


This is the original GW Type 31 amplifier, we are still making it now in the UK.
When a high-energy electron penetrates a crystalline semiconductor, most of its kinetic energy is absorbed by ionization of the silicon atoms as silicon valence electrons are ejected from their orbits. Each ionization creates a free electron and the empty valence site leaves the atom electrically unbalanced with a net positive charge. This net positive charge called a hole appears to migrate from atom to atom under the influence of an external field creating the illusion of a flow of positive charge. At the interface of P-doped and N-doped regions.
There is a narrow zone void of mobile charge carriers due to the electric field (Fermi Potential) created by the redistribution of electrons and holes at the junction. If the electrons and holes created by the impinging electrons can enter this Depletion Zone, then they, too will be swept aside by the Fermi Potential:this movement of charge carriers manifests itself as a current in an external circuit. In Silicon the average electron hole pair requires about 3.6eV of energy so that the external current, which is proportional to the number of carriers entering the Depletion Zone, may well be two to four orders of magnitude greater than the primary beam current depending on the primary beam energy and the percentage of the pairs that can be absorbed into the Depletion Zone. This phenomenon is known as Electron Beam Induced Current or EBIC. This same effect can be induced by photon bombardment and is the basis for the operation of photodiodes and solar cells.
Modern planar semiconductor devices, because of their uniquely two- dimensional structure, lend themselves readily to both qualitative and quantitative investigation by the EBIC technique in the Scanning Electron Microscope and also in the Laser Scanning Microscope (OBIC).
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QUANTAX EDS for SEM -
QUANTAX WDS -
EBSD -
Micro-XRF -
Fourier 80 -
ELEXSYS -
EMXplus -
EMXmicro -
Magnettech ESR5000 -
AvanceCore -
Avance NMR -
GHz Sınıfı NMR -
ASTAR -
TEM STRAIN MAPPING ANALYSIS -
4D STEM WITH TOPSPIN PLATFORM -
3D PRECESSION DIFFRACTION TOMOGRAPHY – MICRO ED -
e-PDF software suite -
4D-Scanning Precession Electron Diffraction (4D-SPED) -
ENHANCED EELS & EDX SPECTROSCOPY -
FireFly -
SyncRay -
3-axes Motorized Stage -
Custom designed systems -
MINISPEC MQ SERIES Contrast Agent Analyzer -
MINISPEC MQ SERIES Toothpaste Analyzer -
MINISPEC MQ SERİSİ Polimer Araştırma Analizörü -
MINISPEC MQ ONE SERİSİ Fiberlerde Daldırma -
MINISPEC MQ ONE SERİSİ Hidrojen Analizörü -
MINISPEC MQ ONE SERİSİ Spin-Finish -
MINISPEC LF Serisi -
MINISPEC MQ SERİSİ SFC Analizörü (Yerinde Güncellenilebilir) -
MINISPEC MQ 20 SERİSİ Toplam Yağ ve Nem -
MINISPEC MQ 20 SERİSİ Droplet Size Analizörü 2.0 -
MINISPEC MQ ONE SERIES Seeds Analyzer -
5'i bir arada -
LUXOR Altın Kaplama -
LUXOR Platin Kaplama -
Aksesuarlar -
SEM Backscattered Electron Detector -
SEM BSE Diode repair & supply -
Centaurus Cathodoluminescence SEM CL, BSE, YAG Detecto -
BF DF HAADF SEM STEM Detector -
HAADF Annular SEM STEM Detector -
AMT sCMOS & CCD TEM Camera Systems -
Model 1064 ChipMill -
Model 1040 NanoMill® TEM Örneği Hazırlama Sistemi -
Model 1080 PicoMill® TEM Örneği Hazırlama Sistemi -
Model 1061 SEM Mill -
Model 1051 TEM Mill -
Model 1062 TrionMill -
Model 1070 NanoClean -
Model 1020 Plasma Cleaner -
Model 9030 Turbo Pumping Station -
Model 9020 Vacuum Pumping Station -
Model 9010 Vacuum Storage Container -
Model 120 Automatic Power Control -
Model 110 Automatic Twin-Jet Electropolisher -
Model 140 Digital Power Control -
Model 200 Dimpling Grinder -
Model 220 Low Temp Container -
Model 160 Specimen Grinder -
Model 2020 Advanced Tomography Holder -
Model 2021 Analytical Tomography Holder -
Model 2023 Analytical Tomography Holder for Ultra-X -
Model 2552 Cryo Cartridge Specimen Holder -
Model 2550 Cryo Transfer Tomography Holder -
Model 2040Dual-Axis Tomography Holder -
Model 2045 Motorized Dual-Axis Tomography Holder -
Model 2050On-Axis Rotation Tomography Holder -
Model 2030Ultra-Narrow Gap Tomography Holder -
Model 2560Vacuum Transfer Tomography Holder -
1490 series Bulk Liquid Electrochemistry -
1405 series Optical Bulk Liquid Electrochemistry -
Liquid Flow -
Multichannel Gas Environment Heating -
MEMS Heating + Biasing -
Cryo Biasing -
Biasing Manipulator -
Tomography -
Magnetizing -
Liquid Flow -
In-Situ SEM Bulk Liquid Electrochemistry 1470 Series SEM -
SEM Gas + Heating 1300 Series – SEM -
SEM MEMS Heating + Biasing 1590 Series – SEM -
300N & 2kN vertical 3&4 point bending stage for Raman -
200N compression & horizontal bending stage -
Dual leadscrew insitu tensile stage for XRD, Optical & Synchrotron -
2kN & 5kN Tensile compression and horizontal bending stage -
200N compression & horizontal bending stage for SEM -
2kN & 5kN Tensile compression and horizontal bending stage for SEM -
300N & 2kN vertical 3&4 point bending stage for SEM -
NEW EBSD testing stages -
Dual screw tensile stage for XRD, Optical & Synchrotron -
2kN & 5kN Tensile compression and horizontal bending stage -
200N compression & horizontal bending stage -
CT500 500N in-situ tensile stage for µXCT applications -
CT5000 5kN in-situ loadcell tensile stage for X-Ray CT applications -
CT Heating and Cooling cell -20°C to +160°C for µXCT applications -
CT20K, Full Open Frame, Tensile, Compression & Torsion rig, designed for Synchrotron and room based X-ray CT imaging systems -
Biaxial & Quadaxial -
Forensic Comparison Stage for SEM -
miniFly -
Software: ESPRIT Family -
QUANTAX EDS for TEM