Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping
This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant en...
Ausführliche Beschreibung
Autor*in: |
Zhi-Hao Zhao [verfasserIn] Rui-Fang Ge [verfasserIn] Yejing Dai [verfasserIn] |
---|
Format: |
E-Artikel |
---|---|
Sprache: |
Englisch |
Erschienen: |
2019 |
---|
Schlagwörter: |
---|
Übergeordnetes Werk: |
In: Journal of Advanced Dielectrics - World Scientific Publishing, 2018, 9(2019), 3, Seite 1950022-1-1950022-7 |
---|---|
Übergeordnetes Werk: |
volume:9 ; year:2019 ; number:3 ; pages:1950022-1-1950022-7 |
Links: |
Link aufrufen |
---|
DOI / URN: |
10.1142/S2010135X1950022X |
---|
Katalog-ID: |
DOAJ00228006X |
---|
LEADER | 01000caa a22002652 4500 | ||
---|---|---|---|
001 | DOAJ00228006X | ||
003 | DE-627 | ||
005 | 20230501173807.0 | ||
007 | cr uuu---uuuuu | ||
008 | 230225s2019 xx |||||o 00| ||eng c | ||
024 | 7 | |a 10.1142/S2010135X1950022X |2 doi | |
035 | |a (DE-627)DOAJ00228006X | ||
035 | |a (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b | ||
040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
041 | |a eng | ||
050 | 0 | |a QC501-721 | |
100 | 0 | |a Zhi-Hao Zhao |e verfasserin |4 aut | |
245 | 1 | 0 | |a Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping |
264 | 1 | |c 2019 | |
336 | |a Text |b txt |2 rdacontent | ||
337 | |a Computermedien |b c |2 rdamedia | ||
338 | |a Online-Ressource |b cr |2 rdacarrier | ||
520 | |a This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. | ||
650 | 4 | |a Lead-free piezoelectric ceramics | |
650 | 4 | |a BNT-based | |
650 | 4 | |a CuO dopant | |
650 | 4 | |a electro-strain | |
653 | 0 | |a Electricity | |
700 | 0 | |a Rui-Fang Ge |e verfasserin |4 aut | |
700 | 0 | |a Yejing Dai |e verfasserin |4 aut | |
773 | 0 | 8 | |i In |t Journal of Advanced Dielectrics |d World Scientific Publishing, 2018 |g 9(2019), 3, Seite 1950022-1-1950022-7 |w (DE-627)778146960 |w (DE-600)2756564-6 |x 20101368 |7 nnns |
773 | 1 | 8 | |g volume:9 |g year:2019 |g number:3 |g pages:1950022-1-1950022-7 |
856 | 4 | 0 | |u https://doi.org/10.1142/S2010135X1950022X |z kostenfrei |
856 | 4 | 0 | |u https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b |z kostenfrei |
856 | 4 | 0 | |u http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X |z kostenfrei |
856 | 4 | 2 | |u https://doaj.org/toc/2010-135X |y Journal toc |z kostenfrei |
856 | 4 | 2 | |u https://doaj.org/toc/2010-1368 |y Journal toc |z kostenfrei |
912 | |a GBV_USEFLAG_A | ||
912 | |a SYSFLAG_A | ||
912 | |a GBV_DOAJ | ||
912 | |a SSG-OLC-PHA | ||
912 | |a GBV_ILN_20 | ||
912 | |a GBV_ILN_22 | ||
912 | |a GBV_ILN_23 | ||
912 | |a GBV_ILN_24 | ||
912 | |a GBV_ILN_39 | ||
912 | |a GBV_ILN_40 | ||
912 | |a GBV_ILN_60 | ||
912 | |a GBV_ILN_62 | ||
912 | |a GBV_ILN_63 | ||
912 | |a GBV_ILN_65 | ||
912 | |a GBV_ILN_69 | ||
912 | |a GBV_ILN_70 | ||
912 | |a GBV_ILN_73 | ||
912 | |a GBV_ILN_95 | ||
912 | |a GBV_ILN_105 | ||
912 | |a GBV_ILN_110 | ||
912 | |a GBV_ILN_151 | ||
912 | |a GBV_ILN_161 | ||
912 | |a GBV_ILN_170 | ||
912 | |a GBV_ILN_213 | ||
912 | |a GBV_ILN_230 | ||
912 | |a GBV_ILN_285 | ||
912 | |a GBV_ILN_293 | ||
912 | |a GBV_ILN_370 | ||
912 | |a GBV_ILN_602 | ||
912 | |a GBV_ILN_2014 | ||
912 | |a GBV_ILN_4012 | ||
912 | |a GBV_ILN_4037 | ||
912 | |a GBV_ILN_4112 | ||
912 | |a GBV_ILN_4125 | ||
912 | |a GBV_ILN_4126 | ||
912 | |a GBV_ILN_4249 | ||
912 | |a GBV_ILN_4305 | ||
912 | |a GBV_ILN_4306 | ||
912 | |a GBV_ILN_4307 | ||
912 | |a GBV_ILN_4313 | ||
912 | |a GBV_ILN_4322 | ||
912 | |a GBV_ILN_4323 | ||
912 | |a GBV_ILN_4324 | ||
912 | |a GBV_ILN_4325 | ||
912 | |a GBV_ILN_4335 | ||
912 | |a GBV_ILN_4338 | ||
912 | |a GBV_ILN_4367 | ||
912 | |a GBV_ILN_4700 | ||
951 | |a AR | ||
952 | |d 9 |j 2019 |e 3 |h 1950022-1-1950022-7 |
author_variant |
z h z zhz r f g rfg y d yd |
---|---|
matchkey_str |
article:20101368:2019----::ageetotaninlfhbttnlafepeolcr |
hierarchy_sort_str |
2019 |
callnumber-subject-code |
QC |
publishDate |
2019 |
allfields |
10.1142/S2010135X1950022X doi (DE-627)DOAJ00228006X (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b DE-627 ger DE-627 rakwb eng QC501-721 Zhi-Hao Zhao verfasserin aut Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain Electricity Rui-Fang Ge verfasserin aut Yejing Dai verfasserin aut In Journal of Advanced Dielectrics World Scientific Publishing, 2018 9(2019), 3, Seite 1950022-1-1950022-7 (DE-627)778146960 (DE-600)2756564-6 20101368 nnns volume:9 year:2019 number:3 pages:1950022-1-1950022-7 https://doi.org/10.1142/S2010135X1950022X kostenfrei https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b kostenfrei http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X kostenfrei https://doaj.org/toc/2010-135X Journal toc kostenfrei https://doaj.org/toc/2010-1368 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2019 3 1950022-1-1950022-7 |
spelling |
10.1142/S2010135X1950022X doi (DE-627)DOAJ00228006X (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b DE-627 ger DE-627 rakwb eng QC501-721 Zhi-Hao Zhao verfasserin aut Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain Electricity Rui-Fang Ge verfasserin aut Yejing Dai verfasserin aut In Journal of Advanced Dielectrics World Scientific Publishing, 2018 9(2019), 3, Seite 1950022-1-1950022-7 (DE-627)778146960 (DE-600)2756564-6 20101368 nnns volume:9 year:2019 number:3 pages:1950022-1-1950022-7 https://doi.org/10.1142/S2010135X1950022X kostenfrei https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b kostenfrei http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X kostenfrei https://doaj.org/toc/2010-135X Journal toc kostenfrei https://doaj.org/toc/2010-1368 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2019 3 1950022-1-1950022-7 |
allfields_unstemmed |
10.1142/S2010135X1950022X doi (DE-627)DOAJ00228006X (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b DE-627 ger DE-627 rakwb eng QC501-721 Zhi-Hao Zhao verfasserin aut Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain Electricity Rui-Fang Ge verfasserin aut Yejing Dai verfasserin aut In Journal of Advanced Dielectrics World Scientific Publishing, 2018 9(2019), 3, Seite 1950022-1-1950022-7 (DE-627)778146960 (DE-600)2756564-6 20101368 nnns volume:9 year:2019 number:3 pages:1950022-1-1950022-7 https://doi.org/10.1142/S2010135X1950022X kostenfrei https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b kostenfrei http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X kostenfrei https://doaj.org/toc/2010-135X Journal toc kostenfrei https://doaj.org/toc/2010-1368 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2019 3 1950022-1-1950022-7 |
allfieldsGer |
10.1142/S2010135X1950022X doi (DE-627)DOAJ00228006X (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b DE-627 ger DE-627 rakwb eng QC501-721 Zhi-Hao Zhao verfasserin aut Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain Electricity Rui-Fang Ge verfasserin aut Yejing Dai verfasserin aut In Journal of Advanced Dielectrics World Scientific Publishing, 2018 9(2019), 3, Seite 1950022-1-1950022-7 (DE-627)778146960 (DE-600)2756564-6 20101368 nnns volume:9 year:2019 number:3 pages:1950022-1-1950022-7 https://doi.org/10.1142/S2010135X1950022X kostenfrei https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b kostenfrei http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X kostenfrei https://doaj.org/toc/2010-135X Journal toc kostenfrei https://doaj.org/toc/2010-1368 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2019 3 1950022-1-1950022-7 |
allfieldsSound |
10.1142/S2010135X1950022X doi (DE-627)DOAJ00228006X (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b DE-627 ger DE-627 rakwb eng QC501-721 Zhi-Hao Zhao verfasserin aut Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain Electricity Rui-Fang Ge verfasserin aut Yejing Dai verfasserin aut In Journal of Advanced Dielectrics World Scientific Publishing, 2018 9(2019), 3, Seite 1950022-1-1950022-7 (DE-627)778146960 (DE-600)2756564-6 20101368 nnns volume:9 year:2019 number:3 pages:1950022-1-1950022-7 https://doi.org/10.1142/S2010135X1950022X kostenfrei https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b kostenfrei http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X kostenfrei https://doaj.org/toc/2010-135X Journal toc kostenfrei https://doaj.org/toc/2010-1368 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2019 3 1950022-1-1950022-7 |
language |
English |
source |
In Journal of Advanced Dielectrics 9(2019), 3, Seite 1950022-1-1950022-7 volume:9 year:2019 number:3 pages:1950022-1-1950022-7 |
sourceStr |
In Journal of Advanced Dielectrics 9(2019), 3, Seite 1950022-1-1950022-7 volume:9 year:2019 number:3 pages:1950022-1-1950022-7 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
topic_facet |
Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain Electricity |
isfreeaccess_bool |
true |
container_title |
Journal of Advanced Dielectrics |
authorswithroles_txt_mv |
Zhi-Hao Zhao @@aut@@ Rui-Fang Ge @@aut@@ Yejing Dai @@aut@@ |
publishDateDaySort_date |
2019-01-01T00:00:00Z |
hierarchy_top_id |
778146960 |
id |
DOAJ00228006X |
language_de |
englisch |
fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ00228006X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230501173807.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230225s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1142/S2010135X1950022X</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ00228006X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">QC501-721</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Zhi-Hao Zhao</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Lead-free piezoelectric ceramics</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">BNT-based</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">CuO dopant</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">electro-strain</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Electricity</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Rui-Fang Ge</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Yejing Dai</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">Journal of Advanced Dielectrics</subfield><subfield code="d">World Scientific Publishing, 2018</subfield><subfield code="g">9(2019), 3, Seite 1950022-1-1950022-7</subfield><subfield code="w">(DE-627)778146960</subfield><subfield code="w">(DE-600)2756564-6</subfield><subfield code="x">20101368</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:9</subfield><subfield code="g">year:2019</subfield><subfield code="g">number:3</subfield><subfield code="g">pages:1950022-1-1950022-7</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1142/S2010135X1950022X</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2010-135X</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2010-1368</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHA</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">9</subfield><subfield code="j">2019</subfield><subfield code="e">3</subfield><subfield code="h">1950022-1-1950022-7</subfield></datafield></record></collection>
|
callnumber-first |
Q - Science |
author |
Zhi-Hao Zhao |
spellingShingle |
Zhi-Hao Zhao misc QC501-721 misc Lead-free piezoelectric ceramics misc BNT-based misc CuO dopant misc electro-strain misc Electricity Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping |
authorStr |
Zhi-Hao Zhao |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)778146960 |
format |
electronic Article |
delete_txt_mv |
keep |
author_role |
aut aut aut |
collection |
DOAJ |
remote_str |
true |
callnumber-label |
QC501-721 |
illustrated |
Not Illustrated |
issn |
20101368 |
topic_title |
QC501-721 Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping Lead-free piezoelectric ceramics BNT-based CuO dopant electro-strain |
topic |
misc QC501-721 misc Lead-free piezoelectric ceramics misc BNT-based misc CuO dopant misc electro-strain misc Electricity |
topic_unstemmed |
misc QC501-721 misc Lead-free piezoelectric ceramics misc BNT-based misc CuO dopant misc electro-strain misc Electricity |
topic_browse |
misc QC501-721 misc Lead-free piezoelectric ceramics misc BNT-based misc CuO dopant misc electro-strain misc Electricity |
format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
format_main_str_mv |
Text Zeitschrift/Artikel |
carriertype_str_mv |
cr |
hierarchy_parent_title |
Journal of Advanced Dielectrics |
hierarchy_parent_id |
778146960 |
hierarchy_top_title |
Journal of Advanced Dielectrics |
isfreeaccess_txt |
true |
familylinks_str_mv |
(DE-627)778146960 (DE-600)2756564-6 |
title |
Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping |
ctrlnum |
(DE-627)DOAJ00228006X (DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b |
title_full |
Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping |
author_sort |
Zhi-Hao Zhao |
journal |
Journal of Advanced Dielectrics |
journalStr |
Journal of Advanced Dielectrics |
callnumber-first-code |
Q |
lang_code |
eng |
isOA_bool |
true |
recordtype |
marc |
publishDateSort |
2019 |
contenttype_str_mv |
txt |
container_start_page |
1950022 |
author_browse |
Zhi-Hao Zhao Rui-Fang Ge Yejing Dai |
container_volume |
9 |
class |
QC501-721 |
format_se |
Elektronische Aufsätze |
author-letter |
Zhi-Hao Zhao |
doi_str_mv |
10.1142/S2010135X1950022X |
author2-role |
verfasserin |
title_sort |
large electro-strain signal of the bnt–bt–knn lead-free piezoelectric ceramics with cuo doping |
callnumber |
QC501-721 |
title_auth |
Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping |
abstract |
This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. |
abstractGer |
This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. |
abstract_unstemmed |
This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics. |
collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 |
container_issue |
3 |
title_short |
Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping |
url |
https://doi.org/10.1142/S2010135X1950022X https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X https://doaj.org/toc/2010-135X https://doaj.org/toc/2010-1368 |
remote_bool |
true |
author2 |
Rui-Fang Ge Yejing Dai |
author2Str |
Rui-Fang Ge Yejing Dai |
ppnlink |
778146960 |
callnumber-subject |
QC - Physics |
mediatype_str_mv |
c |
isOA_txt |
true |
hochschulschrift_bool |
false |
doi_str |
10.1142/S2010135X1950022X |
callnumber-a |
QC501-721 |
up_date |
2024-07-04T00:36:23.773Z |
_version_ |
1803606696946302976 |
fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ00228006X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230501173807.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230225s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1142/S2010135X1950022X</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ00228006X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ3f1b056d69604a1c91bb5dd35495833b</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">QC501-721</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Zhi-Hao Zhao</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Large electro-strain signal of the BNT–BT–KNN lead-free piezoelectric ceramics with CuO doping</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">This paper investigates a system of 0.93Bi0.5Na0.5TiO3–0.06BaTiO3–0.01K0.5Na0.5NbO3–xCuO (BNT–BT–KNN–xCuO, x=0−0.04mol.%) ceramics, which were fabricated by the conventional solid-state process through the granulation of vacuum freeze drier. The results show that the CuO doping made a significant enhancement on the piezoelectric properties of the BNT–BT–KNN ceramics. With the doping of CuO, the transition temperature between ferroelectric phase and ergodic relaxor state is reduced to near room temperature, resulting in pinched P–E loops and “sprout” shape S–E curves. For the composition with x=0.01, a high unipolar strain of 0.39% under 5kV/mm contributes a large d33∗∼780pm/V at room temperature, which is competitive with the other BNT-based ceramics.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Lead-free piezoelectric ceramics</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">BNT-based</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">CuO dopant</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">electro-strain</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Electricity</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Rui-Fang Ge</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Yejing Dai</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">Journal of Advanced Dielectrics</subfield><subfield code="d">World Scientific Publishing, 2018</subfield><subfield code="g">9(2019), 3, Seite 1950022-1-1950022-7</subfield><subfield code="w">(DE-627)778146960</subfield><subfield code="w">(DE-600)2756564-6</subfield><subfield code="x">20101368</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:9</subfield><subfield code="g">year:2019</subfield><subfield code="g">number:3</subfield><subfield code="g">pages:1950022-1-1950022-7</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1142/S2010135X1950022X</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/3f1b056d69604a1c91bb5dd35495833b</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://www.worldscientific.com/doi/pdf/10.1142/S2010135X1950022X</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2010-135X</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2010-1368</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHA</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">9</subfield><subfield code="j">2019</subfield><subfield code="e">3</subfield><subfield code="h">1950022-1-1950022-7</subfield></datafield></record></collection>
|
score |
7.4004498 |