Supplementary Figure 1 Supplementary Figure 2
|
|
- Felix Neal
- 5 years ago
- Views:
Transcription
1 Supplementry Figure 1 Comprtive illustrtion of the steps required to decorte n oxide support AO with ctlyst prticles M through chemicl infiltrtion or in situ redox exsolution. () chemicl infiltrtion usully requires severl deposition nd therml tretment steps followed y reduction to produce the metl prticles M on the outer surfce of the support AO. () in in situ redox exsolution M is incorported in its ction form in the crystl lttice of AO nd exsolved in one step, upon reduction. c Supplementry Figure 2 Rietveld refinement nd corresponding crystl structure of L0.4Sr0.4Ni0.03Ti0.97O3-γ. () Rietveld refinement of the room temperture powder XRD pttern using I4/mcm ( 0 0 c - ) spce group, = = Å, c = Å. Rp = 6.67%, Rwp = 8.82%, Re = 7.77%, χ 2 = 1.29 () Three-dimensionl overview of the crystl structure. (c) Projection long the z xis showing out of phse tilting long this xis.
2 L Sr Ti Supplementry Figure 3 XPS spectr of L, Sr nd Ti for the smples indicted in Fig. 1,, c, d. Blck lines represent experimentl dt, grey lines the ckground, ornge lines Ti 4+ pek fit, nd lue lines Ti 3+ pek fit. Supplementry Figure 4 () TEM imge of the ntive surfce of L0.4Sr0.4Ni0.03Ti0.97O3-γ similr to the one displyed in Fig. 1, in the vicinity of n exsolved prticle; scle r 1 nm. () Schemtic tomic model of the structure of L0.4Sr0.4Ni0.03Ti0.97O3-γ going from ulk to the ntive surfce sed on the XPS surfce stoichiometry presented in Fig. 1,.
3 c Supplementry Figure 5 () Cleved porous L0.52Sr0.28Ni0.06Ti0.94O3 smple reveling ulk-like surfces longside the lredypresent ntive surfces; scle r, 20 μm. () detil from the cleved ulk surfce region of L0.4Sr0.4Ni0.03Ti0.97O3-γ smple with microstructure similr to smple () fter reduction (5% H2/Ar, 900 C, 20 h); scle r, 1 μm. (c) detil of smple () fter reduction (5% H2/Ar, 900 C, 12 h) showing no prticles grow on the ntive surfces in this cse, lthough numerous prticles grow on the cleve surfce; scle rs, 1 μm.
4 c d Supplementry Figure 6 Fcet ngle mesurements y 3D AFM surfce reconstruction for the ntive surfce shown in Fig. 1. The reconstructed 3D imge is shown in Fig. 1e.
5 c Supplementry Figure 7 B-site ction diffusion in perovskites. () 3D view of the curved migrtion pth in the (011) plne. () Projection from the top, [001]. (c) Projection in the direction of diffusion, [100]. Adpted from reference 1.
6 L Sr Ti Supplementry Figure 8 XPS spectr corresponding to Fig. 1g. Blck lines represent experimentl dt, grey lines the ckground, ornge lines Ti 4+ pek fit, nd lue lines Ti 3+ pek fit.
7 c Supplementry Figure 9 Prticle nlysis on the surfce shown in Fig. 1d. () SEM imge corresponding to Fig. 1d. () Ni prticle mpping nd contour extrcted with ImgeJ from Supplementry Fig. 9. (c) Prticle size distriution clculted with ImgeJ sed on Supplementry Fig. 9. Scle rs, 1 μm. Supplementry Figure 10 Comprison etween () norml perovskite crystl structure nd () projection down c of hexgonl tungsten ronze ( high A-site deficient vrint of the perovskite lttice) showing units coupling A-site vcncies with the smller L 3+ ion through B site octhedron. This suggests possile defect unit tht could potentilly couple L, Ni nd n A-site vcncy consistent with the coopertive movement of L nd Ni s tungsten ronzes.
8 Supplementry Figure 11 Exsolved Ni prticles from the ntive surfce of L0.46Sr0.34Ni0.03Ti0.97O3 fter reduction in pure H2 t 900 C for 2.5 hours. Scle rs, 1 μm. Supplementry Figure 12 Prticle shpe nd emedding highlighted on the TEM imge shown in Fig. 3. Scle r, 10 nm.
9 c d e f Supplementry Figure 13 Orienttion reltionship etween exsolved prticles nd prent perovskite for the smple in Fig. 3. (), () nd (c) show selected re electron diffrction (SAED) ptterns contining reflections from the perovskite nd nickel prticle. The ptterns correspond to the [001], [112] nd [011] zone xes of the perovskite oxide, in ech cse nickel reflections corresponding to the sme zone xis re lso visile, s shown in (d), (e), (f), respectively. The presence of these reflections is consistent with the orienttion reltionship [010]P//[010]Ni (001)P//(001)Ni which we hve previously oserved in other system we investigted, ut which hve higher Ni sustitution level (L0.8Ce0.1Ti0.6Ni0.4O3, see reference 2 ), perhps suggesting tht exsolution generlly occurs epitxilly with respect to the prent perovskite. However, in this cse, not ll expected nickel reflections re visile. The sence of these reflections cn e ttriuted to the very smll volume of the nickel prticles, the sence of higher intensity low index reflections close to the centre of the diffrction pttern due to the fce centred cuic structure of nickel nd the possiility of vrition from the idel orienttion reltionship. Of the eight to ten nickel prticles present in the electron trnsprent region of the TEM smple, reflections consistent with this orienttion reltionship could only e otined for two. Whether this is due to em dmge from imging or smple preprtion or the sence of this specific orienttion reltionship could not e determined. c d e Supplementry Figure 14 AFM imges nd height profiles of: () Ni prticles exsolved from L0.4Sr0.4Ti0.97Ni0.03O3-δ (900 C, 5 h, dry H2); () smple () fter etching (HNO3) t room temperture for 20 minutes; (c) Ni prticles from Ni nitrte solution deposition (900 C, 6 h, dry H2); (d) Smple (c) fter etching t room temperture overnight showing now ovious pits; (e) further etching t 70 C for 2 hours. Scle rs, 500 nm.
10 c d Supplementry Figure 15 () ~20 nm Ni prticles formed y infiltrtion on L0.4Sr0.4TiO3. () nm Ni prticles prepred y vpour-deposition on L0.4Sr0.4TiO3 (the inset shows the prticle size distriution). (c) nm size Ni prticles exsolved from L0.52Sr0.28Ni0.06Ti0.94O3 (5% H2/Ar, 1000 C, 12 h; the inset shows the prticle size distriution). (d) Flse colour microgrph of smple (c) fter coking experiment showing prticle uplifting which leves ehind corresponding empty sockets. Scle rs, 1 μm (, c), 100 nm (, d). Supplementry Tle 1 Quntifiction of the XPS spectr in Supplementry Fig. 8 which ws used to derive the dt plotted in Fig. 1g. Pek res re given in ritrry units s clculted y CsXPS softwre nd lso include trnsmission function nd men free pth contriutions. RSF represents the corresponding reltive sensitivity fctor. L 3d5/2 Sr 3d5/2,3/2 Ti 2p3/2,1/2 Atomic rtios Ti 4+ 2p3/2 Ti 3+ 2p3/2 Temperture ( C) Pek re (.u.) RSF Pek re/rsf (.u.) Atomic % Pek re (.u.) RSF Pek re/rsf (.u.) Atomic % Pek re (.u.) RSF Pek re/rsf (.u.) Atomic % L/Ti Sr/Ti (L+Sr)/Ti Pek re (.u.) RSF Pek re/rsf (.u.) Pek re (.u.) RSF Pek re/rsf (.u.) Ti 3+ /(Ti 3+ +Ti 4+ )
11 Supplementry Note 1 The verge numer of Ni toms contined y the prticles shown in Supplementry Fig. 9, clculted sed on the prticle distriution shown in Supplementry Fig. 9d is given y: ( ) (1) Where: is Ni metl density, is the tomic weight of Ni, is Avogdro s numer, is the frction of prticles hving dimeter ccording to Supplementry Fig. 9d. The verge numer of Ni toms in prllelepiped perovskite volume of length width nd depth is given y: (2) Where is the pseudo-cuic perovskite unit cell prmeter nd is Ni stoichiometry in the perovskite. The verge depth of virtul perovskite prllelepiped contining imge shown in Supplementry Fig. 9: toms over n re equl to the one in the ( ) (3) In conclusion, for the microgrph shown in Supplementry Fig. 9, Ni toms pper to e depleted from ~88 nm deep eneth the surfce in order to ccount for the mount of Ni oserved on the surfce in the form of metl prticles. The verge numer of L toms in prllelepiped perovskite volume of length width nd depth is: (4) Where is L stoichiometry in the perovskite. The numer of L toms enriching the surfce during reduction through diffusion from the ulk, over n re equl to the one in Supplementry Fig. 9 is given y: ( ) (5) Where is L surfce stoichiometry in the perovskite fter reduction (from XPS, Fig. 1d) nd is L surfce stoichiometry in the perovskite prior to reduction (from XPS, Fig. 1), lso ssuming the surfce is thick (typicl XPS detection depth): (6) ( ) ( ) In conclusion, the mount of Ni metl contined in the surfce prticles shown in Supplementry Fig. 9, Ni toms, is of the sme order of mgnitude s the numer of L toms tht diffused from the ulk, L toms.
12 Supplementry references 1. De Souz, R. A., Islm, M. S. & Ivers-Tiffée, E. Formtion nd migrtion of ction defects in the perovskite oxide LMnO3. J. Mter. Chem. 9, (1999). 2. Negu, D., Tsekours, G., Miller, D. N., Ménrd, H. & Irvine, J. T. S. In situ growth of nnoprticles through control of non-stoichiometry. Nt. Chem. 5, (2013).
SUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION Synthesis of metl oxide with roomtemperture photoreversile phse trnsition Shin-ichi Ohkoshi 1 *, Yoshihide Tsunouchi, 1 Tomoyuki Mtsud, 1 Kzuhito Hshimoto, 2 Asuk Nmi, 1 Fumiyoshi
More informationa * a (2,1) 1,1 0,1 1,1 2,1 hkl 1,0 1,0 2,0 O 2,1 0,1 1,1 0,2 1,2 2,2
18 34.3 The Reciprocl Lttice The inverse of the intersections of plne with the unit cell xes is used to find the Miller indices of the plne. The inverse of the d-spcing etween plnes ppers in expressions
More informationLECTURE 14. Dr. Teresa D. Golden University of North Texas Department of Chemistry
LECTURE 14 Dr. Teres D. Golden University of North Texs Deprtment of Chemistry Quntittive Methods A. Quntittive Phse Anlysis Qulittive D phses by comprison with stndrd ptterns. Estimte of proportions of
More informationSUPPLEMENTARY INFORMATION
doi:.38/nture8499 doi:.38/nture8499 5 6 5 4.5 Firing rte (Hz) -67-65 -66-6 -58 V m (mv) -7-67 -68-66 -64 c Thet power (mv ) -73-69 -7-7 -7.5.8 3....9.9.4.6.6. 9 8 9 8 9 8 9 8 9 8 Supplementry Figure Firing
More informationMethod of Localisation and Controlled Ejection of Swarms of Likely Charged Particles
Method of Loclistion nd Controlled Ejection of Swrms of Likely Chrged Prticles I. N. Tukev July 3, 17 Astrct This work considers Coulom forces cting on chrged point prticle locted etween the two coxil,
More informationfiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
Solid Stte Physics JEST-0 Q. bem of X-rys is incident on BCC crystl. If the difference between the incident nd scttered wvevectors is K nxˆkyˆlzˆ where xˆ, yˆ, zˆ re the unit vectors of the ssocited cubic
More informationpolyimide Spray-coated ZrP/epoxy film Spray-coated ZrP/epoxy film glass
c d e polyimide Spry-coted ZrP/epoxy film glss Spry-coted ZrP/epoxy film f g Supplementry Figure 1. Opticl microscopy of smectic ( = 0.044) α-zrp/epoxy films., Trnsmission opticl microscopy (TOM) of smectic
More informationPHY 140A: Solid State Physics. Solution to Midterm #1
PHY 140A: Solid Stte Physics Solution to Midterm #1 TA: Xun Ji 1 October 24, 2006 1 Emil: jixun@physics.ucl.edu Problem #1 (20pt)Clculte the pcking frction of the body-centered cubic lttice. Solution:
More informationDirect indirect character of the band gap in methylammonium lead iodide perovskite
Direct indirect chrcter of the nd gp in methylmmonium led iodide perovskite Eline M. Hutter 1, Mrí C. Gélvez-Rued 1, Ann Osherov 2, Vldimir Bulović 2, Ferdinnd C. Grozem 1, Smuel D. Strnks 2,3*, nd Tom
More informationCALCULATED POWDER X-RAY DIFFRACTION LINE PROFILES VIA ABSORPTION
16 17 CALCULATED POWDER X-RAY DFFRACTON LNE PROFLES VA ABSORPTON Keji Liu nd Heifen Chen School of Mteril Science nd Engineering, Shnghi nstitute of Technology, Shnghi, Chin 2233 ABSTRACT We hve clculted
More informationCrystalline Structures The Basics
Crystlline Structures The sics Crystl structure of mteril is wy in which toms, ions, molecules re sptilly rrnged in 3-D spce. Crystl structure = lttice (unit cell geometry) + bsis (tom, ion, or molecule
More informationSupplementary Information
Supplementry Informtion Spontneously mplified homochirl orgnic-inorgnic nno-helix complex vi self-prolifertion Hlei Zhi, Yn Qun, Li Li, Xing-Yng Liu, Xurong Xu c nd Ruikng Tng*,c Centre for Biomterils
More informationSilicon Nanowire Based Single-Molecule SERS Sensor
Supporting informtion Silicon Nnowire Bsed Single-Molecule SERS Sensor Hui Wng, Xuemei Hn, Xuemei Ou, Chun-Sing Lee, Xiohong Zhng* nd Shuit-Tong Lee S1, A series of Si nnowires coted with compct ggregtes
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION doi: 1.138/nnno.29.451 Aove-ndgp voltges from ferroelectric photovoltic devices S. Y. Yng, 1 J. Seidel 2,3, S. J. Byrnes, 2,3 P. Shfer, 1 C.-H. Yng, 3 M. D. Rossell, 4 P. Yu,
More informationAMPERE CONGRESS AMPERE on Magnetic Resonance and Related Phenomena. Under the auspices of The GROUPEMENT AMPERE
AMPERE 2000 th 30 CONGRESS AMPERE on Mgnetic Resonnce nd Relted Phenomen Lison, Portugl, 23-2 July 2000 Under the uspices of The GROUPEMENT AMPERE Edited y: A.F. MARTINS, A.G. FEIO nd J.G. MOURA Sponsoring
More informationANALYSIS OF FAST REACTORS SYSTEMS
ANALYSIS OF FAST REACTORS SYSTEMS M. Rghe 4/7/006 INTRODUCTION Fst rectors differ from therml rectors in severl spects nd require specil tretment. The prsitic cpture cross sections in the fuel, coolnt
More informationDOI:.8/nc5 Cpilities of MCAK Sidesliding, endctching on microtuules MCAKdecorted ed Functions in mitotic spindle Prometphse Slides on the microtuule surfce + Redily slides long the microtuule surfce Strongly
More informationThermal Stability of Ti-C-Ni-Cr and Ti-C-Ni-Cr-Al-Si Nanocomposite Coatings
Journl of Physics: Conference Series PAPER OPEN ACCESS Therml Stility of Ti-C-Ni-Cr nd Ti-C-Ni-Cr-Al-Si Nnocomposite Cotings To cite this rticle: A V Andreev et l 2015 J. Phys.: Conf. Ser. 652 012057 View
More informationThe Properties of Stars
10/11/010 The Properties of Strs sses Using Newton s Lw of Grvity to Determine the ss of Celestil ody ny two prticles in the universe ttrct ech other with force tht is directly proportionl to the product
More informationFully Kinetic Simulations of Ion Beam Neutralization
Fully Kinetic Simultions of Ion Bem Neutrliztion Joseph Wng University of Southern Cliforni Hideyuki Usui Kyoto University E-mil: josephjw@usc.edu; usui@rish.kyoto-u.c.jp 1. Introduction Ion em emission/neutrliztion
More informationSupporting Information
Supporting Informtion Ultrfst nd Stble CO Cpture Using Alkli Metl Slt-Promoted MgO-CCO 3 Sorbents Hongjie Cui, Qiming Zhng, Yunwu Hu, Chong Peng, Xingchen Fng, Zhenmin Cheng, Vldimir V. Glvit nd Zhiming
More informationQUB XRD Course. The crystalline state. The Crystalline State
QUB XRD Course Introduction to Crystllogrphy 1 The crystlline stte Mtter Gseous Stte Solid stte Liquid Stte Amorphous (disordered) Crystlline (ordered) 2 The Crystlline Stte A crystl is constructed by
More informationEnhanced Photocatalytic CO 2 -Reduction Activity of Anatase TiO 2 by Coexposed {001} and {101} Facets
Supplementry Informtion for the Journl of Americn Chemicl Society The Americn Chemicl Society 04 Enhnced Photoctlytic CO -Reduction Activity of Antse TiO y Coexposed {00} nd {0} Fcets Jiguo Yu,*, Jingxing
More informationMaterials Analysis MATSCI 162/172 Laboratory Exercise No. 1 Crystal Structure Determination Pattern Indexing
Mterils Anlysis MATSCI 16/17 Lbortory Exercise No. 1 Crystl Structure Determintion Pttern Inexing Objectives: To inex the x-ry iffrction pttern, ientify the Brvis lttice, n clculte the precise lttice prmeters.
More informationWhat is thin film/layer?
High-esolution XD Wht is thin film/lyer? Mteril so thin tht its chrcteristics re dominted primrily by two dimensionl effects nd re mostly different thn its bulk properties Source: semiconductorglossry.com
More informationInterfacial synergism of Pd-decorated BiOCl ultrathin nanosheets for selective oxidation of aromatic alcohols
Electronic Supplementry Mteril (ESI) for Journl of Mterils Chemistry A. This journl is The Royl Society of Chemistry 2018 Interfcil synergism of Pd-decorted BiOCl ultrthin nnosheets for selective oxidtion
More informationThe development of nanoscale morphology in polymer:fullerene. photovoltaic blends during solvent casting
Supplementry informtion Supplementry Mteril (ES) for Soft Mtter The development of nnoscle morphology in polymer:fullerene photovoltic lends during solvent csting To Wng, * Aln D. F. Dunr, Pul A. Stniec,
More information1 ST ROUND, SOLUTIONS
ST ROUND, SOLUTIONS Problem (Lithuni) Self destructing pper ( points) Solution ( ) ( ) ( ) [Al HO OH ) ph pk lg [Al H O ( ) ( ) [Al H O OH [Al ( ).9 [Al H O.9.47 [Al ( ) ( ) ( ) [Al H O OH.9 pk ph lg.
More informationSTRUCTURAL ISSUES IN SEMICONDUCTORS
Chpter 1 STRUCTURAL ISSUES IN SEMICONDUCTORS Most semiconductor devices re mde from crystlline mterils. The following gures provide n overview of importnt crystlline properties of semiconductors, like
More informationThin Film Scattering: Epitaxial Layers
Thin Film Scttering: Epitxil yers Arturs Vilionis GAM, Stnford University SIMES, SAC 5th Annul SSR Workshop on Synchrotron X-ry Scttering Techniques in Mterils nd Environmentl Sciences: Theory nd Appliction
More informationWhat is solid state physics?
Wht is solid stte physics? Explins the properties of solid mterils. Explins the properties of collection of tomic nuclei nd electrons intercting with electrosttic forces. Formultes fundmentl lws tht govern
More informationDerivations for maximum likelihood estimation of particle size distribution using in situ video imaging
2 TWMCC Texs-Wisconsin Modeling nd Control Consortium 1 Technicl report numer 27-1 Derivtions for mximum likelihood estimtion of prticle size distriution using in situ video imging Pul A. Lrsen nd Jmes
More informationUNIVERSITY OF OSLO. Faculty of Mathematics and Natural Sciences
UNIVERSITY OF OSLO Fculty of Mthemtics nd Nturl Sciences Midterm exm in MENA3100 Dy of exm: 19 th Mrch 2018 Exm hours: 14:30 17:30 This exmintion pper consists of 4 pges including 1 ppendix pge. Permitted
More information6. Photoionization of acridine through singlet and triplet channels
Chpter 6: Photoioniztion of cridine through singlet nd triplet chnnels 59 6. Photoioniztion of cridine through singlet nd triplet chnnels Photoioinztion of cridine (Ac) in queous micelles hs not yet een
More information2. VECTORS AND MATRICES IN 3 DIMENSIONS
2 VECTORS AND MATRICES IN 3 DIMENSIONS 21 Extending the Theory of 2-dimensionl Vectors x A point in 3-dimensionl spce cn e represented y column vector of the form y z z-xis y-xis z x y x-xis Most of the
More informationDETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING MOMENT INTERACTION AT MICROSCALE
Determintion RevAdvMterSci of mechnicl 0(009) -7 properties of nnostructures with complex crystl lttice using DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING
More informationPackaging consideration of two dimensional polymer-based. photonic crystals for laser beam steering
Pckging considertion of two dimensionl polymer-sed photonic crystls for lser em steering Xinyun Dou, Xionn Chen, Mggie Yihong Chen, IEEE Senior Memer, Aln Xiolong Wng, Wei Jing c, Ry T. Chen *, IEEE Fellow
More informationTremor-rich shallow dyke formation followed by silent magma flow at Bárðarbunga in Iceland
In the formt provided y the uthors nd unedited. SUPPLEMENTARY INFORMATION DOI: 1.138/NGEO9 Tremor-rich shllow dyke formtion followed y silent mgm flow t Bárðrung in Icelnd 1,, 1, 3 1, 1 1, NATURE GEOSCIENCE
More informationCHM Physical Chemistry I Chapter 1 - Supplementary Material
CHM 3410 - Physicl Chemistry I Chpter 1 - Supplementry Mteril For review of some bsic concepts in mth, see Atkins "Mthemticl Bckground 1 (pp 59-6), nd "Mthemticl Bckground " (pp 109-111). 1. Derivtion
More informationSupplementary Information
Supplementry Informtion Lignd exchnge triggered controlled-relese trgeted drug delivery system sed on core shell superprmgnetic mesoporous microspheres cpped with nnoprticles Zhogng Teng, Xingng Zhu, Gengfeng
More informationarxiv:hep-ex/ v1 12 Sep 1998
Evidence of the φ ηπ γ decy rxiv:hep-ex/9891v1 12 Sep 1998 Astrct M.N.Achsov, V.M.Aulchenko, S.E.Bru, A.V.Berdyugin, A.V.Bozhenok, A.D.Bukin, D.A.Bukin, S.V.Burdin, T.V.Dimov, S.I.Dolinski, V.P.Druzhinin,
More informationSTRUCTURAL AND MAGNETIC PROPERTIES OF Fe/Si x Fe 1! x MULTILAYERS
MOLECULAR PHYSICS REPORTS 0 (00) 8-86 STRUCTURAL AND MAGNETIC PROPERTIES OF Fe/ x Fe! x MULTILAYERS P. WANDZIUK, M. KOPCEWICZ, B. SZYMAŃSKI, AND T. LUCIŃSKI Institute of Moleculr Physics, Polish Acdemy
More informationSection 6: Area, Volume, and Average Value
Chpter The Integrl Applied Clculus Section 6: Are, Volume, nd Averge Vlue Are We hve lredy used integrls to find the re etween the grph of function nd the horizontl xis. Integrls cn lso e used to find
More informationPoint Lattices: Bravais Lattices
Physics for Solid Stte Applictions Februry 18, 2004 Lecture 7: Periodic Structures (cont.) Outline Review 2D & 3D Periodic Crystl Structures: Mthemtics X-Ry Diffrction: Observing Reciprocl Spce Point Lttices:
More informationReferences and Resources:
Surfce nd Interfce Science Physics 627; Chemistry 542 Lectures 4 Feb 3, 2013 Determining Surfce Structure Diffrction methods: LEED; RHEED Rel Spce: STEM References nd Resources: Woodruff nd Delchr (2 nd
More information8Similarity UNCORRECTED PAGE PROOFS. 8.1 Kick off with CAS 8.2 Similar objects 8.3 Linear scale factors. 8.4 Area and volume scale factors 8.
8.1 Kick off with S 8. Similr ojects 8. Liner scle fctors 8Similrity 8. re nd volume scle fctors 8. Review U N O R R E TE D P G E PR O O FS 8.1 Kick off with S Plese refer to the Resources t in the Prelims
More informationGraduate Students do all problems. Undergraduate students choose three problems.
OPTI 45/55 Midterm Due: Februr, Grdute Students do ll problems. Undergrdute students choose three problems.. Google Erth is improving the resolution of its globl mps with dt from the SPOT5 stellite. The
More information11-755/ Machine Learning for Signal Processing. Algebra. Class Sep Instructor: Bhiksha Raj
-755/8-797 Mchine Lerning for Signl Processing Fundmentls of Liner Alger Clss -3 Sep Instructor: Bhiksh Rj Sep -755/8-797 Administrivi Registrtion: Anyone on witlist still? Homework : Will e hnded out
More informationMeasuring Electron Work Function in Metal
n experiment of the Electron topic Mesuring Electron Work Function in Metl Instructor: 梁生 Office: 7-318 Emil: shling@bjtu.edu.cn Purposes 1. To understnd the concept of electron work function in metl nd
More informationSupplementary Information for Directional Reflective Surface Formed via Gradient- Impeding Acoustic Meta-surfaces
Supplementry Informtion for Directionl Reflective Surfce Formed vi Grdient- Impeding Acoustic Met-surfces Kyungjun Song 1*, Jedo Kim 2, Hur Shin 1, Jun-Hyuk Kwk 1, Seong-Hyun Lee 3,Tesung Kim 4 1 Deprtment
More informationKai Sun. University of Michigan, Ann Arbor
Ki Sun University of Michign, Ann Arbor How to see toms in solid? For conductors, we cn utilize scnning tunneling microscope (STM) to see toms (Nobel Prize in Physics in 1986) Limittions: (1) conductors
More informationAnalytical Methods for Materials
Anlyticl Methods for Mterils Lesson 7 Crystl Geometry nd Crystllogrphy, Prt 1 Suggested Reding Chpters 2 nd 6 in Wsed et l. 169 Slt crystls N Cl http://helthfreedoms.org/2009/05/24/tble-slt-vs-unrefined-se-slt--primer/
More informationconference papers The internal structure of single carbon fibers determined by simultaneous smalland wide-angle X-ray scattering
The internl structure of single cron fiers determined y simultneous smllnd wide-ngle X-ry scttering Oskr Pris *, Dieter Loidl, Herwig Peterlik, Mrtin Müller c, Helg Lichtenegger, nd Peter Frtzl Erich Schmid
More informationAcceptance Sampling by Attributes
Introduction Acceptnce Smpling by Attributes Acceptnce smpling is concerned with inspection nd decision mking regrding products. Three spects of smpling re importnt: o Involves rndom smpling of n entire
More informationPartial Derivatives. Limits. For a single variable function f (x), the limit lim
Limits Prtil Derivtives For single vrible function f (x), the limit lim x f (x) exists only if the right-hnd side limit equls to the left-hnd side limit, i.e., lim f (x) = lim f (x). x x + For two vribles
More informationXX-th ARS SEPARATORIA Szklarska Poręba, Poland 2005
XX-th ARS SEPARATORIA Szklrsk Porę, Polnd 25 DIALYSIS OF METAL IONS THROUGH ULTRAFILTRATION POLYSULFONE MEMBRANES ENHANCED BY POLY(ACRYLIC ACID) Gryzeld POŹNIAK Wroclw University of Technology, Deprtment
More informationTHREE-DIMENSIONAL KINEMATICS OF RIGID BODIES
THREE-DIMENSIONAL KINEMATICS OF RIGID BODIES 1. TRANSLATION Figure shows rigid body trnslting in three-dimensionl spce. Any two points in the body, such s A nd B, will move long prllel stright lines if
More informationWeek 10: Line Integrals
Week 10: Line Integrls Introduction In this finl week we return to prmetrised curves nd consider integrtion long such curves. We lredy sw this in Week 2 when we integrted long curve to find its length.
More informationPH12b 2010 Solutions HW#3
PH 00 Solutions HW#3. The Hmiltonin of this two level system is where E g < E e The experimentlist sis is H E g jgi hgj + E e jei hej j+i p (jgi + jei) j i p (jgi jei) ) At t 0 the stte is j (0)i j+i,
More informationThis chapter will show you. What you should already know. 1 Write down the value of each of the following. a 5 2
1 Direct vrition 2 Inverse vrition This chpter will show you how to solve prolems where two vriles re connected y reltionship tht vries in direct or inverse proportion Direct proportion Inverse proportion
More informationIV. CONDENSED MATTER PHYSICS
IV. CONDENSED MATTER PHYSICS UNIT I CRYSTAL PHYSICS Lecture - II Dr. T. J. Shinde Deprtment of Physics Smt. K. R. P. Kny Mhvidyly, Islmpur Simple Crystl Structures Simple cubic (SC) Fce centered cubic
More information1.Bravais Lattices The Bravais lattices Bravais Lattice detail
1.Brvis Lttices 12.1. The Brvis lttices 2.2.4 Brvis Lttice detil The Brvis lttice re the distinct lttice types which when repeted cn fill the whole spce. The lttice cn therefore be generted by three unit
More informationEnergy (kcal mol -1 ) Force (kcal mol -1 Å -1 ) Pore axis (Å) Mixed Mo-only S-only Graphene
Force (kcl mol -1 Å -1 ) Energy (kcl mol -1 ) 3 1-1 - -3 Mixed Mo-only S-only Grphene 6 5 3 1 Mixed Mo-only S-only Grphene - -1-1 1 Pore xis (Å) -1 1 Pore xis (Å) Supplementry Figure 1 Energy Brriers.
More informationTests for the Ratio of Two Poisson Rates
Chpter 437 Tests for the Rtio of Two Poisson Rtes Introduction The Poisson probbility lw gives the probbility distribution of the number of events occurring in specified intervl of time or spce. The Poisson
More information4.1. Probability Density Functions
STT 1 4.1-4. 4.1. Proility Density Functions Ojectives. Continuous rndom vrile - vers - discrete rndom vrile. Proility density function. Uniform distriution nd its properties. Expected vlue nd vrince of
More informationIntensity transformations
Intensity trnsformtions Stefno Ferrri Università degli Studi di Milno stefno.ferrri@unimi.it Methods for Imge Processing cdemic yer 2017 2018 Sptil domin The sptil domin of n imge is the plne tht contins
More informationColorimetric detection and separation of chiral tyrosine. based on N-acetyl-L-cysteine modified gold. nanoparticles
Colorimetric detection nd seprtion of chirl tyrosine sed on N-cetyl-L-cysteine modified gold nnoprticles Hiyn Su, Qiuling Zheng nd Hiing Li* Key Lortory of Pesticide nd Chemicl Biology (CCNU), Ministry
More informationSection 14.3 Arc Length and Curvature
Section 4.3 Arc Length nd Curvture Clculus on Curves in Spce In this section, we ly the foundtions for describing the movement of n object in spce.. Vector Function Bsics In Clc, formul for rc length in
More informationProbability Distributions for Gradient Directions in Uncertain 3D Scalar Fields
Technicl Report 7.8. Technische Universität München Probbility Distributions for Grdient Directions in Uncertin 3D Sclr Fields Tobis Pfffelmoser, Mihel Mihi, nd Rüdiger Westermnn Computer Grphics nd Visuliztion
More information11-755/ Machine Learning for Signal Processing. Algebra. Class August Instructor: Bhiksha Raj
-755/8-797 Mchine Lerning for Signl Processing Fundmentls of Liner Alger Clss 6 August 9 Instructor: Bhiksh Rj 6 Aug -755/8-797 Administrivi Registrtion: Anyone on witlist still? Our TA is here Sourish
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES Introduction In rigid body kinemtics, e use the reltionships governing the displcement, velocity nd ccelertion, but must lso ccount for the rottionl motion of the body. Description
More informationPoly(vinylamine) Microgels: ph-responsive Particles with High Primary Amine Contents
SUPPLEMENTARY INFORMATION Poly(vinylmine) Microgels: ph-responsive Prticles with High Primry Amine Contents Sineent Thioonro, Cory Berkln, Amir H. Milni, Rein Ulijn c n Brin R. Suners, * Polymer Science
More informationShape and measurement
C H A P T E R 5 Shpe nd mesurement Wht is Pythgors theorem? How do we use Pythgors theorem? How do we find the perimeter of shpe? How do we find the re of shpe? How do we find the volume of shpe? How do
More informationCHEMICAL KINETICS
CHEMICAL KINETICS Long Answer Questions: 1. Explin the following terms with suitble exmples ) Averge rte of Rection b) Slow nd Fst Rections c) Order of Rection d) Moleculrity of Rection e) Activtion Energy
More informationSurfactant-directed assembly of mesoporous metal-organic framework nanoplates in ionic liquid
Electronic supplementry informtion for: Surfctnt-directed ssemly of mesoporous metl-orgnic frmework nnopltes in ionic liquid Li Peng, Jinling Zhng*, Jinshen Li, Buxing Hn*, Zhimin Xue nd Gunying Yng Beijing
More informationLecture V. Introduction to Space Groups Charles H. Lake
Lecture V. Introduction to Spce Groups 2003. Chrles H. Lke Outline:. Introduction B. Trnsltionl symmetry C. Nomenclture nd symols used with spce groups D. The spce groups E. Derivtion nd discussion of
More informationStrategy: Use the Gibbs phase rule (Equation 5.3). How many components are present?
University Chemistry Quiz 4 2014/12/11 1. (5%) Wht is the dimensionlity of the three-phse coexistence region in mixture of Al, Ni, nd Cu? Wht type of geometricl region dose this define? Strtegy: Use the
More informationThings to Memorize: A Partial List. January 27, 2017
Things to Memorize: A Prtil List Jnury 27, 2017 Chpter 2 Vectors - Bsic Fcts A vector hs mgnitude (lso clled size/length/norm) nd direction. It does not hve fixed position, so the sme vector cn e moved
More informationOxidation-reduction mechanism of iron in dioctahedral smectites: 2. Crystal chemistry of reduced Garfield nontronite
Americn Minerlogist, 85, 53-7, Oxidtion-reduction mechnism of iron in diocthedrl smectites:. Crystl chemistry of reduced Grfield nontronite A. MANCEAU,, * V.A. DRITS,,. LANSON, D. CHATEIGNER, J. WU, 3
More informationEquations of Motion. Figure 1.1.1: a differential element under the action of surface and body forces
Equtions of Motion In Prt I, lnce of forces nd moments cting on n component ws enforced in order to ensure tht the component ws in equilirium. Here, llownce is mde for stresses which vr continuousl throughout
More informationAN IMPROVED SMALL CLOSED DRIFT THRUSTER WITH BOTH CONDUCTING AND DIELECT RIC CHANNELS
AN IMPROVED SMALL CLOSED DRIFT THRUSTER WITH BOTH CONDUCTING AND DIELECT RIC CHANNELS A.I.Bugrov, A.D.Desitskov, H.R.Kufmn, V.K.Khrchevnikov, A.I.Morozov c, V.V.Zhurin d Moscow Institute of Rdioelectronics,
More informationMetal-Carbonyl Organometallic Polymers, PFpP, for High- Resolution Positive and Negative Electron Beam Lithography Resist
Electronic Supplementry Mteril (ESI) for ChemComm. This journl is The Royl Society of Chemistry 2015 Supporting informtion Metl-Crbonyl Orgnometllic Polymers, PFpP, for High- Resolution Positive nd Negtive
More informationExam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B
PHY 249, Fll 216 Exm 1 Solutions nswer 1 is correct for ll problems. 1. Two uniformly chrged spheres, nd B, re plced t lrge distnce from ech other, with their centers on the x xis. The chrge on sphere
More informationState space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies
Stte spce systems nlysis (continued) Stbility A. Definitions A system is sid to be Asymptoticlly Stble (AS) when it stisfies ut () = 0, t > 0 lim xt () 0. t A system is AS if nd only if the impulse response
More informationLINEAR ALGEBRA APPLIED
5.5 Applictions of Inner Product Spces 5.5 Applictions of Inner Product Spces 7 Find the cross product of two vectors in R. Find the liner or qudrtic lest squres pproimtion of function. Find the nth-order
More informationTemplate-Free Synthesis of ZSM-5 Type Zeolite Layers on Porous Alumina Disks
Turk J Chem 31 (2007), 233 242. c TÜBİTAK Templte-Free Synthesis of ZSM-5 Type Zeolite Lyers on Porous Alumin Disks Hlil KALIPÇILAR nd Ali ÇULFAZ Chemicl Engineering Deprtment, Middle Est Technicl University,
More information13: Diffusion in 2 Energy Groups
3: Diffusion in Energy Groups B. Rouben McMster University Course EP 4D3/6D3 Nucler Rector Anlysis (Rector Physics) 5 Sept.-Dec. 5 September Contents We study the diffusion eqution in two energy groups
More informationTerminal Velocity and Raindrop Growth
Terminl Velocity nd Rindrop Growth Terminl velocity for rindrop represents blnce in which weight mss times grvity is equl to drg force. F 3 π3 ρ L g in which is drop rdius, g is grvittionl ccelertion,
More informationAnalytically, vectors will be represented by lowercase bold-face Latin letters, e.g. a, r, q.
1.1 Vector Alger 1.1.1 Sclrs A physicl quntity which is completely descried y single rel numer is clled sclr. Physiclly, it is something which hs mgnitude, nd is completely descried y this mgnitude. Exmples
More information8Similarity ONLINE PAGE PROOFS. 8.1 Kick off with CAS 8.2 Similar objects 8.3 Linear scale factors. 8.4 Area and volume scale factors 8.
8.1 Kick off with S 8. Similr ojects 8. Liner scle fctors 8Similrity 8.4 re nd volume scle fctors 8. Review Plese refer to the Resources t in the Prelims section of your eookplus for comprehensive step-y-step
More informationContinuous Random Variables
CPSC 53 Systems Modeling nd Simultion Continuous Rndom Vriles Dr. Anirn Mhnti Deprtment of Computer Science University of Clgry mhnti@cpsc.uclgry.c Definitions A rndom vrile is sid to e continuous if there
More informationReview of Probability Distributions. CS1538: Introduction to Simulations
Review of Proility Distriutions CS1538: Introduction to Simultions Some Well-Known Proility Distriutions Bernoulli Binomil Geometric Negtive Binomil Poisson Uniform Exponentil Gmm Erlng Gussin/Norml Relevnce
More informationNumerical simulation of ohmic heating in idealized thin-layer electrodeposition cells
JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS Vol. 8, No. 1, Ferury 2006, p. 271-279 Numericl simultion of ohmic heting in idelized thin-lyer electrodeposition cells P. BARVINSCHI West University of
More informationLecture 3: Curves in Calculus. Table of contents
Mth 348 Fll 7 Lecture 3: Curves in Clculus Disclimer. As we hve textook, this lecture note is for guidnce nd supplement only. It should not e relied on when prepring for exms. In this lecture we set up
More informationKey for Chem 130 Second Exam
Nme Key for Chem 130 Second Exm On the following pges you will find questions tht cover the structure of molecules, ions, nd solids, nd the different models we use to explin the nture of chemicl bonding.
More information( ) ( ) Chapter 5 Diffraction condition. ρ j
Grdute School of Engineering Ngo Institute of Technolog Crstl Structure Anlsis Tkshi Id (Advnced Cermics Reserch Center) Updted Nov. 3 3 Chpter 5 Diffrction condition In Chp. 4 it hs been shown tht the
More informationhttp:dx.doi.org1.21611qirt.1994.17 Infrred polriztion thermometry using n imging rdiometer by BALFOUR l. S. * *EORD, Technion Reserch & Development Foundtion Ltd, Hif 32, Isrel. Abstrct This pper describes
More informationExamples Using both 2-D sections from Figure 3, data has been modeled for (acoustic) P and (elastic) S wave field
Suslt illumintion studies through longitudinl nd trnsversl wve propgtion Riz Ali *, Jn Thorecke nd Eric Verschuur, Delft University of Technology, The Netherlnds Copyright 2007, SBGf - Sociedde Brsileir
More information2.57/2.570 Midterm Exam No. 1 March 31, :00 am -12:30 pm
2.57/2.570 Midterm Exm No. 1 Mrch 31, 2010 11:00 m -12:30 pm Instructions: (1) 2.57 students: try ll problems (2) 2.570 students: Problem 1 plus one of two long problems. You cn lso do both long problems,
More informationStructures of some surfactant polyelectrolyte complexes
PRAMANA cfl Indin Acdemy of Sciences Vol. 61, No. 2 journl of August 2003 physics pp. 447 454 Structures of some surfctnt polyelectrolyte complexes REMA KRISHNASWAMY 1, V A RAGHUNATHAN 1 nd A K SOOD 2
More information