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000 nam
001 2210080242561
005 20140627141406
008 941213s1994 bnka m FB 000a kor
040 a221008
100 a김선주
245 00 aKNbO3 단결정의 전기적 특성에 관한 연구/d金宣周 著. -
260 a부산:b동아대학교,c1994. -
300 a44장.:b삽도;c27cm. -
502 a학위논문(석사)-b동아대학교 교육대학원c물리교육전공d94년6월
520 b영문초록 : I have grown K (Nb_(l-x)V_(x))O_(3) [x=0, 0.005, 0.01, 0.11] single crystals by Czochraski method : the melt of compound constitutents are more aboundant than (Nb_(l-x)V_(x))O_(3) [x = 0, 0.005, 0.01, 0.1] molecules. X-ray diffraction of K(Nb_(l-x)V_(x))O_(3) [x=0, 0.005, 0.01, 0.1] reveals that they belong to the orthorhombic group at the room temperature. V^(5+) ion substitution does not effect the structure of the crystals. KNbO_(3) single crystal grown from the 0.5 K_(2)CO_(3)+0.5 Nb_(2)CO_(5) melt shown a larger thermal hysteresis curve at the first transition temperature than a KNbO_(3) single crystal grown from 0.58 K_(2)CO_(3)+0.42 Nb_(2)CO_(5) melt. The Curie temperature of the latter is 2.5 ℃ higher than the former. Dielectric constant of both crystals increases, as a function of the frequency in the 1MHz-6MHz range. As I substitute V^(5+) ions more, dielectric constant increases, and the second phase transition temperature and the Curie temperature more to higher temperatures. A.C. conductivity of K(Nb_(l-x)V_(x))O_(3) is measured : it depends on the temperature and the frequency, and increases as more V^(5+) ions are substituted in the crystal. Temperature dependence of the conductivity below 10^(6) Hz can be interpreted as a hopping conduction by charged particles (CBH), and that over 10^(7) Hz which is independent of temperature and proportional to ω^(2) can be explained as a hopping conditions among impurities.
650 a단결정a전기aKNb03
856 adonga.dcollection.netuhttp://donga.dcollection.net/jsp/common/DcLoOrgPer.jsp?sItemId=000002142247
950 aFB
950 a비매품b₩3,000c(추정가)
KNbO3 단결정의 전기적 특성에 관한 연구
종류
학위논문 동서
서명
KNbO3 단결정의 전기적 특성에 관한 연구
저자명
발행사항
부산: 동아대학교 1994. -
형태사항
44장: 삽도; 27cm. -
학위논문주기
학위논문(석사)- 동아대학교 교육대학원 물리교육전공 94년6월
주기사항
영문초록 : I have grown K (Nb_(l-x)V_(x))O_(3) [x=0, 0.005, 0.01, 0.11] single crystals by Czochraski method : the melt of compound constitutents are more aboundant than (Nb_(l-x)V_(x))O_(3) [x = 0, 0.005, 0.01, 0.1] molecules. X-ray diffraction of K(Nb_(l-x)V_(x))O_(3) [x=0, 0.005, 0.01, 0.1] reveals that they belong to the orthorhombic group at the room temperature. V^(5+) ion substitution does not effect the structure of the crystals. KNbO_(3) single crystal grown from the 0.5 K_(2)CO_(3)+0.5 Nb_(2)CO_(5) melt shown a larger thermal hysteresis curve at the first transition temperature than a KNbO_(3) single crystal grown from 0.58 K_(2)CO_(3)+0.42 Nb_(2)CO_(5) melt. The Curie temperature of the latter is 2.5 ℃ higher than the former. Dielectric constant of both crystals increases, as a function of the frequency in the 1MHz-6MHz range. As I substitute V^(5+) ions more, dielectric constant increases, and the second phase transition temperature and the Curie temperature more to higher temperatures. A.C. conductivity of K(Nb_(l-x)V_(x))O_(3) is measured : it depends on the temperature and the frequency, and increases as more V^(5+) ions are substituted in the crystal. Temperature dependence of the conductivity below 10^(6) Hz can be interpreted as a hopping conduction by charged particles (CBH), and that over 10^(7) Hz which is independent of temperature and proportional to ω^(2) can be explained as a hopping conditions among impurities.
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427.2 김53K
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E0514658
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427.2 김53K =2
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E0575917
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427.2 김53K =3
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