical arrangement of

atoms with respect to

each other (RM-O, M-O2,

CN, etc..)

•Short range order.

•Medium range structure.

Chemical structure•Nature of bonding

(covalency, ionicity,

basicity, etc...) between

different kinds of atoms.

•Charge distribution.

Vibrational structure•Bond strength

•Local vibrations of the

mobile atom.

•Vibrations of network

structural units of small and

medium size.

N a S i B O n B O

R a n d o m n e tw o r k st r u c tu r e o f a s o d iu m s il ic a te g la s s in tw o -d im e n s io n (a f te r W a r r e n a n d B is c o e )

Page 5: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

5Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

There are different manifestations of the same

overall glass structure

The various aspects are strongly interdependent, yet we

examine one aspect at a time due to the limitations of the

techniques and our own vision!

Page 6: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

6Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Electron Spectroscopy Techniques

• Photon in, Electron out

• Photoemission Spectroscopy (PES)

X-ray Photoemission Spectroscopy (XPS - 200 to 2,000 eV source)

Ultraviolet Photoemission Spectroscopy (UPS - 10 to 50 eV source)

• Auger Electron Spectroscopy (AES)

•Electron in, Electron out (inelastic)

•Auger Electron Spectroscopy (AES)

•Electron Energy Loss Spectroscopy (EELS)

Page 7: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

7Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

XPS: basic process

•Developed in the mid 1960s by K. Siegbahn et al.

•Awarded the Nobel Prize for Physics in 1981

Page 8: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

8Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Auger spectroscopy

ESCA => XPS + Auger

Auger (vs. XPS): Independent of input energy,

Sensitivity for low Z atoms,

High spatial resolution if e are used as excitation beam,

Minimal matrix effects,

Difficult quantitative analysis.

Auger electron:

KL1L2,3

Page 9: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

9Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

XPS: What do we detect?

e: discrete peak, e’: background that decreases with increasing k.e. Also a step at each peak.XPS info is from 10-100 A, depending on k.e.

K.E. = h – BE; if BE is w.r.t. vacuum level

Often for solids BE is defined w.r.t. Fermi

level. The measured KE should be corrected

for contact potential (i.e. work function of

sample and spectrometer), and any surface

charging of an insulating sample. Then

K.E. = h - BE - (sample) - (spectro.) - S

Page 10: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

10Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Relative intensity of XPS signal from different shells

Calculated cross sections (1.5 keV photon energy) give probabilities for observing electrons from various energy levels.

The intensity of XPS signal decreases with increasing shell, the valence band being the weakest.

Page 11: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

11Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Binding energy of electrons in various elements

BE for a particular electron shell is characteristic of the element

=>

Identify the element from its BE. However, watch out for interference as

the BE of different shell electrons of different elements may overlap!

Page 12: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

12Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Survey spectrum Identification of almost all elements in one experiments

Survey spectrum of an in situ fractured sodium diborate (Na2O-2B2O3) glass

Core levels and Auger

Valence band

Page 13: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

13Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Core level peak attributes:

•Height

•Area

•Asymmetry

•Position

•Spin-orbit split (for higher

than s-levels)

W 4f core level spectrum of W metal

exposed to air. Proctor and Sherwood, Anal. Chem. (1982).

Page 14: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

14Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

What can we learn from core level spectrum?•Compared to valence electrons, the core levels are

little affected by the bonding

•Core level BE is characteristic of the element, but it

is chemically shifted (0 to 10 eV) by interaction with

valence electrons and surrounding (mostly nearest

neighbor) atoms.

•Symmetric for insulator but asymmetric for metals

from excitation of conduction electrons.

•(p3/2, p1/2), (d5/2, d3/2), (f7/2, f5/2).. levels show two

peaks from spin-orbit coupling. The ratio of

respective peaks are: 2/1; 3/2; 4/3

=>

Core level XPS gives qualitative and quantitative

chemical structure around particular element

(excluding H and He).

•The area under a core level peak is concentration of the element =>

Get composition using reference sensitivity factors.

Page 15: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

15Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Change in composition along the glassware height

0

0.1

0.2

0.3

0.4

0.5

0 1 2 3 4 5 6Going down from the Rim

Na/Si

Al/Si

Si/O

Variation of surface composition

5

4

3

2

1

Page 16: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

16Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

After washing

• Na

• Ca

• Al

• Si/O

Rim region

0

0.1

0.2

0.3

0.4

0.5

0.6

Na/Si Al/Si Ca/Si Si/O

Unwashed

washed

Milky region

0

0.1

0.2

0.3

0.4

0.5

Na/Si Al/Si Ca/Si Si/O

Unwashed

Washed

Effect of corrosion on surface composition: leaching vs. uniform dissolution

•Rim is richer in alumina.

Page 17: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

17Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

XPS sees only the surface region

(XPS info is from 10-100 A, depending on k.e.)

Page 18: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

18Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

0

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0.5

Na/Si Ca/Si Si/O

Bulk

Surface

Glass composition: surface vs. bulkHigh resolution X-ray photoelectron spectroscopy

Preferential loss of alkali and alkaline earth oxide from the surface.

Page 19: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

19Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

x-ray

beam

Electron

detectorLaser light

beam

Take-off angle

= 90

specimen

x-ray

beam

Electron

detector

Laser light

beam

Take-off angle

= 5

specimen

Surface sensitivity => Angle Resolved XPS

(XPS info is from 10-100 A, depending on k.e.)

Obtain depth profile of the chemical info!

Page 20: Lecture 7 Chemical/Electronic Structure of Glass Fundamentals and

20Formation and Structure of Glass Feb 7, 2007. Jain/Lehigh slide

Composition as f(depth, ambient)

As50Se50 film on Si, irrad.

in air for ~12 h

0

10

20

30

40

50

60

70

80

0 5 10 15 20 25 30 35

Depth (Angstrom)

Co

ncen

trati

on

(%

)

O (Irradiated in air)

As (Irradiated in air)

Se (Irradiated in air)

As (as-prepared film)

Se (as-prepared film)