Supplementary. respectively.
|
|
- Solomon Price
- 5 years ago
- Views:
Transcription
1 Figure S1. HAADF STEM images of Ag NRod interacting with Au NP (a and b) and Au NRod with Ag NP (c and d). Interface areas are labeled with ellipse. Itt can be seen thatt when interface was oriented parallel to the electron beam, a sharp contrast transition across the interface was observed. Alloying, i.e. atomic intermixing is expected to make the t interface appearance smooth in HAADF STEM image. Therefore we w concluded that merging of Au and Ag NPs was not accompanied by an alloying. HAADF STEM S image of merging between Au NRod and Ag NP (e) and thee EDS line scan acquired along the line 1 shown on the image (f). Blue and red lines are related to X Ray photons of Ag K and Auu M series, respectively.
2 Figure S2. These TEM images preset a projected straight profile that represented an initially flat atomic face of Ag NRod (a) with the flat f projectedd parallel edges labeled by the black line. In due course of merging the projectedd profile of the rod significantly changed in spite of the samee projection angle (b). Namely: i) instead of a single straight profile we observe two t edges (shown in black lines); ii) the lower darker edge appears less curved, but the upper lighter one appears as an ark with the estimated radius of curvature of 50 nm.
3 Figure S3. The red square shows the scanned region at which we collected EDS maps of Ag K (left) and Au M (right) series.
4 Figure S4. Snapshots at molecular dynamics time 10 33ns, the diameter of the dot and rod vary between 7 to 2.3 nm. The red arrow indicates the wetting and welding events in the Ag dot/au rod and Au dot/ /Ag rod structures. Both the Au and Ag rods are <111> exposure. The bottom centered image presents an example of nanoparticles with decahedron shape.
5 Figure S5. (a) RDF plot for the structure with d=3nm, D=5nmm respectively, the simulation time is 10ns. hcp dislocation marked in pink, the dot d part represents the hcp in Silver part, From the RDF we can see in the central part, some Ag and Au atoms are mixing. (b) RDF plot for the structure s with d=5nm, D=5nm respectively, the simulation time is 10ns. (c) Statistical angle distribution plot for the silver wettingg cases.
6 Figure S6. (a) Side and cross sectional views for the contact made of gold NPs and silver rods. The silver rods are bound with {111} and {110}, respectively. The pink (with black dots) balls represent the stacking faults in gold (silver) nanomaterials. (b) The stacking faults in the merged Au and Ag NPs. The pair of green lines notifies a faulty sequence of atomic planes in AuNRod aligned with the same structural fault in AgNP (the red pair of lines).
7 Figure S7. (a and b) For justification of the potential, we found that this set s of EAM potential reproduces experimental data with good agreement on lattice parameters, bulk modulus, cohesive energy, elastic constants, sublimation energies, and heats of solution. Also, we have performed benchmark on phonon band structures s and elastic constants calculations for both Ag and Au bulks, to further checkk the quality of EAM potential used in this work ( Dong, H.; Moon, K. S.; Wong, C. P.; Ieee, Molecular dynamicss study on coalescence of silver (Ag) nanoparticles and their deposition on goldd (Au) substrates. 2004; p ). (c) Comparison with C.P. Wong s work w in a (400K) and b (1000K) (Dong, H.; Moon, K. S.; Wong, C. P.; Molecular dynamicss study on coalescence off silver (Ag) nanoparticles and their deposition on gold (Au) substrates. J. Electronic Mater. 34, 40 (2004)). a and b are from our simulations at 400K and 1000K, respectively.
Supplementary information
Electronic Supplementary Material (ESI) for Nanoscale. This journal is The Royal Society of Chemistry 2014 Supplementary information Real-time imaging and elemental mapping of AgAu nanoparticle transformations
More information1-amino-9-octadecene, HAuCl 4, hexane, ethanol 55 o C, 16h AuSSs on GO
Supplementary Figures GO Supplementary Figure S1 1-amino-9-octadecene, HAuCl 4, hexane, ethanol 55 o C, 16h AuSSs on GO Schematic illustration of synthesis of Au square sheets on graphene oxide sheets.
More informationa b c Supplementary Figure S1
a b c Supplementary Figure S1 AFM measurements of MoS 2 nanosheets prepared from the electrochemical Liintercalation and exfoliation. (a) AFM measurement of a typical MoS 2 nanosheet, deposited on Si/SiO
More informationElastic and Inelastic Scattering in Electron Diffraction and Imaging
Elastic and Inelastic Scattering in Electron Diffraction and Imaging Contents Introduction Symbols and definitions Part A Diffraction and imaging of elastically scattered electrons Chapter 1. Basic kinematical
More informationWeak-Beam Dark-Field Technique
Basic Idea recall bright-field contrast of dislocations: specimen close to Bragg condition, s î 0 Weak-Beam Dark-Field Technique near the dislocation core, some planes curved to s = 0 ) strong Bragg reflection
More informationSupporting Information
Supporting Information Highly Sensitive, Reproducible, and Stable SERS Sensors Based on Well-Controlled Silver Nanoparticles Decorated Silicon Nanowire Building Blocks Xue Mei Han, Hui Wang, Xue Mei Ou,
More informationTechniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications
Techniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications Thomas Neisius Université Paul Cézanne Plan Imaging modes HAADF Example: supported Pt nanoparticles Electron sample interaction
More informationSupplementary Information
Supplementary Information Supplementary Figure 1. X-ray diffraction patterns of (a) pure LDH, (b) AuCl 4 ion-exchanged LDH and (c) the Au/LDH hybrid catalyst. The refined cell parameters for pure, ion-exchanged,
More informationOverview of scattering, diffraction & imaging in the TEM
Overview of scattering, diffraction & imaging in the TEM Eric A. Stach Purdue University Scattering Electrons, photons, neutrons Radiation Elastic Mean Free Path (Å)( Absorption Length (Å)( Minimum Probe
More informationSUPPLEMENTARY MATERIALS FOR PHONON TRANSMISSION COEFFICIENTS AT SOLID INTERFACES
148 A p p e n d i x D SUPPLEMENTARY MATERIALS FOR PHONON TRANSMISSION COEFFICIENTS AT SOLID INTERFACES D.1 Overview The supplementary information contains additional information on our computational approach
More informationSUPPLEMENTARY INFORMATION
Lateral heterojunctions within monolayer MoSe 2 -WSe 2 semiconductors Chunming Huang 1,#,*, Sanfeng Wu 1,#,*, Ana M. Sanchez 2,#,*, Jonathan J. P. Peters 2, Richard Beanland 2, Jason S. Ross 3, Pasqual
More informationTitle of file for HTML: Supplementary Information Description: Supplementary Figures and Supplementary References
Title of file for HTML: Supplementary Information Description: Supplementary Figures and Supplementary References Supplementary Figure 1. SEM images of perovskite single-crystal patterned thin film with
More informationSchool of Chemical and Biological Engineering, College of Engineering, Seoul National University, 599 Gwanangno, Gwanakgu, Seoul , Korea ACS
School of Chemical and Biological Engineering, College of Engineering, Seoul National University, 599 Gwanangno, Gwanakgu, Seoul 151-742, Korea ACS Appl. Mater. Interfaces 2015, 7, 1746 1751 (DOI: 10.1021/am507314t)
More informationSupporting Information
Supporting Information Remarkable Photothermal Effect of Interband Excitation on Nanosecond Laser-induced Reshaping and Size Reduction of Pseudo-spherical Gold Nanoparticles in Aqueous Solution Daniel
More informationElectronic Supplementary Information
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Electronic Supplementary Information CW-Laser-Induced Morphological Changes of
More informationIntroduction to Solid State Physics or the study of physical properties of matter in a solid phase
Introduction to Solid State Physics or the study of physical properties of matter in a solid phase Prof. Germar Hoffmann 1. Crystal Structures 2. Reciprocal Lattice 3. Crystal Binding and Elastic Constants
More informationLight-Controlled Shrinkage of Large-Area Gold Nanoparticles Monolayer Film for Tunable SERS Activity
Light-Controlled Shrinkage of Large-Area Gold Nanoparticles Monolayer Film for Tunable SERS Activity Xuefei Lu a,b, Youju Huang b,c,d, *, Baoqing Liu a,b, Lei Zhang b,c, Liping Song b,c, Jiawei Zhang b,c,
More informationGeSi Quantum Dot Superlattices
GeSi Quantum Dot Superlattices ECE440 Nanoelectronics Zheng Yang Department of Electrical & Computer Engineering University of Illinois at Chicago Nanostructures & Dimensionality Bulk Quantum Walls Quantum
More informationDesigning of metallic nanocrystals embedded in non-stoichiometric perovskite nanomaterial and its surface-electronic characteristics
Designing of metallic nanocrystals embedded in non-stoichiometric perovskite nanomaterial and its surface-electronic characteristics Jagadeesh Suriyaprakash 1,2, Y. B. Xu 1, Y. L. Zhu 1, L. X. Yang 1,
More informationFacile Synthesis of Gold Wavy Nanowires and Investigation of
Supporting Information for Facile Synthesis of Gold Wavy Nanowires and Investigation of Their Growth Mechanism Cun Zhu,, Hsin-Chieh Peng, Jie Zeng, Jingyue Liu, Zhongze Gu and Younan Xia,,* The Wallace
More informationCharacterisation of Nanoparticle Structure by High Resolution Electron Microscopy
Journal of Physics: Conference Series OPEN ACCESS Characterisation of Nanoparticle Structure by High Resolution Electron Microscopy To cite this article: Robert D Boyd et al 2014 J. Phys.: Conf. Ser. 522
More informationOff-Lattice KMC Simulation of Quantum Dot Formation
Off-Lattice KMC Simulation of Quantum Dot Formation T. P. Schulze University of Tennessee Peter Smereka & Henry Boateng University of Michigan Research supported by NSF-DMS-0854920 Heteroepitaxy and Quantum
More informationSupplementary Figure 1 Simulations of the lm thickness dependence of plasmon modes on lms or disks on a 30 nm thick Si 3 N 4 substrate.
Supplementary Figure 1 Simulations of the lm thickness dependence of plasmon modes on lms or disks on a 30 nm thick Si 3 N 4 substrate. (a) Simulated plasmon energy at k=30 µm 1 for the surface plasmon
More informationDetermination of redox reaction rates and orders by in-situ liquid cell. electron microscopy of Pd and Au solution growth
BNL-107596-2014-JA Determination of redox reaction rates and orders by in-situ liquid cell electron microscopy of Pd and Au solution growth Eli A. Sutter * and Peter W. Sutter Center for Functional Nanomaterials,
More informationSCSVMV UNIVERSITY,ENGINEERING PHYSICS
SCSVMV UNIVERSITY,ENGINEERING PHYSICS TWO MARK QUESTION BANK(Common to all branches) UNIT 1 PROPERTIES OF MATTER 1. Define Elasticity. 2. State Hooke s law. 3. What is meant by stress and strain? 4. Give
More informationThree-Dimensional Silicon-Germanium Nanostructures for Light Emitters and On-Chip Optical. Interconnects
Three-Dimensional Silicon-Germanium Nanostructures for Light Emitters and On-Chip Optical eptember 2011 Interconnects Leonid Tsybeskov Department of Electrical and Computer Engineering New Jersey Institute
More informationSupplementary Figures:
Supplementary Figures: Supplementary Figure 1 Cross-sectional morphology and Chemical composition. (a) A low-magnification dark-field TEM image shows the cross-sectional morphology of the BWO thin film
More informationSUPPLEMENTARY MATERIAL
SUPPLEMENTARY MATERIAL Multiphase Nanodomains in a Strained BaTiO3 Film on a GdScO3 Substrate Shunsuke Kobayashi 1*, Kazutoshi Inoue 2, Takeharu Kato 1, Yuichi Ikuhara 1,2,3 and Takahisa Yamamoto 1, 4
More informationSupporting Information
Supporting Information Extraordinary Off-stoichiometric Bismuth Telluride for Enhanced n- type Thermoelectric Power Factor Kunsu Park,,,# Kyunghan Ahn,,# Joonil Cha,, Sanghwa Lee,, Sue In Chae,, Sung-
More informationSupplementary Information for. Silver Nanoparticles Embedded Anti-microbial Paints Based on Vegetable Oil
Supplementary Information for Silver Nanoparticles Embedded Anti-microbial Paints Based on Vegetable Oil Ashavani Kumar #, Praveen Kumar Vemula #, Pulickel M. Ajayan, George John * Department of Chemistry,
More informationSupporting information High density monodispersed cobalt nanoparticles filled into multi-walled carbon nanotubes
Supporting information High density monodispersed cobalt nanoparticles filled into multi-walled carbon nanotubes Walid Baaziz a, Sylvie Begin-Colin a*, Benoit P. Pichon a, Ileana Florea a, Ovidiu Ersen
More informationChapter 10. Nanometrology. Oxford University Press All rights reserved.
Chapter 10 Nanometrology Oxford University Press 2013. All rights reserved. 1 Introduction Nanometrology is the science of measurement at the nanoscale level. Figure illustrates where nanoscale stands
More informationFile name: Supplementary Information Description: Supplementary Figures and Supplementary References. File name: Peer Review File Description:
File name: Supplementary Information Description: Supplementary Figures and Supplementary References File name: Peer Review File Description: Supplementary Figure Electron micrographs and ballistic transport
More informationCHAPTER 3. OPTICAL STUDIES ON SnS NANOPARTICLES
42 CHAPTER 3 OPTICAL STUDIES ON SnS NANOPARTICLES 3.1 INTRODUCTION In recent years, considerable interest has been shown on semiconducting nanostructures owing to their enhanced optical and electrical
More informationNew algoritms for electron diffraction of 3D protein crystals. JP Abrahams, D Georgieva, L Jiang, I Sikhuralidze, NS Pannu
New algoritms for electron diffraction of 3D protein crystals JP Abrahams, D Georgieva, L Jiang, I Sikhuralidze, NS Pannu Why new algorithms? New research questions New experimental techniques Better insight
More informationImaging Methods: Scanning Force Microscopy (SFM / AFM)
Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.
More informationGaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition
Gaetano L Episcopo Scanning Electron Microscopy Focus Ion Beam and Pulsed Plasma Deposition Hystorical background Scientific discoveries 1897: J. Thomson discovers the electron. 1924: L. de Broglie propose
More informationSupporting Information. Emergent, Collective Oscillations of Self- Mobile Particles and Patterned Surfaces under Redox Conditions
Supporting Information Emergent, Collective Oscillations of Self- Mobile Particles and Patterned Surfaces under Redox Conditions Michael E. Ibele, a Paul E. Lammert, b Vincent H. Crespi,* b and Ayusman
More informationTransmission Electron Microscopy and Diffractometry of Materials
Brent Fultz James Howe Transmission Electron Microscopy and Diffractometry of Materials Fourth Edition ~Springer 1 1 Diffraction and the X-Ray Powder Diffractometer 1 1.1 Diffraction... 1 1.1.1 Introduction
More informationElectronic Supplementary Information
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2017 Electronic Supplementary Information Two-dimensional CoNi nanoparticles@s,n-doped
More informationForming Gradient Multilayer (GML) Nano Films for Photovoltaic and Energy Storage Applications
Forming Gradient Multilayer (GML) Nano Films for Photovoltaic and Energy Storage Applications ABSTRACT Boris Gilman and Igor Altman Coolsol R&C, Mountain View CA For successful implementation of the nanomaterial-based
More informationConnecting metallic nanoparticles by optical
Supplementary Information for Connecting metallic nanoparticles by optical printing Julián Gargiulo 1, Santiago Cerrota 1, Emiliano Cortés 1, Ianina L. Violi 1, Fernando D. Stefani* 1,2 1 Centro de Investigaciones
More informationNanoprobing of semiconductor heterointerfaces: quantum dots, alloys and diffusion
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS D: APPLIED PHYSICS J. Phys. D: Appl. Phys. 37 (24) R163 R178 PII: S22-3727(4)37445- TOPICAL REVIEW Nanoprobing of semiconductor heterointerfaces: quantum
More informationLigand coated metal nanoparticles and quantum dots
The Supramolecular Nano Materials Group Ligand coated metal nanoparticles and quantum dots Francesco Stellacci Department of Materials Science and Engineering frstella@mit.edu Outline Self-Assembled Monolayers
More informationSmall-Angle X-ray Scattering (SAXS)/X-ray Absorption Near Edge Spectroscopy (XANES).
S1 Small-Angle X-ray Scattering (SAXS)/X-ray Absorption Near Edge Spectroscopy (XANES). The combined SAXS/XANES measurements were carried out at the µspot beamline at BESSY II (Berlin, Germany). The beamline
More informationCHEM 681 Seminar Mingqi Zhao April 20, 1998 Room 2104, 4:00 p.m. High Resolution Transmission Electron Microscopy: theories and applications
CHEM 681 Seminar Mingqi Zhao April 20, 1998 Room 2104, 4:00 p.m. High Resolution Transmission Electron Microscopy: theories and applications In materials science, people are always interested in viewing
More informationCharacterisation of Nanoparticles using Advanced Electron Microscopy
Wright State University CORE Scholar Special Session 5: Carbon and Oxide Based Nanostructured Materials (2013) Special Session 5 6-2013 Characterisation of Core@Shell Nanoparticles using Advanced Electron
More informationA Comparative Study on the Differences in the Evolutions of Thin Film Morphologies of Co-Al Binary System: Molecular Dynamics Study
Mat. Res. Soc. Symp. Proc. Vol. 777 2003 Materials Research Society T8.10.1 A Comparative Study on the Differences in the Evolutions of Thin Film Morphologies of Co-Al Binary System: Molecular Dynamics
More informationElectrochemical Deposition of Iron Nanoparticles on PPY and H terminated Si substrates. Karan Sukhija Co-op Term # 1 April 28 th, 2005
Electrochemical Deposition of Iron Nanoparticles on PPY and H terminated Si substrates Karan Sukhija Co-op Term # 1 April 28 th, 2005 Future Suggested Experiments Acknowledgments Presentation Outline Background
More informationUltrafast single photon emitting quantum photonic structures. based on a nano-obelisk
Ultrafast single photon emitting quantum photonic structures based on a nano-obelisk Je-Hyung Kim, Young-Ho Ko, Su-Hyun Gong, Suk-Min Ko, Yong-Hoon Cho Department of Physics, Graduate School of Nanoscience
More informationThe Effect of Surface Functionalization of Graphene on the Electrical Conductivity of Epoxy-based Conductive Nanocomposites
The Effect of Surface Functionalization of Graphene on the Electrical Conductivity of Epoxy-based Conductive Nanocomposites Behnam Meschi Amoli 1,2,3,4, Josh Trinidad 1,2,3,4, Norman Y. Zhou 1,3,5, Boxin
More informationSupporting Information
Electronic Supplementary Material (ESI) for Nanoscale. This journal is The Royal Society of Chemistry 2015 Supporting Information Stefanos Mourdikoudis, a,b Mariana Chirea, a Daniele Zanaga, c Thomas Altantzis,
More informationSUPPLEMENTARY FIGURES
1 SUPPLEMENTARY FIGURES Supplementary Figure 1: Initial stage showing monolayer MoS 2 islands formation on Au (111) surface. a, Scanning tunneling microscopy (STM) image of molybdenum (Mo) clusters deposited
More informationSupporting Information. Concave Rhombic Dodecahedral Au Nanocatalyst with Multiple High-Index Facets for CO 2 Reduction
Supporting Information Concave Rhombic Dodecahedral Au Nanocatalyst with Multiple High-Index Facets for CO 2 Reduction Hye-Eun Lee 1, Ki Dong Yang 1, Sang Moon Yoon 1, Hyo-Yong Ahn 1, Yoon Young Lee 1,
More informationSoft X-ray multilayer mirrors by ion assisted sputter deposition
Soft X-ray multilayer mirrors by ion assisted sputter deposition Valentino Rigato INFN Laboratori Nazionali di Legnaro Bologna, September 21, 2010 Source: INFN-LNL-2009 V. RIGATO 1 SIF- Bologna September
More informationRichard Palmer Nanomaterials Lab, College of Engineering
Scale Up, Size Down (SU-SD) Nanomaterials Lab, Swansea University, Wales not England Richard Palmer Nanomaterials Lab, College of Engineering Questions Can we arrange the atoms (in clusters) the way we
More informationSUPPLEMENTARY INFORMATION
DOI: 10.1038/NCHEM.2491 Experimental Realization of Two-dimensional Boron Sheets Baojie Feng 1, Jin Zhang 1, Qing Zhong 1, Wenbin Li 1, Shuai Li 1, Hui Li 1, Peng Cheng 1, Sheng Meng 1,2, Lan Chen 1 and
More informationStructure of Surfaces
Structure of Surfaces C Stepped surface Interference of two waves Bragg s law Path difference = AB+BC =2dsin ( =glancing angle) If, n =2dsin, constructive interference Ex) in a cubic lattice of unit cell
More informationSurface Sensitive X-ray Scattering
Surface Sensitive X-ray Scattering Introduction Concepts of surfaces Scattering (Born approximation) Crystal Truncation Rods The basic idea How to calculate Examples Reflectivity In Born approximation
More informationThese authors contributed equally to this work. 1. Structural analysis of as-deposited PbS quantum dots by Atomic Layer Deposition (ALD)
Supporting information for: Atomic Layer Deposition of Lead Sulfide Quantum Dots on Nanowire Surfaces Neil P. Dasgupta 1,*,, Hee Joon Jung 2,, Orlando Trejo 1, Matthew T. McDowell 2, Aaron Hryciw 3, Mark
More informationPhysics and Material Science of Semiconductor Nanostructures
Physics and Material Science of Semiconductor Nanostructures PHYS 570P Prof. Oana Malis Email: omalis@purdue.edu Course website: http://www.physics.purdue.edu/academic_programs/courses/phys570p/ Lecture
More informationTunable Nanoparticle Arrays at Charged Interfaces
Tunable Nanoparticle Arrays at Charged Interfaces Supporting Material Sunita Srivastava 1, Dmytro Nykypanchuk 1, Masafumi Fukuto 2 and Oleg Gang 1* 1 Center for Functional Nanomaterials, Brookhaven National
More informationStructural Analysis of Nanoparticles Using Scanning Transmission Electron Microscopy
Structural Analysis of Nanoparticles Using Scanning Transmission Electron Microscopy Shinya Maenosono and Derrick Mott School of Materials Science, Japan Advanced Institute of Science and Technology (JAIST)
More informationPOSITRON AND POSITRONIUM INTERACTIONS WITH CONDENSED MATTER. Paul Coleman University of Bath
POSITRON AND POSITRONIUM INTERACTIONS WITH CONDENSED MATTER Paul Coleman University of Bath THE FATE OF POSITRONS IN CONDENSED MATTER POSITRON-SURFACE INTERACTIONS positron backscattering BACKSCATTERED
More informationCHEM-E5225 :Electron Microscopy Imaging
CHEM-E5225 :Electron Microscopy Imaging 2016.10 Yanling Ge Outline Planar Defects Image strain field WBDF microscopy HRTEM information theory Discuss of question homework? Planar Defects - Internal Interface
More informationSupplementary information
1 2 Supplementary information 3 4 5 6 Supplementary Figure 1 7 8 Supplementary Figure 1 ǀ Characterization of the lysozyme fibrils by atomic force microscopy 9 (AFM) and scanning electron microscopy (SEM).
More informationPrecise control of size and density of self-assembled Ge dot on Si(1 0 0) by carbon-induced strain-engineering
Applied Surface Science 216 (2003) 419 423 Precise control of size and density of self-assembled Ge dot on Si(1 0 0) by carbon-induced strain-engineering Y. Wakayama a,*, L.V. Sokolov b, N. Zakharov c,
More informationIntroduction of Nano Science and Tech. Basics of Solid Mechanics in Nanostructures. Nick Fang
Introduction of Nano Science and Tech Basics of Solid Mechanics in Nanostructures Nick Fang Course Website: nanohub.org Compass.illinois.edu ME 498 2006-09 Nick Fang, University of Illinois. All rights
More informationSupporting Information: Analysis of protein coatings on gold nanoparticles by XPS and liquid-based particle sizing techniques
Supporting Information: Analysis of protein coatings on gold nanoparticles by XPS and liquid-based particle sizing techniques Natalie A. Belsey, a) Alex G. Shard a) and Caterina Minelli a),b) National
More informationSize-dependent Metal-insulator Transition Random Materials Crystalline & Amorphous Purely Electronic Switching
Nanometallic RRAM I-Wei Chen Department of Materials Science and Engineering University of Pennsylvania Philadelphia, PA 19104 Nature Nano, 6, 237 (2011) Adv Mater,, 23, 3847 (2011) Adv Func Mater,, 22,
More informationBoosting the hydrogen evolution performance of ruthenium clusters. through synergistic coupling with cobalt phosphide
Electronic Supplementary Material (ESI) for Energy & Environmental Science. This journal is The Royal Society of Chemistry 2018 Electronic Supplementary Information for Boosting the hydrogen evolution
More informationSYNTHESIS AND PROCESSING OF METALLIC NANOMATERIALS USING CO 2 EXPANDED LIQUIDS AS A GREEN SOLVENT MEDIUM
SYNTHESIS AND PROCESSING OF METALLIC NANOMATERIALS USING CO 2 EXPANDED LIQUIDS AS A GREEN SOLVENT MEDIUM Christopher Kitchens Dept. of Chemical and Biomolecular Engineering Clemson University, SC ENGINEERED
More informationProtection of excited spin states by a superconducting energy gap
Protection of excited spin states by a superconducting energy gap B. W. Heinrich, 1 L. Braun, 1, J. I. Pascual, 1, 2, 3 and K. J. Franke 1 1 Institut für Experimentalphysik, Freie Universität Berlin, Arnimallee
More informationSupporting Information
Supporting Information Retrieving the Quantitative Chemical Information at Nanoscale from Scanning Electron Microscope Energy Dispersive X-ray Measurements by Machine Learning B.R. Jany*, A. Janas, F.
More informationNanoplasmonics: Classical down to the Nanometer Scale
Supporting Information Nanoplasmonics: Classical down to the Nanometer Scale Huigao Duan #, Antonio I. Fernández-Domínguez 2#, Michel Bosman #, Stefan A. Maier 2* & Joel K. W. Yang * Institute of Materials
More informationLIGHT. A beam is made up of several rays. It maybe parallel, diverging (spreading out) or converging (getting narrower). Parallel Diverging Converging
LIGHT Light is a form of energy. It stimulates the retina of the eye and produces the sensation of sight. We see an object when light leaves it and enters the eye. Objects such as flames, the sum and stars
More informationSupplementary Figure 1 Detailed illustration on the fabrication process of templatestripped
Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped gold substrate. (a) Spin coating of hydrogen silsesquioxane (HSQ) resist onto the silicon substrate with a thickness
More informationNanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems
Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems Photonics group W. Claeys, S. Dilhair, S. Grauby, JM. Rampnoux, L. Patino Lopez,
More informationSupporting information. The role of halide ions in the anisotropic growth. of gold nanoparticles: a microscopic, atomistic.
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 26 Supporting information The role of halide ions in the anisotropic growth of gold
More informationOne-Pot Synthesis of Core-Shell-like Pt 3 Co Nanoparticle Electrocatalyst with Pt-enriched Surface for Oxygen Reduction Reaction in Fuel Cells
Electronic Supplementary Information for One-Pot Synthesis of Core-Shell-like 3 Co Nanoparticle Electrocatalyst with -enriched Surface for Oxygen Reduction Reaction in Fuel Cells Ji-Hoon Jang b, Juyeong
More informationStructural and Mechanical Properties of Nanostructures
Master s in nanoscience Nanostructural properties Mechanical properties Structural and Mechanical Properties of Nanostructures Prof. Angel Rubio Dr. Letizia Chiodo Dpto. Fisica de Materiales, Facultad
More informationOptical Characterization of Self-Assembled Si/SiGe Nano-Structures
Optical Characterization of Self-Assembled Si/SiGe Nano-Structures T. Fromherz, W. Mac, G. Bauer Institut für Festkörper- u. Halbleiterphysik, Johannes Kepler Universität Linz, Altenbergerstraße 69, A-
More informationSupplementary information. Derivatization and Interlaminar Debonding of Graphite-Iron Nanoparticles Hybrid
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2017 Supplementary information Derivatization and Interlaminar Debonding of Graphite-Iron
More informationCitation PHYSICAL REVIEW LETTERS (2009), Right 2009 The American Physical Societ
TitleInterface Structures of Gold Nanopa Author(s) Shibata, N.; Goto, A.; Matsunaga, K S. D.; Yamamoto, T.; Ikuhara, Y. Citation PHYSICAL REVIEW LETTERS (2009), 102 Issue Date 2009-04 URL http://hdl.handle.net/2433/109848
More informationSupporting Information. Optical Scattering Spectral Thermometry and Refractometry of a Single Gold Nanoparticle under CW laser excitation
Supporting Information Optical Scattering Spectral Thermometry and Refractometry of a Single Gold Nanoparticle under CW laser excitation Kenji Setoura, Daniel Werner, and Shuichi Hashimoto* Department
More informationExploring the Formation of Symmetric Gold Nanostars by Liquid-Cell Transmission Electron Microscopy
Supplementary information Exploring the Formation of Symmetric Gold Nanostars by Liquid-Cell Transmission Electron Microscopy Nabeel Ahmad, 1,2 Guillaume Wang, 1 Jaysen Nelayah, 1 Christian Ricolleau,
More informationNanomaterials and their Optical Applications
Nanomaterials and their Optical Applications Winter Semester 2012 Lecture 04 rachel.grange@uni-jena.de http://www.iap.uni-jena.de/multiphoton Lecture 4: outline 2 Characterization of nanomaterials SEM,
More informationThree-dimensional Visualization and Quantification of Gold Nanomaterial Deposition and Aggregation in Porous Media via Raman Spectroscopy
Raman Spectroscopy Nanomaterials Exposure? Three-dimensional Visualization and Quantification of Gold Nanomaterial Deposition and Aggregation in Porous Media via Raman Spectroscopy Matthew Y. Chan, Weinan
More informationTuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE
1 Chapter 3 Load and Stress Analysis 2 Chapter Outline Equilibrium & Free-Body Diagrams Shear Force and Bending Moments in Beams Singularity Functions Stress Cartesian Stress Components Mohr s Circle for
More informationalloys at high pressures. The central peaks at 0 mev correspond to the elastic scattering.
1 2 3 4 5 Supplementary Figure 1 Representative NRIXS spectra of the basaltic glass and Fe-rich alloys at high pressures. The central peaks at 0 mev correspond to the elastic scattering. Open symbols:
More informationElectronic supplementary information for:
Electronic supplementary information for: Charge-transfer-induced suppression of galvanic replacement and synthesis of (Au@Ag)@Au double shell nanoparticles for highly uniform, robust and sensitive bioprobes
More informationMonte Carlo simulations of alloy segregation in PtAg octahedral nanoparticles
Monte Carlo simulations of alloy segregation in PtAg octahedral nanoparticles Louis C. Jones 6/8/12 Abstract Simulations were carried out to investigate phase segregation of insoluble alloy nanoparticles
More informationIn the name of Allah
In the name of Allah Nano chemistry- 4 th stage Lecture No. 1 History of nanotechnology 16-10-2016 Assistance prof. Dr. Luma Majeed Ahmed lumamajeed2013@gmail.com, luma.ahmed@uokerbala.edu.iq Nano chemistry-4
More informationAn EAM potential for the dynamical simulation of Ni-Al alloys
J. At. Mol. Sci. doi: 10.4208/jams.022310.031210a Vol. 1, No. 3, pp. 253-261 August 2010 An EAM potential for the dynamical simulation of Ni-Al alloys Jian-Hua Zhang, Shun-Qing Wu, Yu-Hua Wen, and Zi-Zhong
More informationSupporting Information
Supporting Information Improved Working Model for Interpreting the Excitation Wavelength- and Fluence-Dependent Response in Pulsed aser-induced Size Reduction of Aqueous Gold Nanoparticles Daniel Werner
More informationSub-Stoichiometric Germanium Sulfide Thin-Films as a High-Rate Lithium Storage Material
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2014 Sub-Stoichiometric Germanium Sulfide Thin-Films as a High-Rate Lithium
More informationFocused Ion Beam Induced Local Tungsten Deposition
Focused Ion Beam Induced Local Tungsten Deposition H. Langfischer, B. Basnar, E. Bertagnolli Institute for Solid State Electronics, Vienna University of Technology, Floragasse 7, 1040 ien, Austria H. Hutter
More informationSelf-assembled nanostructures for antireflection optical coatings
Self-assembled nanostructures for antireflection optical coatings Yang Zhao 1, Guangzhao Mao 2, and Jinsong Wang 1 1. Deaprtment of Electrical and Computer Engineering 2. Departmentof Chemical Engineering
More informationSolid State Physics FREE ELECTRON MODEL. Lecture 14. A.H. Harker. Physics and Astronomy UCL
Solid State Physics FREE ELECTRON MODEL Lecture 14 A.H. Harker Physics and Astronomy UCL 6 The Free Electron Model 6.1 Basic Assumptions In the free electron model, we assume that the valence electrons
More information6. Plasmon coupling between a flat gold interface and gold nanoparticles.
6. Plasmon coupling between a flat gold interface and gold nanoparticles. 6.1. Introduction In this outlook oriented chapter the applicability of the multilayered system used in chapter 4.1., for the study
More information