Investigation of polarization reversal and analysis of switching current data in KTP single crystals

2017 ◽  
Vol 508 (1) ◽  
pp. 1-8 ◽  
Author(s):  
A. R. Akhmatkhanov ◽  
E. M. Vaskina ◽  
M. A. Chuvakova ◽  
E. V. Pelegova ◽  
V. Ya. Shur
Crystals ◽  
2018 ◽  
Vol 8 (8) ◽  
pp. 315 ◽  
Author(s):  
Andrey Akhmatkhanov ◽  
Ekaterina Vaskina ◽  
Ekaterina Gachegova ◽  
Vladimir Shur

Studies of polarization reversal processes in potassium titanyl phosphate (KTiOPO4, KTP) single crystals with surface dielectric layer are important due to their potential applications as the basis of bottom-up technology for creation of periodically poled nonlinear-optical crystals. We present the results of switching currents analysis accompanied by in situ visualization of domain kinetics during polarization reversal in KTP with 3 m-thick photoresist dielectric layer. Qualitative change of the switching current shape has been revealed as compared to the polarization reversal without surface dielectric layer. Two stages of domain structure evolution have been distinguished by in situ visualization of domain kinetics. The formation of submicron domain streamers in front of the moving domain walls has been revealed. The broadening of the domain streamers (1D domain growth) was observed at the second stage. The switching currents were approximated by the modified Kolmogorov-Avrami formula taking into account the change of the growth dimensionality (“geometrical catastrophe”). The sufficient input of the 1D growth to the switching process decreased with increase of the switching field. The obtained results were attributed to the domain wall shape instability induced by retardation of the depolarization field screening in ferroelectric with surface dielectric layer.


1999 ◽  
Vol 604 ◽  
Author(s):  
Uma Belegundu ◽  
Xiaohong Du ◽  
Kenji Uchino

AbstractSwitching current measurements have been carried out on relaxorferroelectric single crystal-pure PZN, and the solid solution (1-x) Pb(Zni1/3 Nb2/3)O3 - x PbTiO3 with x= 0.04, 0.09, 0.10. Measurements have been done for crystallographic directions [001] and [111] for all these compositions. Switching times versus the applied field showed the following results. Pure PZN along [111] and 0.90PZN—O. 10PT along [001], and [111] showed an exponential dependence. Along [001] the PZN showed a linear fit. For solid solution single crystals-0.96PZN -0.04PT and 0.91PZN £ 0.09PT, a linear fit was obtained for the reciprocal switch times versus applied field for both the directions. If we draw a parallel picture with the reported barium titanate data, it appears that the polarization reversal is controlled by nucleation along [111]- spontaneous direction for PZN and [001], [111]for 0.90PZN - O.10PT. The mobility of the reversed domains controls the reversal along [001] for PZN and the solid solution single crystals with rhombohedral composition along [001] and [111]. The transient current curves showed two maximum points for crystals with x = 0.04 and 0.09. This is attributed to the co-existence of the two phases in 0.96PZN -0.04PT and 0. 91PZN - 0.09PT crystals.


2020 ◽  
Vol 559 (1) ◽  
pp. 1-7
Author(s):  
A. R. Akhmatkhanov ◽  
M. A. Chuvakova ◽  
N. A. Dolgushin ◽  
D. B. Kolker ◽  
V. N. Vedenyapin ◽  
...  

2011 ◽  
Vol 53 (11) ◽  
pp. 2311-2315 ◽  
Author(s):  
V. Ya. Shur ◽  
V. A. Shikhova ◽  
D. V. Pelegov ◽  
A. V. Ievlev ◽  
L. I. Ivleva

2003 ◽  
Vol 291 (1) ◽  
pp. 27-35 ◽  
Author(s):  
V. Ya. Shur ◽  
I. S. Baturin ◽  
E. I. Shishkin ◽  
M. V. Belousova

1999 ◽  
Vol 27 (1-4) ◽  
pp. 179-194 ◽  
Author(s):  
V. Ya. Shur ◽  
E. L. Rumyantsev ◽  
S. D. Makarov ◽  
N. Yu. Ponomarev ◽  
E. V. Nikolaeva ◽  
...  

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