development of electron microscope - dr. norhayati ahmad · pdf file9/2/2011 ·...
TRANSCRIPT
1
Development of electron microscope
1897 : Thompson describes the existence of negativelycharged particles (electrons)
1925: De Broglie theorised that electrons have wave-likecharacteristics, addressing the wave/particle duality
1927: Thompson and reid demonstrated the wave natureof electrons by diffraction expeiments
1931: Ruska et. Al. build the first electron microscope(Nobel prize in 1986)
1949: Philips commercialises the EM100….
~ 80 years
Near-field scanning optical microscopy
Scanning Probe Microscopy
Atomic force microscopy
scanning tunnelingmicroscope
2
OPTICAL OPTICAL
MICRSOCOPEMICRSOCOPE
SEMSEM
TEMTEM
OMOM
TEMTEM
SEMSEM Diffraction pattern
3
SCANNING ELECTRON MICROSCOPE (SEM)SCANNING ELECTRON MICROSCOPE (SEM)
The basic steps involved in all Electron Microscopy are:
�� AA streamstream ofof electronselectrons isis formedformed byby thethe electronelectron sourcesource ((electricelectric gungun))
andand acceleratedaccelerated towardtoward thethe specimenspecimen usingusing aa positivepositive potentialpotential..
�� ThisThis streamstream ofof electronelectron isis focusedfocused usingusing aperturesapertures andand magneticmagnetic
lenseslenses intointo aa thin,thin, focused,focused, monochromaticmonochromatic beambeam
�� ThisThis beambeam isis focusedfocused ontoonto thethe specimenspecimen usingusing aa magneticmagnetic lenslens
�� InteractionsInteractions occuroccur insideinside thethe specimenspecimen,, affectingaffecting thethe electronelectron beambeam..
TheseThese interactionsinteractions areare detecteddetected andand transformedtransformed intointo anan imageimage
SEM componentsSEM components
1.1. Microscope column:Microscope column:
�� Electron gun (source of electrons)Electron gun (source of electrons)
�� Electromagnetic lensesElectromagnetic lenses
�� AperturesApertures
�� Scan coils (used to adjust beam position)Scan coils (used to adjust beam position)
2. Specimen stage (chamber)Specimen stage (chamber)
3.3. Vacuum pumping systemVacuum pumping system (keep clean, filament oxidation, air will scatter e(keep clean, filament oxidation, air will scatter e--s)s)
4.4. Secondary electronSecondary electron and and backscattered electronbackscattered electron detectorsdetectors (receive signals used (receive signals used in imaging)in imaging)
5.5. XX--ray detectorray detector (EDX or EDS) (EDX or EDS) –– used to detect xused to detect x--rays for chemical analysisrays for chemical analysis
6.6. Electronic control and imaging systemElectronic control and imaging system: to control the SEM, including focusing, : to control the SEM, including focusing, magnification and imagingmagnification and imaging
4
5
Material Analysis
Clay Nylon Gold wire
Fiber Copper interconnect WoodDiamond powder
SEM PRINCIPLESSEM PRINCIPLES
•• The SEM The SEM uses electronsuses electrons instead of light to form an image.instead of light to form an image.
•• A beam of electrons is produced by the A beam of electrons is produced by the electron gunelectron gun
•• An anode attracts the electrons and directs them towards the sampleAn anode attracts the electrons and directs them towards the sample
•• A series of electromagnetic lenses focuses the beam A series of electromagnetic lenses focuses the beam
�� One type of lens is the One type of lens is the condenser lenscondenser lens, which demagnifies the , which demagnifies the
beam to decrease the divergence angle.beam to decrease the divergence angle.
�� A second type of lens is the A second type of lens is the objective lensobjective lens, which further narrows , which further narrows
the beam to focus it on the sample.the beam to focus it on the sample.
6
• Once the beam hits the sample, several electrons are ejected from the
sample. These include:
�� Secondary Electrons (SE)Secondary Electrons (SE)
�� BackBack--Scattered Electrons (BSE)Scattered Electrons (BSE)
�� XX--raysrays
�� Auger ElectronsAuger Electrons
�� Cathodoluminescence (CL)Cathodoluminescence (CL)
• Detectors collect these secondary and back-scattered electrons and
convert them into a signal that is sent to a viewing screen similar to a
TV, thus producing an image
1.1. TYPES OF ELECTRON GUNS (electron source)TYPES OF ELECTRON GUNS (electron source)
�� Tungsten hairpin Filament (most commonly used)Tungsten hairpin Filament (most commonly used)
�� Lanthanum Hexaboride (LaBLanthanum Hexaboride (LaB66))
�� Field Emission (FE) (W or C cathode)Field Emission (FE) (W or C cathode)
•• ElectronsElectrons areare producedproduced fromfrom thethe filamentfilament byby thermionicthermionic emissionemission..
•• CurrentCurrent isis passedpassed throughthrough thethe filamentfilament inin orderorder toto heatheat itit sufficientlysufficiently toto aa
TT ==27002700 KK..
•• HeatingHeating isis accomplishedaccomplished byby runningrunning aa 33--44 ampamp currentcurrent throughthrough thethe
filamentfilament..
•• ThereThere isis aa largelarge spreadspread inin electronselectrons fromfrom thethe filamentfilament tiptip..
•• TheThe filamentfilament isis aa atat largelarge negativenegative potentialpotential
7
Tungsten hair pin gun
•• TheThe electronselectrons areare initiallyinitially focusedfocused byby thethe WehneltWehnelt gridgrid cylindercylinder “cap”“cap”
whichwhich isis biasedbiased negativenegative atat --200200 toto --300300 VV withwith respectrespect toto thethe filamentfilament..
••
•• TheThe WehneltWehnelt reducesreduces thethe spacespace chargecharge (suppresses(suppresses emissionemission fromfrom thethe
filamentfilament exceptexcept atat itsits tips)tips)..
•• TheThe electronselectrons areare acceleratedaccelerated towardstowards thethe anodeanode ((1010--100100 µµmm inin
diameter)diameter)
•• TheThe electronselectrons convergeconverge atat aa pointpoint betweenbetween thethe WehneltWehnelt capcap andand anodeanode..
ThisThis pointpoint isis calledcalled thethe “cross“cross--over”over” andand isis thethe locationlocation ofof thethe effectiveeffective
electronelectron sourcesource
8
•• The anode has a hole in its centre and is biased from 1 to 50 keV with The anode has a hole in its centre and is biased from 1 to 50 keV with
respect to the filamentrespect to the filament--WehneltWehnelt
•• This bias accelerates the electrons and forms the beam. This bias accelerates the electrons and forms the beam.
•• The electron flux is minimal until the temperature of the filament is The electron flux is minimal until the temperature of the filament is
approximately 2500 K.approximately 2500 K.
•• Above this temperature it is predicted that the electron flux will increase Above this temperature it is predicted that the electron flux will increase
with increasing temperature, until the filament melts.with increasing temperature, until the filament melts.
•• In practice, however, the electron emission reaches a plateau termed In practice, however, the electron emission reaches a plateau termed
“saturation”, due to the self“saturation”, due to the self--biasing effects of the Wehnelt cap. biasing effects of the Wehnelt cap.
Oxidation
9
ELECTRON BEAM LOCATIONELECTRON BEAM LOCATION
•• Filament position is very importantFilament position is very important
•• Correct position optimises the electron flow Correct position optimises the electron flow
�� Less heat requiredLess heat required
�� Extended filament lifeExtended filament life
FILAMENT LIFEFILAMENT LIFE
•• Maintenance of high vacuumMaintenance of high vacuum
•• Cleanliness of the electron gunCleanliness of the electron gun
•• Filament currentFilament current
ACCELERATING VOLTAGEACCELERATING VOLTAGE
•• Voltage varies between 2 Voltage varies between 2 -- 30 KV30 KV
•• Electrons have energy of the Electrons have energy of the
accelerating voltageaccelerating voltage
•• at 25 KV, the energy of the at 25 KV, the energy of the
electrons = 25 eV. electrons = 25 eV.
2.2. ELECTROMAGNETIC LENSESELECTROMAGNETIC LENSES
• Electrons are negatively charged particles
� Path can be changed by a magnetic field
• Electron microscope lenses are essentially a coil of wire around a metal
cylinder, called solenoid.
• The electron path diversion depends on:
� magnetic field
� velocity
� direction
10
2.1.2.1. CONDENSER LENSESCONDENSER LENSES
•• TheThe electronelectron beambeam isis divergentdivergent afterafter
passingpassing throughthrough thethe anodeanode andand mustmust bebe
collimatedcollimated byby thethe condensercondenser lens(es)lens(es) andand
aperturesapertures intointo aa relativelyrelatively parallelparallel beambeam..
•• TheThe electronelectron beambeam convergesconverges andand passespasses
throughthrough aa focalfocal pointpoint (which(which movesmoves upup andand
downdown withwith thethe strengthstrength ofof thethe magneticmagnetic
field)field)
•• TheThe condensercondenser lenslens controlscontrols thethe amountamount ofof
currentcurrent thatthat passespasses downdown thethe restrest ofof thethe
microscopemicroscope columncolumn (controls(controls thethe intensityintensity
oror brightnessbrightness ofof thethe electronelectron beambeamElectromagnetic lensElectromagnetic lens
2.2. OBJECTIVE LENSES2.2. OBJECTIVE LENSES
•• TheThe objectiveobjective lenslens isis locatedlocated atat thethe basebase ofof thethe columncolumn justjust aboveabove thethe
samplesample..
•• ThisThis lenslens focusesfocuses thethe electronelectron beambeam ontoonto thethe samplesample andand controlscontrols itsits
finalfinal sizesize andand positionposition..
33.. SCANNINGSCANNING COILSCOILS
•• TheThe scanningscanning coilscoils areare housedhoused insideinside thethe objectiveobjective lenslens..
•• TheyThey causecause thethe beambeam toto scanscan overover thethe specimenspecimen surfacesurface inin anan
adjustableadjustable wayway..
11
4. ASTIGMATISM4. ASTIGMATISM
•• Astigmatism enlarges the effective beam size (spot size)Astigmatism enlarges the effective beam size (spot size)
•• The spot size may not be clear due to:The spot size may not be clear due to:
�� aberrationsaberrations
�� aperture contaminationaperture contamination
�� column contaminationcolumn contamination
•• StigmatorStigmator coilscoils housedhoused withinwithin thethe scanningscanning coilscoils consistconsist ofof aa setset ofofelectromagneticelectromagnetic lenseslenses thatthat controlcontrol thethe finalfinal beambeam shapeshape byby applyingapplying aamagneticmagnetic fieldfield toto makemake thethe beambeam circularcircular..
•• TheyThey alsoalso correctcorrect forfor anyany dirtydirty columncolumn oror aperturesapertures
12
44.. APERTURESAPERTURES
•• AperturesApertures areare usedused toto
�� reducereduce oror excludeexclude extraneousextraneous
electronselectrons
�� reducereduce aberrationsaberrations
SPECIMENSPECIMEN CHAMBERCHAMBER
•• HousesHouses thethe specimenspecimen andand thethe variousvarious
detectorsdetectors (SE,(SE, BSE,BSE, EDX,EDX, ……))
SPECIMENSPECIMEN STAGESTAGE
•• ThereThere areare fivefive typestypes ofof motionmotion (TXYZR)(TXYZR)
�� Tilt,Tilt, X,X, Y,Y, Z,Z, && RotationRotation
Large SEM specimen chamber
13
MAGNIFICATIONMAGNIFICATION
•• The mechanism by which the image is magnified is very simple and The mechanism by which the image is magnified is very simple and does not involve any lensesdoes not involve any lenses
•• The CRT area is fixed, and only the area scanned varies.The CRT area is fixed, and only the area scanned varies.
•• The magnification depends on the The magnification depends on the
�� Spot (beam) sizeSpot (beam) size
�� Area scannedArea scanned
•• The magnification The magnification M = the side length of the CRT / side length of the M = the side length of the CRT / side length of the scanned area. scanned area.
•• Magnification is proportional to the applied voltage (M Magnification is proportional to the applied voltage (M ↑↑ with with ↑↑ V)V)
•• Magnification is inversely proportional to the working distance (WD) (M Magnification is inversely proportional to the working distance (WD) (M ∝∝ 1/ WD)1/ WD)
14
Electron Beam Electron Beam –– Specimen InteractionSpecimen Interaction
•• As the beam strikes each point on the specimen, various responses are As the beam strikes each point on the specimen, various responses are
produced due to produced due to specimen specimen -- electron interactionselectron interactions. .
•• In almost all types of electron microscopes primary electrons enter the In almost all types of electron microscopes primary electrons enter the
specimen and the same or different electrons leave it again to form the specimen and the same or different electrons leave it again to form the
image.image.
•• Several of these responses can be collected by suitable detectors, Several of these responses can be collected by suitable detectors,
amplified and displayed in the CRT to form an image (or for chemical amplified and displayed in the CRT to form an image (or for chemical
analysis)analysis)
Incident Beam
SpecimenSpecimen
X-rays
• Through thickness
• Composition info
Auger electrons• Surface sensitive
• Composition information
Primary backscattered
electrons (BSE)
• Atomic number
• Topographical/ Imaging
Cathodoluminescence
Electrical information
Secondary electrons (SE)
Topographical/Imaging
Specimen current• Electrical current
The types of signals producedThe types of signals produced
15
Interaction VolumeInteraction Volume
•• Electron penetration volume and depth Electron penetration volume and depth
depend on:depend on:
–– Electron beam energyElectron beam energy
–– More energy, deeper penetration and More energy, deeper penetration and
larger interaction volumelarger interaction volume
–– Atomic number (Z) of specimenAtomic number (Z) of specimen
–– Higher Z, lower penetration and Higher Z, lower penetration and
volumevolume
Effect of accelerating voltage on size Effect of accelerating voltage on size
of interaction volume specimenof interaction volume specimen
Voltage decreases
16
Effect of atomic number on size of Effect of atomic number on size of
interaction volume specimeninteraction volume specimen
Z increases
High voltage
Low voltage
LOW ATOMIC NUMBER HIGH ATOMIC NUMBER
e-
e-e-
e-
e-
X-ray X-ray
17
Types of Electron ScatteringTypes of Electron Scattering
•• There are two types of electron scattering when the electron beam There are two types of electron scattering when the electron beam
strikes the specimen:strikes the specimen:
1.1. Elastic ScatteringElastic Scattering
�� Electrons Electrons retain retain all of their energy all of their energy -- backscattered electrons (BSE)backscattered electrons (BSE)
2.2. Inelastic ScatteringInelastic Scattering
�� Electrons Electrons loselose energy by interacting with the specimen energy by interacting with the specimen –– Secondary Secondary
electrons (SE) and Xelectrons (SE) and X--raysrays
SECONDARY ELECTRONS (SE)SECONDARY ELECTRONS (SE)
�� SESE havehave veryvery lowlow energyenergy (<(< 5050 eV)eV)comparedcompared toto 3030 KVKV ofof thethe electronelectronbeambeam
�� TheyThey areare traveltravel veryvery slowlyslowly asas theytheyleaveleave thethe specimenspecimen
�� TheThe SESE areare createdcreated throughoutthroughout thetheprimaryprimary excitationexcitation volume,volume, butbut ifif theytheyareare nearnear thethe surface,surface, theythey cancanescapeescape
�� SinceSince theythey havehave lowlow energy,energy, deeperdeeperonesones areare easilyeasily absorbedabsorbed (other(otherinteractions)interactions)
SE DetectorSE Detector
18
SECONDARY ELECTRONS DETECTIONSECONDARY ELECTRONS DETECTION
•• TheThe SESE areare detecteddetected byby aa detectordetector
knownknown asas thethe EverhartEverhart--ThornleyThornley
detectordetector ((19601960))..
•• ScintillatorScintillator
�� WhenWhen thethe ee-- strikestrike thethe scintillator,scintillator, itit
producesproduces lightlight
•• LightLight guideguide
�� TransportTransport lightlight toto PMTPMT
•• PhotomultiplierPhotomultiplier (PMT)(PMT)
�� AmplifyAmplify lightlight andand
�� ConvertConvert itit toto electricalelectrical signalsignal
Number of SE that escape from the sample Number of SE that escape from the sample
depends on the sample surfacedepends on the sample surface
Sample surface
19
BACKSCATTERED ELECTRON (BSE) BACKSCATTERED ELECTRON (BSE)
DETECTIONDETECTION
�� The BSE have energies > 50 eV The BSE have energies > 50 eV
�� They travel in straight linesThey travel in straight lines
�� They have weaker signal than SEThey have weaker signal than SE
�� They are detected by using purpose They are detected by using purpose
built backscattered electron built backscattered electron
detectors. detectors.
BSE DetectorBSE Detector
20
EFFECT OF MICROSCOPE VARIABLESEFFECT OF MICROSCOPE VARIABLES
Polymer Metal
21
EFFECT OF BEAM (SPOT) SIZE ON EFFECT OF BEAM (SPOT) SIZE ON IMAGEIMAGE QUALITYQUALITY
Better ResolutionBetter ResolutionPoorer ResolutionPoorer Resolution
Bigger spot (Beam) size Bigger spot (Beam) size
Smaller spot (Beam) size Smaller spot (Beam) size
22
Longer WD: poor resolution Longer WD: poor resolution
Shorter WD: better resolutionShorter WD: better resolution
23
24
�� Higher voltageHigher voltage will provide will provide better better
resolutionresolution (since high voltage generates (since high voltage generates
shorter wavelength of electrons)shorter wavelength of electrons)
�� However, higher voltage also causes an However, higher voltage also causes an
increase in the interaction volumeincrease in the interaction volume: this : this
will will reduce resolutionreduce resolution
Voltage and Resolution
25
�� Smaller electron beam angle Smaller electron beam angle increases increases the the
interaction volumeinteraction volume: thus : thus reducing reducing
resolutionresolution
Electron Beam Angle and Resolution
DEPTH OF FIELD (DOF)DEPTH OF FIELD (DOF)
�� The DOF is increased:The DOF is increased:
1.1. By reducing the final lens apertureBy reducing the final lens aperture
2.2. By increasing the working distance (lower the specimen: increase By increasing the working distance (lower the specimen: increase
the distance between the final lens and the specimen)the distance between the final lens and the specimen)
26
Increasing the DOF by reducing the Increasing the DOF by reducing the final lens aperturefinal lens aperture
Increasing the DOF by increasing the WDIncreasing the DOF by increasing the WD
Aperture size vs. Resolution and DOFAperture size vs. Resolution and DOF
WD vs. Resolution and DOFWD vs. Resolution and DOF
27
Filament Filament -- DOFDOF Filament Filament -- ResolutionResolution
VARIABLE PRESSURE DETECTOR VARIABLE PRESSURE DETECTOR (VPSE)(VPSE)
�� VariableVariable pressurepressure technologytechnologyenablesenables investigatinginvestigating nonnon--conductingconductingspecimensspecimens withoutwithout priorprior preparationpreparation
VPSE DetectorVPSE Detector
28
NonNon--conducting material: conducting material:
charging effect, difficult to imagecharging effect, difficult to image
VariableVariable PressurePressure TechnologyTechnology::
TheThe VPVP systemsystem operatesoperates toto
neutraliseneutralise thethe surfacesurface byby emittingemitting
aa gasgas intointo thethe samplesample chamberchamber
SEM with VPSE detectorSEM with VPSE detector
29
SPECIMEN PREPARATION FOR SEMSPECIMEN PREPARATION FOR SEM
•• Image quality can be limited by specimen preparationImage quality can be limited by specimen preparation
•• There are 3 requirements for preparing specimens for SEMThere are 3 requirements for preparing specimens for SEM
1.1. Remove all water, solvents, or other materials that could evaporate Remove all water, solvents, or other materials that could evaporate while in the vacuumwhile in the vacuum
2.2. Firmly mount the specimenFirmly mount the specimen
3.3. NonNon--metallic samples (nonmetallic samples (non--conductive) should be coated so they conductive) should be coated so they are electrically conductive. Metallic samples can be directly placed are electrically conductive. Metallic samples can be directly placed into the SEM. (noninto the SEM. (non--conducting materials will lead to charging: conducting materials will lead to charging: deflection of SE, beam deflection and SE burstsdeflection of SE, beam deflection and SE bursts))
Note: conditions 1 & 3 are valid for conventional SEM’s onlyNote: conditions 1 & 3 are valid for conventional SEM’s only
Gold Sputtering MachineGold Sputtering Machine