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MSE-602 2013 advanced SEM Marco Cantoni 7. advanced SEM SEM Low voltage SE imaging Condition of the surface, coatings, plasma cleaning Low voltage BSE imaging Polishing for BSE, EDX and EBSD, effect of ion beam etching/polishing 1 MSE-602 2013 advanced SEM Marco Cantoni 100 50 10 5 1 0.5 1 2 5 10 20 30 FE LaB 6 W Tension d'accélération (kV) Résolution (nm) Haute tension/haute résolution: - effets de bord - détails fins non-résolus - fort endommagement dû au faisceau 1985 2010 Field emission gun monochromators beam boosters, beam deceleration, Lens-design: In-lens, Semi-in- lens, immersion lens Short working distance Detectors: Everhard-Thornley (SE) In-column (through the lens, in- lens, “in-beam”) Low Voltage BSE detection, energy filtering (separation of materials and topography contrast) Analytical SEM: SDD EDX detectors (high throughput, large collection angle) High-speed EBSD detectors Beam currents of several 100 nA Latest generation of SEM High voltage, high resolution: Edge effects Charging effects Beam damage low voltage, high resolution: Observation of the “real” surface Non-metallic samples Reduced beam damage 2

7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

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Page 1: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

7. advanced SEM

SEM• Low voltage SE imaging

• Condition of the surface, coatings, plasma cleaning

• Low voltage BSE imaging

• Polishing for BSE, EDX and EBSD, effect of ion beam

etching/polishing

1

MSE-602 2013 advanced SEM Marco Cantoni

100

50

10

5

10.5 1 2 5 10 20 30

FE LaB6

W

Tension d'accélération (kV)

Rés

olut

ion

(nm

)

Basse tension/haute résolution: - observation de la surface réelle - échantillons non-métallisés - faible endommagement dû au faisceau

Haute tension/haute résolution: - effets de bord - détails fins non-résolus - fort endommagement dû au faisceau

1985

2010

Field emission gun monochromatorsbeam boosters, beam deceleration,Lens-design: In-lens, Semi-in-lens, immersion lensShort working distance

Detectors:Everhard-Thornley (SE)In-column (through the lens, in-lens, “in-beam”)Low Voltage BSE detection, energy filtering (separation of materials and topography contrast)

Analytical SEM:SDD EDX detectors (high throughput, large collection angle)High-speed EBSD detectorsBeam currents of several 100 nA

Latest generation of SEM

High voltage,high resolution:• Edge effects• Charging effects• Beam damage

low voltage, high resolution:• Observation of the “real” surface• Non-metallic samples• Reduced beam damage

2

Page 2: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

No specimen preparation needed:Low kV imaging of non-conducting, low density samples

FEI MagellanOperator: Ingo GestmannSamples: Marco Cantoni

Al2O3 Nano-crystals

3

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

No specimen preparation needed:Low kV imaging of non-conducting, low density samples

FEI MagellanOperator: Ingo GestmannSamples: Marco Cantoni

Carbon nano-tubes(MWCT)

4

Page 3: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

No specimen preparation needed:Low kV imaging of non-conducting samples

Liquid filledorganic membranes

Zeiss Nvision 40Marco Cantoni

5

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

No specimen preparation needed:Low kV imaging of non-conducting samples

Liquid filledorganic membranes

Zeiss Nvision 40Marco Cantoni

6

Page 4: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

Purely organic specimen: non-conductive, low density:Metal coating

HeLa Cells, Graham KnottMarco Cantoni, Nvision 40

15nm Ag/Pd coating

3nm Os coating3nm Os coating

7

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

“Easy” sample:

SC wireNb3Sn in Cu matrix

8

Page 5: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging

“Easy” samples: Everhard-Thornleydetector (SE)

Solid state BSEdetector

9

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV BSE imaging

Solid state BSEdetector

2keV, In-ColumnEsB detector

10

Page 6: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging “Easy” samples:

11

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging “Easy” samples:

12

Page 7: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

SEM low kV imaging “Easy” samples:

13

MSE-602 2013 advanced SEM Marco Cantoni

Contamination by hydro-carbons

• contamination “spoils” imaging at low kV

• How to avoid (at CIME):– plasma cleaning of the sample before

inserting– Plasma clean the chamber at each

insertion (multi-user environment)

XL30 FEG & EVACTRON

NVision40 & EVACTRON

SEM low kV imaging

14

Page 8: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

0.5 mmNb3Sn multifilament superconducting cable

Nb3Sn superconductor multifilament cable:14’000 Nb3Sn filaments (diameter ~5um) in bronze matrix

SEM: Preparation for analytical EM

Solid State BSE detector20kV acceleration voltage

Mechanical polishing <-> Ar ion beam polished

EDX maps

Sn

Cu

Nb

15

MSE-602 2013 advanced SEM Marco Cantoni

Mechanical polishing:• Grains of harder phase

incorporated in softer matrix• Deformed microstructure at

surface reduces formation of Kikichi lines in EBSD

SEM BSE/EDX/EBSD

After Ar ion polishing (Gatan PIPS)

Sn

Cu

Nb

16

Page 9: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

in-chamberET-detectorSE

in-column“InLens”SE-detector

in-column, “energy-selective” EsBBSE-detector

Ion polishing

17

MSE-602 2013 advanced SEM Marco Cantoni

Nb3Sn multifilament Superconductors

Materials & orientation contrast

SEM low kV BSE imaging

NVision 401.8kV EsB detector5µm

18

Page 10: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

Nb3Sn multifilament Superconductors

Materials & orientation contrast

FIB/SEM low kV BSE imaging

19

MSE-602 2013 advanced SEM Marco Cantoni

Goal of final polishing:Removal of the damaged surface layermechano-chemical polishing (EBSD) or ion polishing

Interaction volumeBlue: scattered electronsRed: backscattered electrons (leaving the sample surface)

Monte-Carlo Simulation CASINO v2.42

escape depth of BSE: Nb3Sn 30kV: 800nm

5kV: 50nm

1kV: < 5nm

SEM preparation: polishing

1kV5kV

30kV

20

Page 11: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

New HR-SEM at CIME

• Starting point: XL-30 SFEG SIRION (since 2001)• First semi-in-lens HR-SEM:

in-lens (through the lens) detection of SE and BSE

Resolution in UHR mode: 1.5 nm at 10 kV (or higher); 2.5 nm at 1 kV

21

MSE-602 2013 advanced SEM Marco Cantoni 22

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MSE-602 2013 advanced SEM Marco Cantoni 23

MSE-602 2013 advanced SEM Marco Cantoni

Best “SEM” at EPFL: FIB Nvision@CIME

24

Page 13: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

Two different contrasts with one scan: parallel detectors

25

MSE-602 2013 advanced SEM Marco Cantoni 26

Page 14: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni 27

MSE-602 2013 advanced SEM Marco Cantoni 28

Page 15: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni 29

MSE-602 2013 advanced SEM Marco Cantoni 30

Page 16: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni 31

MSE-602 2013 advanced SEM Marco Cantoni

Introducing...MERLIN™– Analytical power for the sub-nanometer world –

32

Page 17: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

Double condenser lens Aperture independent probe current adjustment

Beam Booster Brightness of the electron probe

maintained for low landing energies

MERLIN™– Analytical power for the sub-nanometer world –

Proven GEMINI® final lens design New double condenser lens for highest

probe current possibilities (300 nA) Beam booster technology maintains

brightness of all electron probes including low landing energies

True on-axis in-lens SE and BSE detectors

► GEMINI® II designComplete detection

system

High stability field emitter cathode Maximum probe current 300 nA

Energy selective Backscatter detector (EsB)

In-lens Secondary Electron detector

GEMINI® II final lens

33

MSE-602 2013 advanced SEM Marco Cantoni 34

Page 18: 7. advanced SEM low kV imaging 14 MSE-602 2013 advanced SEM Marco Cantoni Nb 0.5 mm 3Sn multifilament superconducting cable Nb3Sn superconductor multifilament cable: 14’000 Nb3Sn

MSE-602 2013 advanced SEM Marco Cantoni

In-lens SE(Secondary Electrondetector)

Topographical informationwith on-axis in-lens SE detector

MERLIN™– Analytical power for the sub-nanometer world –

GEMINI® II design► Complete detection

system

Complete detection system: Unique double in-lens detection Acquisition of pure secondary and

backscatter electron signals Separation of compositional, topographical

and crystalline surface information

35

MSE-602 2013 advanced SEM Marco Cantoni

EsB(Energy selective Backscatter detector)

Energy filtering grid

Si

Si3N4

TiN

Ti

Compositional contrastwith on-axis in column EsB detector

MERLIN™– Analytical power for the sub-nanometer world –

Complete detection system: Unique double in-lens detection Acquisition of pure secondary and

backscatter electron signals Separation of compositional, topographical

and crystalline surface information

GEMINI® II design► Complete detection

system

36

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MSE-602 2013 advanced SEM Marco Cantoni 37

MSE-602 2013 advanced SEM Marco Cantoni 38

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MSE-602 2013 advanced SEM Marco Cantoni 40

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MSE-602 2013 advanced SEM Marco Cantoni 43

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MSE-602 2013 advanced SEM Marco Cantoni 45

MSE-602 2013 advanced SEM Marco Cantoni

Sapphire

46