Ab Initio Studies of Size and Coordination Effects:尺寸和協(xié)同效應(yīng)的從頭計(jì)算研究_第1頁(yè)
Ab Initio Studies of Size and Coordination Effects:尺寸和協(xié)同效應(yīng)的從頭計(jì)算研究_第2頁(yè)
Ab Initio Studies of Size and Coordination Effects:尺寸和協(xié)同效應(yīng)的從頭計(jì)算研究_第3頁(yè)
Ab Initio Studies of Size and Coordination Effects:尺寸和協(xié)同效應(yīng)的從頭計(jì)算研究_第4頁(yè)
Ab Initio Studies of Size and Coordination Effects:尺寸和協(xié)同效應(yīng)的從頭計(jì)算研究_第5頁(yè)
已閱讀5頁(yè),還剩21頁(yè)未讀, 繼續(xù)免費(fèi)閱讀

下載本文檔

版權(quán)說(shuō)明:本文檔由用戶提供并上傳,收益歸屬內(nèi)容提供方,若內(nèi)容存在侵權(quán),請(qǐng)進(jìn)行舉報(bào)或認(rèn)領(lǐng)

文檔簡(jiǎn)介

1、1Ab Initio Studies of Size and Coordination EffectsShobhana NarasimhanJawaharlal Nehru Centre for Advanced Scientific ResearchBangalore, Indiashobhanajncasr.ac.inKolkata, January 8 20072First: A ConfessionOnce upon a time3Confession (continued)Today4Our group Use ab initio density functional theory

2、(DFT) calculations to explore various aspects of the consequences of reduced co-ordination.+ Other applications of DFT to materials problems.http:/www.jncasr.ac.in/shobhana5Reduced CoordinationLowering of dimensionality usually accompanied by reduction in coordination number.Examples: surfaces, inte

3、rfaces, nanotubes, nanowires, nanoclusters.Reduced coordination results in altered structures.Differences in other properties too: vibrational, thermal, electronic, magnetic, chemical reactivity, transport.dimensionality C.N. 6Systems/Phenomena of Interest to Us Structure (Reconstruction) of surface

4、s, nanowires, clusters. Elastic properties of these systems (e.g., size dependence of hardness). Vibrational properties of these systems (e.g., surface phonons, etc.). Thermal behaviour (e.g., thermal expansion, melting) of bulk systems, surfaces, nanosystems Reactivity: dependence on local environm

5、ent, e.g., rough vs. smooth surfaces, microcrystals vs. nanoclusters. Magnetic properties: especially with reference to how magnetism affects the above.7The Techniques We Use Fairly standard implementations of ab initio density functional theory (plane wave basis, pseudopotentials). Density function

6、al perturbation theory for vibrational and elastic properties.Quasiharmonic approximation / full anharmonicity (from frozen phonons) for anharmonic thermal properties. Nudged elastic band method for reaction barriers. Parametrized model potentials for larger scale problems.8Reconstruction on close-p

7、acked metal surfaces Au(111) reconstructs into herringbone pattern*STM image of Au(111)30nm Pt(111) reconstructs into honey- comb or triangular pattern on: -heating above 1330 K* -placing in supersaturated vapor*STM images of Pt(111)*Barth et al.,1990; Huang et al. 1990; Narasimhan & Vanderbilt,

8、 1991* Sandy et al., 1992; * Bott et al., 1993; Hohage, Michely & Comsa, 1995.To reduce surface stress, some surfaces reconstruct into patterns of alternating domains of FCC and HCP stacking:9Reconstruction on vicinal (stepped) Au(111)Repain, Rousset et al. Also consist of tilings of FCC & H

9、CP domains Pattern depends on terrace width and type of step.10Modelling the Reconstruction We perform ab initio calculations to parametrize a classical model. Excellent agreement with experiments.Simulated STM imagesof the lowest energystructures on Au(111) and Pt(111) Narasimhan & Vanderbilt;

10、Pushpa & Narasimhan11Self-Ordered Magnetic NanostructuresThese reconstructed surfaces act as templates for growing ordered arrays of nanomagnets: Can use to study nanomagnetism High-density nanomagnetic storage devices? Questions for theorists: - Site preference - Mechanism: place exchange or ad

11、sorption? - Magnetic propertiesSTM image of O.1 ML of Co on Au(111)60 nm STM image of the Au(788) surface. Each bright dot corresponds to a cobalt cluster (around 100 atoms each). Repain, Rousset et al.12ClustersSi6Pb11Pb14Si20Our primary interests: Algorithms to find lowest energy structures Elasti

12、c properties Vibrational properties Melting Behaviour Catalysis 13 k ia,jb force induced on atom j in direction b, upon moving atom i in direction a (by unit length) Dimensions of energy/length2 Can obtain from DFT calculations by performing “frozen phonon” calculations or from “density functional p

13、erturbation theory” (DFPT). Measure of bond stiffnessForce Constant Tensor14As size reduced:Coordination Bond lengths Frequencies Bond stiffness Size-dependent trends in nanoclustersR. Pushpa, U.V. Waghmare & SN15Coordination-dependent trends in nanoclustersBonds in Si clusters are longer and so

14、fter than in bulkBonds in Sn (Pb) clusters are (much) shorter and stiffer than in bulkCoordinationnumber is thekey parameter16Scaling RelationsStiffness (length)-11 for a given elementClustersPeriodic systemsJ. Paul & SN17Competition between fewer bonds and stiffer bonds.Results for elastic modu

15、lus for dilation for Si, Sn and Pb (clusters & bulk)Clusters softer than bulkData collapse due to scaling relations between stiffness, length and coordination.Higher the CN in the bulk, less the relative softening in clusters.R. Pushpa, U.V. Waghmare & SN18Consequences of enhanced stiffnessu

16、rms decreases as N decreases (for small N) non-monotonically Lindemann melting temperature increases as N decreases, very non-monotonicallyCompetition between fewer bonds and stiffer bonds.When CN in bulk is high/low, clusters have lower/higher urms & higher/lower Tm than bulkR. Pushpa, U.V. Wag

17、hmare & SN19Enhanced magnetism in low-d systemsClusters/monolayers tend to be more magnetic than bulk (Stoner criterion)FeCoNiRuRhPdOsIrPtBulk is magneticClusters and monolayers ferromagnetic Fascinating magnetic properties Lower coordination + magnetism affects reaction rate when used as cataly

18、sts20Factors affecting catalysisModel systems:Catalytic dissociation of NO on Rh - Surfaces, monolayers and clusters- At various lattice constants- Free standing or on MgO substrates- Non-magnetic or spin polarized calculationsAim: to separate out effects of coordination number, strain, charge trans

19、fer & magnetismSpin catalysts?NORh21Spin of Rh clusters + NO adsorptionSystemMagnetic moment (bare clusters)(B/Rh atomMagnetic moment (with NO)(B/Rh atom)Eads of NO(eV/NO molecule)N-O bond length ()RhNO3.00.03.231.19Rh2NO2.00.543.101.21Rh3NO1.670.722.891.23P. Ghosh, R. Pushpa, S.de Gironcoli &am

20、p; SN22Anharmonic Effects Expand energy in powers of displacements: E(x) = T + c(x-x0)2 g(x-x0)3 + f(x-x0)4 + harmonic anharmonic Some consequences: pressure dependence of bulk modulus, Grneisen parameters, thermal expansion, phonon frequency shifts and finite lifetimes,. Have studied using frozen phonons, quasiharmonic approximation, etc. Exchange-correlation errors less for anharmonic than harmonic properties(?), increase with temperature(?).23Thermal expansion

溫馨提示

  • 1. 本站所有資源如無(wú)特殊說(shuō)明,都需要本地電腦安裝OFFICE2007和PDF閱讀器。圖紙軟件為CAD,CAXA,PROE,UG,SolidWorks等.壓縮文件請(qǐng)下載最新的WinRAR軟件解壓。
  • 2. 本站的文檔不包含任何第三方提供的附件圖紙等,如果需要附件,請(qǐng)聯(lián)系上傳者。文件的所有權(quán)益歸上傳用戶所有。
  • 3. 本站RAR壓縮包中若帶圖紙,網(wǎng)頁(yè)內(nèi)容里面會(huì)有圖紙預(yù)覽,若沒(méi)有圖紙預(yù)覽就沒(méi)有圖紙。
  • 4. 未經(jīng)權(quán)益所有人同意不得將文件中的內(nèi)容挪作商業(yè)或盈利用途。
  • 5. 人人文庫(kù)網(wǎng)僅提供信息存儲(chǔ)空間,僅對(duì)用戶上傳內(nèi)容的表現(xiàn)方式做保護(hù)處理,對(duì)用戶上傳分享的文檔內(nèi)容本身不做任何修改或編輯,并不能對(duì)任何下載內(nèi)容負(fù)責(zé)。
  • 6. 下載文件中如有侵權(quán)或不適當(dāng)內(nèi)容,請(qǐng)與我們聯(lián)系,我們立即糾正。
  • 7. 本站不保證下載資源的準(zhǔn)確性、安全性和完整性, 同時(shí)也不承擔(dān)用戶因使用這些下載資源對(duì)自己和他人造成任何形式的傷害或損失。

最新文檔

評(píng)論

0/150

提交評(píng)論