JP2013180907A - 誘電体磁器組成物および電子部品 - Google Patents
誘電体磁器組成物および電子部品 Download PDFInfo
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- JP2013180907A JP2013180907A JP2012044014A JP2012044014A JP2013180907A JP 2013180907 A JP2013180907 A JP 2013180907A JP 2012044014 A JP2012044014 A JP 2012044014A JP 2012044014 A JP2012044014 A JP 2012044014A JP 2013180907 A JP2013180907 A JP 2013180907A
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- 229910052748 manganese Inorganic materials 0.000 claims abstract description 8
- 229910052750 molybdenum Inorganic materials 0.000 claims abstract description 8
- 239000010937 tungsten Substances 0.000 claims abstract description 7
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- 229910052772 Samarium Inorganic materials 0.000 claims abstract description 5
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Abstract
【解決手段】一般式{A1−x(RE)2x/3}y−B2O5+yで表され、タングステンブロンズ構造を持つ化合物を有する誘電体磁器組成物である。上記式中、Aは、Ba、Ca、SrおよびMgから選ばれる少なくとも1つ、Bは、Nbおよび/またはTa、REは、Sc、Y、La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、YbおよびLuから選ばれる少なくとも1つであり、xおよびyが、0<x<1、y>1.000の関係を満足する。該誘電体磁器組成物は、V、Mo、Fe、W、MnおよびCrから選ばれる少なくとも1つの酸化物をさらに有することが好ましい。
【選択図】なし
Description
一般式{A1−x(RE)2x/3}y−B2O5+yで表され、タングステンブロンズ構造を有する化合物を有し、
前記Aは、Ba、Ca、SrおよびMgからなる群から選ばれる少なくとも1つ、前記Bは、NbおよびTaからなる群から選ばれる少なくとも1つ、前記REは、Sc、Y、La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、YbおよびLuからなる群から選ばれる少なくとも1つであり、
前記xおよびyが、0<x<1、y>1.000の関係を満足する。
図1に示すように、積層セラミックコンデンサ1は、誘電体層2と内部電極層3とが交互に積層された構成のコンデンサ素子本体10を有する。このコンデンサ素子本体10の両端部には、素子本体10の内部で交互に配置された内部電極層3と各々導通する一対の外部電極4が形成してある。コンデンサ素子本体10の形状に特に制限はないが、通常、直方体状とされる。また、その寸法にも特に制限はなく、用途に応じて適当な寸法とすればよい。
誘電体層2は、本実施形態に係る誘電体磁器組成物から構成されている。該誘電体磁器組成物は、一般式{A1−x(RE)2x/3}y−B2O5+yで表され、タングステンブロンズ構造を有する化合物を含む。
内部電極層3に含有される導電材としては特に限定されないが、誘電体層と同時焼成される場合には、Ag、Pd、Ptあるいは、Ag−Pd合金など、貴金属として公知の導電材を用いればよい。また、内部電極層3がスパッタリング等で形成される場合、あるいは、誘電体層の焼成後に、内部電極層3が形成される場合、導電材として公知の卑金属を用いることができる。内部電極層3の厚さは用途等に応じて適宜決定すればよい。
外部電極4に含有される導電材は特に限定されず、たとえばNi,Cuあるいはこれらの合金など公知の導電材を用いればよい。外部電極4の厚さは用途等に応じて適宜決定すればよい。
本実施形態の積層セラミックコンデンサ1は、公知の方法により製造すればよい。本実施形態では、ペーストを用いてグリーンチップを作製し、これを焼成することで、積層セラミックコンデンサを製造する。以下、製造方法について具体的に説明する。
まず、一般式{A1−x(RE)2x/3}y−B2O5+yで表される化合物の粉末を準備し、これを誘電体原料とした。一般式における「A」元素はBa、「RE」元素はLa、「B」元素はNbであり、xは0.40、yは表1に示す値とした。
まず、得られた焼結体の直径Rを測定した。そして、金型の直径RAと、直径Rとに基づき、以下の式を用いて、縮率を算出した。
縮率(%)=100×(RA−R)/RA
縮率が大きいと、焼結体の密度が高いことを意味する。焼結体の密度が高まると耐湿性が向上するため、高湿度環境下でも好適に使用できる電子部品が得られる。さらに密度が高まることで焼結体の硬さも向上し構造欠陥を防ぐことが可能となる。本実施例では、縮率が17%以上を良好とした。結果を表1に示す。
コンデンサ試料に対し、基準温度25℃において、HP社製4284Aを用いて、周波数1kHz、測定電圧1Vrmsとし、静電容量Cを測定した。そして、比誘電率を、焼結体の厚みと、有効電極面積と、測定の結果得られた静電容量Cとに基づき算出した。本実施例では、比誘電率は高い方が好ましく、250以上がより好ましい。結果を表1に示す。
コンデンサ試料に対し、HP社製4339B HIGH RESISTANCE METERと、HP社製16339A COMPONENT TEST FIXTUREと、を用いて、絶縁抵抗を測定し、抵抗率を算出した。測定条件は、印加電圧を50V、印加時間を30secとした。抵抗率が高いと、高い絶縁抵抗が得られ、高い電界強度下においても、電荷が逃げにくく、コンデンサに蓄積されたエネルギーが損失しにくいという利点がある。本実施例では、抵抗率が1.0×1011(Ω・m)以上を良好とした。抵抗率が1.0×1011(Ω・m)未満の場合、漏れ電流が大きくなることで電気的特性が低下する恐れがあるためである。結果を表1に示す。
(DCバイアス特性)
まず、DCバイアス特性を測定するための試料を作製した。上記で準備した誘電体原料にバインダ樹脂と溶剤とを混合してペーストを作製した。得られたペーストを用いてグリーンシートを形成し、その上にPt電極を印刷し、脱バインダ処理、空気中での焼成を行って、積層セラミックコンデンサ試料を作製した。Pt電極間の距離(誘電体層の厚み)は5μmであり、誘電体層の層数は4層とした。得られた試料に対し、直流電圧を加えない状態と、20V/μmの直流電圧を加えた状態で、周波数1kHz、測定電圧1Vrmsの測定条件下で静電容量を測定した。そして、直流電圧を加えない状態での静電容量に対して、直流電圧を加えた状態での静電容量が変化した割合をDC−Bias特性とした。すなわち、DC−Bias特性が負である場合には、直流電圧を加えると、静電容量が低下したことを示す。本実施例では、DC−Bias特性は0に近い方が好ましく、±5%以内を良好とした。結果を表1に示す。
誘電体原料として、実験1で用いた化合物の粉末と、表2に示す酸化物粉末とを混合したものを用いた以外は、実験1の試料番号2と同様にして、セラミックコンデンサの試料を作製し、実験1と同様の評価を行った。結果を表2に示す。
Vの酸化物の含有量を表3に示す量とした以外は、実験2の試料番号20と同様にして、セラミックコンデンサの試料を作製し、実験1と同様の評価を行った。結果を表3に示す。なお、試料番号26〜28については、「y」の値を表3に示す値とした。
実験1で用いた化合物の一般式における「x」の値を表4に示す値とした以外は、実験1の試料番号2と同様にして、セラミックコンデンサの試料を作製し、実験2と同様の評価を行った。結果を表4に示す。
10… コンデンサ素子本体
2… 誘電体層
3… 内部電極層
4… 外部電極
Claims (3)
- 一般式{A1−x(RE)2x/3}y−B2O5+yで表され、タングステンブロンズ構造を有する化合物を有し、
前記Aは、Ba、Ca、SrおよびMgからなる群から選ばれる少なくとも1つ、前記Bは、NbおよびTaからなる群から選ばれる少なくとも1つ、前記REは、Sc、Y、La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、YbおよびLuからなる群から選ばれる少なくとも1つであり、
前記xおよびyが、0<x<1、y>1.000の関係を満足することを特徴とする誘電体磁器組成物。 - V、Mo、Fe、W、MnおよびCrからなる群から選ばれる少なくとも1つの酸化物をさらに有する請求項1に記載の誘電体磁器組成物。
- 請求項1または2に記載の誘電体磁器組成物から構成される誘電体層と、電極と、を有する電子部品。
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