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Advanced Vitreous State The Physical Properties of Glass Passive Optical Properties of Glass Lecture 3: Pierre Lucas Department of Materials Science & Engineering University of Arizona Tucson AZ Pierre@u.arizona.edu 1 Impurities in


  1. Advanced Vitreous State – The Physical Properties of Glass Passive Optical Properties of Glass Lecture 3: Pierre Lucas Department of Materials Science & Engineering University of Arizona Tucson AZ Pierre@u.arizona.edu 1

  2. Impurities in Optical Glass: In a pure glass, the optical window is controlled by intrinsic limitations of the material : the electronic and vibrational transitions of the glass. Specific glass compositions are then selected for applications requiring transparency in various ranges of wavelength. However, if foreign atoms are introduced in the glass (accidentally or purposedly) they can modify the optical window by generating additional: • Electronic transitions • Vibrational transitions Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass 2

  3. Optical window • When plotted in Absorption instead of Transmission, the optical window corresponds to the region of zero absorption. • Absorption is high at short wavelength due to eletronic excitation and high at long wavelength due to vibrational excitations. • In silicate glasses, the visible wavelengths range is within the window. 100 Absorption 50 optical window visible Wavelength λ Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  4. Absorption due to electronic transition from impurities • A glass beer bottle is made of silicate glass which is transparent in the visible, yet it appears colored due to Fe impurities in the glass. Green 100 transmission Absorption Fe 2+ Fe 2+ 50 violet yellow-red absorption absorption Wavelength λ • Because of electronic transitions involving the d orbitals, transition metals absorb visible light within the transparency window and produce colors. They are used as colorant in glasses . Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  5. Crystal Field Theory: colors in glass and gems • Transition metals and have five d orbitals. • The 5 d orbitals have different shape but are equivalent in energy and are degenerated in a free (lone) ion. Five d orbitals in lone Cr 3+ ion Cr 3+ Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  6. Crystal Field Theory: colors in glass and gems • In solids, transition metals occupy interstitial sites such as tetrahedra or octahedra. • For example, Cr 3+ often sits into an octahedra of oxygen. • Only two d orbitals are pointing to the oxygens and are destabilized. This generates splitting of the d orbitals energy. The energy split Δ =10Dq results from the crystal field and O strongly depends on O Δ O the material’s Cr 3+ composition and O O structure. O Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  7. Crystal Field Theory: colors in glass and gems The Physics and Chemistry of Colors , K. Nassau, Wiley, Second Edition (2001) • Many splitting patterns are possible depending on the site geometry and level of distortion (significant in glass). • This results in several possible electronic transitions and absorptions peaks. Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  8. Crystal Field Theory: Chromium Cr 3+ in Ruby and Emeralds Emerald Ruby • The energy of electronic levels is also highly dependent on the O O strength of the crystal field. O Cr 3+ • While Cr 3+ is in octahedral sites in both gems, the crystal field is O O slightly lower in emerald (2.05eV) than in ruby (2.23eV). O • This results in distinctly different absorptions and bright colors. The Physics and Chemistry of Colors , K. Nassau, Wiley, Second Edition (2001) Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  9. Crystal Field Theory: Ruby and Emeralds Al 2 O 3 with 1% of Cr impurity substituting Al in octahedral sites. Beryl (Be 3 Al 2 Si 6 O 18 ) with 1% of Cr impurity substituting Al in octahedral sites. Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  10. Colors in glass Optical Materials , J. H. Simmons, K. S. Potter, Accademic Press (2000) Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  11. Glasses Transparent in the Infrared Chaclogenide Glass 70 60 Transmission (%) 50 Thermal imaging 40 requires high 30 transparency in 20 Thermal imaging the infrared 10 region around 0 10 microns 0 2 4 6 8 10 12 14 16 18 20 Longueur d'onde (µm) wavelength Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass 11

  12. Absorption due to vibrational transition from impurities: Te 2 As 3 Se 5 fiber Te 2 As 3 Se 5 10 100 9 90 Δ L = 1.08 m 8 Se-H 80 attenuation (dB/m) 7 Transmission (%) 70 Φ = 460 μ m 6 60 H 2 O 50 5 Se-O vibrations 40 4 30 3 20 2 10 1 0 0 0 5 10 15 20 2 3 4 5 6 7 8 9 10 11 12 Longueur d'onde (µm) Wavelength (µm) ( μ m) longueurs d'onde (µm) wavelength non-purified glass purified glass ⎛ ⎞ 1 1 1 ⎜ ⎟ ω = + k ⎜ ⎟ π 2 ⎝ ⎠ m m 1 2 • Low mass impurities such as O or H generate phonon absorption peaks at lower wavelength within the transmission window of chalcogenide glasses. Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass 12

  13. Optical losses • The fraction of absorbed light is a function of the path − α = e l length ℓ I through the sample and the absorption coefficient of the material. α I o • The higher the concentration of [Fe 2+ ] colorant, the higher the absorption coefficient α and the lower the transmitted intensity. A glass window contain minute amount of Fe 2+ and appears clear while a beer bottle contains a significant amount of Fe 2+ and appear distinctly green. α =c[Fe 2+ ], Beer’s law is often used to measure concentrations when ℓ is fixed. ℓ • The longer the path length through the sample , the lower the transmitted intensity. • The edge of a transparent glass tube appears greenish because of the longer path length ℓ < ℓ 2 1 I o I 1 I o I 2 ℓ 2 ℓ 1 Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  14. Optical losses in fibers − α = e l In fibers, the path length ℓ • is extremely long. In return the I absorption coefficient α of the material must be extremely low. I o • α is measured using the cut-back method: ℓ > ℓ 1 2 1 I I ℓ I I ℓ I α = ln 2 o 1 1 o 2 2 l − l I 2 1 1 • In the optical fiber industry the decrease of transmitted intensity is expressed in terms of losses rather than absorption coefficient. It is reported in decibel (dB) per unit length: dB/km or dB/m. The decibel is defined as: dB = 10log 10 (I 1 /I 0 ) where I 1 is the output power and I 0 is the input power. − 10 log ( / ) I I = ( / ) 10 = − o ( ) 10 log ( / ) loss dB m loss dB I I 10 ( ) l o m A loss of 1 dB corresponds to about 80% transmission. Losses of silica telecom fibers are below 1dB/km. Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass

  15. Attenuation in silica fibers • Because the light is transmitted through a very long path length in the fiber, all the light loss mechanisms become important. Attenuation due to • scattering, • transition metals absorption • water vibrations • SiO 2 network vibrations leaves only two small transmission windows for efficient long distance transmission of light: 1.3 μ m 1.3 μ m and 1.55 μ m 1.55 μ m Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass 15

  16. Low-OH fibers • Nowadays, state of the art fibers contain very low OH-impurities and the optical window is extended from 1.1 to 1.7 microns. This wide window is advantageous for wavelength-division multiplexing ( WDM ). Er 3+ In WDM, laser pulses of different wavelength carry different signals. More than 100 channels can transmitted at once with wavelength only 0.2 nm apart (25Ghz). Erbium doped fiber amplifiers (EDFAs), are effective for wavelengths between approximately 1525 nm - 1565 nm (C band), or 1570 nm - 1610 nm (L band). Much research is currently underway to develop amplifiers for the remaining window. Pierre@u.arizona.edu Advanced Vitreous State - The Properties of Glass: Passive Optical Properties of Glass 16

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