Specific Process Knowledge/Characterization/SEM: Scanning Electron Microscopy

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Scanning electron microscopy at Danchip

At Danchip there are five SEMs (Scanning Electron Microscopes) that all cover a wide range of needs both in the cleanroom and outside: From fast in-process verification of different process parameters such as etch rates, step coverages or lift-off quality to ultra high resolution images on any type of sample intended for publication.

  • The SEM Supra 1 is located in the basement outside the cleanroom. It is serving two purposes: Serving the users that have samples from outside the cleanroom and serving as training tool; all new SEM users with no/little SEM experience must be trained on this tool and gain basic knowledge (typically 10 hours of usage) here before being qualified for training on the SEMs in the cleanroom.
  • The SEM 2 and 3 are located in the cleanroom where they serve as general imaging tools for samples that have been fabricated in the cleanroom. Like SEM Supra 1, they are VP models from Carl Zeiss and will produce excellent images on any sample. The possibility of operating at higher chamber pressures in the VP mode makes imaging of bulk non-conducting samples possible. The SEM Supra 2 is also equipped with an airlock and an EDX detector.
  • The SEM Leo s a very reliable and rugged instrument that provides high quality images of most samples. It is exclusively dedicated to the users of the Raith E-beam lithography system so general imaging of user samples is not allowed.
  • The SEM Tabletop 1 is a tabletop SEM that is located in the basement outside the cleanroom. It has a limited resolution, but it is fast and easy to use, also for non-conducting samples. Training in the others SEMs is not required to use this SEM.

SEM Supra 1, 2 and 3 SEM Leo s all manufactured by Carl Zeiss and have the same graphical user interface and very identical electron optics. But there are there are small hardware and software differences, thus a training is needed for each SEM you want to use.

The SEM Tabletop 1 is manufactured by Hitachi.

Common challenges in scanning electron microscopy

Comparison of SEM's at Danchip

Equipment SEM LEO SEM Supra 1 SEM Supra 2 SEM Supra 3 SEM Tabletop 1
Purpose Imaging and measurement of
  • Conducting samples
  • Semi-conducting samples
  • Thin (~ 5 µm <) layers of non-conducting materials such as polymers
  • Conducting samples
  • Semi-conducting samples
  • Thin (~ 5 µm <) layers of non-conducting materials such as polymers
  • Thick polymers, glass or quartz samples
  • Conducting samples
  • Semi-conducting samples
  • Thin (~ 5 µm <) layers of non-conducting materials such as polymers
  • Thick polymers, glass or quartz samples
  • Conducting samples
  • Semi-conducting samples
  • Thin (~ 5 µm <) layers of non-conducting materials such as polymers
  • Thick polymers, glass or quartz samples
  • Conducting samples
  • Semi-conducting samples
  • Thin (~ 5 µm <) layers of non-conducting materials such as polymers
  • Thick polymers, glass or quartz samples
Other purpose
  • E-beam lithography using Raith Elphy Quantum system
  • Surface material analysis using EDX
Instrument Position
  • Cleanroom of DTU Danchip
  • Basement of DTU Danchip
  • Cleanroom of DTU Danchip
  • Cleanroom of DTU Danchip
  • Basement of DTU Danchip
Performance Resolution The resolution of a SEM is strongly dependent on the type of sample and the skills of the operator. The highest resolution is probably only achieved on special samples
  • ~ 5 nm (limited by vibrations)
  • 1-2 nm (limited by vibrations)
  • 1-2 nm (limited by vibrations)
  • 1-2 nm (limited by vibrations)
  • ~25 nm (limited by instrument)
Instrument specifics Detectors
  • Secondary electron (Se2)
  • Inlens secondary electron (Inlens)
  • Backscatter electron (BSD)
  • Secondary electron (Se2)
  • Inlens secondary electron (Inlens)
  • 4 Quadrant Backscatter electron (QBSD)
  • Variable pressure secondary electron (VPSE)
  • Secondary electron (Se2)
  • Inlens secondary electron (Inlens)
  • 4 Quadrant Backscatter electron (QBSD)
  • Variable pressure secondary electron (VPSE)
  • Secondary electron (Se2)
  • Inlens secondary electron (Inlens)
  • High Definition four quadrant Angular Selective Backscattered electron detector (HDAsB)
  • Variable pressure secondary electron (VPSE)
  • Secondary electron (SE)
  • Backscatter electron (BSE)
Stage
  • X, Y: 125 × 100 mm
  • T: 0 to 90o
  • R: 360o
  • Z: 48 mm
  • X, Y: 130 × 130 mm
  • T: -4 to 70o
  • R: 360o
  • Z: 50 mm
  • X, Y: 150 × 150 mm
  • T: -10 to 70o
  • R: 360o
  • Z: 50 mm
  • X, Y: 130 × 130 mm
  • T: -4 to 70o
  • R: 360o
  • Z: 50 mm
  • X, Y: 35 mm
  • T: No tilt
  • R: No rotation
  • Z: 0 mm
Electron source FEG (Field Emission Gun) source
  • Thermionic tungsten filament
Operating pressures
  • Fixed at High vacuum (2 × 10-5mbar - 10-6mbar)
  • Fixed at High vacuum (2 × 10-4mbar - 10-6mbar)
  • Variable at Low vacuum (0.1 mbar-2 mbar)
  • Fixed at High vacuum (2 × 10-4mbar - 10-6mbar)
  • Variable at Low vacuum (0.1 mbar-2 mbar)
  • Fixed at High vacuum (2 × 10-4mbar - 10-6mbar)
  • Variable at Low vacuum (0.1 mbar-2 mbar)
  • Conductor vacuum mode: 5 Pa
  • Standard vacuum mode: 30 Pa
  • Charge-up reduction vacuum mode: 50 Pa
Options
  • Raith Elphy Quantum E-Beam Litography system
  • All software options available
  • Antivibration platform
  • Fjeld M-200 airlock taking up to 8" wafers
  • Oxford Instruments X-MaxN 50 mm2 SDD EDX detector and AZtec software package
  • High Definition four quadrant Angular Selective Backscattered electron detector (HDAsB)
Substrates Sample sizes
  • Wafers up to 6" (only full view up to 4")
  • Up to 6" wafer with full view
  • Up to 8" wafer with 6" view
  • Up to 6" wafer with full view
  • Up to 70 mm with full wiew
Allowed materials
  • Any standard cleanroom materials
  • Any standard cleanroom material and samples from the Laser Micromachining tool and the Polymer Injection Molding tool
  • Any standard cleanroom materials
  • Any standard cleanroom materials
  • Any standard cleanroom material and samples from the Laser Micromachining tool and the Polymer Injection Molding tool
  • Some biological samples (ask for permission)



SEM TPTUnder construction.png

  • The next course is the 21rd of March from 9:00 - please sign up now by writing to SEM@danchip.dtu.dk
  • Here you will find links to tool packages learning material, training videos and the lecture slides.
    • Before the lecture please read “Scanning Electron Microscopy Primer” by Bob Hafner. You can find it on the cleanroom drive: U:\DCH\CleanroomDrive\_TPT\TPT SEM\Learning material or Click here
    • Training videos can be found on the cleanroom drive: U:\DCH\CleanroomDrive\_TPT\TPT SEM\Training videos
    • Lecture slide will be uploaded here after the lecture
  • For more information take a look at the Danchip homepage: SEM TPT

Comparison of the SEM's at CEN Under construction.png

Equipment SEM Inspect S SEM FEI Nova 600 NanoSEM SEM FEI Quanta 200 ESEM FEG FIB-SEM FEI QUANTA 200 3D Dual Beam FEI Helios Nanolab 600
Purpose
  • Conductive samples in High Vac
  • Charge reduction in Low Vac
  • X Ray Analysis with EDS and WDS
  • Conductive samples in High Vac
  • Charge reduction in Low Vac
  • X Ray Analysis with EDS
  • Crystallographic analysis using EBSD and both On and Off axis TKD
  • Conductive samples in High Vac
  • Charge reduction in Low Vac
  • Environmental control using Peltier stage
  • Cryogenic sample fixing/stabilization using cryo stage
  • X Ray Analysis with EDS
  • Conductive samples in High Vac
  • Charge reduction in Low Vac
  • Micro and Nano milling/fabrication using various gases and FIB
  • Conductive samples in High Vac
  • Micro and Nano milling/fabrication using various gases and FIB
  • X Ray Analysis with EDS
  • Crystallographic analysis using EBSD and Off Axis TKD
Equipment position CEN Building 314 CEN Building 314 CEN Building 314 CEN Building 307 Room 111 CEN Building 314
Resolution The resolution of a SEM is strongly dependent on sample type and the operator. Resolution quoted is using sputtered gold on carbon
  • High-vacuum

•3.0nm at 30kV (SE) •10nm at 3kV (SE) •4.0nm at 30kV (BSE)

  • Low-vacuum

•3.0nm at 30kV (SE) • 4.0nm at 30kV (BSE) • > 12nm at 3kV (SE)

B
  • High vacuum

• 0.8 nm at 30 kV (STEM) • 1.0 nm at 30 kV (SE) • 2.5 nm at 30 kV (BSE) - 3.0 nm at 1 kV (SE)

  • High vacuum with beam deceleration option

• 3.0 nm at 1 kV (BD mode + BSE)

  • Low vacuum - 1.4 nm at 30 kV (SE)

•2.5 nm at 30 kV (BSE) •3.0 nm at 3 kV (SE)

  • Extended vacuum mode (ESEM)

•1.4 nm at 30 kV (SE)

  • Electron Column

•5nm @30kV

  • Ion Column

•7nm @ 30kV

  • Electron Column

•0.8nm @15kV •0.9nm @1kV

  • Ion Column

•4.5nm @ 30kV

Detectors
  • ETD Secondary Electrons
  • BSED Back Scatter Electrons
  • LVD/LFD Low Vac SE
  • EDS X Ray by energy
  • WDS X Ray by wavelength
  • STEM Scanning Transmission Electron Microscopy
  • ETD/TLD Secondary Electrons
  • BSED Back Scatter Electrons
  • LVD/LFD Low Vac SE
  • Helix Low Vac SE
  • EDS X Ray by energy
  • EBSD Electron Back Scatter Diffraction
  • TKD Transmission Kikuchi Diffraction
  • STEM Scanning Transmission Electron Microscopy
  • GAD Low Vac BSED
  • ETD Secondary Electrons
  • BSED Back Scatter Electrons
  • LVD/LFD Low Vac SE
  • GSED ESEM SE
  • EDS X Ray by energy
  • STEM Scanning Transmission Electron Microscopy
  • ETD Secondary Electrons
  • BSED Back Scatter Electrons
  • LVD/LFD Low Vac SE
  • STEM Scanning Transmission Electron Microscopy
  • GAD Low VAC BSED
  • GSED ESEM SE
  • ETD/TLD Secondary Electrons
  • ABS Annular BSED
  • EDS X Ray by energy
  • EBSD Electron Back Scatter Diffraction
  • CDEM Continuos Dinode Electron Multiplier
Stage specifications
  • X 50mm
  • Y 50mm
  • Z 50mm
  • R 360⁰
  • T 70⁰ Manual
  • X 150mm Piezo
  • Y 150mm Piezo
  • Z 10mm
  • R 360⁰ Piezo
  • T 70⁰
  • X 50mm
  • Y 50mm
  • Z 50mm
  • R 360⁰
  • T 70⁰ Manual
  • X 100mm
  • Y 100mm
  • Z 50mm
  • R 360⁰
  • T 70⁰
  • X 150mm Piezo
  • Y 150mm Piezo
  • Z 10mm
  • R 360⁰ Piezo
  • T 70⁰
Options A B C D E
Max sample size Consult with CEN staff as weight, dimensions, pumping capacity and technique all play a roll in the sample size