• Aucun résultat trouvé

Comments on "Ion beam sputter deposition of YBa2Cu3O7−δ thin films” [J. Mater. Res. 8, 3032 (1993)]

N/A
N/A
Protected

Academic year: 2021

Partager "Comments on "Ion beam sputter deposition of YBa2Cu3O7−δ thin films” [J. Mater. Res. 8, 3032 (1993)]"

Copied!
1
0
0

Texte intégral

(1)

COMMENTS AND REPLY

Comments on papers previously published in Journal of Materials Research and replies from the author of the original paper are published together in this section.

Comments on "Ion beam sputter deposition of

thin films" [J. Mater. Res. 8, 3032 (1993)]

Andrea Gauzzi and Davor Pavuna

Department of Physics-IMO, Swiss Federal Institute of Technology at Lausanne (EPFL), CH-1015 Lausanne, Switzerland

(Received 2 June 1994; accepted 23 June 1995)

In this brief letter we want to comment on several statements published

recently in the Journal of Materials Research by our former co-workers Kellett and James (KJ) in the paper entitled "Ion beam sputter deposition of

YBa2Cu307-5 thin films".

KJ have presented some results on ion beam depo-sition of YBCO films that were carried out at the Swiss Federal Institute of Technology in Lausanne (EPFL, Switzerland) until early 1991. The detailed results of this research have already been published elsewhere by Gauzzi et al.23 Hence, here we present the comments on the aforementioned KJ article, based on detailed and comparative data concerning the single target and the multitarget ion beam sputtering technique which were determined in our laboratory and are in our records.

The essence of our interpretation can be summarized as follows:

(1) KJ present the multitarget ion-beam deposition (or co-deposition) technique as an improvement over the single-target technique. From our results, the opposite is true, since x-ray scans on co-deposited films system-atically indicate the presence of secondary phases. On the other hand, the scans on the films deposited in the single "123" target configuration exhibit only weak lines of CuO.2 Hence, stoichiometry control is automatically achieved by using the single-target configuration, while it is difficult to achieve and reproduce it with the multitarget configuration.2-3

(2) KJ use a convincing example of the sharp resis-tive transition at 92 K (p vs T, Fig. 12) of the film from run #354, implying it was obtained by the multitarget ion beam sputtering technique. This work was done in our laboratory, and according to our laboratory records, film was deposited with the single-target configuration with a beam current and voltage of 20 mA and 500 V, respec-tively. Furthermore, the high Tc's and sharp transitions

reported in the paper have never been obtained with the multitarget configuration, but only with the single-target configuration.

Therefore, our initial, complex multitarget tech-nique45 has been abandoned in our laboratory starting

from run #348 (October 1990). The multitarget configu-ration always produced films with Tc's typically <80 K;

resistive transitions are broad and the composition of the films deviates significantly from the "123" composition.45 The main reason is that it is difficult to reproduce the same beam conditions from run to run for several ion sources operating simultaneously.

As mentioned above, since October 1990 we use much a simpler single-target technique operated at low ion-beam energy.2'3 Such a simplified technique indeed produces high quality, reproducible YBCO films with the desired "123" composition and excellent structural7 and electrical properties.6-7

In conclusion, in our view, the KJ paper1 may be misleading to other workers. The present state of art for ion beam sputtering of cuprates is not the multitarget co-deposition, but rather a simple, single target sputtering as reported in detail in Refs. 2 and 3.

ACKNOWLEDGMENT

This work was supported by the Swiss PTT and National Fund for Scientific Research in Bern.

REFERENCES

1. B.J. Kellett and J. H. James, J. Mater. Res. 8, 3032 (1993). 2. A. Gauzzi, M. L. Lucia, B.J. Kellett, J. H. James, and D. Pavuna,

Physica 182C (3), 57 (1991).

3. A. Gauzzi, M. L. Lucia, M. Affronte, and D. Pavuna, Physica 185-189, 2563 (1991).

4. J.H. James, B.J. Kellett, A. Gauzzi, B. Dwir, and D. Pavuna, Appl. Surf. Sci. 43, 393 (1989).

5. S. Michel, J.H. James, B. Dwir, M. Affronte, B. Kellett, and D. Pavuna, J. Less-Comm. Met. 151, 419 (1989).

6. A. Gauzzi and D. Pavuna, Physica 235-240, 1305 (1994). 7. A. Gauzzi and D. Pavuna, Appl. Phys. Lett. 66 (14), 1836 (1995). 2676 J. Mater. Res., Vol. 10, No. 10, Oct 1995 © 1995 Materials Research Society

https:/www.cambridge.org/core/terms. https://doi.org/10.1557/JMR.1995.2676

Références

Documents relatifs

The original article BMethylmalonic acidaemia: Examination of genotype and biochemical data in 32 patients belong- ing to mut, cblA or cblB complementation group^ by Begona Merinero

Energy flux measurements were performed in front of the Ti target in UB-DCMS discharge at a pressure of 0.66 Pa and for different powers applied to the magnetron cathode.. signals

trie substrate. These results confirm that it is possible by this technique to elaborate cermets.. a) Micrograph of a Bi-SiO~ cermet (20 nm thickness). b) Corresponding size

7 - Logarithmic plot of the growth rate for polycrystalline cubic boron monophosphide (BP) on alumina substrates versus the reciprocal absolute temperature.. The PBr3 pressure

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

2 we consider the ith beam of an array of beams traversing the target, and evaluate the total energy deposition rate per unit volume at a point L. The component of the ith beam

Concernant les trois autres groupes, le groupe I, était composé de 4 souches isolées au Mexique et de 3 souches isolées en Côte d’Ivoire, avec une similarité à 60 Figure 76

Soft X-ray reflectometry applied to the evaluation of surface roughness variation during the deposition of thin films... Soft X-ray reflectometry applied to the evaluation