Phase transitions in BaTiO3 thin films and BaTiO3/BaZrO3 superlattices
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作者:
Yuzyuk, Yu. I.
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Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, RussiaSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Yuzyuk, Yu. I.
[1
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Sakhovoy, R. A.
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Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, RussiaSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Sakhovoy, R. A.
[1
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Maslova, O. A.
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Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, RussiaSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Maslova, O. A.
[1
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Shirokov, V. B.
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Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Southern Sci Ctr RAS, Rostov Na Donu 344006, RussiaSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Shirokov, V. B.
[1
,2
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Zakharchenko, I. N.
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Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, RussiaSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Zakharchenko, I. N.
[1
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Belhadi, J.
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Univ Picardie Jules Verne, Lab Phys Matiere Condensee, F-80039 Amiens, FranceSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
Belhadi, J.
[3
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El Marssi, M.
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Univ Picardie Jules Verne, Lab Phys Matiere Condensee, F-80039 Amiens, FranceSouthern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
El Marssi, M.
[3
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机构:
[1] Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia
[2] Southern Sci Ctr RAS, Rostov Na Donu 344006, Russia
Using pulsed laser deposition, we grew a ferroelectric [BaTiO3](Lambda/2)/[BaZrO3](Lambda/2) (BT/BZ) superlattice with a stacking periodicity of Lambda = 256 angstrom and a BT single film on a La1/2Sr1/2CoO3-buffered (001)MgO substrate, and then studied the phase transitions of these materials. At room temperature, the polarized Raman spectra of the BT film corresponded to a ferroelectric orthorhombic C-2V(14) phase with the polar axis oriented in the plane of the substrate. A ferroelectric-paraelectric phase transition in the BT film occurred at similar to 450 K. Upon cooling to similar to 300 K, a phase transition to the monoclinic C-s(3) phase occurred. These experimental results agree well with a theoretical "temperature-misfit strain" phase diagram of the BT film. We found no evidence of phase transitions in the BT/BZ superlattice below room temperature. The phase transition to the paraelectric phase in the BT/BZ superlattice increased in temperature because of lattice mismatch between the BT and BZ layers. A desirable Curie temperature can be tailored rather precisely by varying the layer thicknesses or the BT/BZ ratio in the superlattice. The BT/BZ superlattices are very good for device applications because their ferroelectric phase with in-plane polarization can remain stable at least from 0 K up to 723 K, and even at higher temperatures in superlattices with smaller periodicities. (C) 2014 AIP Publishing LLC.
机构:
Department of Materials Science and Engineering, Materials Research Center, Northwestern University, EvanstonDepartment of Materials Science and Engineering, Materials Research Center, Northwestern University, Evanston
Meier A.L.
Desai A.Y.
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Department of Materials Science and Engineering, Materials Research Center, Northwestern University, Evanston
Department of Materials Science and Engineering, North Carolina State University, RaleighDepartment of Materials Science and Engineering, Materials Research Center, Northwestern University, Evanston
Desai A.Y.
Wang L.
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Department of Chemistry, Materials Research Center, Northwestern University, EvanstonDepartment of Materials Science and Engineering, Materials Research Center, Northwestern University, Evanston
Wang L.
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Marks T.J.
Wessels B.W.
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Department of Materials Science and Engineering, Materials Research Center, Northwestern University, Evanston
Department of Electrical and Computer Engineering, Northwestern University, EvanstonDepartment of Materials Science and Engineering, Materials Research Center, Northwestern University, Evanston