Short range ordering in InxGa1-xAs1-yNy, a dilute III-V nitride

Slides:



Advertisements
Similar presentations
01/09/ Subnanosecond spectral diffusion of a single quantum dot in a nanowire G. Sallen, A. Tribu, T. Aichele*, R. André, L. Besombes,
Advertisements

RHESSI Studies of Solar Flare Hard X-Ray Polarization Mark L. McConnell 1, David M. Smith 2, A. Gordon Emslie 4, Martin Fivian 3, Gordon J. Hurford 3,
Raman Spectroscopy A) Introduction IR Raman
The physics of blue lasers, solar cells, and stop lights Paul Kent University of Cincinnati & ORNL.
1 Electron magnetic circular dichroism Pavel Novák Institute of Physics ASCR, Prague, Czech Republic.
Molecular Fluorescence Spectroscopy
Approaches to Data Acquisition The LCA depends upon data acquisition Qualitative vs. Quantitative –While some quantitative analysis is appropriate, inappropriate.
Center to Limb Variation of Hard X-Ray Spectra from RHESSI J.McTiernan (SSL/UCB) ABSTRACT: We use the RHESSI flare database to measure the center to limb.
Center to Limb Variation of Hard X-Ray Spectra from RHESSI J. McTiernan SSL/UCB.
Atom and Quantum. Atomic Nucleus Ernest Rutherford Rutherford’s Gold Foil Experiment Deflection of alpha particles showed the atom to be mostly.
X-ray Polarization as a Probe of Strong Magnetic Fields in X-ray Binaries Shane Davis (IAS) Chandra Fellows Symposium, Oct. 17, 2008.
MACRO Atmospheric Neutrinos Barry Barish 5 May 00 1.Neutrino oscillations 2.WIMPs 3.Astrophysical point sources.
Synchrotron Radiation Interaction with Matter; Different Techniques Anders Nilsson Stanford Synchrotron Radiation Laboratory What can we hope to learn?
Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Ray Absorption Spectroscopy J. Stöhr, NEXAFS SPECTROSCOPY,
1 M. Aslam Baig National Center for Physics Quaid-i-Azam University Campus, Islamabad Pakistan
1 Lecture: Solid State Chemistry (Festkörperchemie) Part 2 (Further spectroscopical methods, ) H.J. Deiseroth, SS 2004.
Lyes Lakhal Institut Polytechnique LaSalle Beauvais Rue Pierre WAGUET
Determination of Crystal Structure (From Chapter 10 of Textbook 2) Unit cell  line positions Atom position  line intensity (known chemistry) Three steps.
Hard X and Gamma-ray Polarization: the ultimate dimension (ESA Cosmic Vision ) or the Compton Scattering polarimetery challenges Ezio Caroli,
Conception of cross section 1) Base conceptions – differential, integral cross section, total cross section, geometric interpretation of cross section.
Atomic Scale Ordering in Metallic Nanoparticles Structure: Atomic packing: microstructure? Cluster shape? Surface structure? Disorder?
Precision analysis of Geant4 condensed transport effects on energy deposition in detectors M. Batič 1,2, G. Hoff 1,3, M. G. Pia 1 1 INFN Sezione di Genova,
ChE 553 Lecture 9 Statistical Mechanics Of Adsorption 1.
Electron Energy Loss Spectroscopy (EELS) Suggested Reading: Used electron spectrometer Used TEM Review of theory for elastic + inelastic scattering Examples.
Raman Spectroscopy A) Introduction IR Raman
Generalized van der Waals Partition Function
Ion Beam Analysis of the Composition and Structure of Thin Films
Chapter 13 Sampling distributions
Information content: EXAFS, SEXAFS: Bond lengths. Especially useful because these technique probe the local order.
Figure 2: raw absorption spectra for all the samples: EXAFS region. In red is the Fourier filtered nearest neighbour signals. XANES features reflects the.
EXAFS-spectroscopy method in the condensed matter physics: First results on energy-dispersive EXAFS station in RSC “Kurchatov Institute” Vadim Efimov Joint.
F. *Gonella and P. Mazzoldi, "Metal Nanocluster Composite Glasses", in: Handbook of Nanostructured Materials and Nanotechnology, H.S. Nalwa, ed., Vol.
K. Klementiev – Introduction to XAFS theory 1 of 11 Introduction to X-ray Absorption Spectroscopy: Introduction to XAFS Theory K. Klementiev,
Energy Bands and Charge Carriers in Semiconductors
Presentation on SEM (Scanning of Electron Microscope) Represented by:-Ravi Kumar Roll:- (BT/ME/1601/006)
Polarization Dependence in X-ray Spectroscopy and Scattering
Measurement of high energy cosmic rays by the new Tibet hybrid experiment J. Huang for the Tibet ASγCollaboration a a Institute of high energy physics,
Regression Analysis.
Sol–gel preparation of efficient red phosphor Mg2TiO4:Mn4+ and XAFS investigation on the substitution of Mn4+ for Ti4+ Tiannan Ye, Shan Li, Xueyan Wu,
Nature of the Band Gap in the Transparent Conducting Oxide In2O3
Electromagnetic Waves
Conductivity Charge carriers follow a random path unless an external field is applied. Then, they acquire a drift velocity that is dependent upon their.
Theoretical study of a domain wall through a cobalt nano-contact
Today’s objectives- Semiconductors and Integrated Circuits
A.P. Potylitsyn, I.S. Tropin Tomsk Polytechnic University,
Spin-orbit interaction in a dual gated InAs/GaSb quantum well
Davide De Salvador INFN-Laboratori Nazionali di Legnaro &
Interaction between Photons and Electrons
International Workshop on radiosensitization
THE SIMULATION OF POLARIZED BARYONS
Presented by UGA’s Academic Resource Center 02/28/16
UV SPECTROSCOPY Absorption spectra.
Light Interactions The law of reflection states that the angle of incidence is equal to the angle of reflection. Things that are luminous can be seen because.
Effects of Si on the Electronic Properties of the Clathrates
Exclusive Neutral Pion Production at JLab Hall A
Local Structure around In Atoms in InxGa1-xN Single-Quantum-Well by XAFS T. Miyanaga Department of Materials Science and Technology, Faculty of Science.
Searching for states analogous to the 12C Hoyle state in heavier nuclei using the thick target inverse kinematics technique. Marina Barbui 5/17/2018, Galveston,
BAND GAP ENGINEERING Trends in cubic UC parameters and Eg As a function of composition x for the solid solution ternary semiconductor AlxGa1-xAs.
Presented by Rhee, Je-Keun
Raman Spectroscopy A) Introduction IR Raman
Lecture 4.
X- and gamma-ray focal plane for future space missions
Absorption Corrections Spencer Howells
Volume 83, Issue 3, Pages (September 2002)
Instrumental Analysis
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
3.5 Energy levels and spectra
Sensitivity curves beyond the Advanced detectors
Body centered cubic Note that each corner atom is in eight cubes so only 1/8 of the corner atom is in this cell Number of atoms = 1 center + 8 x 1/8 corners.
Raman Spectroscopy A) Introduction IR Raman
Presentation transcript:

Short range ordering in InxGa1-xAs1-yNy, a dilute III-V nitride G. Ciatto,1 F. d'Acapito,2 F. Boscherini,3 S. Mobilio,4 D. Batchelor,5 D. De Salvador,6 G. Bisognin,6 R. Carboni,3 L. Floreano,7 R. Gotter,7 L. Grenouillet,8 and H. Mariette9 GILDA – CRG General purpose Italian beam Line for X-ray Diffraction and Absorption  1CNR c/o ESRF - Gilda CRG, Grenoble, France; 2INFM c/o ESRF - Gilda CRG, Grenoble, France; 3INFM and Physics Dept., University of Bologna, Italy. 4 Physics Dept, University of Rome III, Italy; 5 BESSY, Berlin, Germany;6 INFM and Physics Dept., Univ. of Padova, Italy; 7TASC-INFM, Trieste, Italy; 8CEA/LETI, Grenoble, France; 9 CEA-CNRS, University J.Fourier, Grenoble, France What do we mean for short range ordering (SRO) ? Why is it important ? N In As Ga In a quaternary alloy the relative number of bonds is not fixed by the composition, a particular bonding can be energetically favored with respect to an other. In InxGa1-xAs1-yNy an excess of In-N bonds with respect to the random case has been predicted at the equilibrium by Monte Carlo simulations (Kim and Zunger, PRL, 2001). SRO causes a larger statistical presence of N-centered In3Ga1 clusters, whose energy level is higher than that of N-centered In0Ga4 clusters. This leads to a diminished downward repulsion of the conduction band, so to a larger band gap. Since the technological interest of these alloys resides in the emission at very high wavelengths what predicted would result in an intrinsic material limitation. What do we do ? By In K-edge EXAFS we measure the relative In-N coordination, which we can compare with the random one: this allows us to quantify the actual SRO. Due to N dilution and low backscattering amplitude N-related paths have a small amplitude and a statistical analysis following standard criteria (Sayers, IXS 2000) is necessary in order to demonstrate their reliability. The results indicate a weak ordering in annealed samples. By N K-edge XANES we qualitative exclude the presence of strong ordering, even in annealed (closer to equilibrium) samples. Simulations performed in the Full Multiple Scattering approach (in dots) show that N K-edge XANES cannot exclude the presence of weak ordering and are compatible with In K-edge results. By exploiting the polarization dependency of XAFS we can demonstrate that N is totally substitutional to As. Spectra taken at different incidence angles, in fact, are virtually identical and XANES resonances do not show any angular dependence, which is a fingerprint of the cubic geometry of the zinc blend structure (G. Ciatto et. al., Phys. Scripta, 2004). What have we found out ? We gave the first quantitative determination of SRO in InxGa1-xAs1-yNy.. Virgin samples are virtually random alloys while annealed samples (closer to the equilibrium condition of the predictions) show a weak ordering, to which we are sensitive with our techniques. Even if the probability of an N atom to occupy a In-nearest neighbor site is up to three times the random one, our measured order parameters are about one order of magnitude smaller than the predicted (G. Ciatto et al., PRB - RC , 2003).