2013
DOI: 10.1016/j.tsf.2013.06.080
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Band diagram of the Si-LiNbO3 heterostructures grown by radio-frequency magnetron sputtering

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Cited by 14 publications
(6 citation statements)
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“…Apparently, formation of the intermediate layer is mainly attributed to the extensive in situ bombardment of the sputtered species. Note that films obtained at lower reactive gas pressure do not manifest an inhomogeneous layer [17]. As regards the sample LN3, a highly conducting intermediate SiO 2 layer is formed between Si substrate and LiNbO 3 film grown at the similar sputtering conditions [18].…”
Section: Resultsmentioning
confidence: 93%
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“…Apparently, formation of the intermediate layer is mainly attributed to the extensive in situ bombardment of the sputtered species. Note that films obtained at lower reactive gas pressure do not manifest an inhomogeneous layer [17]. As regards the sample LN3, a highly conducting intermediate SiO 2 layer is formed between Si substrate and LiNbO 3 film grown at the similar sputtering conditions [18].…”
Section: Resultsmentioning
confidence: 93%
“…Analysis of the X-ray diffraction results for LN2-T sample demonstrates (see Fig. 6) that TA of Si-LiNbO 3 heterostructures triggers recrystallization of the films with an increase of the average grain size up to 1.5 times (about 70 nm) and weakens of the texture compared with as-grown films [13,17]. It is important to emphasize, that TA of the as grown LiNbO 3 films leads to the formation of LiNb 3 O 8 phase.…”
Section: Resultsmentioning
confidence: 99%
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“…8 that Richardson-Schottky emission is the main conduction mechanism for the sample LN 134 and graph V o vs. kT/q is a straight line with a slope n = 40. We obtained parameter β through the graph ln(J/(ET 2/3 ) vs. 1/T (not shown) as has been done in [19], and taking into account that ε = 28 [7] we calculated the value of the barrier height φ b = 0.012eV following the expressions (13) for the average electric field E = 4·10 6 V/m. Too low value of the apparent barrier height φ app can be explained by the fact that ferroelectric polarization P can reduce the true barrier height φ b as has been mentioned earlier (see (4)).…”
Section: Resultsmentioning
confidence: 99%
“…The magnitudes of changes in the bandedge energies are critically important for many devices such as random-access memory units, ferroelectric capacitors, etc. Taking into account that C-V and I-V characteristics of the heterostructures being powerful investigative tools, are greatly influenced by barrier properties [18,19], it is important to study the electron phenomena at the Si-LiNbO 3 heterostructures formed in different technological conditions inside out.…”
Section: Introductionmentioning
confidence: 99%