Optical Properties II: Emission of Light, Displays and Transparent Conductors

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Optical Properties II: Emission of Light, Displays and Transparent Conductors. Chemistry 754 Solid State Chemistry Lecture #22 May 21, 2003. Emission of Light. The optical properties of extended solids are utilized not only for their color, but also for the way in which they emit light. - PowerPoint PPT Presentation

Transcript of Optical Properties II: Emission of Light, Displays and Transparent Conductors

  • Optical Properties II:Emission of Light, Displays and Transparent Conductors Chemistry 754Solid State Chemistry Lecture #22May 21, 2003

  • Emission of LightThe optical properties of extended solids are utilized not only for their color, but also for the way in which they emit light.

    Luminescence Emission of light by a material as a consequence of it absorbing energy. There are two categories:Fluorescence: Emission involves a spin allowed transition (short excited state lifetime)Phosphorescence: Emission involves a spin forbidden transition (long lived excited state).

    Luminescence can also be classified according to the method of excitation:Photoluminescence: Photon excitation (i.e. fluorescent lights)Cathodoluminescence: Cathode rays (TV & Computer displays)Electroluminescence: Electrical injection of carriers (LEDs)

  • Sensitizers and ActivatorsSensitizer Absorbs the incident energy (photon or excited electron). Often times the host lattice acts as the sensitizer.Activator The site where the electron radiatively relaxes. Some common ions which act as activators:

    Host Lattice Typically, the host lattice should have the following properties:Large Band Gap So as not to absorb the emitted radiation.Stiff Easily excited lattice vibrations can lead to non-radiative relaxation, which decreases the efficiency.

  • Common Luminescent Ions*The energy of transitions involving d, p or s orbitals is very sensitive to the crystal field splitting induced by the lattice.

    Ion

    Excited State

    Ground State

    max Emission

    Mn2+ (3d5)

    t24e1 (4T1)

    t23e2 (6A1)

    Green-Orange-Red*

    Sb3+ (5s2)

    5s15p1

    5s2

    Blue*

    Ce3+ (4f1)

    4f05d1

    4f15d0

    Near UV to Red*

    Eu2+ (4f7)

    4f65d1

    4f75d0

    Near UV to Red*

    Tm3+ (4f12)

    1G4

    3H6

    450 nm (Blue)

    Er3+ (4f11)

    4S3/2

    4I15/2

    545 nm (Green)

    Tb3+ (4f8)

    5D4

    7F5

    545 nm (Green)

    Pr3+ (4f2)

    3P0

    3H5 (3F2)

    605 (635) nm (Red)

    Eu3+ (4f6)

    5D0

    7F2

    611 nm (Red)

  • Conventional Fluorescent LightsExcitation SourceHg gas discharge UV Light (photoluminescence)Sensitizer/Host LatticeFluoroapatite Ca5(PO4)3FActivatorsBlue = Sb3+ (5s15p1 5s2) lmax = 480 nmOrange-Red = Mn2+ (t2g4eg1 t2g3eg2) lmax = 580 nm

  • Tricolor Fluorescent LightsTricolor fluorescent lights are more commonly used today because they give off warmer light, due to more efficient luminescence in the red region of the spectrum. Such lights contain a blend of at least three phosphors.

    Red PhosphorHost Lattice = (Y2-xEux)O3 x = 0.06-0.10 (Bixbyite structure)Sensitizer = O2- 2p Eu3+ 5d charge transfer (lmax ~ 230 nm)Activator = 5D0 7F2 transition on Eu3+ [f6 ion] (lmax ~ 611 nm)Green PhosphorHost Lattice = (La0.6Ce0.27Tb0.13)PO4 (Monazite structure)Sensitizer = 4f1 5d1 excitation on Ce3+ [f1 ion] (lmax ~ 250 nm)Activator = 5D4 7F5 transition on Tb3+ [f8 ion] (lmax ~ 543 nm)Blue PhosphorHost Lattice = (Sr,Ba,Ca)5(PO4)3Cl (Halophosphate structure)Sensitizer = 4f75d0 4f65d1 transition on Eu2+Activator = 4f65d1 4f75d0 transition on Eu2+ (lmax ~ 450 nm)

    For a detailed yet very readable description of fluorescent light phosphors see:http://www.electrochem.org/publications/interface/summer98/IF6-98-Page28-31.pdf

  • Cathode Ray TubeThe cathode ray tube is the technology used in most computer monitors and TVs. The details of a typical commercial CRTs are as follows.

    Excitation SourceElectron beam (cathodoluminescence)RedSensitizer/Host - YVO4Activator Eu3+GreenSensitizer/Host ZnS (CB)Activator Ag+BlueSensitizer/Host ZnS (CB)Activator Cu+

    Image taken from http://www.howstuffworks.com/tv2.htm

  • Luminscence in ZnSWhile the insulating red phosphor (Y1-xEux)VO4 operates on a principle very similar to fluorescent light phosphors (with a different excitation source of course), the blue and green phosphors employ a different scheme for electronic excitation and luminescence.

    The electronic excitation in ZnS (Eg = 3.6 eV) is from the valence band to the conduction band. While the relaxation that leads to the luminescence is from the conduction band to an impurity level in the band gap. Typically either Ag+ or Cu+, which are substitutional impurities. The energy of the emitted light can be tuned by changing impurities or changing the band gap of the semiconductor.Cu+Ag+e-e-Valence BandConduction Bandhnhn

  • ElectroluminescenceFlat Panel DisplaysTaken from the Planar systems website.http://www.planar.com/technology/el.aspIn electroluminescence an electron is directly injected into the phosphor (in the excited state) and it relaxes giving off a photon.

    This diagram shows how by running current through a single row (absorbant back electrode) and a single column (transparent front electrode) it is possible to light up a single pixel.

  • Self Luminescence in AWO4The AWO4 (A= Ca, Sr, Ba) tungstates, based upon the scheelite structure with isolated tetrahedra, are self luminescent. Luminescence in these materials can be described by the following process. 1. WO42- group absorbs a UV photon via a charge transfer from oxygen to tungsten.

    2. Excited state electron is in an antibonding state, weakens/lengthens the bond lowering the energy of the excited state.

    3. Electron returns to the ground state giving off a longer wavelength photon.

  • Solid State LasersA Laser gives off light at a single wavelength. To achieve this the activator needs to have the following propertiesA long lived excited stateA very narrow emission spectrum (localized luminescence centers)Ruby laserHost = Al2O3Activator = Cr3+Lifetime = 5 ms l = 693.4 nmNd:YAG laserHost = Y3Al5O12 (Garnet)Activator = Nd3+ (4f3)Lifetime = 10-4 s l = 1064 nm

  • Transparent Conducting OxidesCharacteristics of a transparent conducting oxide (TCO)High transparency in the visible (Eg > 3.0 eV)High electrical conductivity (s > 103 S/cm)Applications of transparent conductorsOptoelectronic devices (LEDs, Semiconductor lasers, photovoltaic cells, etc.)Flat Panel Displays (liquid crystals, electroluminescent displays)Heat efficient windows (reflect IR, transparent to visible light)Smart windows and displays based on electrochromicsDefrosting windows and antistatic coatingsTCO MaterialsIn2O3:Sn (ITO)SnO2:Sb & SnO2-xFxZnO:F & ZnO:M (M=Al, In, B, Ga)Cd2SnO4CuAlO2 & CuGaO2

  • TCO Structure Types IIn2O3Bixbyite (Ia3)6-coordinate In3+4-coordinate O2-Edge & Corner SharingZnSnO3Ilmenite (R-3)6-coordinate Sn4+6-coordinate Zn2+4-coordinate O2-Edge & Face SharingCd(CdSn)O4Inverse Spinel (Fd3m)6-coordinate Sn4+/Cd2+4-coordinate O2-Edge & Corner Sharing

  • TCO Structure Types IISnO2Rutile (P42/mnm)6-coordinate Sn4+3-coordinate O2-Edge & Corner SharingZnOWurtzite (P63mc)4-coordinate Zn2+4-coordinate O2-Corner Sharing

  • Desirable Properties-TCOsThe following guidelines were put forward* as guidelines for the most desirable features of the electronic band structure for a TCO material. (*See Freeman, et al. in MRS Bulletin, August 2000, pp. 45-51)A highly disperse single s-band at the bottom of the conduction band.in order to give the carriers (electrons) high mobilityTo achieve this condition we need main group s0 ions (Sn2+, In3+, Cd2+, Zn2+)Separation of this band from the valence band by at least 3 eV in order to be transparent across the visible spectrumWe need the appropriate level of covalency so that the conduction band falls 3-4 eV above the O 2p band (Bi5+ & Pb4+ are too electronegative, In3+, Zn2+, Cd2+, Sn4+ are of roughly the proper energy)A splitting of this band from the rest of the conduction band in order to keep the plasma frequency in the IR rangeDirect M ns - M ns interactions across the shared octahedral edge are useful to stabilize the s-band wrt the rest of the CB.

  • Electronic Structure In2O3Taken from Freeman, et al. in MRS Bulletin, August 2000, pp. 45-51