spettroscopia - university of cagliari · 2013. 9. 18. · 1997 - steven chu, claude...

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Spettroscopia http://www.dsf.unica.it/~michele/spettroscopia

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  • Spettroscopia

    http://www.dsf.unica.it/~michele/spettroscopia

  • Topics - Absorption and Emission of Light

    -  Quantum theory of atom-light interaction

    -  Instrumentation

    -  Lasers

    -  Absorption and Fluorescence Spectroscopy

    -  Nonlinear Spectroscopy

    -  Ultrafast laser spectroscopy

    -  Guest lectures - M.A. Loi (Visiting Professor): Organic materials and solar cells

    -  Lab Experiments: Photodetection noise and lock-in amplifier; Optical pumping; Transform-limited ultrafast optical pulses; Time-resolved photoluminescence; Femtosecond pump-probe; Raman; Confocal microscope; Solar cell efficiency.

  • Nobel Prizes in Physics

    2009 - Charles K. Kao, Willard S. Boyle, George E. Smith 2005 - Roy J. Glauber, John L. Hall, Theodor W. Hänsch 2001 - Eric A. Cornell, Wolfgang Ketterle, Carl E. Wieman 1997 - Steven Chu, Claude Cohen-Tannoudji, William D. Phillips 1989 - Norman F. Ramsey, Hans G. Dehmelt, Wolfgang Paul 1981 - Nicolaas Bloembergen, Arthur L. Schawlow, Kai M. Siegbahn 1966 - Alfred Kastler 1964 - Charles H. Townes, Nicolay G. Basov, Aleksandr M. Prokhorov 1944 - Isidor Isaac Rabi 1930 - Venkata Raman 1921 - Albert Einstein 1907 - Albert A. Michelson

  • Textbook

  • Exam requirements

    Attendance 6 CFU = 48 hrs

    Weekly exercises

    Lab reports

    Final test (written or oral)

  • Absorption and Emission of Light

  • Maxwell

    ∇ ⋅ε = ρε0

    ∇ ⋅ B = 0

    ∇ ×ε = − ∂B∂t

    ∇ × B = µ0 j + ε0∂ε∂t

    ⎝ ⎜

    ⎠ ⎟

    D = ε 0ε + PP = ε 0χεD = ε 0ε rεε r =1+ χ

    ∇⋅ D = ρ∇⋅ B = 0

    ∇ ×ε = − ∂B∂t

    ∇ × H = j + ∂D∂t

    H = 1µ0B −M

    M = χMH

    B = µ0 H + M( ) = µ0 1+ χM( )H= µ0µrH

  • EM waves

    ∇⋅ D = ρ∇⋅ B = 0

    ∇ ×ε = − ∂B∂t

    ∇ × H = j + ∂D∂t

    ρ = 0j = 0χM = 0D = ε 0ε rεB = µ0µrH = µ0H

    ∇ × B = ε0εrµ0∂ε∂t

    ∇ × ∇ ×ε( ) =∇ × −∂B∂t

    ⎝ ⎜

    ⎠ ⎟

    ∇ × ∇ ×ε( ) = − ∂∂t

    ∇ × B( )

    ∂∂t

    ∇ × B( ) = ε0εrµ0∂2ε∂t 2

    ∇ × ∇ ×ε( ) = −ε0εrµ0∂2ε∂t 2

    ∇ × ∇ ×ε( ) =∇ ∇⋅ε( ) −∇2ε

    ∇2ε= ε0εrµ0∂2ε∂t 2

  • EM waves

    ∇2ε= ε0εrµ0∂2ε∂t 2

    c = 1ε0µ0

    v = 1εrc = c

    n

    ∂εx∂z

    = −∂By∂t

    −∂By∂z

    = µ0ε0εr∂εx∂t

    εx z,t( ) =εx0 cos kz −ωt +ϕ( )By z,t( ) = By0 cos kz −ωt +ϕ( )

    c = ωk

    =1ε0µ0

    ⎣ ⎢

    ⎦ ⎥

    By0 =kωεx0 =

    ncεx0

  • Mode density for em waves in a cavity

  • Mode density for em waves in a cavity

  • Blackbody radiation

  • Two level atom and radiation

    At equilibrium

    Thermal equilibrium

  • Einstein’s coefficients

  • Einstein’s coefficients