X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital...

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X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from the atom, the energy released from an electron ادر ق ل د ا ب ع ر م ع د.

Transcript of X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital...

Page 1: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray Microanalysis

An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from the atom, the energy released from an electron replacement event produces a photon with an energy exactly equal to the drop in energy.

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Page 2: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray Microanalysis

X-rays can have an energy nearly equal to that of the primary beam electron and thus can escape from very deep within the specimen

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Page 3: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray MicroanalysisEnergy Dispersive Spectroscopy (EDS)

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Page 4: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

When an electron from a K-shell is replaced by one from the next closest shell (L), it is designated as a Kα event

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Page 5: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

When an electron from a K-shell is replaced by one from the second closest shell (M), it is designated as a Kβ event

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Page 6: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

When an electron from a L-shell is replaced by one from the next closest shell (M), it is designated as a Lα event. The K shell will never donate its electron as this would require an increase in energy, not a drop.

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Page 7: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray Microanalysis

Certain events such as Mα, Lβ, and Kγ are only possible in atoms of sufficient atomic weight

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Page 8: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray Microanalysis

There are actually a wide variety of subsets of these X-rays since each electron shell has multiple orbitals

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Page 9: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

An X-ray spectrum for a sample is composed of all the possible signals for that given set of elements. These will differ in terms of energies (KeV) and probabilities (likelihood) scored as number of such signals collected over a given period of time.

# Counts

X-ray Energy in KeV

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Page 10: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Each element has a family of characteristic X-

rays associated with it .القادر عبد عمر د

Page 11: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Positive identification of an element is best done by collection of the entire family of peaks for a given element.

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Page 12: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

"Bremsstrahlung" means "braking radiation" and comes from the original German to describe the radiation which is emitted when electrons are decelerated or "braked" when they interact with the specimen. Although they contribute to the total X-ray signal they contain no useful information because their energies are nonspecific and therefore are considered as part of the background .

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Page 13: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Bremsstrahlung X-rays are the major part of the continuum X-ray signal that can escape from the deepest portion of the interaction region.

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Page 14: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Chrysotile Asbestos FibersChrysotile Asbestos Fibers

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Page 15: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Chrysotile Asbestos FibersChrysotile Asbestos Fibers

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Page 16: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Bullet fragments (blue) can be identified on cloth fibers and distinguished from other metal pieces by their elemental composition

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Page 17: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Gunshot Residue (GSR) AnalysisGunshot Residue (GSR) Analysis

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Page 18: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Gunshot Residue (GSR) AnalysisGunshot Residue (GSR) Analysis

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Page 19: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Gunshot Residue (GSR) AnalysisGunshot Residue (GSR) Analysis

Particles are very characteristic, therefore presence of these particles forms evidence of firing a gun.

Particles normally consist of Pb (lead), Sb (antimony) and Ba (barium).

New ammunition: environmentally friendly (no Sb).

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Page 20: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

The proportion of elements present in GSR differ slightly and databases of GSR from different manufacturers can be used to identify what ammunition was used in a crime.GSR is often found on criminals and also on victims if shot at close range.

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Page 21: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray Mapping

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Page 22: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray analysis of paint fragmentsX-ray analysis of paint fragments

Combined with backscatter imaging and X-ray maps of (a) Au, (b) Ba and (c) Ca different layers of paint can be identified

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Page 23: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

EDS = Energy Dispersive Spectroscopy

WDS = Wavelength Dispersive Spectroscopy

X-ray Detection

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Page 24: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

EDS WDS

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Page 25: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Energy Dispersive Spectroscopy (EDS)

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Page 26: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Lithium doped Silicon (SiLi) crystal detectoracts as a semiconductor that carries current in a rate proportional to the number of ionization events and acts as an indirect measurement of the energy contained in the X-ray. .القادر عبد عمر د

Page 27: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Absorbed X-rays create an ionization event similar to that of a scintillator

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Page 28: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Each ionized atom of silicon absorbs 3.8 eV of energy, so an X-ray of 3.8 KeV will ionize approximately 1000 silicon atoms.

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Page 29: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Expanded view of an EDS detector

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Page 30: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Energy Dispersive SpectroscopyCollimator to limit BSE and stray X-rays Window usually made of beryllium (limited to sodium, atomic number 11) or thin plastic to detect down to boron (Atomic number 5) protects cooled crystal from air.

Detector crystal silicon wafer with lithium added in. For each 3.8 eV from an X-ray, produce an electron and hole. This produces a pulse of current, the voltage of which is proportional to the X-ray energy. Must keep the crystal at LN temperature to keep noise to a minimum.

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Page 31: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Multichannel Analyzer (MCA)

The changes in conductivity of the SiLi crystal can be counted for a given time and displayed as a histogram using a multichannel analyzer.

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Page 32: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Multichannel Analyzer (MCA)

MCA consists of an analog to digital converter which “scores” the analog signal coming from the field effect transistor (FET). Newer systems employ a digital pulse processor which converts the signal on the fly

Then Now

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Page 33: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Factors affecting signal collection

Distance between detector and X-ray source, angle at which detector is struck, and volume of signal collected.

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Page 34: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

For a given angle of electron incidence, the length of the absorption path is directly proportional to the cosecant of the take-off angle, φ

Take-off Angle

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Page 35: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Solid Angle

The solid angle Ω of a detector is defined as angle of the cone of signal entering the detector. The greater the size of the detector surface area the greater will be the solid angle.

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Page 36: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Larger SiLi crystals will be able to sample a larger volume of signal (better Ω) but because of imperfections in the crystal they have slightly greater noise and thus slightly lower resolution. القادر. عبد عمر د

Page 37: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

One can also increase the solid angle by placing the detector closer to the source. One then tries to maximize both the solid angle and the take-off angle. القادر. عبد عمر د

Page 38: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

One reason that the final lens of an SEM is conical in shape is so that the EDS detector can be positioned at a high take-off angle and inserted close to the specimen for a high solid angle. .القادر عبد عمر د

Page 39: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

William Henry Bragg 1862 – 1942Nobel Prize in Physics 1915

X-ray diffraction in a crystal.Like an electron beam an X-ray has its own wavelength which is proportional to its energy

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Page 40: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Crystal: A solid formed by the solidification of a chemical and having a highly regular atomic structure. May be composed of a single element (C = diamond) or multiple elements.

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Page 41: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Cubic Hexagonal

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Page 42: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

If a wavelength enters a crystal at the appropriate angle it will be diffracted rather than being absorbed or scattered by the crystal

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Page 43: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

For a given wavelength λ there is a specific angle θ (Bragg’s angle) at which diffraction will occur. Bragg’s angle is determined by the d-spacing (interplanar spacing) of the crystal and the order of diffraction (n = 1, 2, 3….). .القادر عبد عمر د

Page 44: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

A WDS detector takes advantage of the fact that an X-ray of a given wavelength can be focused by a crystal if it encounters the crystal at the proper Bragg’s angle.

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Page 45: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

To better accomplish this crystals are bent and ground to form a curved surface which will bring all the diffracted X-ray wavelengths to a single focal point, thus the crystal acts as a focusing lens. .القادر عبد عمر د

Page 46: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

To change the Bragg’s angle the diffracting crystal and detector can be moved together relative to the stationary specimen along a circle known as the Roland Circle.

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Page 47: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

WDS detectors are quite large and must be positioned around the specimen chamber at an angle to take advantage of maximum take-off angle and maximum solid angle

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Page 48: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

A Microprobe is a specialized SEM that is outfitted with an EDS detector and array of several WDS detectors. القادر. عبد عمر د

Page 49: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Different diffracting crystals can only diffract certain wavelengths (even with the changes in Bragg’s angle) so an array of detectors must be used if one is to be able to detect K, L, and M events for many different elements. Since WDS detectors do not need to be cooled they are windowless and can detect down to Berylium

LiF = Lithium fluoride; PET =Pentaerythritol; and TAP = Thallium acid phthalate.

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Page 50: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Specimen preparation for WDS

Samples must be conductive since high KeV is used (Carbon coating if not naturally conductive)

Samples must be flat (polished) as geometry of sample to detector is crucial and also minimizes artifacts when doing quantitative measurements.

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Page 51: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

WDS vs. EDS

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Page 52: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

A comparison of two spectra collected with EDS and WDS shows how peak overlap and energy spread can serve to obscure the information in an EDS spectrum

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Page 53: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Quantitative X-ray Analysis

If one wants to quantify the relative amounts of different elements present in a complex sample one has to account for a number of factors and carry out a correction of the data

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Page 54: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

One must account for other elements present in the sample and whether their individual peaks overlap with each other creating a “shoulder” that can mask the presence of one element or distort the midpoint of another.

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Page 55: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Several methods to correct the spectra. ZAF takes into account the Atomic Weight (Z), effects of Absorbance (A) and effects of Fluorescence (F) in adjusting the data to give the correct values.

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Page 56: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

Applications of X-ray Microanalysis

Secondary Electron

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Page 57: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

EDS can be added as a component of a TEMRequires an angled detector (for take-off angle) and scan coils in the column to function as a Scanning Transmission Electron Microscope or STEM. القادر. عبد عمر د

Page 58: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

EDS can be used to identify elements present vacuoles or inclusions. Must take into account elements present in the embedding medium

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Page 59: X-ray Microanalysis An inelastic collision between a primary beam electron and an inner orbital electron results in the emission of that electron from.

X-ray microanalysis enables the SEM and TEM to be used as analytical instruments. Limitations include the quantities of given element and an inability to distinguish isotopes. By placing a focussed beam over an object allows one to carry out microchemical analysis on very small or very discrete objects or to map the presence of various elements within a specimen.

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