Hitachi SU8230 Cold Field Emission SEM Yale West Campus Materials Characterization Core (MCC) ywcmatsci.yale.edu
Core Policies • DO NOT let other people use the facility under your account. • DO NOT try to fix parts or software issues by yourself! • DO NOT surf web using instrument computer! • Follow checklist and SOP! DO NOT explore program! • Facility usage time at least twice a month, OR receive training again (two practice sessions within one week). • No trainings on monthly users Materials Characterization Core (MCC) Yale West Campus 2/20 ywcmatsci.yale.edu
SEM: Basic Theory Electron source Condensor lens 1 Objective aperture Condensor lens 2 Deflection coils Objective lens Sample Materials Characterization Core (MCC) Yale West Campus 3/20 ywcmatsci.yale.edu
SEM: Electron Sources Tungsten wire Cold Field Emission (CFE) LaB 6 single crystal Field Assisted Thermionic Source - Schottky Extraction Voltage Acc Voltage Brightness: 10 5 A/cm 2 sr Brightness: 1000 x Brightness: 10 x Brightness: 500 x Beam size = 30 - 50 Å Beam size = 50 - 100 kÅ Beam size = 50- 100 kÅ Beam size = 100 - 250 Å Operation temperature: 300 K Operation temperature: 3000 K Operation temperature: 2500 K Operation temperature: 2500 K Vacuum: 10 -11 Torr Vacuum: 10 -5 Torr Vacuum: 10 -7 Torr Vacuum: 10 -9 Torr Lifetime: > 10000 hrs Lifetime: 300 hrs Lifetime: 500 - 1000 hrs Lifetime: > 4000 hrs Materials Characterization Core (MCC) Yale West Campus 4/20 ywcmatsci.yale.edu
Demagnification Optics • Demagnification image resolution • Resolution image intensity Beam size at condenser lens focus plane 𝑒 B = 𝑒 G 𝑞 1 𝑟 1 d G : Beam size exiting the gun p 1 : Object distance of condenser lens q 1 : Image distance of condenser lens Beam size on specimen surface at objective lens focus plane 𝑒 p = 𝑒 B 𝑞 2 𝑋𝐸 p 2 : Object distance of objective lens q 2 : Image distance of objective lens WD : Working Distance between the bottom of the objective lens and sample surface Materials Characterization Core (MCC) Yale West Campus 5/20 ywcmatsci.yale.edu
Accelerating voltage ( V acc ) Increasing accelerating voltage less spherical aberration smaller probe diameter and better resolution Increase beam penetration obscure surface detail Increase the probe current at the specimen. A minimum probe current is necessary to obtain an image with good contrast and a high signal to noise ratio. Potentially increase charge-up and damage in specimens that are non-conductive and beam sensitive. SEM images of vanadium oxide nanotubes at different acc voltages Penetration depth V acc Image courtesy http://www.microscopy.ethz.ch/ Materials Characterization Core (MCC) Yale West Campus 6/20 ywcmatsci.yale.edu
Factors Affecting SE Emission: Working Distance (WD) Working Distance : the distance between the bottom of the objective lens and the specimen Increasing WD • increased depth of focus • Increased probe size lower resolution • increased effects of stray magnetic fields lower resolution • increased aberrations due to the need for a weaker lens to focus. 200 um aperture and 10 mm WD. 200 um aperture and 38 mm WD Materials Characterization Core (MCC) Yale West Campus 7/20 ywcmatsci.yale.edu
SEM: Electron-Specimen Interactions Secondary electrons (SE < 50 eV) Electron beam Topographical information Back-scattered electrons (BSE) AE (1-5 nm) SE (5 – 50 nm) Composition (atomic number) and topographical information EDX BSE (~300 nm) Characteristic X-ray (EDX) Composition (1-3 µm) information (Energy Dispersive X-ray CL X-ray Spectroscopy) Continuous X-ray (1-3 µm) Auger electrons (AE) Surface sensitive composition information Cathodoluminescence (CL) Electric states information Fluorescence Phosphorescence Continuous X-ray (Bremsstrahlung) Insulator charging Imaging resolution Interaction volume Sample Materials Characterization Core (MCC) Yale West Campus 8/20 ywcmatsci.yale.edu
Schematic Electron Energy Spectrum SE forms a large low-energy peak < 50 eV BSE Shallow depth of SE production topography information Small interaction volume high imaging Counts Elastic resolution, comparable to reflection e-beam size Auger Electron (AE) AE produces relatively small peaks on the BSE distribution 50 eV 2000 eV Kinetic Energy (eV) Goldstein et al. 1981 Materials Characterization Core (MCC) Yale West Campus 9/20 ywcmatsci.yale.edu
Lens Aberrations: Astigmatism The SEM electromagnetic lenses can not be machined to perfect symmetry. A lack of symmetry an oblong beam: a disk of minimum confusion stronger focusing plane narrower beam diameter weaker focusing plane wider diameter Astigmatism correction Apply current differentially to stigmator coils circular beam Materials Characterization Core (MCC) Yale West Campus 10/20 ywcmatsci.yale.edu
SE Detector: Everhart-Thornley (E-T) Detector E-T detector: low-secondary 1-2 kV electrons are attracted by +200 V on grid and accelerated onto scintillator by +10 kV bias; Photocathode Faraday Cage The light produced by -50 to +200 V scintillator (phosphor surface) passes along light pipe to E-beam external photomultiplier (PM) Output (0.5 – 30 kV) which converts light to electric signal. Optical Dynodes Back scattered electrons also waveguide SE<50 eV detected but less efficiently Scintillator because they have higher Electron Multiplier +10kV BSE energy and are not significantly deflected by grid Sample potential. Materials Characterization Core (MCC) Yale West Campus 11/20 ywcmatsci.yale.edu
Schematic of SU8200: Optics and detection system • SE detectors: • SE(L): SE lower detector • SE(U): SE upper detector • HA(T): HA-BSE top detector • Control/filtering electrode • Conversion electrode • Hi-Pass Top Filter Materials Characterization Core (MCC) Yale West Campus 12/20 ywcmatsci.yale.edu
SE(L) in normal modes ( V acc : 0.5 ~ 30 kV) Sample: photocatalyst V acc : 3 kV Signal : SE(L) Sample courtesy of : Nagaoka University of Technology, Faculty of Engineering, Dr. Kazunori Sato SE + BSE signal • SE(L) (secondary electron Lower detector) • Signal amount is relatively low, but will increase when WD is longer. • Highly topographical information shadowing effect • Less sensitive to specimen charge-up • Signal of the Lower detector is less sensitive to charging artifacts • Low resolution comparing to upper detector Materials Characterization Core (MCC) Yale West Campus 13/20 ywcmatsci.yale.edu
SE(U) in normal modes ( V acc : 0.5 ~ 30 kV) Sample: photocatalyst V acc : 3 kV Signal : SE(U) Sample courtesy of : Nagaoka University of Technology, Faculty of Engineering, Dr. Kazunori Sato • SE(U) (secondary electrons detected with the Upper detector through the objective lens) • Large signal amount, high detection efficiency • High resolution at the topmost surface information • High edge contrast • Sensitive to specimen charge-up • BSE not detected. Materials Characterization Core (MCC) Yale West Campus 14/20 ywcmatsci.yale.edu
LA-BSE in normal modes ( V acc : 0.5 ~ 30 kV) Sample: photocatalyst V acc : 3 kV Signal : LA-BSE(U) Sample courtesy of : Nagaoka University of Technology, Faculty of Engineering, Dr. Kazunori Sato • LA-BSE SE at the control electrode and detected with the Upper detector. • Amount of SE controlled by variable negative electrode voltage. • Compositional + Topographic information Mixture of SE and LA-BSE image • Less sensitive to specimen charging-up Materials Characterization Core (MCC) Yale West Campus 15/20 ywcmatsci.yale.edu
HA-BSE in normal modes ( V acc : 0.5 ~ 30 kV) Mixed particles of electrode BaCO 3 /TiO 2 V acc : 1.5 kV Signal: HA-BSE • HA-BSE (High-Angle Backscattered Electron) • HA-BSE SE at the conversion electrode and detected with Top detector HA(T). • Small signal amount • Rich Compositional information • Less topographic information • Less sensitive to specimen charge-up Materials Characterization Core (MCC) Yale West Campus 16/20 ywcmatsci.yale.edu
Beam Deceleration (Landing voltage 10 V ~ 2 kV) Al electrolytic capacitor y electron V acc : 500 V Magnification: 100kx • A negative voltage (deceleration voltage, V rtd up to 3.5 kV) applied to the specimen, thereby slowing down the primary electron beam to the desired landing energy. • Landing voltage (10 V – 2 kV): V lnd = V acc – V rtd ; V rtd : Deceleration voltage Courtesy of St. Jude Medical, CRMD-U.S.A. • Resolution improved in deceleration mode V acc : 500 V Magnification: 100kx Materials Characterization Core (MCC) Yale West Campus 17/20 ywcmatsci.yale.edu
Scanning Transmission Electron Microscope (STEM) Mode SE detector Photon guide STEM detector BF-STEM image Internal DF-STEM image surface information information • A STEM image providing internal specimen Specimen: Carbon nanotubes V acc : 30 kV Magnification : 250kx information can be obtained simultaneously with the secondary electron image. • The optional Bright Field STEM Aperture Unit is often utilized to generate enhanced contrast differentiation on materials of similar density. Materials Characterization Core (MCC) Yale West Campus 18/20 ywcmatsci.yale.edu
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