Theoretical approaches to the ab-initio study of complex systems

Size: px
Start display at page:

Download "Theoretical approaches to the ab-initio study of complex systems"

Transcription

1 Theoretical approaches to the ab-initio study of complex systems Olivia Pulci European Theoretical Spectroscopy Facilty (ETSF), and CNR-INFM, Dipartimento di Fisica Università di Roma Tor Vergata NAST-ISM Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

2 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 3-D 2-D Surfaces bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

3

4 BEAMLINES: Optics (O. Pulci) EELS (F. Sottile) X-ray (J. Rehr) Transport (P. Bokes) Time-resolved excitations (M. Marques) Photoemission (C. Verdozzi) Raman (G. Rignanese) new

5 Developmen t of theory training Undergraduates PhD Students Post Docs Other colleagues exp + Industry! Developmen t of codes Distribution: ABINIT FHI OCTOPUS Yambo DP+EXC TOSCA Research Carrying on Projects for users

6 METHODS c MBPT c EXC hν v DFT 1) c ωcv hν v GW 2) TDDFT W ωcv v BSE 3) Excitonic effects

7 Theory development: MB kernel for TDDFT (M. Marsili, A. Marini, R. Del Sole) PRB2003, PRL2003, PRB2007 Electron-phonon coupling (A. Marini) A. Marini Phys. Rev. Lett. 101, (2008) Vertex corrections (M. Marsili, R. Del Sole) M. Marsili, R. Del Sole, in preparation

8 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 2-D Surfaces 3-D bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

9 Daniele Varsano Andrea Marini YAMBO is a multipurpose Ab-Initio Many-Body code for excited state calculations. Conor Hogan released under the Myrta Gruning GPL license on Sept 1 st 2008 Particles(DFT) In these first 6 months... more the 5000 contacts... more the 600 downloads of the source... documentation and tutorials visited 1000 times Quasiparticles(GW) Plasmons (TDDFT) doi: /j.cpc Excitons (BetheSalpeter equation)

10 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 3-D 2-D Surfaces bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

11 0D na no do ts nanoclusters: electronic gap vs. size En = π 2 h2 n 2 2me L2 Quantum confinement M. Marsili, M. Palummo, O. Pulci

12 0D na no do ts : a bs o rption a nd em is s ion Absorption E2 C-DFT E3 Eabs Eem Excited state Ground state Emission e-h pair E4 E1 Cluster geometry Structural minimization performed both in the ground state and in presence of the e-h pair

13 0D na no do ts (O. P ulc i) h Absorption a.u. Emission Ψ exc ( re, rh ) 2 Experiment PRB 2007 PL peak related to O bridge O. Pulci in collaboration with S. Ossicini group (Modena)Ma et al. APL, (1999))

14 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 3-D 2-D Surfaces bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

15 1D na no w ires (P a lum m o ) Si Wires atomic structure d=4å

16 1D na no w ires Si NWs Excitonic Gap: theory vs exp. M.Bruno et al. PRL 2007

17 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 3-D 2-D Surfaces bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

18 2D: surfaces (ongoing projects) GaSb(001) c2x6 Conor Hogan C(111)2x1 Margherita Marsili Ice (0001) Viviana Garbuio x y

19 ISM-NAST collaboration (1): Ge(111):Sn ( 3 ) 3 R 30 : RT 3 3 : LT Eur. Phys. Lett Top view Metal semiconductor interfaces: electronic properties at the GW level and comparison experimental/calculated STM images With Paola Gori, Fabio Ronci, Stefano Colonna, and Antonio Cricenti (ISM)

20 ISM-NAST collaboration (2): 3C-SiC(001) c(4x2) Group IV surfaces: determination of actual ground state via comparison with RAS results O. Pulci, Paola Gori and Antonio Cricenti (ISM)

21 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 3-D 2-D Surfaces bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

22 ISM-NAST collaboration (3): oxides excitonic effects in ZnO Optical properties of oxides: inclusion of excitonic effects at the BSE or TDDFT level with Paola Gori and Antonio Cricenti (ISM)

23 G ro up a c tivities Biological systems Theory Ab-initio: (NOT one puts nothing in, one gets nothing out!!) Code development 0-D Generality, transferability 0D-3D detailed physical informations 1-D Nanowires Nanoclusters 3-D 2-D Surfaces bulks Olivia Pulci, Maurizia Palummo, Conor Hogan, Andrea Marini, Margherita Marsili, Viviana Garbuio, Adriano Mosca Conte, Elena Cannuccia, Rodolfo Del Sole

24 H 2O (G a rbuio -P ulc i) Absorption Electronic Gap Exp DFT BSE PRL 2006 Exciton binding energy 2.4 ev EXP-L.R. Painter et al., Phys. Rev. Lett. 21, 282 (1968) G.D. Kerr et al., Phys. Rev. A 5, 2523 (1972)

25 B io : c o nquering the enviro nm ent (M o s c a OPTICAL PROPERTIES OF INDOLE IN WATER SOLUTION BY MBPT/MM C o nte-p ulc i) A COMBINATION OF MANY BODY METHODS (GW+BSE) WITH QM/MM TO STUDY BIOLOGICAL MOLECULES IN SOLUTION QM MM A. Mosca Conte, E. Ippoliti,R. Del Sole, P. Carloni, O. Pulci, JCTC (in press)

26 Towards Biological Systems Ongoing projects: Study of solutions: formamide in water V. Garbuio Rhodopsin: retinal photoisomerization osca Conte, NAST project with L. Guidoni Flavin Cannuccia

27 Conclusions and Perspectives WHAT WE DO ab-initio electronic and optical properties of 0-3D systems WHAT WE CAN DO WITH SOME EFFORT atoms all ab-initio (hybrid methods needed) WHAT (RIGHT NOW) WE CANNOT DO (but we are working on it) excited state molecular dynamics

28 Call for projects always opened Thank you for your attention

29

30 T heo ry (M a rs ili-d el S o le) GWΓ approch to band energies calculations

31 T heo ry (S a ng a lli)

32 T heo ry (S a ng a lli)

33 T heo ry (S a ng a lli)

34 T heo ry (S a ng a lli)

35 T heo ry (A tta c a lite-m a rini) Luminescence by using non-equilibrium Green Function

36 T heo ry (A tta c a lite-m a rini) Prospective: Create a theoretical and computational tool to study and predict light emission 1) Luminescence: Catho and photo luminescence 2) Role of temperature, defects and confinement 3) Non-linear Optics, optical gain, Optical Switching

37 T heo ry (A tta c a lite-m a rini) Working Plan I. Real-time dynamics of electrons by using Non-Equilibrium Green Functions. Luminescence of bulk materials i H 0 G t 1, t 2 =[U t 1 HF t 1 ]G t 1, t 2 I t 1, t 2 t1 II. Electron-phonon coupling. Relaxation through emission of phonons. Luminescence from indirect-gap systems 2 q t 1, t 2 =i g D t 1, t 2 G k q q k q t 1, t 2 III.Forces in the excited state. Luminescence from cluster, wires, polymers and defects (exciton trapping)

38 T heo ry (A tta c a lite-m a rini) Ab-initio Approach The single particle electronic states are first evaluated using density functional theory (DFT) Why Non-equilibrium G t 1, t 2 =i a t 2 a t 1 Green Functions? G t 1, t 2 = i a t 1 a t 2 Systematic approach to progressively include electronic correlation effects and electron-phonon interaction Can be used as starting point to derive approximate theory (Kinetic equations, Bloch equations, Boltzmann equations) All this theory will be implemented in ->

39 1D C O N J U G A T E D P O L Y M E R S (C a nnuc c ia -M a rini) EXCITON-VIBRON INTERACTION IN ONE DIMENSIONAL CONJUGATED POLYMERS poly(p-phenylene vinylene)... Exp. 80K Exp. 300K Bound exciton characterized by an asymmetric line-shape, together with strong vibronicinduced side bands Exp. K Pichler et al 1993 J. Phys.: Condens. Matter Theory Trans polyacetylene Phys. Rev. Lett. 82, (1999) Phys. Rev. B 38, (1988)

40 1D na no w ires (P a lum m o ) Experiment: Ma et al., Science 2003

41 1D na no w ires (P a lum m o ) Si NWs Exchange splitting : BSE theory vs Exp.

42 Y A M B O (H o g a n-m a rini) doi: /j.cpc Many-body perturbation theory: - Quasiparticle corrections (GW) - Optical and energy loss spectra including excitons and local field effects...and much more! Finite temperature. Electronphonon and polarons Real-axis GW Self-consistent COHSEX, HF, EXX... (_SC) Surface Spectroscopy Collinear and non-collinear spin Many-Body TDDFT kernel Total Energy (ACFDT)

43 1D na no w ires (P a lum m o ) Doping Si NWs: influence on the optical properties

44 1D na no w ires (P a lum m o ) GW corrections: doping and surface termination

45 2D G a S b(001) (H o g a n ) Structure and Optical Properties of Sb-stabilized G asb(001) C onor Hogan, R odolfo Del Sole (R ome) R ita M agri (M odena) c(2x10) RHEED c(2x6) (1x3) c(2x10) Houze (2007) Resch-Esser (1997) Barvosa-Carter (2000) c(2x6) (1x3)

46 2D G a S b(001) ( H o g a n) Surface optical spectra for c(2x6) Houze et al., (2007) All previous structures fail to reproduce correctly the experimental RA spectra

47 2D G a S b(001) (H o g a n ) New structure: Second layer Ga 'doping' Electron counting rule fulfilled (1 Ga per (2x6) unit) Low energy, semiconducting surface (stable at 500C?) Better agreement with RA spectra True surface based on long chains with interruptions

48 Ab-initio Finite-Temperatures Excitons A. Marini Phys. Rev. Lett. 101, (2008) BSE is solved, in ab-initio manner, including the coupling with the lattice vibrations. E-ph interaction is treated in the Heine, Allen and Cardona approach. q k k k k p k p k p Exp. BSE

49 3D B io (G a rbuio -P ulc i) FORMAMIDE in water

50 0D : na no do ts Formation energy: Single- vs co-doping Si87H76 Si147H100 Largest possible distance Nearest neigbours Co-doping easier due to charge compensation No size dependence Cantele et al, Phys. Rev. B 72, (2005) S. Ossicini, F. Iori et al, Appl. Phys. Lett (2005) F. Iori, E. Degoli, S. Ossicini et al., J. Lum. (2006)

51 0D na no do ts Gap Homo-Lumo Eg decrease as nc s size increase Eg of codoped is shifted towards lower energies undoped codoped

52 0D na no do ts Absorption and Emission processes AbsorptionEmission E2 E3 Eabs Eem E4 E1 Excited state Ground state e-h pair

53 0D na no do ts (P ulc i-m a rs ili-p a lum m o ) Optical spectra within GW+BSE Si33BPH36 DFT Abs. (ev) 2.77 Emis. (ev) 1.78 Ψ exc ( re, rh ) 2 GW+BSE Stokes shift Hole fixed on B Electron localizes on P Agreement with experimental outcomes: With F. Iori et al PRB2007 M. Fujii, et al., Appl. Phys. Lett. 85, 1158 (2004)

54 PARIS (Reining) ROME (Del Sole) MILAN (Onida) YORK (Godby) LOUVAIN (Gonze) NANOQUANTA nnetwork of Excellence S.SEBASTIAN (Rubio) Nanoscale Quantum Simulations for Nanostructures and Advanced Materials BERLIN FHI (Scheffler) LUND (von Barth) JENA (Bechstedt) BERLIN FU (Gross)

55 MBPT/MM Method Application to indole in water solution

56 3D B io (G a rbuio -P ulc i) LIQUID WATER Liquid water = disordered system= huge unit cell 20 MD snapshots and average of results.

57 QM MM

58 3D B io (M o s c a C o nte-p ulc i) PHOTO-ISOMERIZATION OF RETINAL IN RHODOPSIN FIRSTS STEPS OF THE MECHANISMS OF VISION IN LIVING BEINGS Adriano Mosca Conte, Olivia Pulci, Rodolfo Del Sole, Leonardo Guidoni

59 3D B io (M o s c a C o nte-p ulc i) PHOTO-ISOMERIZATION OF RETINAL IN RHODOPSIN MINIMAL BASE MODEL Adriano Mosca Conte, Olivia Pulci, Rodolfo Del Sole, Leonardo Guidoni

Introduction to Green s functions

Introduction to Green s functions Introduction to Green s functions Matteo Gatti ETSF Users Meeting and Training Day Ecole Polytechnique - 22 October 2010 Outline 1 Motivation 2 Green s functions 3 The GW Approximation 4 The Bethe-Salpeter

More information

Prof. Olivia Pulci Curriculum Vitae

Prof. Olivia Pulci Curriculum Vitae Prof. Olivia Pulci Curriculum Vitae Personal Data: Name: Pulci, Olivia Birth: Civitavecchia (Italy), March 3, 1966 Languages: Italian (mother tongue), English (fluent), German (basic knowledge) Private

More information

Hard Condensed Matter WZI

Hard Condensed Matter WZI Hard Condensed Matter WZI Tom Gregorkiewicz University of Amsterdam VU-LaserLab Dec 10, 2015 Hard Condensed Matter Cluster Quantum Matter Optoelectronic Materials Quantum Matter Amsterdam Mark Golden Anne

More information

The Application of Density Functional Theory in Materials Science

The Application of Density Functional Theory in Materials Science The Application of Density Functional Theory in Materials Science Slide 1 Outline Atomistic Modelling Group at MUL Density Functional Theory Numerical Details HPC Cluster at the MU Leoben Applications

More information

Chemical Synthesis. Overview. Chemical Synthesis of Nanocrystals. Self-Assembly of Nanocrystals. Example: Cu 146 Se 73 (PPh 3 ) 30

Chemical Synthesis. Overview. Chemical Synthesis of Nanocrystals. Self-Assembly of Nanocrystals. Example: Cu 146 Se 73 (PPh 3 ) 30 Chemical Synthesis Spontaneous organization of molecules into stable, structurally well-defined aggregates at the nanometer length scale. Overview The 1-100 nm nanoscale length is in between traditional

More information

Electronic transport properties of nano-scale Si films: an ab initio study

Electronic transport properties of nano-scale Si films: an ab initio study Electronic transport properties of nano-scale Si films: an ab initio study Jesse Maassen, Youqi Ke, Ferdows Zahid and Hong Guo Department of Physics, McGill University, Montreal, Canada Motivation (of

More information

Lecture 3: Optical Properties of Bulk and Nano. 5 nm

Lecture 3: Optical Properties of Bulk and Nano. 5 nm Lecture 3: Optical Properties of Bulk and Nano 5 nm The Previous Lecture Origin frequency dependence of χ in real materials Lorentz model (harmonic oscillator model) 0 e - n( ) n' n '' n ' = 1 + Nucleus

More information

Exciton dissociation in solar cells:

Exciton dissociation in solar cells: Exciton dissociation in solar cells: Xiaoyang Zhu Department of Chemistry University of Minnesota, Minneapolis t (fs) 3h! E, k h! Pc Bi e - 1 Acknowledgement Organic semiconductors: Mutthias Muntwiler,

More information

Applied Physics of solar energy conversion

Applied Physics of solar energy conversion Applied Physics of solar energy conversion Conventional solar cells, and how lazy thinking can slow you down Some new ideas *************************************************************** Our work on semiconductor

More information

Surface-state engineering for interconnects on H-passivated Si(100)

Surface-state engineering for interconnects on H-passivated Si(100) Surface-state engineering for interconnects on H-passivated Si(100) Roberto Robles, Mikaël Kepenekian, Christian Joaquim, Nicolás Lorente International Workshop on Nanopackaging Grenoble, June 27th 28th,

More information

Lecture 3: Optical Properties of Bulk and Nano. 5 nm

Lecture 3: Optical Properties of Bulk and Nano. 5 nm Lecture 3: Optical Properties of Bulk and Nano 5 nm First H/W#1 is due Sept. 10 Course Info The Previous Lecture Origin frequency dependence of χ in real materials Lorentz model (harmonic oscillator model)

More information

Spatially separated excitons in 2D and 1D

Spatially separated excitons in 2D and 1D Spatially separated excitons in 2D and 1D David Abergel March 10th, 2015 D.S.L. Abergel 3/10/15 1 / 24 Outline 1 Introduction 2 Spatially separated excitons in 2D The role of disorder 3 Spatially separated

More information

Introduction OLEDs OTFTs OPVC Summary. Organic Electronics. Felix Buth. Walter Schottky Institut, TU München. Joint Advanced Student School 2008

Introduction OLEDs OTFTs OPVC Summary. Organic Electronics. Felix Buth. Walter Schottky Institut, TU München. Joint Advanced Student School 2008 Felix Buth Joint Advanced Student School 2008 Outline 1 Introduction Difference organic/inorganic semiconductors From molecular orbitals to the molecular crystal 2 Organic Light Emitting Diodes Basic Principals

More information

Introduction to many-body Green s functions

Introduction to many-body Green s functions Introduction to many-body Green s functions Matteo Gatti European Theoretical Spectroscopy Facility (ETSF) NanoBio Spectroscopy Group - UPV San Sebastián - Spain [email protected] - http://nano-bio.ehu.es

More information

New magnetism of 3d monolayers grown with oxygen surfactant: Experiment vs. ab initio calculations

New magnetism of 3d monolayers grown with oxygen surfactant: Experiment vs. ab initio calculations New magnetism of 3d monolayers grown with oxygen surfactant: Experiment vs. ab initio calculations 1. Growth and structure 2. Magnetism and MAE 3. Induced magnetism at oxygen Klaus Baberschke Institut

More information

Lecture 15 - application of solid state materials solar cells and photovoltaics. Copying Nature... Anoxygenic photosynthesis in purple bacteria

Lecture 15 - application of solid state materials solar cells and photovoltaics. Copying Nature... Anoxygenic photosynthesis in purple bacteria Lecture 15 - application of solid state materials solar cells and photovoltaics. Copying Nature... Anoxygenic photosynthesis in purple bacteria Simple example, but still complicated... Photosynthesis is

More information

Solid State Detectors = Semi-Conductor based Detectors

Solid State Detectors = Semi-Conductor based Detectors Solid State Detectors = Semi-Conductor based Detectors Materials and their properties Energy bands and electronic structure Charge transport and conductivity Boundaries: the p-n junction Charge collection

More information

Electrophoretic Gold Nanoparticles Depostion On Carbon Nanotubes For NO 2 Sensors

Electrophoretic Gold Nanoparticles Depostion On Carbon Nanotubes For NO 2 Sensors European Network on New Sensing Technologies for Air Pollution Control and Environmental Sustainability - EuNetAir COST Action TD1105 2 nd International Workshop EuNetAir on New Sensing Technologies for

More information

Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications

Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications Saulius Marcinkevičius Optics, ICT, KTH 1 Outline Optical near field. Principle of scanning near field optical microscope

More information

Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting

Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting Optical Hyperdoping: Transforming Semiconductor Band Structure for Solar Energy Harvesting 3G Solar Technologies Multidisciplinary Workshop MRS Spring Meeting San Francisco, CA, 5 April 2010 Michael P.

More information

Nanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture

Nanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture Nanoelectronics 09 Atsufumi Hirohata Department of Electronics 12:00 Wednesday, 4/February/2015 (P/L 006) Quick Review over the Last Lecture ( Field effect transistor (FET) ): ( Drain ) current increases

More information

Ph.D Brochure Department of Physics

Ph.D Brochure Department of Physics Ph.D Brochure Department of Physics Year 2016 Introduction High Energy Physics Optics, Spectroscopy and Laser-Plasma Physics Computational Condensed Matter Physics Experimental Condensed Matter Physics

More information

- particle with kinetic energy E strikes a barrier with height U 0 > E and width L. - classically the particle cannot overcome the barrier

- particle with kinetic energy E strikes a barrier with height U 0 > E and width L. - classically the particle cannot overcome the barrier Tunnel Effect: - particle with kinetic energy E strikes a barrier with height U 0 > E and width L - classically the particle cannot overcome the barrier - quantum mechanically the particle can penetrated

More information

Size effects. Lecture 6 OUTLINE

Size effects. Lecture 6 OUTLINE Size effects 1 MTX9100 Nanomaterials Lecture 6 OUTLINE -Why does size influence the material s properties? -How does size influence the material s performance? -Why are properties of nanoscale objects

More information

The plasmoelectric effect: optically induced electrochemical potentials in resonant metallic structures

The plasmoelectric effect: optically induced electrochemical potentials in resonant metallic structures The plasmoelectric effect: optically induced electrochemical potentials in resonant metallic structures Matthew T. Sheldon and Harry A. Atwater Thomas J. Watson Laboratories of Applied Physics, California

More information

Theory of Light Scattering in Condensed Matter

Theory of Light Scattering in Condensed Matter Proceedings of the First Joint USA USSR Symposium Theory of Light Scattering in Condensed Matter Edited by Bernard Bendow Solid State Sciences Division Rome Air Development Center Hanscom AFB, Massachusetts

More information

Thermal unobtainiums? The perfect thermal conductor and the perfect thermal insulator

Thermal unobtainiums? The perfect thermal conductor and the perfect thermal insulator Thermal unobtainiums? The perfect thermal conductor and the perfect thermal insulator David G. Cahill Materials Research Lab and Department of Materials Science and Engineering, U. of Illinois Gratefully

More information

PCV Project: Excitons in Molecular Spectroscopy

PCV Project: Excitons in Molecular Spectroscopy PCV Project: Excitons in Molecular Spectroscopy Introduction The concept of excitons was first introduced by Frenkel (1) in 1931 as a general excitation delocalization mechanism to account for the ability

More information

Microcavity Quantum Electrodynamics:

Microcavity Quantum Electrodynamics: Microcavity Quantum Electrodynamics: From atoms to quantum dots Boris Anghelo Rodríguez Rey Grupo de Física Atómica y Molecular Instituto de Física, Universidad de Antioquia September 26, IWQCD 2012 Universidad

More information

The influence of graphene curvature on hydrogen adsorption. Sarah Goler

The influence of graphene curvature on hydrogen adsorption. Sarah Goler The influence of graphene curvature on hydrogen adsorption Sarah Goler Laboratorio NEST, Istituto Nanoscienze CNR and Scuola Normale Superiore, Piazza San Silvestro 12, 56127 Pisa, Italy Center for Nanotechnology

More information

Developments in Photoluminescence Characterisation for Silicon PV

Developments in Photoluminescence Characterisation for Silicon PV Developments in Photoluminescence Characterisation for Silicon PV School of Photovoltaic and Solar Energy Engineering Bernhard Mitchell 1, Thorsten Trupke 1,2, Jürgen W. Weber 2, Johannes Greulich 3, Matthias

More information

Chapter 5. Second Edition ( 2001 McGraw-Hill) 5.6 Doped GaAs. Solution

Chapter 5. Second Edition ( 2001 McGraw-Hill) 5.6 Doped GaAs. Solution Chapter 5 5.6 Doped GaAs Consider the GaAs crystal at 300 K. a. Calculate the intrinsic conductivity and resistivity. Second Edition ( 2001 McGraw-Hill) b. In a sample containing only 10 15 cm -3 ionized

More information

From Quantum to Matter 2006

From Quantum to Matter 2006 From Quantum to Matter 006 Why such a course? Ronald Griessen Vrije Universiteit, Amsterdam AMOLF, May 4, 004 vrije Universiteit amsterdam Why study quantum mechanics? From Quantum to Matter: The main

More information

Photoinduced volume change in chalcogenide glasses

Photoinduced volume change in chalcogenide glasses Photoinduced volume change in chalcogenide glasses (Ph.D. thesis points) Rozália Lukács Budapest University of Technology and Economics Department of Theoretical Physics Supervisor: Dr. Sándor Kugler 2010

More information

SUPERCONDUCTIVITY. PH 318- Introduction to superconductors 1

SUPERCONDUCTIVITY. PH 318- Introduction to superconductors 1 SUPERCONDUCTIVITY property of complete disappearance of electrical resistance in solids when they are cooled below a characteristic temperature. This temperature is called transition temperature or critical

More information

High Open Circuit Voltage of MQW Amorphous Silicon Photovoltaic Structures

High Open Circuit Voltage of MQW Amorphous Silicon Photovoltaic Structures High Open Circuit Voltage of MQW Amorphous Silicon Photovoltaic Structures ARGYRIOS C. VARONIDES Physics and EE Department University of Scranton 800 Linden Street, Scranton PA, 18510 United States Abstract:

More information

Optics and Spectroscopy at Surfaces and Interfaces

Optics and Spectroscopy at Surfaces and Interfaces Vladimir G. Bordo and Horst-Gunter Rubahn Optics and Spectroscopy at Surfaces and Interfaces WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Contents Preface IX 1 Introduction 1 2 Surfaces and Interfaces 5

More information

Organic semiconductors

Organic semiconductors Plastic (Organic) Solar Cells: Accomplishments, Challenges, and Strategies Sumit Chaudhary Assistant Professor Department of Electrical and Computer Engineering Materials Science and Engineering Iowa State

More information

Molecular Dynamics Simulations

Molecular Dynamics Simulations Molecular Dynamics Simulations Yaoquan Tu Division of Theoretical Chemistry and Biology, Royal Institute of Technology (KTH) 2011-06 1 Outline I. Introduction II. Molecular Mechanics Force Field III. Molecular

More information

Darrick Chang ICFO The Institute of Photonic Sciences Barcelona, Spain. April 2, 2014

Darrick Chang ICFO The Institute of Photonic Sciences Barcelona, Spain. April 2, 2014 Darrick Chang ICFO The Institute of Photonic Sciences Barcelona, Spain April 2, 2014 ICFO The Institute of Photonic Sciences 10 minute walk 11 years old 22 Research Groups 300 people Research themes: Quantum

More information

SEMICONDUCTOR I: Doping, semiconductor statistics (REF: Sze, McKelvey, and Kittel)

SEMICONDUCTOR I: Doping, semiconductor statistics (REF: Sze, McKelvey, and Kittel) SEMICONDUCTOR I: Doping, semiconductor statistics (REF: Sze, McKelvey, and Kittel) Introduction Based on known band structures of Si, Ge, and GaAs, we will begin to focus on specific properties of semiconductors,

More information

Molecular Spectroscopy

Molecular Spectroscopy Molecular Spectroscopy UV-Vis Spectroscopy Absorption Characteristics of Some Common Chromophores UV-Vis Spectroscopy Absorption Characteristics of Aromatic Compounds UV-Vis Spectroscopy Effect of extended

More information

1 The water molecule and hydrogen bonds in water

1 The water molecule and hydrogen bonds in water The Physics and Chemistry of Water 1 The water molecule and hydrogen bonds in water Stoichiometric composition H 2 O the average lifetime of a molecule is 1 ms due to proton exchange (catalysed by acids

More information

What is molecular dynamics (MD) simulation and how does it work?

What is molecular dynamics (MD) simulation and how does it work? What is molecular dynamics (MD) simulation and how does it work? A lecture for CHM425/525 Fall 2011 The underlying physical laws necessary for the mathematical theory of a large part of physics and the

More information

Pina Romaniello Department of Physics Phone: +39 02 50317377 Università degli Studi di Milano Fax: +39 02 503174 82 via Celoria 16

Pina Romaniello Department of Physics Phone: +39 02 50317377 Università degli Studi di Milano Fax: +39 02 503174 82 via Celoria 16 Curriculum Vitae Pina Romaniello Department of Physics Phone: +39 02 50317377 Università degli Studi di Milano Fax: +39 02 503174 82 via Celoria 16 [email protected] 20133 Milano, Italy http://www.etsf.it/milan_group_link1.html/

More information

Comprehensive Investigation of Sequential Plasma Activated Si/Si Bonded Interface for Nano-integration

Comprehensive Investigation of Sequential Plasma Activated Si/Si Bonded Interface for Nano-integration Comprehensive Investigation of Sequential Plasma Activated Si/Si Bonded Interface for Nano-integration M G Kibria, F Zhang, T H Lee, M J Kim and M M R Howlader Dept. Electrical and Computer Engineering,

More information

Laboratorio Regionale LiCryL CNR-INFM

Laboratorio Regionale LiCryL CNR-INFM Laboratorio Regionale LiCryL CNR-INFM c/o Physics Department - University of Calabria, Ponte P. Bucci, Cubo 33B, 87036 Rende (CS) Italy UNIVERSITÀ DELLA CALABRIA Dipartimento di FISICA Researchers Dr.

More information

Modification of Graphene Films by Laser-Generated High Energy Particles

Modification of Graphene Films by Laser-Generated High Energy Particles Modification of Graphene Films by Laser-Generated High Energy Particles Elena Stolyarova (Polyakova), Ph.D. ATF Program Advisory and ATF Users Meeting April 2-3, 2009, Berkner Hall, Room B, BNL Department

More information

An organic semiconductor is an organic compound that possesses similar

An organic semiconductor is an organic compound that possesses similar MSE 542 Final Term Paper Title: Organic Semiconductor for Flexible Electronics Name: Chunhung Huang Introduction: An organic semiconductor is an organic compound that possesses similar properties to inorganic

More information

What is Nanophysics: Survey of Course Topics. Branislav K. Nikolić

What is Nanophysics: Survey of Course Topics. Branislav K. Nikolić What is Nanophysics: Survey of Course Topics Branislav K. Nikolić Department of Physics and Astronomy, University of Delaware, Newark, DE 19716, U.S.A. http://wiki.physics.udel.edu/phys824 Definition of

More information

Anharmonicity and Weak Mode Assignment in La 2 x Sr x CuO 4 with Oxygen Isotopic Substitution

Anharmonicity and Weak Mode Assignment in La 2 x Sr x CuO 4 with Oxygen Isotopic Substitution Vol. 111 (2007) ACTA PHYSICA POLONICA A No. 1 Proceedings of the Symposium K: Complex Oxide Materials for New Technologies of E-MRS Fall Meeting 2006, Warsaw, September 4 8, 2006 Anharmonicity and Weak

More information

Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs

Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs TracePro Opto-Mechanical Design Software s Fluorescence Property Utility TracePro s Fluorescence Property

More information

Electron spectroscopy Lecture 1-21. Kai M. Siegbahn (1918 - ) Nobel Price 1981 High resolution Electron Spectroscopy

Electron spectroscopy Lecture 1-21. Kai M. Siegbahn (1918 - ) Nobel Price 1981 High resolution Electron Spectroscopy Electron spectroscopy Lecture 1-21 Kai M. Siegbahn (1918 - ) Nobel Price 1981 High resolution Electron Spectroscopy 653: Electron Spectroscopy urse structure cture 1. Introduction to electron spectroscopies

More information

Project 2B Building a Solar Cell (2): Solar Cell Performance

Project 2B Building a Solar Cell (2): Solar Cell Performance April. 15, 2010 Due April. 29, 2010 Project 2B Building a Solar Cell (2): Solar Cell Performance Objective: In this project we are going to experimentally measure the I-V characteristics, energy conversion

More information

UV-Vis Vis spectroscopy. Electronic absorption spectroscopy

UV-Vis Vis spectroscopy. Electronic absorption spectroscopy UV-Vis Vis spectroscopy Electronic absorption spectroscopy Absortpion spectroscopy Provide information about presence and absence of unsaturated functional groups Useful adjunct to IR Determination of

More information

Singlet fission for solar energy conversion A theoretical insight. David Casanova

Singlet fission for solar energy conversion A theoretical insight. David Casanova Singlet fission for solar energy conversion A theoretical insight David Casanova Quantum Days in Bilbao July 16, 2014 Harvesting Solar Energy Solar energy 1h = 1 year human consumption We use ~ 0.07% Earth

More information

Magnetization dynamics in lanthanides new frontiers in spin-dependent band mapping at BESSY VSR

Magnetization dynamics in lanthanides new frontiers in spin-dependent band mapping at BESSY VSR 1 FEMTOMAGNETISM BESSY VSR 1 Magnetization dynamics in lanthanides new frontiers in spin-dependent band mapping at BESSY VSR Martin Weinelt 2 FEMTOMAGNETISM BESSY VSR 2 Photon flux Ti:Sa UV 10 mw 86 MHz,

More information

Ultrahigh-efficiency solar cells based on nanophotonic design

Ultrahigh-efficiency solar cells based on nanophotonic design Ultrahigh-efficiency solar cells based on nanophotonic design Albert Polman Piero Spinelli Jorik van de Groep Claire van Lare Bonna Newman Erik Garnett Marc Verschuuren Ruud Schropp Wim Sinke Center for

More information

Free Electron Fermi Gas (Kittel Ch. 6)

Free Electron Fermi Gas (Kittel Ch. 6) Free Electron Fermi Gas (Kittel Ch. 6) Role of Electrons in Solids Electrons are responsible for binding of crystals -- they are the glue that hold the nuclei together Types of binding (see next slide)

More information

Nano-Spectroscopy. Solutions AFM-Raman, TERS, NSOM Chemical imaging at the nanoscale

Nano-Spectroscopy. Solutions AFM-Raman, TERS, NSOM Chemical imaging at the nanoscale Nano-Spectroscopy Solutions AFM-Raman, TERS, NSOM Chemical imaging at the nanoscale Since its introduction in the early 80 s, Scanning Probe Microscopy (SPM) has quickly made nanoscale imaging an affordable

More information

Controlling Gold Nanoparticles with Atomic Precision: Synthesis and Structure Determination

Controlling Gold Nanoparticles with Atomic Precision: Synthesis and Structure Determination Controlling Gold Nanoparticles with Atomic Precision: Synthesis and Structure Determination Huifeng Qian Department of Chemistry, Carnegie Mellon University, USA Advisor: Prof. Rongchao Jin Background

More information

NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION

NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION Olivier Palais, Damien Barakel, David Maestre, Fabrice Gourbilleau and Marcel Pasquinelli 1 Outline Photovoltaic today

More information

Optical Properties of Solids. Claudia Ambrosch-Draxl Chair of Atomistic Modelling and Design of Materials University Leoben, Austria

Optical Properties of Solids. Claudia Ambrosch-Draxl Chair of Atomistic Modelling and Design of Materials University Leoben, Austria Optical Properties of Solids Claudia Ambrosch-Draxl Chair of Atomistic Modelling and Design of Materials University Leoben, Austria Outline Basics Program Examples Outlook light scattering dielectric tensor

More information

bulk 5. Surface Analysis Why surface Analysis? Introduction Methods: XPS, AES, RBS

bulk 5. Surface Analysis Why surface Analysis? Introduction Methods: XPS, AES, RBS 5. Surface Analysis Introduction Methods: XPS, AES, RBS Autumn 2011 Experimental Methods in Physics Marco Cantoni Why surface Analysis? Bulk: structural function Electrical/thermal conduction Volume increases

More information

Applications of Quantum Chemistry HΨ = EΨ

Applications of Quantum Chemistry HΨ = EΨ Applications of Quantum Chemistry HΨ = EΨ Areas of Application Explaining observed phenomena (e.g., spectroscopy) Simulation and modeling: make predictions New techniques/devices use special quantum properties

More information

High Efficiency Black Polymer Solar Cells November 2012 Annual Report

High Efficiency Black Polymer Solar Cells November 2012 Annual Report High Efficiency Black Polymer Solar Cells November 2012 Annual Report PI: Dr. Franky So External Collaborators: John Reynolds, Georgia Tech Industry Partner: Sestar Technologies, LLC Students: Cephas Small

More information

Orbital Dynamics coupled with Jahn-Teller phonons in Strongly Correlated Electron System

Orbital Dynamics coupled with Jahn-Teller phonons in Strongly Correlated Electron System The 5 th Scienceweb GCOE International Symposium 1 Orbital Dynamics coupled with Jahn-Teller phonons in Strongly Correlated Electron System Department of Physics, Tohoku University Joji Nasu In collaboration

More information

Nano Optics: Overview of Research Activities. Sergey I. Bozhevolnyi SENSE, University of Southern Denmark, Odense, DENMARK

Nano Optics: Overview of Research Activities. Sergey I. Bozhevolnyi SENSE, University of Southern Denmark, Odense, DENMARK Nano Optics: Overview of Research Activities SENSE, University of Southern Denmark, Odense, DENMARK Optical characterization techniques: Leakage Radiation Microscopy Scanning Near-Field Optical Microscopy

More information

XCVII Congresso Nazionale

XCVII Congresso Nazionale XCVII Congresso Nazionale The Fe(001)-p(1x1)O surface: scanning tunneling microscopy (STM) results and related issues Lamberto Duò CNISM - Dipartimento di Fisica Politecnico di Milano Oxides and thin (few

More information

Matter, Materials, Crystal Structure and Bonding. Chris J. Pickard

Matter, Materials, Crystal Structure and Bonding. Chris J. Pickard Matter, Materials, Crystal Structure and Bonding Chris J. Pickard Why should a theorist care? Where the atoms are determines what they do Where the atoms can be determines what we can do Overview of Structure

More information

Chem 1A Exam 2 Review Problems

Chem 1A Exam 2 Review Problems Chem 1A Exam 2 Review Problems 1. At 0.967 atm, the height of mercury in a barometer is 0.735 m. If the mercury were replaced with water, what height of water (in meters) would be supported at this pressure?

More information

Section 5 Molecular Electronic Spectroscopy (lecture 9 ish)

Section 5 Molecular Electronic Spectroscopy (lecture 9 ish) Section 5 Molecular Electronic Spectroscopy (lecture 9 ish) Previously: Quantum theory of atoms / molecules Quantum Mechanics Vl Valence Molecular Electronic Spectroscopy Classification of electronic states

More information

Lecture 1: Basic Concepts on Absorption and Fluorescence

Lecture 1: Basic Concepts on Absorption and Fluorescence Lecture 1: Basic Concepts on Absorption and Fluorescence Nicholas G. James Cell and Molecular Biology University of Hawaii at Manoa, Honolulu The Goal The emission of light after absorption of an outside

More information

Outline. Self-assembled monolayer (SAM) formation and growth. Metal nanoparticles (NP) anchoring on SAM

Outline. Self-assembled monolayer (SAM) formation and growth. Metal nanoparticles (NP) anchoring on SAM From functional nanostructured surfaces to innovative optical biosensors Giacomo Dacarro Dipartimento di Fisica A.Volta Dipartimento di Chimica Generale Università degli Studi di Pavia Dalla scienza dei

More information

h e l p s y o u C O N T R O L

h e l p s y o u C O N T R O L contamination analysis for compound semiconductors ANALYTICAL SERVICES B u r i e d d e f e c t s, E v a n s A n a l y t i c a l g r o u p h e l p s y o u C O N T R O L C O N T A M I N A T I O N Contamination

More information

NMR and IR spectra & vibrational analysis

NMR and IR spectra & vibrational analysis Lab 5: NMR and IR spectra & vibrational analysis A brief theoretical background 1 Some of the available chemical quantum methods for calculating NMR chemical shifts are based on the Hartree-Fock self-consistent

More information

Raman and AFM characterization of carbon nanotube polymer composites Illia Dobryden

Raman and AFM characterization of carbon nanotube polymer composites Illia Dobryden Raman and AFM characterization of carbon nanotube polymer composites Illia Dobryden This project is conducted in High Pressure Spectroscopy Laboratory (Materials Physics group) Supervisor: Professor Alexander

More information

PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. IV Femtosecond Measurements Combined With Near-Field Optical Microscopy - Artyom A.

PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. IV Femtosecond Measurements Combined With Near-Field Optical Microscopy - Artyom A. FEMTOSECOND MEASUREMENTS COMBINED WITH NEAR FIELD OPTICAL MICROSCOPY Artyom A. Astafiev, Semyonov Institute of Chemical Physics, Moscow, Russian Federation. Keywords: diffraction limit nearfield scanning

More information

Quantum control of individual electron and nuclear spins in diamond lattice

Quantum control of individual electron and nuclear spins in diamond lattice Quantum control of individual electron and nuclear spins in diamond lattice Mikhail Lukin Physics Department, Harvard University Collaborators: L.Childress, M.Gurudev Dutt, J.Taylor, D.Chang, L.Jiang,A.Zibrov

More information

Introduction to Quantum Dot Nanocrystals and Nanocrystal Solids. Nuri Yazdani, 10.03.15

Introduction to Quantum Dot Nanocrystals and Nanocrystal Solids. Nuri Yazdani, 10.03.15 Introduction to Quantum Dot Nanocrystals and Nanocrystal Solids Nuri Yazdani, 10.03.15 What is a QD Nanocrystal Time: ~15m What is a QD nanocrystal? Bulk Crystal Periodic lattice of atoms which extends

More information

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy 5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy Resolution of optical microscope is limited by diffraction. Light going through an aperture makes diffraction

More information

nanohub.org Toward On-Line Simulation for Materials and Nanodevices by Design

nanohub.org Toward On-Line Simulation for Materials and Nanodevices by Design Univ. of Florida, Univ. of Illinois, Morgan State Univ., Northwestern Univ. Purdue Univ. Stanford Univ., UTEP nanohub.org Toward On-Line Simulation for Materials and Nanodevices by Design 1 Gerhard Klimeck,

More information

Concept 2. A. Description of light-matter interaction B. Quantitatities in spectroscopy

Concept 2. A. Description of light-matter interaction B. Quantitatities in spectroscopy Concept 2 A. Description of light-matter interaction B. Quantitatities in spectroscopy Dipole approximation Rabi oscillations Einstein kinetics in two-level system B. Absorption: quantitative description

More information

Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation

Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation Outline MAE 493R/593V- Renewable Energy Devices Solar Energy Electromagnetic wave Solar spectrum Solar global radiation Solar thermal energy Solar thermal collectors Solar thermal power plants Photovoltaics

More information

Perfect Fluidity in Cold Atomic Gases?

Perfect Fluidity in Cold Atomic Gases? Perfect Fluidity in Cold Atomic Gases? Thomas Schaefer North Carolina State University 1 Hydrodynamics Long-wavelength, low-frequency dynamics of conserved or spontaneoulsy broken symmetry variables τ

More information

Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser

Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser V.Nassisi #, G.Caretto #, A. Lorusso #, D.Manno %, L.Famà %, G.Buccolieri %, A.Buccolieri %, U.Mastromatteo* # Laboratory of Applied

More information

C o m p u te r M o d e lin g o f M o le c u la r E le c tro n ic S tru c tu re

C o m p u te r M o d e lin g o f M o le c u la r E le c tro n ic S tru c tu re C o m p u te r M o d e lin g o f M o le c u la r E le c tro n ic S tru c tu re P e te r P u la y D e p a rtm e n t o f C h e m is try a n d B io c h e m is try, U n iv e rs ity o f A rk a n s a s, F a

More information

Instability, dispersion management, and pattern formation in the superfluid flow of a BEC in a cylindrical waveguide

Instability, dispersion management, and pattern formation in the superfluid flow of a BEC in a cylindrical waveguide Instability, dispersion management, and pattern formation in the superfluid flow of a BEC in a cylindrical waveguide Michele Modugno LENS & Dipartimento di Fisica, Università di Firenze, Italy Workshop

More information