q
play

Q UANTITATIVE TEXTURE OF OF FERROELECTRIC MODIFIED LEAD ED LEAD - PowerPoint PPT Presentation

Q UANTITATIVE TEXTURE Q UANTITATIVE TEXTURE OF OF FERROELECTRIC MODIFIED LEAD ED LEAD FERROELECTRIC MODIFI TITANATE THIN FILMS TITANATE THIN FILMS J. Ricote, D. Chateigner, L. Pardo , M. Alguer , J. Mendiola , M.L. Calzada


  1. Q UANTITATIVE TEXTURE Q UANTITATIVE TEXTURE OF OF FERROELECTRIC MODIFIED LEAD ED LEAD FERROELECTRIC MODIFI TITANATE THIN FILMS TITANATE THIN FILMS J. Ricote, D. Chateigner, L. Pardo † , M. Algueró ‡ , J. Mendiola † , M.L. Calzada † Laboratoire de Physique de l'Etat Condensé. Université du Maine-Le Mans (FRANCE) † Instituto de Ciencia de Materiales de Madrid. CSIC. (SPAIN) ‡ Queen Mary and Westfield College, Univ. of London (UK)

  2. WHY TEXTURE STUDIES IN FERROELECTRIC THIN WHY TEXTURE STUDIES IN FERROELECTRIC THIN FILMS ? FILMS ? F ERROELECTRICS : ❖ Polar materials ❖ Characterised by a spontaneous electric polarisation ❖ The polarisation can be inverted by the application of an electric field ð H YSTERESIS LOOPS . P OLAR AXIS for tetragonal compositions is [001] In polycrystalline materials a P OLING PROCESS (application of a strong electric field) is required to obtain spontaneous polarisation.

  3. Polycrystalline thin films showing a preferred orientation with the polar axis perpendicular to the film: Ä DO NOT REQUIRE THE POLING PROCESS Ä HAVE AN IMPROVED FERROELECTRIC BEHAVIOUR F F A THOROUGH TEXTURE CHARACTERISATION IS NEEDED : FOR THE CONTROL AND OPTIMISATION OF THE PREPARATION PROCESS OF HIGHLY ORIENTED FERROELECTRIC THIN FILMS REQUIRED FOR APPLICATIONS . F F U NTIL RECENTLY QTA HAVE NOT BEEN CARRIED OUT IN THIN FILMS OF FERROELECTRICS Chateigner et al., Int. Ferro. 19, 1998, 121 Bornand et al., Int. Ferro. 19, 1998, 1 CORRELATION WITH PHYSICAL PROPERTIES NEITHER

  4. MODIFIED LEAD TITANATE THIN FILMS MODIFIED LEAD TITANATE THIN FILMS - interesting piezo and pyroelectric properties - suitable for infrared sensors and electromechanical applications. F ILMS WERE OBTAINED BY SOL - GEL PROCESSING AND DEPOSITION BY SPIN - COATING PTL ð Pb 0.92 La 0.08 TiO 3 (20% PbO excess) PTC ð Pb 0.76 Ca 0.24 TiO 3 (10% PbO excess) S AMPLE S UBSTRATE N UMBER A NNEALING CONDITIONS LAYERS H EAT . RATE T EMP -- TIME PTL-4c Pt/TiO 2 /Si (100) 4 10ºC/min 650°C--12 min PTL-1 to 5 Pt/TiO 2 /Si (100) 1-5 >500°C/min 650°C--12 min PTC-Si Pt/TiO 2 /Si (100) 1 30ºC/s 650°C--50 s PTC-Mg Pt/MgO (100) 2 30ºC/s 700°C--50 s PTC-Sr Pt/SrTiO 3 (100) 2 30ºC/s 700°C--50 s

  5. QUANTITATIVE TEXTURE ANALYSIS QUANTITATIVE TEXTURE ANALYSIS ❖ Experimental X-ray POLE FIGURES : - asymmetric reflection mode (Cu K α radiation) - 4-circle goniometer with Euler cradle + PSD CPS-120

  6. Intensity ❖ Corrections for asymmetry, volume/absorption ❖ Scans: 5° x 5° grid, at incidence ω = 11°: sum diagrams 1000 2000 3000 4000 5000 6000 0 20 001/100 25 TiO 2 30 101/110 35 111 + 111-Pt 40 45 Heizmann et al., J. Appl. Cryst. 19 (1986) 467 002/200 +200-Pt + 220 Si 50 102/201/210 2 θ ( 0 ) 55 112/211 + 311-Si 60 65 202/220 +220-Pt + 400-Si 70 75 PTC ω = 11 0 PTC-452 103/301 + 311-Si 80 113/311 + 311-Pt 85 222 + 222-Pt 90 Intensity (a.u.) 1000 2000 3000 4000 5000 6000 0 20 001/100 25 TiO 2 30 101/110 35 111 + 111-Pt 40 45 002/200 +200-Pt + 220-Si 50 102/201/210 2 θ (°) 55 112/211 + 311-Si 60 65 400-Si + 220-Pt 70 221/103/300 PTL PTL-3 75 310 + 331-Si 80 311 + 311-Pt 85 222 + 222-Pt 90

  7. ❖ Cyclic integration of {100/001}, {101/110}, {102/201/210}, {112/211} and {221/103/300} overlaps ❖ Corrections for location Bunge et al., Text. Micr. 5 (1982) 153 ❖ ORIENTATION DISTRIBUTION (OD) refinement - WIMV algorithm (BEARTEX) - crystal symmetry: tetragonal, PTL: 3.93 Å x 4Å sample triclinic PTC: 3.89 Å x 4.04 Å - pole figure ranges: 100/001: 0-70 101/110: 5-70 102/201/210: 15-70 112/211: 35-70 (substrate) 221/103/300: 25-70 - Overlaps: as for the powder

  8. OD- -RELIABILITY RELIABILITY OD Separation of tetragonal peaks appeared better than a cubic perovskite-like refinement 23 Hopefully !! ⇓ {100} vs {001} separation 1 mrd ⇓ polarisation 0.3

  9. PTL S INVERSE POLE FIGURE ( NORMAL TO THE FILM ) PTL S INVERSE POLE FIGURE ( NORMAL TO THE FILM ) PTL-4c PTL-1 PTL-2 PTL-3 PTL-4 PTL-5

  10. PTL S INVERSE POLE FIGURE ( NORMAL TO THE FILM ) PTL S INVERSE POLE FIGURE ( NORMAL TO THE FILM ) PTC-Si PTC-Mg 49.16 1 mrd PTC-Sr 0

  11. RESULTS FOR PTL THIN FILMS FILMS RESULTS FOR PTL THIN Sample Thickness Components Texture RP0 RP1 Remanent of texture index polarisation (m.r.d. 2 ) ( µ C cm -2 ) (nm) (%) (%) ð low heat. PTL-4c 485 weak <110>,<101> 1.3 14 10 13.8 rate PTL-1 130 <001>,<100> 10.5 36 16 -- ð affected by leakage weak <221> PTL-2 210 <001>,<100> 7.5 24 19 7.4 weak <221> PTL-3 420 <001>,<100> 6.2 22 16 27 F 2 ➘ weak <221> with PTL-4 500 <001>,<100> 4.6 18 12 19 thickness weak <221> . PTL-5 560 <001>,<100> 3.9 19 15 10.7 weak <221> High heating rates results in stronger textures .

  12. RESULTS FOR PTC THIN FILMS FILMS RESULTS FOR PTC THIN Sample Components Texture RP0 RP1 Pyroelectric coef. of texture index γ S γ P (m.r.d. 2 ) (%) (%) spontaneous poled (8V) (10 -8 C cm -2 K -1 ) Less PTC-Si weak <001>,<100> 2.4 23 12 0.28 2.5 textured <110>,<101> Pt/TiO 2 /Si films are easier to PTC-Mg <001>,<100> 5.2 22 10 1.5 3.2 pole Pt/MgO weak <111> PTC-Sr <001>,<100> 32.1 26 24 1.1 2.0 Pt/SrTiO 3 Poled values are not ò Substrate: determinant retained with time components factor of the final texture . contribution

  13. RECALCULATED POLE FIGURES OF PTL THIN GURES OF PTL THIN RECALCULATED POLE FI FILMS FILMS 25.72 Similar contribution 1 m.r.d. of texture components 0 Thickness é Texture index ê Polar axis contribution ê PTL-1 PTL-3 PTL-5 (<001>) Spontaneous polarisation ê

  14. RECALCULATED POLE FIGURES OF PTC THIN GURES OF PTC THIN RECALCULATED POLE FI FILMS FILMS PTC-Mg 50.77 1 m.r.d. PTC-Sr 0 <100> contribution é Strong contribution ( ⊥ polar axis and of <100> non –contributing to component polarisation) Spontaneous polarisation ê Spontaneous pyroelectricity ê

  15. THICKNESS EFFECTS ON TEXTURE AND THICKNESS EFFECTS ON TEXTURE AND PROPERTIES PROPERTIES T HE USE OF A HIGH HEATING RATE ENHANCES THE APPEARANCE OF PREFERENTIAL ORIENTATION . During slow heating several variants of texture can be nucleated, resulting in a random thin film. A S THE NUMBER OF LAYERS INCREASES THE TEXTURE INDEX DECREASES . T HIS SEEMS TO INDICATE HETEROGENEOUS NUCLEATION , I . E ., WHEN CRYSTALS NUCLEATE IN SITES THROUGHOUT THE THICKNESS OF THE FILM . Except for the very thin PTL-1 and PTL-2 films, which present high leakage currents, the remanent polarisation decreases as the texture strength of the film decreases. An increase of the texture index involves in this case a higher fraction of crystals oriented with the polar axis, <001>, perpendicular to the film surface. The largest contribution to the net polarisation comes from these crystals. Therefore, there is an increase of the polarisation of the film.

  16. T HE INCREASE OF THE FILM THICKNESS BY INCREASING THE NUMBER OF DEPOSITED LAYERS LEADS TO A DECREASE OF THE TEXTURE STRENGTH THAT RESULTS IN A REDUCTION OF THE REMANENT POLARISATION .

  17. SUBSTRATE EFFECTS ON TEXTURE AND TEXTURE AND SUBSTRATE EFFECTS ON PROPERTIES PROPERTIES - DIFFERENT SUBSTRATES LEAD TO : DIFFERENT OVERALL DEGREE OF ORIENTATION DIFFERENT CONTRIBUTIONS FROM <100> AND <001> COMPONENTS U SE OF THE TRADITIONAL P T /T I O 2 /S I SUBSTRATE RESULTS IN : WEAKLY TEXTURED FILMS LOW SPONTANEOUS PYROELECTRIC COEFFICIENTS - PTC-Sr: largest <100> ⊥ component: lowest PYROELECTRIC COEFFICIENTS T HE USE OF A P T /S R T I O 3 SUBSTRATE , COMPARED TO P T /M G O, PRODUCES HIGHLY TEXTURED FILMS , BUT WITH A STRONG CONTRIBUTION FROM CRYSTALS WHOSE POLAR AXIS IS IN THE PLANE OF THE FILM , WHICH REDUCES THE SPONTANEOUS PYROELECTRIC COEFFICIENTS OF THE FILMS .

  18. SUMMARY SUMMARY A QUANTITATIVE TEXTURE ANALYSIS HAS BEEN CARRIED OUT FOR THE FIRST TIME ON SEVERAL FERROELECTRIC THIN FILMS OF MODIFIED LEAD TITANATE . The effects of different processing parameters on the final texture have been studied: F rapid thermal annealing gives highly texture films F heterogeneous nucleation of the perovskite: for higher thicknesses, lower texture strengths F choice of substrate: determinant factor for texture, then properties Remanent polarisation and pyroelectric coefficients can be correlated to the texture strength and the contribution of the different texture components. A CKNOWLEDGEMENTS A CKNOWLEDGEMENTS Grant awarded by the regional government of Pays de Loire and the French Education Ministry Work financed by projects MAT98-1068 (Spanish CICYT) and COPERNICUS CIPA-CT94-0236 Declared of technological interest by the EU COST514 action on ferroelectric thin films.

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend