Towards the limit of ferroelectric nanosized grains

被引:68
作者
Roelofs, A [1 ]
Schneller, T
Szot, K
Waser, R
机构
[1] Rhein Westfal TH Aachen, Inst Werkstoffe Elecktrotech, D-52056 Aachen, Germany
[2] Forschungszentrum Julich, Inst Festkorperforsch, D-52425 Julich, Germany
关键词
D O I
10.1088/0957-4484/14/2/328
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Ferroelectric random access memories are non-volatile, low voltage, high read/write speed devices which have been introduced into the market in recent years and which show the clear potential of future gigabit scale universal non-volatile memories. The ultimate limit of this concept will depend on the ferroelectric limit (synonymous superparaelectric limit), i.e. the size limit below which the ferroelectricity is quenched. While there are clear indications that 2D ferroelectric oxide films may sustain their ferroelectric polarization below 4 nm in thickness (Tybell T, Ahn C H and Triscone J M 1999 Appl. Phys. Lett. 75 856), the limit will be quite different for isolated 3D nanostructures (nanograins, nanoclusters). To investigate scaling effects of ferroelectric nanograins on Si wafers, we studied PbTiO3 (PTO) and Pb(ZrxTi1-x)O-3 grown by a self-assembly chemical solution deposition method. Preparing highly diluted precursor solutions we achieved single separated ferroelectric grains with grain sizes ranging from 200 nm down to less than 20 nm. For grains smaller than 20 nm, no piezoresponse was observed and we suppose this could be due to the transition from the ferroelectric to the paraelectric phase which has no spontaneous polarization. Recent calculations (Zhong W L, Wang Y G, Zhang P L and Qu B D 1994 Phys. Rev. B 50 698) and experiments (Jiang B, Peng J L, Zhong W L and Bursill L A 2000 J. Appl. Phys. 87 3462) showed that the ferroelectricity of fine ferroelectric particles decrease with decreasing particle size. From these experiments the extrapolated critical size of PTO particles was found to be around 4.2-20 nm.
引用
收藏
页码:250 / 253
页数:4
相关论文
共 26 条
[1]   Mapping the domain distribution at ferroelectric surfaces by scanning force microscopy [J].
Abplanalp, M ;
Eng, LM ;
Gunter, P .
APPLIED PHYSICS A-MATERIALS SCIENCE & PROCESSING, 1998, 66 (Suppl 1) :S231-S234
[2]   Nanoscale scanning force imaging of polarization phenomena in ferroelectric thin films [J].
Auciello, O ;
Gruverman, A ;
Tokumoto, H ;
Prakash, SA ;
Aggarwal, S ;
Ramesh, R .
MRS BULLETIN, 1998, 23 (01) :33-42
[3]  
BINNIG G, 1982, HELV PHYS ACTA, V55, P726
[4]  
Bolten D, 1999, FERROELECTRICS, V225, P923, DOI 10.1080/00150199908009118
[5]  
BOTTGER U, 2003, IN PRESS NANOELECTRO
[6]   SIZE-INDUCED DIFFUSE PHASE-TRANSITION IN THE NANOCRYSTALLINE FERROELECTRIC PBTIO3 [J].
CHATTOPADHYAY, S ;
AYYUB, P ;
PALKAR, VR ;
MULTANI, M .
PHYSICAL REVIEW B, 1995, 52 (18) :13177-13183
[7]   Ferroelectric domain switching in tri-glycine sulphate and barium-titanate bulk single crystals by scanning force microscopy [J].
Eng, LM ;
Abplanalp, M ;
Guner, P .
APPLIED PHYSICS A-MATERIALS SCIENCE & PROCESSING, 1998, 66 (Suppl 1) :S679-S683
[8]   Nanoscale reconstruction of surface crystallography from three-dimensional polarization distribution in ferroelectric barium-titanate ceramics [J].
Eng, LM ;
Güntherodt, HJ ;
Schneider, GA ;
Köpke, U ;
Saldaña, JM .
APPLIED PHYSICS LETTERS, 1999, 74 (02) :233-235
[9]   MODIFICATION AND DETECTION OF DOMAINS ON FERROELECTRIC PZT FILMS BY SCANNING FORCE MICROSCOPY [J].
FRANKE, K ;
BESOLD, J ;
HAESSLER, W ;
SEEGEBARTH, C .
SURFACE SCIENCE, 1994, 302 (1-2) :L283-L288
[10]   Role of 90° domains in lead zirconate titanate thin films [J].
Ganpule, CS ;
Nagarajan, V ;
Li, H ;
Ogale, AS ;
Steinhauer, DE ;
Aggarwal, S ;
Williams, E ;
Ramesh, R ;
De Wolf, P .
APPLIED PHYSICS LETTERS, 2000, 77 (02) :292-294