The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC

Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was invest...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Guo, Mei [verfasserIn] Li, Yuxia [verfasserIn] Dou, Gang [verfasserIn] Gong, Shuping [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2014

Schlagwörter:	TiO2 Nb2O5 Microwave Dielectric Property BaCu TiO2 Ceramic

Übergeordnetes Werk:	Enthalten in: Journal of materials science - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1990, 25(2014), 10 vom: 22. Juli, Seite 4319-4325
Übergeordnetes Werk:	volume:25 ; year:2014 ; number:10 ; day:22 ; month:07 ; pages:4319-4325

Links:	Volltext

DOI / URN:	10.1007/s10854-014-2168-8

Katalog-ID:	SPR013987259

Internformat


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245	1	4	\|a The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC
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520			\|a Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different.
650		4	\|a TiO2 \|7 (dpeaa)DE-He213
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650		4	\|a TiO2 Ceramic \|7 (dpeaa)DE-He213
700	1		\|a Li, Yuxia \|e verfasserin \|4 aut
700	1		\|a Dou, Gang \|e verfasserin \|4 aut
700	1		\|a Gong, Shuping \|e verfasserin \|4 aut
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912			\|a GBV_ILN_161
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912			\|a GBV_ILN_213
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912			\|a GBV_ILN_2006
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912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
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912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
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912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
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912			\|a GBV_ILN_4307
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912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4338
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912			\|a GBV_ILN_4700
936	b	k	\|a 33.61 \|q ASE
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936	b	k	\|a 51.40 \|q ASE
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951			\|a AR
952			\|d 25 \|j 2014 \|e 10 \|b 22 \|c 07 \|h 4319-4325

Indexfelder

author_variant	m g mg y l yl g d gd s g sg
matchkey_str	article:1573482X:2014----::hefcottnucmonsdiinnhmcoaeilcrcrprisfh
hierarchy_sort_str	2014
bklnumber	33.61 51.10 51.40 53.09
publishDate	2014
allfields	10.1007/s10854-014-2168-8 doi (DE-627)SPR013987259 (SPR)s10854-014-2168-8-e DE-627 ger DE-627 rakwb eng 600 670 620 ASE 33.61 bkl 51.10 bkl 51.40 bkl 53.09 bkl Guo, Mei verfasserin aut The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different. TiO2 (dpeaa)DE-He213 Nb2O5 (dpeaa)DE-He213 Microwave Dielectric Property (dpeaa)DE-He213 BaCu (dpeaa)DE-He213 TiO2 Ceramic (dpeaa)DE-He213 Li, Yuxia verfasserin aut Dou, Gang verfasserin aut Gong, Shuping verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1990 25(2014), 10 vom: 22. Juli, Seite 4319-4325 (DE-627)317827154 (DE-600)2016994-2 1573-482X nnns volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325 https://dx.doi.org/10.1007/s10854-014-2168-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.61 ASE 51.10 ASE 51.40 ASE 53.09 ASE AR 25 2014 10 22 07 4319-4325
spelling	10.1007/s10854-014-2168-8 doi (DE-627)SPR013987259 (SPR)s10854-014-2168-8-e DE-627 ger DE-627 rakwb eng 600 670 620 ASE 33.61 bkl 51.10 bkl 51.40 bkl 53.09 bkl Guo, Mei verfasserin aut The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different. TiO2 (dpeaa)DE-He213 Nb2O5 (dpeaa)DE-He213 Microwave Dielectric Property (dpeaa)DE-He213 BaCu (dpeaa)DE-He213 TiO2 Ceramic (dpeaa)DE-He213 Li, Yuxia verfasserin aut Dou, Gang verfasserin aut Gong, Shuping verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1990 25(2014), 10 vom: 22. Juli, Seite 4319-4325 (DE-627)317827154 (DE-600)2016994-2 1573-482X nnns volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325 https://dx.doi.org/10.1007/s10854-014-2168-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.61 ASE 51.10 ASE 51.40 ASE 53.09 ASE AR 25 2014 10 22 07 4319-4325
allfields_unstemmed	10.1007/s10854-014-2168-8 doi (DE-627)SPR013987259 (SPR)s10854-014-2168-8-e DE-627 ger DE-627 rakwb eng 600 670 620 ASE 33.61 bkl 51.10 bkl 51.40 bkl 53.09 bkl Guo, Mei verfasserin aut The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different. TiO2 (dpeaa)DE-He213 Nb2O5 (dpeaa)DE-He213 Microwave Dielectric Property (dpeaa)DE-He213 BaCu (dpeaa)DE-He213 TiO2 Ceramic (dpeaa)DE-He213 Li, Yuxia verfasserin aut Dou, Gang verfasserin aut Gong, Shuping verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1990 25(2014), 10 vom: 22. Juli, Seite 4319-4325 (DE-627)317827154 (DE-600)2016994-2 1573-482X nnns volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325 https://dx.doi.org/10.1007/s10854-014-2168-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.61 ASE 51.10 ASE 51.40 ASE 53.09 ASE AR 25 2014 10 22 07 4319-4325
allfieldsGer	10.1007/s10854-014-2168-8 doi (DE-627)SPR013987259 (SPR)s10854-014-2168-8-e DE-627 ger DE-627 rakwb eng 600 670 620 ASE 33.61 bkl 51.10 bkl 51.40 bkl 53.09 bkl Guo, Mei verfasserin aut The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different. TiO2 (dpeaa)DE-He213 Nb2O5 (dpeaa)DE-He213 Microwave Dielectric Property (dpeaa)DE-He213 BaCu (dpeaa)DE-He213 TiO2 Ceramic (dpeaa)DE-He213 Li, Yuxia verfasserin aut Dou, Gang verfasserin aut Gong, Shuping verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1990 25(2014), 10 vom: 22. Juli, Seite 4319-4325 (DE-627)317827154 (DE-600)2016994-2 1573-482X nnns volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325 https://dx.doi.org/10.1007/s10854-014-2168-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.61 ASE 51.10 ASE 51.40 ASE 53.09 ASE AR 25 2014 10 22 07 4319-4325
allfieldsSound	10.1007/s10854-014-2168-8 doi (DE-627)SPR013987259 (SPR)s10854-014-2168-8-e DE-627 ger DE-627 rakwb eng 600 670 620 ASE 33.61 bkl 51.10 bkl 51.40 bkl 53.09 bkl Guo, Mei verfasserin aut The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different. TiO2 (dpeaa)DE-He213 Nb2O5 (dpeaa)DE-He213 Microwave Dielectric Property (dpeaa)DE-He213 BaCu (dpeaa)DE-He213 TiO2 Ceramic (dpeaa)DE-He213 Li, Yuxia verfasserin aut Dou, Gang verfasserin aut Gong, Shuping verfasserin aut Enthalten in Journal of materials science Dordrecht [u.a.] : Springer Science + Business Media B.V, 1990 25(2014), 10 vom: 22. Juli, Seite 4319-4325 (DE-627)317827154 (DE-600)2016994-2 1573-482X nnns volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325 https://dx.doi.org/10.1007/s10854-014-2168-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 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_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.61 ASE 51.10 ASE 51.40 ASE 53.09 ASE AR 25 2014 10 22 07 4319-4325
language	English
source	Enthalten in Journal of materials science 25(2014), 10 vom: 22. Juli, Seite 4319-4325 volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325
sourceStr	Enthalten in Journal of materials science 25(2014), 10 vom: 22. Juli, Seite 4319-4325 volume:25 year:2014 number:10 day:22 month:07 pages:4319-4325
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	TiO2 Nb2O5 Microwave Dielectric Property BaCu TiO2 Ceramic
dewey-raw	600
isfreeaccess_bool	false
container_title	Journal of materials science
authorswithroles_txt_mv	Guo, Mei @@aut@@ Li, Yuxia @@aut@@ Dou, Gang @@aut@@ Gong, Shuping @@aut@@
publishDateDaySort_date	2014-07-22T00:00:00Z
hierarchy_top_id	317827154
dewey-sort	3600
id	SPR013987259
language_de	englisch
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The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). 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author	Guo, Mei
spellingShingle	Guo, Mei ddc 600 bkl 33.61 bkl 51.10 bkl 51.40 bkl 53.09 misc TiO2 misc Nb2O5 misc Microwave Dielectric Property misc BaCu misc TiO2 Ceramic The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC
authorStr	Guo, Mei
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topic_title	600 670 620 ASE 33.61 bkl 51.10 bkl 51.40 bkl 53.09 bkl The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC TiO2 (dpeaa)DE-He213 Nb2O5 (dpeaa)DE-He213 Microwave Dielectric Property (dpeaa)DE-He213 BaCu (dpeaa)DE-He213 TiO2 Ceramic (dpeaa)DE-He213
topic	ddc 600 bkl 33.61 bkl 51.10 bkl 51.40 bkl 53.09 misc TiO2 misc Nb2O5 misc Microwave Dielectric Property misc BaCu misc TiO2 Ceramic
topic_unstemmed	ddc 600 bkl 33.61 bkl 51.10 bkl 51.40 bkl 53.09 misc TiO2 misc Nb2O5 misc Microwave Dielectric Property misc BaCu misc TiO2 Ceramic
topic_browse	ddc 600 bkl 33.61 bkl 51.10 bkl 51.40 bkl 53.09 misc TiO2 misc Nb2O5 misc Microwave Dielectric Property misc BaCu misc TiO2 Ceramic
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title	The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC
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title_full	The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC
author_sort	Guo, Mei
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author_browse	Guo, Mei Li, Yuxia Dou, Gang Gong, Shuping
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format_se	Elektronische Aufsätze
author-letter	Guo, Mei
doi_str_mv	10.1007/s10854-014-2168-8
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title_sort	effect of titanium compounds addition on the microwave dielectric properties of the zno–$ nb_{2} %$ o_{5} $ ceramics for ltcc
title_auth	The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC
abstract	Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different.
abstractGer	Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different.
abstract_unstemmed	Abstract The ZnO–$ Nb_{2} %$ O_{5} $ ceramics with titanium compounds were prepared by solid state reaction method. The effect of titanium compounds addition on the densification, phase development, microstructure and microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics was investigated. Adding $ TiO_{2} $ to the ZnO–$ Nb_{2} %$ O_{5} $ ceramics in different order, the X-ray diffraction patterns showed that $ ZnTiNb_{2} %$ O_{8} $ was the main crystalline phase, only the minor crystalline phases were different. The $ TiO_{2} $ phase could not coexist with $ ZnNb_{2} %$ O_{6} $ phase, but the $ CaTiO_{3} $ phase could coexist with $ ZnNb_{2} %$ O_{6} $ phase. The effect of adding $ TiO_{2} $ in different order on the microstructures of ZnO–$ Nb_{2} %$ O_{5} $ ceramics is unconspicuous. Compared to the $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics, it is easier to lower the sintering temperature of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics by doping BaCu($ B_{2} %$ O_{5} $). The τf values of the $ ZnNb_{2} %$ O_{6} $–1.$ 8TiO_{2} $ ceramics and $ ZnNb_{2} %$ O_{6} $–0.$ 2CaTiO_{3} $ ceramics can be adjusted to zero by doping opposite τf values compounds, but the two mechanisms of adjusting τf are different.
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container_issue	10
title_short	The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC
url	https://dx.doi.org/10.1007/s10854-014-2168-8
remote_bool	true
author2	Li, Yuxia Dou, Gang Gong, Shuping
author2Str	Li, Yuxia Dou, Gang Gong, Shuping
ppnlink	317827154
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isOA_txt	false
hochschulschrift_bool	false
doi_str	10.1007/s10854-014-2168-8
up_date	2024-07-03T23:26:51.890Z
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The effect of titanium compounds addition on the microwave dielectric properties of the ZnO–$ Nb_{2} %$ O_{5} $ ceramics for LTCC

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