Plan : intro Characterization of thin films and bulk materials using x-ray and electron scattering...
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![Page 1: Plan : intro Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,](https://reader035.fdocuments.us/reader035/viewer/2022070402/56649f225503460f94c3a1b8/html5/thumbnails/1.jpg)
Plan : intro
Characterization of thin films and bulk materials using x-ray and electron scattering
V. Pierron-BohnesIPCMS-GEMME, BP 43, 23 rue du Loess, 67034 Strasbourg Cedex 2
electronic properties magnetism, optics, transport…
structural properties
preparation conditionssmall dimensions
Research topics:- superalloys NiAl, FeAl, (Co,Fe,Mn)Pt3 (order – kinetics – magnetism)- multilayers Co/Mn, Co/Ru (stucture – magnetism)- anisotropic alloy thin films (MBE, sputtering) CoRu, CoPt, FePt, NiPt
-(structure – magnetism – interdiffusion)
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Plan : interactions
Characterization of thin films and bulk materials using x-ray and electron scattering
V. Pierron-BohnesIPCMS-GEMME, BP 43, 23 rue du Loess, 67034 Strasbourg Cedex 2
1) electron and x-ray interaction with matter2) real lattice and reciprocal lattice in 3D and 2D samples3) experimental set-ups4) studies on single crystals 5) synchrotron radiation 6) strains measurements using x-ray scattering and TEM7) powder scattering measurement8) texture analysis9) reflectometry10) chemical analysis11) short and long range order measurements
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electron-matter interaction 1An electron has:- a mass:9.1 x 10-31 kg - a charge1.6 x 10-19 Cto interact with other electrons and nuclei
in V511 kV
Vacc=100kV =0.0037 nm
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electron-matter interaction 2
Electronic structure of atoms
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electron-matter
interaction 3
energy loss electron
Incident electron
secondary electron (E < 50eV)
Transmitted beam with energy loss
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electron-matter
interaction 4
primary electron
energy loss electron
incident electron
Emission of a primary electronInelastically scattered electron
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electron-matter
interaction 5
Auger electron
energy loss electron
photon
wavelength
inte
nsi
ty
dis-excitation
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electron-matter
interaction 6
secondary electron (E < 50eV)
Emission of a secondary electron
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x-ray interaction with
matter
Incident x-ray beam
E = h0Rayleigh + Thomson
diffusion (coherent + elastic)
E ≈ h0
Compton diffusion (incoherent
+ slightly inelastic)
E ≠ h0
Absorption + reemission: fluorescence… (incoherent
+ strongly inelastic)
E = h0
X-rays: no mass, no charge → interaction as the effect of electro-magnetic field on charges
electrons(photoelectric
effect)
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Thomsonsmall
large h0
x-ray-matter
interaction
Incident x-ray beam
E = h0Rayleigh + Thomson
diffusion (coherent + elastic)
E = h0
Rayleighlarge
small h0
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x-ray-matter
interaction
Incident x-ray beam
E = h0 E ≈ h0
Compton diffusion (incoherent
+ slightly inelastic)
nucleus
hole
Photon: particle with E = h and p = hc/
=
with
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x-ray-matter
interaction
Incident x-ray beam
E = h0Compton diffusion
(incoherent+ slightly inelastic)
E << h0
Absorption + reemission: fluorescence… (incoherent
+ strongly inelastic)
excited electron
incident photon
emittedphoton
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Incident x-ray beam
E = h0
photoelectric effect
e-
nucleus
hole
Energy
probabilty
x-ray-matter
interaction
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x-ray interaction with matter
Incident x-ray beam
E = h0Rayleigh + Thomson
diffusion (coherent + elastic)
E ≈ h0
Compton diffusion (incoherent
+ slightly inelastic)
E ≠ h0
Absorption + reemission: fluorescence… (incoherent
+ strongly inelastic)
E = h0
electrons(photoelectric
effect)
Hard x-rays : within 0.01 – 0.1nm
Soft x-rays: within 0.1 – 0.25 nm
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x-ray diffusion by one electron
electron acceleration
field emitted in direction k
=/2
angle between k and
E
E
2
per solid angle
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x-ray diffusion by one atom
Electronic distribution electronic
states
atomic volume
Contribution of extended states
Contribution of localized states
Interference effects(diffusion factor)
Hartree-Fock calculations:
F
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dependent on the energy only
dependent on the direction only
diffusion factor at absorption edge
absorption edge
energy
anomal diffraction:enhanced contrastat the edge of the
light element
Mn edge
Cromer –Liberman method
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Relations between , f’ and f’’Kramers-Kronig relations
f’ and f” obey the Kramers-
Kronig relations
Absorption: the intensity decreases as exp(-z)
Maxwell equations If is complex, k is complex
because
or : in the international tables of crystallography
x-rays pass through some m atomic volume
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Sasaki tables
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Co edge
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electron diffusion by one atom
The deviation of the electron is due to their electrostatic interactionbecause the mechanical interaction (collision) has a too small probability
The elastic part is due to the deviation by the electric potential due to both nuclei and electrons, but the nuclei is predominant.
≈ Q-2
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compared diffusion amplitudes
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compare scattering amplitudes and
atomic scattering
factors for x-rays, electrons and neutrons
comparison of the thickness to absorb99% of the beamfor different rays
absorption