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Improvements in the X Improvements in the X - - ray characterisation of ray characterisation of electroceramic electroceramic thin films thin films by the application by the application of a of a novel combined analysis novel combined analysis procedure procedure J. J. Ricote Ricote ICMM ICMM - - CSIC. (Spain) CSIC. (Spain) D. D. Chateigner Chateigner CRISMAT CRISMAT - - ENSICAEN (France) ENSICAEN (France) L. L. Lutterotti Lutterotti Università Università di Trento di Trento (Italy) (Italy) Dr. J. Dr. J. Ricote Ricote Ferroelectric Materials Department Materials Science Institute of Madrid Spanish Council of Scientific Research
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  • Improvements in the XImprovements in the X--ray characterisation of ray characterisation of

    electroceramicelectroceramic thin filmsthin films by the applicationby the application of a of a

    novel combined analysisnovel combined analysis procedureprocedureJ. J. RicoteRicote ICMMICMM--CSIC. (Spain)CSIC. (Spain)

    D. D. ChateignerChateigner CRISMATCRISMAT--ENSICAEN (France)ENSICAEN (France)

    L. L. LutterottiLutterotti UniversitàUniversità di Trentodi Trento (Italy)(Italy)

    Dr. J. Dr. J. RicoteRicote

    Ferroelectric Materials DepartmentMaterials Science Institute of Madrid Spanish Council of Scientific Research

  • OUTLINEOUTLINE

    Introduction Introduction Ferroelectric thin films and textureFerroelectric thin films and textureCombined method of XCombined method of X--ray diffraction analysisray diffraction analysis

    Results of the analysis of ferroelectric thin films with Results of the analysis of ferroelectric thin films with the combined method the combined method

    Separation of the contribution of different texture Separation of the contribution of different texture components.components.Simultaneous texture and structure determination Simultaneous texture and structure determination of substrate and film.of substrate and film.

    ConclusionsConclusions

    Ferroelectric Materials Department

  • The figures of merit that determine the efficiency of ferroelectric materials in technological applications (i.e. piezoelectric coefficient in MEMS) strongly depends on the net polarization of the materialThe polarization value depends on several factors, among them: TEXTURE. Preferential orientation along the polar axis produces an improved ferroelectric behaviour

    Improvement of performance by texture Improvement of performance by texture control in ferroelectric thin films control in ferroelectric thin films

    Ferroelectrics are polar dielectrics in which the direction of polarization can be re-oriented by application of an electric field.

    Ferroelectrics are polar dielectrics in which the direction of polarization can be re-oriented by application of an electric field.

    In general, the polycrystalline ferroelectric materials need a Poling process with an intense electric field, in order to obtain any spontaneous polarization. This is not needed in highly textured thin films along the polar axis

    Ferroelectric Materials Department

  • Generation of a pole figureGeneration of a pole figure

    XX--rayray

    χχSampleSample

    ϕϕ

    ωω

    25.72

    1 m.r.d.

    0

    (111) ϕ

    χ0 90

    m.r.d. = multiple of a random distribution

    (a sample without any preferred orientation shows pole figures with

    constant values of 1 m.r.d.)

    Pole figurePole figure

    ω = 20°

    χ

    60°

    Refinement of individual spectraRefinement of individual spectra

    Ferroelectric Materials Department

  • Equipment used for pole figure measurementsEquipment used for pole figure measurements

    DIFFRACTOMETER EQUIPED WITH:• Four-circle goniometer

    • Curve position sensitive detector (PSD)

    (MDM-Italy; developed in the ESQUI project)

    European-GROWTH project“x-ray Expert System for electronic films QUalityImprovement-ESQUI”

    Ferroelectric Materials Department

  • Advanced texture determination: Advanced texture determination: Quantitative Texture AnalysisQuantitative Texture Analysis

    11.54

    1 m.r.d.

    0.01

    From the experimental pole figures we obtain by an iterative process anORIENTATION DISTRIBUTION FUNCTION (ODF)

    Recalculated pole figures from ODF

    Experimental pole figures (incomplete)f(g); g = α,β,γ

    Ferroelectric Materials Department

  • Quantitative Texture AnalysisQuantitative Texture Analysis

    [ ] ii

    i ggfF ∆= ∑ 222 )(81π

    Orientation Distribution Function (ODF)

    Texture Index (F2) Inverse pole figures(degree of orientation) (texture components)

    PZTp252b PZTp252c

    110

    101

    011

    010

    001 100

    111

    1 m.r.d.

    0.01

    32.07

    Inverse pole figure:It describes the densities for crystal directions falling into the fixed sample direction y.

    Contributions of the different components can be estimated

    Ferroelectric Materials Department

  • Quantitative Texture Analysis of polycrystalline Quantitative Texture Analysis of polycrystalline ferroelectric thin filmsferroelectric thin films

    Ferroelectric Materials Department

    Thickness dependence of texture

    0

    1 m.r.d.

    25.72

    PTL-1 PTL-3 PTL-5

    110 nm 250 nm 370 nm

    Similar contribution of the texture components(mixed and orientation)

    0

    2

    4

    6

    8

    10

    12 direct insertion

    Text

    ure

    inde

    x (m

    .r.d.

    2 )

    0 1 2 3 4 50

    2

    4

    6

    8

    10

    12

    number of layers

    RTP layer-by-layer

    Thickness effect disappears with the layer-by-layer crystallizationPTL on Pt/TiO2/(100)Si

    *PTL: Lanthanum modified lead titanate

    J. Ricote et al. J. Am. Ceram. Soc., 86 [9], 1571-77 (2003)

  • Deduction of effective physical propertiesDeduction of effective physical properties

    Ferroelectric Materials Department

    *PTL: Lanthanum modified lead titanate

    GPax /10

    6.90000005.140000005.140000003.331.71.70001.75.635.00001.735.05.6

    3−

    −−−−−−

    S =

    Geometric mean

    PTL on Ti/Pt/Ti/(100)SiMixed and, orientation

    PTL on Pt/TiO2/(100)Si Mixed , orientation

    GPax /10

    3.130000009.120000009.120000003.104.34.30004.31.102.30004.32.31.10

    3−

    −−−−−−

    GPax /10

    2.130000002.130000003.130000009.92.32.30002.39.92.30002.32.39.9

    3−

    −−−−−−

    Elastic properties of tetragonal PbTiO3 single crystalKalinichev et al. J. Mater. Res. 12, 2623 (1997)

    Sc =

    J. Ricote et al. Mat. Sci. Forum 426-432, 3433-38 (2003)

  • Further advances in XFurther advances in X--ray characterisation: ray characterisation: Combined analysisCombined analysis

    RESIDUAL STRESSStress distribution function

    Stress analysis

    Rietveld refinement

    LATTICEPARAMETERS

    Software used is MAUD

    General purpose program for diffraction spectra fitting developed by L.Lutterotti. http://www.ing.unitn.it/~luttero/maud/

    Generally, labs perform a partial determination of these parameters

    It allows a simultaneous and more precise determination of parameters

    INTEGRATED INTENSITIES

    Iterative process WIMV

    Orientation Distribution Function

    Ferroelectric Materials Department

  • RESULTS OF THE APPLICATION RESULTS OF THE APPLICATION OF THE COMBINED METHODOF THE COMBINED METHOD

    Limitations of the simple Quantitative Texture Analysis (I)Limitations of the simple Quantitative Texture Analysis (I)

    21.0 21.5 22.0 22.5 23.0 23.5 24.0 24.5

    0

    2

    4

    6

    8

    10

    12

    14

    16

    18

    20

    001

    100

    PCT thin film on MgO based substrate

    PCT thin film on Si based substrate

    Bulk PCT ceramic

    Inte

    nsity

    (a.u

    .)

    2θ (º)

    Ferroelectric Materials Department

    We need to know the lattice parameters prior to the texture analysis

    PCT thin films on Pt/TiO2/(100)Si:

    a = ? Åc = ? Å

    Lattice parameters are affected by STRESS in thin films

    Ca modified lead titanates (PCT):

    a = 3.8939 Åc = 4.0496 Å

    (bulk ceramic values JCPDS 39-1336)

  • 20 25 30 35 40 45 50 55 600

    5

    10

    15

    20

    25

    30

    112211

    102201210

    002, 200200-Pt

    111111-Pt

    100

    101,110

    001In

    tens

    ity (a

    .u.)

    2θ (º)

    PCT thin film

    We need a simultaneous analysis of texture and structure of both film and substrate to

    solve completely the texture of the films Ferroelectric Materials Department

    TEXTURE effects:peaks that do not appear at low χ angles

    Pt reflections

    Substrate influence:overlapping of reflections from the film and the substrate

    Limitations of the simple Quantitative Texture Analysis (II)Limitations of the simple Quantitative Texture Analysis (II)

    Structural parameters are difficult to obtain due to:

  • Separation of the contribution of texture contributionsSeparation of the contribution of texture contributions(simple Quantitative Texture Analysis)

    20 22 24 260

    20

    40

    60

    80

    100

    120

    χ = 20º

    χ = 15º

    χ = 5º

    χ = 0º

    χ =10º

    Inte

    nsity

    (a.u

    .)

    2θ (º)

    20 22 24 260

    20

    40

    60

    80

    100

    χ = 10º

    χ = 15º

    χ = 5º

    χ = 0º

    Inte

    nsity

    (a.u

    .)

    2θ (º)

    PCT/Pt/MgOPCT/Pt/MgO orientation orientation

    orientation orientation

    001 100

    (simple Quantitative Texture Analysis)

    χ = 20º001 100PCT/Pt/TiO2/SiPCT/Pt/TiO2/Si PCT film under tensile stress:

    σ = +1182 Mpa

    PCT film under compressive stress:σ = -700 Mpa

    QTA results:Estimated contribution

    texture components.

    62%!!62%!! 38%!!38%!!

    QTA results:Estimated contribution

    texture components

    55%!!55%!! 45%!!45%!!

    Ferroelectric Materials Department

  • Separation of the contribution of texture contributionsSeparation of the contribution of texture contributions(Combined Method)(Combined Method)

    Ferroelectric Materials Department

    QTA results:

    Estimated contrib.

    c = 3.877 Åc = 3.877 Åa = 3.977 Åa = 3.977 Å 7%7% 93%93%

    PCT/Pt/TiO2/SiPCT/Pt/TiO2/Si

    PCT/Pt/MgOPCT/Pt/MgOc = 3.883 Åc = 3.883 Åa = 4.020 Åa = 4.020 Å 68%68% 32%32%

    Instead of the integration of the overlapped peak (“integral approach”), and separating both contributions during the WIMV process, the combined method allows to deconvolute the peaks first, before the ODF calculation starts. As a result a more correct estimation of the contributions of and contributions is possible.

    PyroelectricCoefficient(10-8 C cm-2 K-1)

    σ = +1182 MPa0.3

    1.5σ = -700 MPa

    Simultaneously, we observe the effect of the applied stress on the lattice parameters

  • SimultaneousSimultaneous texture determination of substrate and filmtexture determination of substrate and film(Combined Method)(Combined Method)

    0.01

    75

    1 m.r.d.

    Texture indexF2 (mrd2) R factors (%)

    non-treated substratePt 129 RW=13, RB=12annealed substratePt 199 RW=8, RB=14Pt (Recryst. 1h) 199 RW=9, RB=20Pt (Recryst. 2h) 195 RW=9, RB=14Pt (Recryst. 3h) 222 RW=27, RB=12

    Ferroelectric Materials Department

    Pt layer fibre orientation

    Pt layer fibre orientation

    Annealing of the substrate, which involves crystal growth, results in an increase of the degree of orientation of the Pt layer.

    New information on the Pt layer provided by the combined method

  • Texture determination of filmTexture determination of film(Combined Method)(Combined Method)

    1 m.r.d.

    0.01

    9.5

    Texture indexF2 (mrd2)

    non-treated substratePTC 5.2

    annealed substratePTC 2.1 PTC (Recryst. 1h) 2.1 PTC (Recryst. 2h) 2.5 PTC (Recryst. 3h) 2.5

    PCT filmPCT film

    Effect on the degree of orientation of the PCT film

    PCT film on untreated substrateStrong orientation

    5.8

    1 m.rd.

    0.04

    PCT film on annealed substrateStrong orientation

    Effect of the annealing of the substrate in the type of texture developed Ferroelectric Materials Department

    New information on contribution of texture components provided by the combined method

    Small texture contribution not observed by conventional QTA

  • CONCLUSIONSCONCLUSIONS

    The application of the combined method to ferroelectric calcium modified lead titanate thin films has proved to produce more accurate and reliable results than more traditional X-ray diffraction analysis approaches. It also provides simultaneously information on the structure, microstructure and texture of both the deposited film and the substrate, revealing important characteristics of the Pt layer used in this study as bottom electrode.

    An important aspect covered is the better resolution of the texture and, specifically of the contribution of the different texture components, obtained by the combined method. We have shown two examples:

    Separation of , componentsReveal of small texture component

    Ferroelectric Materials Department

    see also:J. Ricote and D. Chateigner J. Appl. Cryst. 37, 91-95 (2004) J. Ricote et al. Thin Solid Films 450, 128-133 (2004)

  • AcknowledgementsAcknowledgements

    European-GROWTH project (G6TD-CT99-00169)“x-ray Expert System for electronic films QUality Improvement-ESQUI”

    CSIC-CNRS collaboration projects

    Advanced fellowship “Ramón y Cajal”

    Additional funding:

    Delegation Regionale a la Recherche et a la Technologie de Basse Normandie

    COST Action 528Chemical Solution Deposition of Thin Films


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