Coherent X-ray Diffraction on Quantum Dots
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1 Coherent X-ray Diffraction on Quantum Dots Ivan Vartaniants HASYLAB, DESY, Hamburg, Germany Or Coming Back to Crystallography
2 Participants of the Project University of Illinois, Urbana-Champaign, IL, USA Prof. Ian Robinson G. Williams M. Pfeifer J. Onken M.Liang F. Pfeiffer, Swiss Light Source, PSI, Switzerland Zh. Zhong, MPI, Stuttgart Prof. Gunter Bauer, Inst. für Halbleiter-und Festkörperphysik, Austria H. Metzger, ESRF, France 2
3 CONTENTS 1. Introduction 2. Imaging of QD s with Coherent X-ray Beams 3. Experiment (Ge islands on Si 4. Reconstruction of QD s from GISAXS data 5. Problems & Future Direction 6. Conclusions 7. Coherent X-ray Diffraction Project at DESY 3
4 Motivations 1. Electronic and optical properties of nano-devices depend on the structure (shape and strain 2. Development of different scattering methods for imaging nano-structures is extremely important Imaging Can we compete with electron microscopy? 4
5 Coherent X-ray Diffraction or X-ray Lensless Microscopy CCD Partially Coherent X-rays sample CCD First approach: Focusing Optics 5
6 Focusing Optics KB mirrors mirrors sample 100(V 200(H mm Focal spot size 1.5(H 1.0(V µm Robinson et.al., (2003 Optics Express, 11, 2329 Coherent X-ray Diffraction pattern from Ag nanocrystals of size D=170 nm 6
7 Alternative Approach: Using Periodic Array of Quantum Dots Motivations: Using a periodic patterned array for bio-molecules imaging I. Vartanyants & I. Robinson, J. Synchrotr. Rad. (2003, 710, 409
8 Imaging of biomolecules with femtosecond X-ray pulses Explosion of T4 lysozyme induced by radiation damage R. Neutze, et al., Nature ( , 752 8
9 Imaging of Biomolecules with Femtosecond X-ray Pulses Simulated continuous scattering image of a single T4 lysozyme molecule under ideal conditions without sample movement or damage. R. Neutze, et al., Nature ( , 752 9
10 Imaging of Quantum Dots with Coherent Beams Source Sample CCD [ s ( r p ( ] p( r S( r r = z S(r shape of coherently illuminated area s z (r projection of shape of one island s(r,z Electron density of periodic array of QD s p ( r = δ ( r rn n Diffracted intensity: I 2 2 coh ( q = A coh ( q = s z ( hn S( q hn n 10 2
11 2D array of QD s and it s diffraction pattern 2D array of QD s Diffraction pattern of 2D array Image of individual island Diffraction pattern of individual island 11
12 Iterative phase retrieval algorithm s k (x FFT A k (q Real Space Constraints Reciprocal Space Constraints s' k (x FFT -1 A' k (q Real space constraints: finite support real, positive Reciprocal space constraint: A k ( q I exp ( q J.R. Fienup, Appl Opt. ( , R.P. Millane & W.J. Stroud, J. Opt. Soc. Am. (1997 A14, 568
13 Reconstructed image of 2D array of QD s Support used for reconstruction Diffraction intensity of reconstructed image Reconstructed image Reconstructed image with superposition of twin images 13
14 Experiment 14
15 Experiment (Sector 34 APS 1.95 Qz AFM image of 2D ordered Ge islands with corresponding line scans Z. Zhong & G. Bauer Q x Diffraction pattern around Ge (202 peak I. Vartaniants et. al., PRB 71, (2005
16 GISAXS measurements α i > α c ; α f < α i α i < α c ; α f > α i 1.2 deg α f =α i α f 0.7 deg α f =α c 0.2 deg µm µm -1 Q y -160 µm µm -1 Q y 16
17 Ewald sphere construction Q z CCD 2π/d x k f 2π/s z 2π/N x d x k i Q x 17
18 Reconstruction of quantum dot shape GISAXS measurements (α i < α c 930 µm µm 1 µm Q z Experimental Data (Log scale 240 µm µm µm -1 Q y Reconstruction 18
19 Reconstruction of quantum dot shape GISAXS measurements (α i < α c Final support 0.43 µm Best real space image Comparable with resolution in electron microscopy Average size: 128(H 45(V nm Resolution: 20(H 5(V nm 19
20 Reconstruction of quantum dot shape GISAXS measurements (α i < α c 930 µm -1 Q z 240 µm µm -1 0 Q y 190 µm µm -1 Q y 190 µm -1 Experimental Data (Log scale Reconstruction 20
21 Questions Problems Future Directions 21
22 Simulation of diffraction pattern Beam stop effects An array of quantum dots used for simulation 786 px Simulated diffraction pattern R 0 Beam stop 444 px 22
23 Test Reconstructions for the Different Size of the Beam Stop R 0 =0 px R 0 =10 px R 0 =20 px R 0 =30 px R 0 =40 px R 0 =50 px 23
24 Anomalous Ge K-edge Energy E(keV In this way we hope to separate Ge and Si contributions 24
25 25 Simulations Using DWBA Theory + = island i dv e A r q q r q ( ( ( χ + = island i f dv e R A r q q r q ( ( ( ( χ α + = island i f i dv e R R A r q q r q ( ( ( ( ( χ α α + = island i i dv e R A r q q r q ( ( ( ( χ α M. Schmidbauer et al., Phys. Rev. B ( ,
26 Simulations Using DWBA Theory 60 nm q z (Å -1 α i =0.1 Ge 60 nm Si 120 nm q z (Å -1 α i =0.3 D. Grigoriev, HU Berlin q y (Å -1 26
27 Simulations Using DWBA Theory I(q= A 1 (q 2 I(q= A 1 (q+ A 4 (q 2 I(q= A 1 (q+ A 2 (q+ A 4 (q 2 I(q= A 1 (q+ A 2 (q+ A 3 (q+ A 4 (q 2 27
28 Conclusions and Outlook Periodic systems of quantum dots can be effectively imaged with coherent x-rays with nanometer resolution Coherent X-ray Diffraction on buried quantum dot systems Coherent X-ray Diffraction on a patterned biological samples (viruses, molecules and etc. 28
29 Coherent X-ray Diffraction Project at HASYLAB Andreas Schropp Christian Schroer Edgar Weckert
30 Experiment on ID-01 in ESRF Staff of ID-01: Hartmut Metzger Christian Mocuta, Peter Boesecke CCD Sample 100 µm 40 µm 4.2 m 18 cm 80 cm 30
31 Diffraction Pattern 7 kev 700 px (120 µm px (85 µm -1 Simulation 31
32 Samples Electron Microscopy O. Kuparova, II Physikalishes Institut, Aachen First Results of Reconstruction 32
33 Thank you for your attention 33
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