Sample Preparation TEM

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    Contamination Free

    TEM Specimen Preparation

    Contamination Free

    TEM Specimen Preparation

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    TEM Specimen Requirements

    Thin

    Representative of the bulk

    Uniform thickness

    Flat

    Rugged

    Conducting Clean

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    Topics

    Electropolishing > Model 110 Twin Jet EP

    Disk cutting > Model 170 Ultrasonic Disk Cutter

    Sample grinding > Model 160 Specimen Grinder

    Dimple grinding > Model 150 Dimpling Grinder Ion milling > Model 1010 LAMP Ion Mill

    Plasma cleaning > Model 1020 Plasma Cleaner

    Mechanical preparation methods

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    Cut a slice

    Diamond saw

    Damage ~ 100 m

    Acid saw Wire saw

    Cleaving as with silicon wafers

    Initial Thinning

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    Site specific cutting of specimen disks Fast

    Cutting by mechanical grinding removalof material

    Rate dependent on abrasive (SiC, CBN) Automatic termination of cutting

    Ultrasonic Disk Cutting

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    Take cut disk down to

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    Dimple GrindingDimple Grinding

    Location specific thinning

    Selected location

    Reduces ion milling time

    Creates thin center thick edge

    Sample is more robust

    Easier to handle

    Single or double sided dimpling

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    Dimple Grinding

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    Cross-Section of a Dimple

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    Dimpling rate Abrasive size

    Lubricant

    Wheel speed Wheel pressure

    Dimple geometry Round

    Oblong

    Important Dimpling Parameters

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    Cross-Sectional TEM (XTEM)

    Semiconductor industry Study microstructure of each layer in an

    integrated circuit

    Thin film thickness Computer hard drives

    Interface science Multiple sections in one

    XTEM specimen

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    XTEM Step-by-Step - I

    Cleave small section of wafer to work with

    Mount to ultrasonic disk cutter specimenplate Face up (blank) or face down (with pattern)

    Face up cover surface with thin glass cover sideto protect surface during cutting process

    Cut out desired sections

    Remove cover slips and discard. Removesections from specimen plate

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    Wafer Mounting and Cutting

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    XTEM Step-by-Step - II

    Remove sections from specimen grinder andsoak and rinse several times

    Create stack

    Three thick dummy pieces on each endsandwiching sections in between. Innermostdummy pieces can be unthinned real material.

    Place dummy pieces and sections into teflonchuck, placing droplet of epoxy on each piece

    Clamp stack in vise and place on hot plate to cure

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    Create Stack

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    XTEM Step-by-Step - III

    Core stack

    Ultrasonically cut 2.3 mm diameter cylinderfrom stack

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    Core Stack

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    XTEM Step-by-Step - IV

    Place core into 3 mm brass tube, epoxy into

    place and cure Slice 3 mm disks from brass tube

    Place disks on specimen grinder and polish

    away damaged region from both sides ofdisk.

    Dimple cross-section Ion mill to electron transparency

    Plasma clean in Ar/25%O2 ( 2 5 min.)

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    Interface

    Place Stack in Tube & Slice

    RegionofInterest

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    Rough grind with 600 grit SiC paper

    Step down grinding/polishing with diamondfilms 30 m, 15 m, 9 m, 6 m, 3 m, 1 m,

    0.5 m

    Final polish with colloidal silica

    Flip over and repeat on secondside, finishing with specimen< 100 m thick

    Grind 3mm Disk

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    19 Piece Cross Section

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    Ion Milling

    Non-reactive ions directed at specimen

    Thinning by momentum transfer

    Thinning rate dependent upon:

    Relative mass of thinning ion and specimenatom ion energy

    Specimen crystal structure Angle of incidence of ion beam

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    Ion MillingIon Milling

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    High Angles

    Angles >15

    Leads to surface topography as a functionof atomic number

    Rapid thinning

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    Low Angles

    Angles < 15 Leads to flat surface but slower thinning

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    Energy

    Higher energies

    Thinning rates decreased for some materials

    Implantation

    Amorphous layers Point defects

    Propagated artifacts

    Lower energies Thinning rates more predictable

    No / reduced damage to specimen

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    Temperature

    Without cooling Heat sample to as high as 200C Changes in phase chemistry

    Changes in sample chemistry Mobility of defects increases

    Structural changes

    Differential / preferential milling

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    Hollow Anode Discharge Ion Source

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    Ion Milled Ca dopedIon Milled Ca dopedYBaCuOYBaCuO (123)(123) BicrystalsBicrystals

    Y/BaCu/O

    350 400 450 500 550 6000

    20

    40

    60

    80

    100

    energy-loss (eV)

    intensity(electrons)x10

    00

    Ca-LCa-L2,32,3

    O-KO-KO-K

    at dislocation core

    3nm away from grain boundary

    at dislocation core

    3nm away from grain boundary

    Chemical composition

    at dislocation core

    Ca/O = 0.1atom%

    Chemical compositionChemical composition

    at dislocation coreat dislocation core

    Ca/O = 0.1atom%Ca/O = 0.1atom%

    Cour tesy of Dr.Cour tesy of Dr. GerdGerd DuscherDuscher and Jul ia Luck, ONRLand Jul ia Luck, ONRL

    ADF STEM Image EELS Spectra

    I Mill d XTEM f TiI Mill d XTEM f Ti SiSi O l iO t l t i

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    Ion Milled XTEM of TiIon Milled XTEM of Ti--SiSi OptoelectronicOptoelectronic

    SiO2(CVD)

    TiN (CVD)

    /TiSi2

    Via

    1.0 m

    SiO2(Grown)

    Si

    TiN(CVD)

    / Ti

    Court esy of I van Petrov and Young Kim, Universit y of I l l inois

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    Ion Milled X-TEM Sample

    Polycrystalline copper film onepitaxial Ti0.5W0.5 N/TiN

    superlattice on MgO (001)

    ll d f /I Mill d XTEM f C /R L i

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    Ion Milled XTEM of Co/Ion Milled XTEM of Co/RuRu LatticesLattices

    HREM image show ing alt ernat ingmonolayers of Co and Ru w ithin the

    Co / Ru ordered superlatt ice

    (0002)Rumonolayers(largeratoms)

    (0001) Co

    Court esy by Kazuhi ro Hono & D. H. Ping, Nat ional Research I nstit ut e for Metals

    Imaging of LaTiO3 Multilayers

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    Imaging of LaTiO3 Multilayers

    2 nm

    1

    2

    3

    456

    2 nm

    Wedge polishing, followed by IBEat low incident angle, low ion energy

    and low temperature LaTiO3 multilayers in SrTiO3imaged in a FE TEM

    Material (in box) thin enough forADF lattice imaging over 0.4 mfield of view

    Courtesy of D. A. Muller, J. Grazul,A. Ohtomo, H. Hwang, Bell Labs,Lucent Technologies, NJ (USA)

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    Plasma Cleaning

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    Plasma Cleaning

    Theory Chemical reaction (oxygen plasma) Plasma disassociates oxygen

    Disassociated oxygen reacts with hydrocarbonon specimen holder to form CO, CO2, and H2O

    These species are pumped away

    D i

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    Plasma Chamber

    Inductively Coupled HF Plasma

    Design

    Ion Impingement Energies

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    Ion Impingement Energies

    50

    0

    5

    10

    15

    2025

    30

    35

    40

    45

    5 10 15 20 25 30 35 40 45 50

    Chamber Pressure (mTorr)

    Ion

    Ene

    rgy

    (eV)

    Z = 0 cm

    Z = 10 cm

    0

    EELS for Contamination Thickness Determination

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    I0 - Intensity UnderZero Loss Peak

    It - Total Intensity in

    Spectrum

    t=l ln(It/I0)

    t/l - Mass Thickness

    EELS for Contamination Thickness Determination

    C t i ti Thi k Ti S TiO3

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    2.1

    0.9

    1.1

    1.3

    1.5

    1.7

    1.9

    0 100 200 300 400 500 600

    Time (seconds)

    MassThickness

    No Cleaning

    One Minute Plasma Clean

    Two Minute Plasma Clean

    Contamination Thickness vs. Time SrTiO3

    Plasma Cleaning of 304 Stainless Steel

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    Plasma Cleaning of 304 Stainless Steel

    1 Minute

    2 Minutes

    3 Minutes

    4 Minutes

    5 Minutes Arrow

    After plasma cleaning

    5 minute spot

    1 Minute of Plasma Cleaning

    Concluding Remarks

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    Concluding Remarks

    Integrated approach using instrumentsin series

    Plan view or XTEM specimens ready for

    transfer to and analysis by FE TEM

    Resulting electron transparent regions

    are free of artifacts and contamination