anomalous x-ray diffraction studies for photovoltaic applications

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Anomalous X- ray Diffraction Studies for Photovoltaic Applications Grisel Rivera Batista Science Undergraduate Laboratory Internship Program August 12, 2010.

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Grisel Rivera Batista Science Undergraduate Laboratory Internship Program August 12, 2010. Anomalous X-ray Diffraction Studies for Photovoltaic Applications. Advantages of AXRD. Sensitive to: N eighboring elements in the periodic table. Specific crystallographic phase. - PowerPoint PPT Presentation

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Page 1: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Anomalous X-ray Diffraction Studies for Photovoltaic ApplicationsGrisel Rivera BatistaScience Undergraduate Laboratory Internship ProgramAugust 12, 2010.

Page 2: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Advantages of AXRD

Sensitive to: Neighboring

elements in the periodic table.

Specific crystallographic phase.

Specific crystallographic site in a phase.

Page 3: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
Page 4: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

AXRD – Combination of Structural & Chemical TechniqueStructural (XRD) Chemical (XAS)

X-rays diffract from specific

planes

Diffraction peak

Near resonant absorption

energy

X-raysabsorbed

RESULT

Diffracted peak intensity ↓ depending on elements present on diffracting planes

0.0

0.2

0.4

0.6

0.8

1.0

2.182.23

2.289600 9650 9700 9750 9800

Inten

sity,

I (a.u

.)

Misra, S., Bettinger J., Anomalous X-ray Diffraction (AXRD), 5thAnnual SSRL School on Synchrotron X-ray Scattering Techniques in Materials and Environmental Sciences: Theory and Application. June 1st, 2010

Page 5: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

fn = f0(Q) + f ′(E) + i f ′ ′(E)f0(Q) = normal (E independent)f ’(E) = anomalous (E dependent)f ’’(E) = absorption (E dependent)

atoms

n

lzkyhxinlkh

nnneEfF1

2),,( )(

• fn is the atomic scattering factor• xn, yn, zn are the (fractional) positions of the nth atom

• Atomic scattering strength (fn) varies near X-ray absorption edge• Varying X-ray energy near absorption edge → total intensity changes• fn depends on oxidation state of the elementVariation for Zn

Energy, E (eV)9000 9200 9400 9600 9800 10000 10200

Scatt

erin

g Stre

ngth

10

12

14

16

18

20

22

24

Scatt

erin

g Stre

ngth

0

2

4

6

8

10

f0+ f'f''

Anomalous X-ray Diffraction (AXRD)

2hklhkl FI

Misra, S., Bettinger J., Anomalous X-ray Diffraction (AXRD), 5thAnnual SSRL School on Synchrotron X-ray Scattering Techniques in Materials and Environmental Sciences: Theory and Application. June 1st, 2010

Page 6: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

ZnO loaded with Gallium

Zinc

oxygen

Tetrahedral sites in ZnO cell

Page 7: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Q (Å -1)2.0 2.5 3.0 3.5 4.0

Inten

sity (

a.u.)

0.020.040.060.080.100.120.140.160.18

(101)

(002)

(102)

(110)

(100)

(103)

(200)

(112)(201)

ZnO loaded with Ga

Page 8: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Peak 100

Page 9: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
Page 10: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
Page 11: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
Page 12: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Spinel: ZnCo2O4

Zn, Co

Oxygen

Page 13: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Spinel Inversion

Inversion determines the amount of each cation found on either the tetrahedral or octahedral site, and has a big effect on the electrical properties.

MixedSpinel

(0 <n < 1

Normal spinel (n 0

(Co) (Zn) (Co)B A B

Inverse spinel (n 1

(Co) (Co) (Zn)B A B

Degree of Inversion Continuum

Page 14: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

Peak 311

Page 15: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
Page 16: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
Page 17: Anomalous X-ray Diffraction Studies for Photovoltaic Applications
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ConclusionAXRD is an effective technique to characterize bulk and nanomaterials.

Page 19: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

AcknowledgmentsU.S. Department of Energy, Office of Science, through the Summer Undergraduate Laboratory Internship Program (SULI)

Stanford Synchrotron Radiation Lightsource (SSRL) at SLAC National Accelerator Laboratory.

My mentors Michael Toney, Sumohan Misra, and Joanna Bettinger for their guidance during the realization of my project.

Stephen Rock and all the SULI staff at SLAC for give me the opportunity to work during this summer under their program.

Page 20: Anomalous X-ray Diffraction Studies for Photovoltaic Applications

References Bettinger, J., Misra, S. Anomalous X-ray Diffraction (AXRD), California. 2010.  Bettinger, J. Probing the Effects of Dopants, Defects, and Crystal Structure in

Spinel Transparent Conducting Oxides for Photovoltaic Applicationsi, California.  Granqvist, C. G., Transparent conductors as solar energy materials: A panoramic

review, Department of Engineering Sciences, The Ångström Laboratory, Uppsala University, Uppsala, Sweeden. 2007.

  Introduction to X-ray Diffraction, Materials Research laboratory, University of

California, Santa Barbara. 2010.  Thomas, R.K., Simple Solids and their Surfaces [Online]. Available:

http://rkt.chem.ox.ac.uk/tutorials/surfaces/solids.html  Pecharsky, V. K., Zavalij, P.Y., Fundamentals of Powder Diffraction and Structural

Characterization of Materials, Page 146-152, Springer, New York. 2005.

Cullity, B.D., Stock, S.R., Elements of X-Ray Diffraction, Page 31-47, Prentice Hall, New Jersey. 2001.

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Questions?