Introduction API

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& X-ray absorption, emission, Moseley http://hyperphysics.phy-astr.gsu.edu Haken H and Wolf H C: Atomic and quantum physics (Springer)*** Eisberg R and Resnick R; Quantum physics of atoms, molecules, solids, nuclei and particles (2nd ed) Wiley** Softley T P; Atomic spectra (Oxford)** White H E; Introduction to Atomic Spectra (McGraw-Hill)** Woodgate G K; Elementary atomic structure (Oxford)** Herzberg G; Atomic spectra and atomic structure (Dover Reprint)*

description

Energy level (Grotrian) diagrams

Transcript of Introduction API

  • & X-ray absorption, emission, Moseleyhttp://hyperphysics.phy-astr.gsu.edu

    Haken H and Wolf H C: Atomic and quantum physics

    (Springer)***

    Eisberg R and Resnick R; Quantum physics of atoms,

    molecules, solids, nuclei and particles (2nd ed) Wiley**

    Softley T P; Atomic spectra (Oxford)**

    White H E; Introduction to Atomic Spectra (McGraw-Hill)**

    Woodgate G K; Elementary atomic structure (Oxford)**

    Herzberg G; Atomic spectra and atomic structure (Dover

    Reprint)*

  • Energy level (Grotrian) diagramsAs predicted by Bohr As predicted by QM

  • 1s

    2s

    3s

    3p

    2p

    3d

    1s

    2s

    3s

    3p

    2p

    3d

    From WhiteFrom Bransden and Joachain

    SE prediction of radialSE prediction of radial functions (left) and radial distribution functions (right)

    Comparison of the old (orbital) quantum theory and the SE

  • Stern-Gerlach experiment

  • Total a.m (j) and the vector diagram The H Balmer alpha (H, n=3 2) transition

    Dirac theory suggestions energy of transitions marked * (d & e) and + (f & g) should have the same energy. Measurement (and QED) show they do not. This is referred to as the Lamb shift. Thus, there are 7 components to the H (Balmer alpha) line.

    For a D-term (L=2) there are 10 states= (2j+1) = 2(2L+1)

    H 3d 2D5/2

    H 3d 2D3/2

    mj = +5/2 shown

    mj = -1/2 shown

    l = 2

    J = l + s

    j = 2 + = 5/2

    (2j + 1) = 6

    states

    mj = 5/2

    3/2

    1/2

    l = 2

    J = l + s

    j = 2 = 3/2

    (2j + 1) = 4

    states

    mj = 3/2

    1/2

    2s 2S1/2 2p 2P1/2

    2p 2P3/2

  • BohrEnergy level diagram for Sodium

    SodiumD-line589 nm

    n=5

    n=4

    n=3

    n=1

    n=2

    Comparison of the quantum-mechanical with the semi-classical of the neutral sodium atom. Three of the lowest possible states (3s, 3p, 3d) for the single valence electron are shown. Note the size of the core of closed (n=1 and 2) shells.

    The neutral Sodium atom (Z = 11)Ground state 1s22s22p63s 2S1/2

  • Energy level diagram for Sodium showing fine structure and the emission lines

    Quantum defect () for the Alkali metals

    eV 2

    22*l,n

    )(n

    16.13

    )(n

    1hcR

    n

    1hcRE

    Effective principal quantum number n*

    for the Alkali metals ground states

    Sodium D-lines2P1/2

    2S1/22P3/2

    2S1/2

    n=2

    3

    4

    5

    6

  • X-ray production and emission

    Bombard an anode with an energetic electron beam to produce x-rays. The emission spectrum is beam energy dependent

    A spectrum consists of a smooth bremsstrahlung component and characteristic lines.

    K-level refers to n = 1L-level n = 2M-level n = 3 etc

    K refers to n = 2-1K n = 2-1etc

    L refers to n = 3-2L n=4-2etc

    refers to a n =1 transitionn =2 transition

    etc

  • Characteristic x-rays

    ON

    M

    L

    K

    P

    K K K

    L L L

    M M M

    n=1

    2

    3

    4

    65

    The spin-orbit interaction results in significant level splitting (or fine structure) in high atomic number atoms

    Platinum (Z=78), notice the K- etc are split the vertical energy scale is in keV

    Selection rules = 1j = 0, 1

  • Moseleys Law Moseley diagram plots ZhcR

    E ,n vs.

    2

    2n

    nn

    sZhcRE

  • Apparatus for studying x-ray absorption

    Mas

    s ab

    sorp

    tio

    n c

    oef

    . m