Slide 1OutLinephotoemissiona Historical IntroductionARPESSlide 6Slide 7Slide 8Slide 9Slide 10Slide 11three-step modelSlide 13Slide 14Golden RuleSlide 16Slide 17Slide 18ApplicationSlide 20SummaryReferencesINTRODUCTION TO PHOTOEMISSIONAPPLICATION TO LAYERED OXIDESAmal Al-WahishCourse: Solid state 672Prof. DagottoDepartment of Physics, UTKOUTLINEWhat is the photoemission? Why we need it?Present a Historical IntroductionARPES and Mathematical FormulasThree-Step ModelApplications How far this good compare to theorySummaryReferencesPHOTOEMISSIONIt utilizes the photoelectric effect , Photoelectric effect takes place with photons with energies of about a few eVstudy of the electronic structure of solids.powerful widely-used way to study the properties of atoms, molecules, solids and surfaces Angular resolved photoemission spectroscopy (ARPES), provides rich information about the electron structure of crystals and of their surfacesA HISTORICAL INTRODUCTION In1887 Hertz observed that a spark between two electrodes occurs more easily if the negative electrode is illuminated by UV radiation.A few years later J.J. Thompson demonstratedthat the effect was due to emission of electrons by the electrode while under illumination.Einstein postulated that light was composed of discrete quanta of energy E hv=ARPESA powerful imaging techniquemeasuring the energy and momenta of electrons ejected from a sample struck by energetic photons makes it possible to calculate the electrons' initial energy and momenta, and from this determine the sample's electronic structure.Photoemission Spectroscopy's system.The ARPES sensor now sits inside the vacuum chamber. This picture was taken before it was completely builtSensor, in blue displays the intensity of detected electrons, N(E), that have various kinetic energies, EKin. These values obtained by the ARPES sensor correspond to the actual values of the "Sample", displayed red. In a solid material, the electrons are distributed to an energy level below EFermi, the Fermi Level.An ARPES sensor collects the photoelectrons, provide information about the photoelectron energy, applying conservation laws of energy and momentum, where the energy and the momentum is conserved before and after the photoelectric effect.The crystal- momentum inside the solidK i n BE h v Ef= - -| | | |2K i np k m E S i n q= =hMost ARPES experiments are performed at photon energies in theultraviolet (100 eV).Why?Conservation of momentum, we can neglect the photon momentum compare to the e-momentum.Achieve higher energy and momentum resolution.How?Mapping out the electronics dispersion relations by tracking the energy position of the peaks of ARPES spectral at various angles to achieve higher energy and momentum resolution .||( )E kLOW PHOTON ENERGIES2||2 / . .Kink mE CosJ JD D; hcorresponds to the finite acceptance angle ofthe electron analyzer.JDfor 100-eV photons the momentum is 3%of the typical Brillouin-zone size of the cuprates0.05 A-1 2π/a ≈ 1.6 A-1 for 21.2-eV photons the momentum is 0.5%of the typical Brillouin-zone size of the cuprates0.008 A-1 2π/a ≈ 1.6 A-1THREE-STEP MODELEscape Transport of the excited photoelectron to the surfaceTransport of the excited photoelectron to the surfaceAbsorption of the x-ray inside the solidSKETCH FOR THREE MODEL BY STEFAN HÜFNERThe three step model developed on ARPES from solid by Berglund and Spicer.THE TOTAL PHOTOEMISSION INTENSITY IS THEN GIVEN BY THE PRODUCT OF THREE INDEPENDENT TERMS:WGOLDEN RULEThe Hamiltonian of one electron in a system described by a potential V(r), to which anExternal electromagnetic field is applied:Hp22mVre2mAr. pp . Ar e22mAr 2. Ar0Ar. pp . Ar i. Ar0Dipole approximation.The interaction with the photon is treated as a perturbation given byHi n t emAr. pApproximations:1- One-electron picture 2- First-order perturbation theory to calculate the interaction between the incident radiation and the system.3- The flux of incident photons is relatively low.4- Neglecting terms of order |A|2 in the calculation of the photocurrent.The one-electron dipole matrix element, int| |k k kf i f iM Hf=The wave functions for the photoelectrons with the momentum k after and before the optical transition.The total photoemission intensity I(k, EKin ) is proportional to2 2 1, ,,| | | | ( )k N Nf i m i Kin m if i mM C E E E hvd-+ - -� �2 2 1, ,,| | | | ( )k N Nf i m i Kin m if i mM C E E E hvd-+ - -� �2,| |m iC =2 1 1 2,| | | | |N Nm i m iC- -= Y Yprobability that the removal of an electron from state i will leave the (N-1)-particle system in the excited state m.APPLICATIONARPES on studying the high temperature superconductors such as copper oxide and Ione-based superconductor,record the photoemission intensity versus the photoelectron kinetic energy. ex. Bi2Sr2CaCu2O8+xShen’s group studied the electronic structure of LaOFeP by using ARPES. The purpose of this study was to understand the nature of the ground state of the parent compounds LaOFeP, and to reveal the important differences between Iron Oxypnictide and Copper based superconductors.SUMMARYBasic definition of Photoemissionphotoemission offer a powerful widely-used way to study the properties of atoms, molecules, solids and surfacesAngle-resolved photoemission spectroscopy (ARPES) is one of the most powerful methods for studying high-Temperature superconductor.Brief summary about Three- step modelModern application of PS, on HTSC.REFERENCES{1] C. Fadley, Basic Concept of X-ray Photoelectron Spectroscopy (Dapartment of Chemistry, University of Hawaii, Honolulu, Hawaii, 1978).[2] S. Hufner, Very High Resolution Photoelectron Spectroscopy, Lecture Notes in Physics 715 (Springer, Berlin, Heidelberg, 2007), 1st ed.[3] P. Y. Y. M. Cardona, Fundamentals of Semiconductors physics and Materials properties (Springer, Berline, Germany, 2005), 3rd ed.[4] Z.-X. S. Andrea Damascelli, Zahid Hussain, Reviews of Modern Physics 75, 473 (2003).[5] A. K. Frank de Groot, Core level Spectroscopy of Solids (CRC Press, Taylor and Francies Group, USA, 1964), 1st ed.[6] M. A. H. Wolfgang Schattke, Solid-State Photoemission and related Methods, theory and experiment (WiLey-Vch GmbH and Co.KGaA, Weinheim, Germany, 2003), 1st