2015
DOI: 10.1103/physrevb.92.035438
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Model of two-dimensional electron gas formation at ferroelectric interfaces

Abstract: The formation of a two-dimensional electron gas at oxide interfaces as a consequence of polar discontinuities has generated an enormous amount of activity due to the variety of interesting effects it gives rise to. Here we study under what circumstances a similar processes can also take place underneath ferroelectric thin films. We use a simple Landau model to demonstrate that in the absence of extrinsic screening mechanisms a monodomain phase can be stabilized in ferroelectric films by means of an electronic … Show more

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Cited by 40 publications
(59 citation statements)
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“…On the other hand, similar to n-type interface, the stability of ferromagnetic ordering also depends on the polarization strength of bulk PbTiO 3 . As shown in Figure 7(a), there is no energy difference between FM and AFM ordering when the polarization strength is small and the interface is paramagnetic 13 without persistent spin-polarization. When the ferroelectric polarization increases above ~0.6 C/m 2 , the conductive state becomes spin-polarized and the FM ordering is energetically more favorable than the AFM ordering.…”
mentioning
confidence: 97%
“…On the other hand, similar to n-type interface, the stability of ferromagnetic ordering also depends on the polarization strength of bulk PbTiO 3 . As shown in Figure 7(a), there is no energy difference between FM and AFM ordering when the polarization strength is small and the interface is paramagnetic 13 without persistent spin-polarization. When the ferroelectric polarization increases above ~0.6 C/m 2 , the conductive state becomes spin-polarized and the FM ordering is energetically more favorable than the AFM ordering.…”
mentioning
confidence: 97%
“…As a prototypical ferroelectric material, barium titanate (BaTiO 3 , BTO) plays a vital role in numerous applications and has been intensively studied theoretically [9][10][11][12][13][14][15][16] As shown in Fig. 1, BTO has a perovskite structure and undergoes a structural transition from highsymmetry cubic phase to low-symmetry tetragonal phase when lowering temperature across ∼400 K [17].…”
mentioning
confidence: 99%
“…We note that the obtained distribution ρ ( z ) is in contrast to a model assumption in ref. 44 , where the free charges were a priori placed at the film’s surfaces only and not in the film’s interior.…”
Section: Resultsmentioning
confidence: 99%