Processing and Characterisation of Single‐Phase Superconducting Thin Films in the Bi‐Sr‐Ca‐Cu‐O System from Chemical Precursors

1989 ◽  
Vol 169 ◽  
Author(s):  
S. J. Golden ◽  
T. E. Bloomer ◽  
F. F. Lange ◽  
A. M. Segadaes ◽  
K. J. Vaidya ◽  
...  

AbstractThin films in the Bi‐Sr‐Ca‐Cu‐O system have been synthesized from liquid ethyl hexanoate precursors by spin pyrolysis. An extensive solid solution range was determined for the two Cu‐layer phase through the study of c‐axis oriented, single‐phase thin films fabricated on single‐crystal MgO (100). Extensive cation non‐stoichiometry was observed in all cases. The variation of important thin film properties with composition within the solid solution range have been described.Utilising the results from the thin film study together with data relating to liquid formation in mixtures of bulk material a working model describing the formation of the two‐layer phase has been formulated. The two‐layer phase is formed as the result of precipitation from a fugitive liquid at temperatures exceeding 730 *C.

2015 ◽  
Vol 51 (6) ◽  
pp. 1143-1146 ◽  
Author(s):  
Monika Warzecha ◽  
Jesus Calvo-Castro ◽  
Alan R. Kennedy ◽  
Alisdair N. Macpherson ◽  
Kenneth Shankland ◽  
...  

Sensitive optical detection of nitroaromatic vapours with diketopyrrolopyrrole thin films is reported for the first time.


2001 ◽  
Vol 691 ◽  
Author(s):  
Ichiro Matsubara ◽  
Ryoji Funahashi ◽  
Masahiro Shikano ◽  
Kei Sasaki ◽  
Hiroyuki Enomoto

ABSTRACTWe have prepared (Ca1−x−yMxBiy)3Co4Oz (M = Mg, Sr, and Ba) thin films by a combinatorial approach using a solution process. In the systems of (Ca1−x−yMxBiy)3Co4Oz (M = Mg, Sr, and Ba), solid solution range was determined to be × < 0.8 (M = Sr, y = 0), x < 1.0 (M = Mg, y = 0), x = 0.0 (M = Ba, y = 0), and x < 0.4 (M = Bi, x = 0). No solid solution range was obtained for the substitution of Ba for Ca site. The in-plane compressive stress in the CoO2 sublattice is controllable by the cation substitution for Ca in the (Ca2CoO3) sublattice. With increasing in-plane stress, the magnitude of thermoelectric power and resistivity increased.


2017 ◽  
Vol 5 (26) ◽  
pp. 13665-13673 ◽  
Author(s):  
Suttipong Wannapaiboon ◽  
Kenji Sumida ◽  
Katharina Dilchert ◽  
Min Tu ◽  
Susumu Kitagawa ◽  
...  

Addition of a modulator in the LPE process enhances MOF thin film properties by boosting their crystallinity, orientation uniformity, and adsorption capacity.


1998 ◽  
Vol 520 ◽  
Author(s):  
A. Maldonado ◽  
D.R. Acosta ◽  
M. De La Luz Olvera ◽  
R. Castanedo ◽  
G. Torres ◽  
...  

ABSTRACTZinc oxide thin films doped with zirconium were prepared from solutions with doping material dispersed at several concentrations and using the spray pyrolysis technique.The films were deposited over sodocalcic glasses at different substrate temperatures. Effects of doping material concentration and substrate temperatures on electrical, optical, structural and morphological film properties are presented. Results show an evolution in morphology and grains size as the doping concentration is increased. Preferential growth in the (002) orientation was detected for each thin film from X ray diffractograms.


2009 ◽  
Vol 1165 ◽  
Author(s):  
Sebastian Lehmann ◽  
David Fuertes Marrón ◽  
José Manuel Merino Álvarez ◽  
Maximo Léon ◽  
Michael Tovar ◽  
...  

AbstractChalcopyrite-based devices show highest conversion efficiencies among present thin film architectures with values of 20% at laboratory scale. This outstanding performance has been achieved for quaternary Cu(Inx,Ga1-x)Se2 (x˜0.7) compound material. However, a strong correlation between the performance and the gallium content or, in other words, low versus high bandgap materials has been recognized. One critical issue in this discussion is the formation of a copper-depleted near-surface phase with 1:3:5 and 1:5:8 stoichiometries. In earlier reports, surface phases with corresponding compositions have been found on CuInSe2, CuGaSe2 and Cu(Inx,Ga1-x)Se2 thin films. These near-surface phases show a positive influence on the performance of cells based on low bandgap Cu(Inx,Ga1-x)Se2 material due to n-type inversion and band gap widening compared to bulk properties. A tendency towards a neutral or even a negative impact of the near-surface phase on wide band gap material (high gallium content) has recently been reported [1]. Nevertheless, the structural models of copper-poor chalcopyrite-related compounds have been controversially discussed in literature but a stannite-type structural model is most suitable as will be presented. In any case, the relation of the structural properties between chalcopyrite and 1:3:5 phases is crucial for the performance of related devices.In this contribution we will report about the structural analysis of the Cu(Inx,Ga1-x)3Se5 solid solution series by means of anomalous x-ray scattering using synchrotron radiation, powder and single crystal neutron diffraction. Contributions of the isoelectronic species Cu+ and Ga3+ could be separated by these experiments. Bulk samples synthesized from the elements and heat treated at 650°C after the main reaction step - the latter in order to allow equilibrium structure formation - were investigated. Structural data like lattice parameters, tetragonal distortion and cation distribution were obtained for the complete Cu(Inx,Ga1-x)3Se5 solid solution series. The stannite-type structural model was assigned to all members of the investigated 1:3:5s which will be strengthened by simulations. We observed that the tetragonal distortion vanishes for compositions close to a gallium content as used for highest efficiency Cu(Inx,Ga1-x)Se2 devices. However, the tetragonal distortion depends critically on the cation distribution which is in turn controlled by the thermal history of the sample, as we have recently reported for pure CuGaSe2 [1]. This means that we can plot a direct correlation for the misfit between chalcopyrite and 1:3:5 phases depending on the gallium content and the thermal treatment of the considered thin films. These results will widen the understanding of the chalcopyrite-based thin film photovoltaic devices.[1] S. Lehmann et al., Phys. Stat. Sol. A (in press)


1997 ◽  
Vol 505 ◽  
Author(s):  
P. Müllner ◽  
E. Arzt

ABSTRACTDislocation structures in Al-Cu thin films have been studied by transmission electron microscopy (TEM). We have observed that the contrast of interface dislocations disappears in the electron beam. We assume that the contrast dissolution is due to the spreading of the dislocation core at the crystalline/amorphous interface or due to a diffusive movement of the dislocation through the oxide. In any case, the relaxation is assumed to be controled by irradiation induced diffusion. As a consequence, the short range stresses and at least partly also the long range stresses of the dislocations relax. This relaxation changes the interaction force between dislocations and may thus significantly affect the mechanical properties of thin films. It is concluded that interaction between interface dislocations may not be responsible for the high temperature strength of aluminum films.


2015 ◽  
Vol 39 (12) ◽  
pp. 9471-9479 ◽  
Author(s):  
Shrividhya Thiagarajan ◽  
Mahalingam Thaiyan ◽  
Ravi Ganesan

Highly crystalline α-V2O5 thin film nanostructures with a single phase exhibiting higher mobility were prepared by the EB-PVD technique.


2000 ◽  
Vol 14 (09) ◽  
pp. 1007-1016
Author(s):  
Z. MORI ◽  
T. NAKAGAMA ◽  
S. HIGO ◽  
T. DOI ◽  
S. KOBA ◽  
...  

SrTiO 3 (STO) thin film was prepared on single crystal MgO (100) substrate by rf magnetron sputtering as a buffer layer of superconducting thin film. Sputtering conditions influence to the structural property were investigated. Highly epitaxial a-axis oriented STO thin film with extremely smooth surface was obtained by optimizing the sputtering parameters. YBa 2 Cu 3 O 7-δ (YBCO) thin film with critical temperature (T c ) of 89.8 K was obtained on STO buffer. Surface morphology of YBCO thin film was also improved. The effects of STO buffer were discussed in comparison with YBCO thin films on MgO substrate.


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