理学胶体与表面化学课件TEM-surf-Chem

1、理学胶体与表面化学课件TEM-surf-Chem理学胶体与表面化学课件TEM-surf-Chem一、Interactions of Electrons with Matter 1. Elastic Interactions No energy is transferred from the electron to the sample (direct beam or is scattered). TEM, SAED2. Inelastic Interactions Energy is transferred from the incident electrons to the sample:(

2、EDX analysis )9/21/20222h一、Interactions of Electrons wi1. Elastic Interactions An electron penetrating into the electron cloud of an atom is attracted by the positive potential of the nucleus (Coulombic interaction), and its path is deflected towards the core as a result. The Coulombic force F is de

3、fined as: with r being the distance between the charges Q1 and Q2 and 0 the dielectric constant. The closer the electron comes to the nucleus, i.e. the smaller r, the larger is F and consequently the scattering angle. In rare cases, even complete backscattering can occur (back scattered electrons BS

4、E). 9/21/20223h1. Elastic Interactions An ele2. Inelastic InteractionsIonization: The high-energy electrons of the incident beam can transfer a critical amount of energy to an inner-shell electron of an atom, leading to the ejection of this electron. The ionization energy is provided by the incident

5、 electron, reducing its energy. This leads to an ionization edge in the electron energy loss spectrum (EELS). Subsequently, the hole in the inner-shell is filled up by an electron with higher energy from an outer shell. This electron gives away a part of its energy, leading to the emission of charac

6、teristic X-rays or Auger electrons.Secondary electrons: Electrons in the conduction or valence band do not need much energy (low work function) to be transferred into vacuum. Thus, the energy of secondary electrons (SE) is low (50 eV). The SEs are mainly exploited in SEM. Phonons: Phonons are lattic

7、e vibrations, which are equal to heating the specimen. This effect may lead to a damage of the sample. Plasmons: Plasmons are longitudinal oscillations of free electrons, which decay either in photons or phonons. Cathodoluminescence: If semiconductors are hit by high-energy electrons, electron-hole

8、pairs can be formed by promoting an valence electron into the conduction band. Filling this hole with an electron from the conduction band (recombination) leads to the emission of light with a frequency that corresponds to the band gap.9/21/20224h2. Inelastic InteractionsIonizBasic contrast mechanis

9、ms in TEM and STEM. Electrons, which come from the condenser system of the TEM, are scattered by the sample, situated in the object plane of the objective lens. Electrons scattered in the same direction are focused in the back focal plane, and as a result, a diffraction pattern is formed there. Elec

10、trons coming from the same point of the object are focused in the image plane. In the TEM, the first intermediate image is magnified by further lenses (projective system). 9/21/20225hBasic contrast mechanisms in Tbasic contrast mechanisms in TEM and STEM. Bright field (BF) mode:Mass-thickness and di

11、ffraction contrast contribute to image formation: thick areas, areas in which heavy atoms are enriched, and crystalline areas appear with dark contrast. In dark field (DF) images: Since diffracted beams have strongly interacted with the specimen, very useful information is present in DF images, e.g.

12、, about planar defects, stacking faults or particle size. 9/21/20226hbasic contrast mechanisms in TBF and DF TEM images of ZrO2 Electron diffraction pattern: the spots indicate the presence of single microcrystals. The apertures (red circles) are localized around the direct beam for recording the br

13、ight field (BF) image and around a few diffracted beams for the dark field (DF) image. The intense direct beam is blocked by a metal rod (black shadow on the left center) to avoid overexposure. BFDF9/21/20227hBF and DF TEM images of ZrO2 EHRTEM modeIf the point resolution of the microscope is suffic

14、iently high and a suitable sample oriented along a zone axis, then (HRTEM) images are obtained. In many cases, the atomic structure of a specimen can directly be investigated by HRTEM. 9/21/20228hHRTEM modeIf the point resolutHRTEM modesingle crystals of (Ce0.5Zr0.5)O2 Ag particle supported on ZnO R

15、eO3 Structure9/21/20229hHRTEM modesingle crystals of (Scanning Electron Microscopy (SEM)compact samples can thus be investigated by SEM. A valuable information about morphology, surface topology and composition can be obtained. SEM microscopes achieving resolutions below 1 nm are available now. 9/21

16、/202210hScanning Electron Microscopy (SEM: Imaging with Back-scattered ElectronsSEM images of Fe particles in carbon recorded with the secondary electron (left) and the back-scattered (right) electron detector. The BSE image shows the Fe particles with bright contrast. 9/21/202211hSEM: Imaging with

17、Back-scatter 二、Imaging and Diffraction 1. objective lens forms a diffraction pattern in the back focal plane 2. diffraction pattern and image are simultaneously present 3. real space (image) to reciprocal space (diffraction pattern) is easily achieved by changing the strength of the intermediate len

18、s.4. Aperture regulation9/21/202212h 二、Imaging and Diffraction 1. 三、Scheme of a CM30 TEMElectron gun: 2. Condenser system3. Objective lens 4.Diffraction/inter-mediate lens:5. Projective lenses: 6.Image observation:7. Vacuum system: 9/21/202213h三、Scheme of a CM30 TEMElectron四、Bragg Description of Dif

19、fraction If the incident plane wave hits the crystal at an arbitrary angle, the interference of the reflected waves can be either destructive or constructive.Destructive interference of reflected waves (Max. and Min. of the wave amplitude are superimposed). Constructive Interference of reflected wav

20、es (maxima are superimposed).9/21/202214h四、Bragg Description of DiffracTo obtain constructive interference, the path difference between the two incident and the scattered waves, which is 2dsin, has to be a multiple of the wavelength . For this case, the Bragg law then gives the relation between inte

21、rplanar distance d and diffraction angle : 9/21/202215hTo obtain constructive interfeElectron Diffraction (ED) Electron diffraction is a collective elastic scattering phenomenon with electrons being scattering by atoms in a regular array (crystal). The incoming plane electron wave interact with the

22、atoms. Secondary waves are generated which interfere with each other. This occurs either constructively (reinforcement) or destructively (extinguishing). As in X-ray diffraction (XRD), the scattering event can be described as a reflection of the beams at planes of atoms (lattice planes). The Bragg l

23、aw gives the relation between interplanar distance d and diffraction angle :9/21/202216hElectron Diffraction (ED) ElecSince the wavelength of the electrons is known, interplanar distances can be calculated from ED patterns. Furthermore, information about crystal symmetry can be obtained. Consequentl

24、y, electron diffraction represents a valuable tool in crystallography. 9/21/202217hSince the wavelength of the Estimate of scattering anglesel = 0.00197 nm (1.97 pm) for 300 kV electrons. A typical value for the interplanar distance is d = 0.2 nm.If these values are put in the Bragg law, then the sc

25、attering angle is: = 0.28.As a rule, the scattering angles in ED are very small: 0 2.9/21/202218hEstimate of scattering angles1. Reflecting lattice planes are almost parallel to the direct beam. 2. Incident electron beam is the zone axis of the reflecting sets of lattice planes 9/21/202219h1. Reflec

26、ting lattice planes aComparison of Electron (ED) and XRD Both, ED and XRD, are caused by positive interference of scattered waves, and the same fundamental laws (e.g., Bragg law, extinction rules) can be applied for the interpretation of the resulting diffraction patterns. In both cases, diffraction

27、 patterns of powders and of single crystals appear.However, ED shows some unique characteristics:9/21/202220hComparison of Electron (ED) an1. The wavelength of electrons (e.g., 1.97 pm for 300 keV electrons) is much shorter than that of X-rays (about 100 pm). Therefore, the radius of the Ewald spher

28、e is much larger and more reflections arise.2. The diffraction angles are very small: ED 0-2 (cf., XRD 0-180)3. Electrons are scattered by the positive potential inside the electron cloud, while X-rays interact with the electron cloud. As the result, the interaction of electrons with matter is much

29、(106-107) stronger than that of X-rays. 9/21/202221h1. The wavelength of electronsThe advantage and the disadvantage of EDthe diffracted electron beams have a high intensity and exposure times. ED patterns can directly be observed on viewing screen of TEM. diffraction patterns can be obtained from v

30、ery small crystals selected with a diffracted aperture (Selected Area Electron Diffraction SAED)1. multiple scattering plays an important role, This makes structure determination from ED more difficult and less reliable than that from XRD data. 9/21/202222hThe advantage and the disadvanEwald Sphere

31、of Diffraction The diffraction, which mathematically corresponds to a Fourier transform, results in spots (reflections) at well-defined positions. Each set of parallel lattice planes is represented by spots （distance of 1/d：d: interplanar spacing) from the origin and which are perpendicular to the r

32、eflecting set of lattice plane. 9/21/202223hEwald Sphere of Diffraction ThLa2NiO4(4 cm/2 cm)*5 1/nm= (10 1/nm)= (1/ 10 nm) = 0.1 nmCatal. Today, 131 (2008) :5339/21/202224hLa2NiO4(4 cm/2 cm)*5 1/nmCatalCarbon deposition over Mo2C/ZSM-59/21/202225hCarbon deposition over Mo2C/ZSCalculation:(0.81 cm/2

33、cm)*5 1/nm= (2.025 1/nm)= 0.494 nm1/d = 0.493 nm1/d = 0.294 nmSAED of Mo2CUnit Cell: Hexagonala= 0.3002 nmb= 0.4724 nmAIChE J 57 (2011):18529/21/202226hCalculation:1/d = 0.493 nm1/d The diffraction can be described in reciprocal space by the Ewald sphere construction (Figure below). A sphere with ra

34、dius 1/ is drawn through the origin of the reciprocal lattice. Now, for each reciprocal lattice point that is located on the Ewald sphere of reflection, the Bragg condition is satisfied and diffraction arises. 9/21/202227hThe diffraction can be describpoint 0: origin of reciprocal latticek0: wave ve

35、ctor of the incident wavekD: wave vector of a diffracted waveZOLZ: Zero Order Laue ZoneFOLZ(SOLZ): First (Second) Order Laue Zone 9/21/202228hpoint 0: origin of reciprocal Due to the small wavelength of electrons (e.g., = 1.97 pm for 300 keV electrons), the radius of the Ewald sphere is larger and m

36、any reflections appear. Furthermore, the lattice points are elongated in ED to form rods so that the Ewald sphere intersects more points (see figure). Because of that, diffraction occurs even then the Bragg condition is not exactly satisfied. In fact, ED patterns are 2D cuttings of reciprocal lattic

37、e. The rod-shape is due to the fact that TEM specimens are very thin in real space, leading to an elongation in reciprocal space.If the interplanar distance in direction of observation is large (that means a small distance between ZOLZ and FOLZ in reciprocal space), higher order Laue zones (HOLZ) ca

38、n be observed as well.A general introduction into diffraction is given in an interactive tutorial by Proven and Neder. 9/21/202229hDue to the small wavelength ofElectron diffraction patterns of Ta97Te60 along two perpendicular directions. The parameters of the tetragonal unit cell can be determined

39、from these SAED patterns: a = 27.6, c= 20.6 .9/21/202230hElectron diffraction patterns Electron diffraction pattern of YbSi1.41 along 001. The reflection condition: h + k = 2n for hkl (C face centering) is fulfilled.9/21/202231hElectron diffraction pattern oED pattern of polycrystalline platinum. Th

40、e indices are assigned to the diffraction rings in accordance of the face-centered cubic lattice of Pt (reflection condition: h, k, l all even or all odd). 9/21/202232hED pattern of polycrystalline In the pseudo-binary system Nb2O5/WO3, Nb8W9O47, crystallizing in a threefold superstructure of the te

41、tragonal tungsten bronze (TTB) type, represents the most stable compound. The superstructure arises from a systematic occupation of a part of the pentagonal channels with metal-oxygen strings (see figure). HRTEM image of Nb4W13O47 along 001. The insets show the structural model and a simulation (EMS

42、 program). 9/21/202233hIn the pseudo-binary system NbHRTEM image and SAED (inset) of Al-MCM-41 (50).Liu BS et al J Phys Chem. C 2008, 112: 15490SBA-159/21/202234hHRTEM image and SAED (inset) oSBA-159/21/202235hSBA-159/21/202237hSTEM + EDXSPoint Analysis in STEMIn STEM, an electron beam is scanned ov

43、er a defined area of the sample. The beam can be localized on a certain point in the image and used to measure an EDX and/or EEL spectrum at there. Moreover, line scans and mappings can be obtained by this powerful technique. Example: Molybdenum Tungsten Oxide9/21/202236hSTEM + EDXSPoint Analysis in

44、 STo solve the question whether the nanorods consist of a mixed Mo-W oxide or of the separated binary oxides MoO3 and WO3, spot analyses were performed. The EDX spectrum obtained at the position encircled in the HAADF-STEM image shows both metals and thus proves the presence of a mixed oxide X-ray S

45、pectroscopy X-ray spectroscopy is a valuable tool for qualitative and quantitative element analysis. Each element has characteristic peak positions corresponding to the possible transitions in its electron shell. 9/21/202237hTo solve the question whether The presence of copper, for example, is indic

46、ated by two K peaks at about 8.0 and 8.9 keV and a L peak at 0.85 eV. In heavy elements like tungsten, a lot of different transitions are possible and many peaks are therefore present. TEMs are almost exclusively equipped with energy-dispersive spectrometers (energy-dispersive X-ray spectroscopy EDX

47、S).9/21/202238hThe presence of copper, for exGeneration of X-rays 1. Ionization: A hole in an inner shell (here: K shell) is generated by an incident high-energy electron that loses the corresponding energy E transferred to the ejected electron.* 2. X-ray emission: The hole in the K shell is filled

48、by an electron from an outer shell (here: L3). The superfluous energy is emitted as a characteristic X-ray quantum. In a typical X-ray spectrum, there are many peaks caused by such a process. The X-ray energy corresponds to a certain difference in inner-shell energies. Thus, the detection of charact

49、eristic X-ray is specific for a element in the sample, and X-ray spectroscopy can be employed for qualitative analysis.9/21/202239hGeneration of X-rays 1.Generation of X-rays Another inelastic interaction of the incident electron with matter represents its deceleration by the Coulomb field of the nu

50、cleus. This process creates X-ray with any energy smaller than the beam energy. These X-rays are called bremsstrahlung and form the uncharacteristic spectrum background. If the X-ray spectrum was measured on a TEM, the Cliff-Lorimer ratio technique can be applied for the quantification: NA/NB = kAB

51、IA/IBNA, NB: atomic % of element A, B.IA/IB: measured intensity of element A, B.kAB: Cliff-Lorimer factor.Quantitative X-rays Analysis9/21/202240hGeneration of X-rays Another iGeneration of X-rays The Cliff-Lorimer factor is NOT a constant but depends on the TEM voltage, on the detector efficiency and several other parameters. Thus, accurate results can only be obtained if a stand