Growth and study of antiferroelectric lead zirconate thin films by pulsed laser ablation

1999 ◽  
Vol 86 (10) ◽  
pp. 5862-5869 ◽  
Author(s):  
S. S. N. Bharadwaja ◽  
S. B. Krupanidhi
1999 ◽  
Vol 14 (3) ◽  
pp. 940-947 ◽  
Author(s):  
Sucharita Madhukar ◽  
S. Aggarwal ◽  
A. M. Dhote ◽  
R. Ramesh ◽  
S. B. Samavedam ◽  
...  

We report on the feasibility of using molybdenum silicide as a conducting barrier for integration of ferroelectric lead zirconate titanate capacitors on Si. Thin films of MoSi2 were deposited by pulsed laser-ablation deposition (PLD). The silicide films showed a structural transition from amorphous to orthorhombic to tetragonal phase as the temperature of deposition was changed from room temperature to 900 °C. The four-probe resistivity and surface roughness of the films decreased with an increase in the deposition temperature and crystallinity of the phase. Ferroelectric (La, Sr)CoO3/Pb(Nb, Zr, Ti)O3/(La, Sr)CoO3 capacitors were grown on Si/poly Si/MoSi2, and Si/poly Si/MoSi2/Pt structures. Transmission electron microscopy (TEM) studies of the MoSi2/LSCO and MoSi2/Pt/LSCO heterostructures indicated the formation of a thin layer of SiO2. In the case of Pt/MoSi2, Pt reacts with the silicide and forms PtSi, consuming the entire platinum layer and, thus, makes it unsuitable as a composite barrier. Electrical testing of the LSCO/PNZT/LSCO capacitors through capacitive coupling showed desirable ferroelectric properties on these substrates.


1994 ◽  
Vol 361 ◽  
Author(s):  
Jyrki Lapp Alainen ◽  
Johannes Frantti ◽  
Seppo Leppävuori

ABSTRACTPulsed laser ablation was used to deposit Nd-doped lead zirconate titanate (PZT) thin films with a thickness of from 100 to 800 nm from a Pb0.97 Nd0.02(Zr0.55Ti0.45)O3 target. The films were ablated onto sapphire and MgO substrates using a XeCl excimer laser (pulse energy 50 mJ, wavelength 308 nm, pulse duration 20 ns). The distance between the target and the substrates was 40 mm, and the angle between the target normal and the incident beam was 45 °. The films were post-annealed in air at various temperatures (600 – 900 °C) with PZT powder. It was found that the laser beam energy density on the surface of the target had a significant effect on the composition of the films, the number of particulates on the surface of the films and the growth rates of the films. Lead deficiency was found in the films in the case of high fluence (> 1.5 J/cm2) while low fluence values (< 1.0 J/cm2) gave an excess of lead and too low Zr/(Zr+Ti) ratios. The particulate number density was low for fluence values between 0.5 and 1.5 J/cm2. EDS and X-ray diffraction was used to determine the composition and the crystal structure of the annealed films. The films deposited using a low fluence showed increasing tetragonal c/a-ratio with increasing post-annealing temperatures. Raman spectra measured from annealed films were found to be typical of PZT.


Author(s):  
M. Grant Norton ◽  
C. Barry Carter

Pulsed-laser ablation has been widely used to produce high-quality thin films of YBa2Cu3O7-δ on a range of substrate materials. The nonequilibrium nature of the process allows congruent deposition of oxides with complex stoichiometrics. In the high power density regime produced by the UV excimer lasers the ablated species includes a mixture of neutral atoms, molecules and ions. All these species play an important role in thin-film deposition. However, changes in the deposition parameters have been shown to affect the microstructure of thin YBa2Cu3O7-δ films. The formation of metastable configurations is possible because at the low substrate temperatures used, only shortrange rearrangement on the substrate surface can occur. The parameters associated directly with the laser ablation process, those determining the nature of the process, e g. thermal or nonthermal volatilization, have been classified as ‘primary parameters'. Other parameters may also affect the microstructure of the thin film. In this paper, the effects of these ‘secondary parameters' on the microstructure of YBa2Cu3O7-δ films will be discussed. Examples of 'secondary parameters' include the substrate temperature and the oxygen partial pressure during deposition.


2001 ◽  
Vol 177 (1-2) ◽  
pp. 73-77 ◽  
Author(s):  
K.T Hillie ◽  
C Curren ◽  
H.C Swart

Ionics ◽  
2007 ◽  
Vol 13 (5) ◽  
pp. 343-348 ◽  
Author(s):  
P. Kuppusami ◽  
K. Muthukkumaran ◽  
R. Divakar ◽  
R. Kesavamoorthy ◽  
E. Mohandas ◽  
...  

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