Geri Dön

Ferroelektrik faz geçişinde iki alt örgü, Dvorak ve Levanyuk-Sannikov modelleri ile modifikasyonları

Başlık çevirisi mevcut değil.

  1. Tez No: 55591
  2. Yazar: METİN TOKLUOĞLU
  3. Danışmanlar: PROF. DR. HAMİT YURTSEVEN
  4. Tez Türü: Yüksek Lisans
  5. Konular: Fizik ve Fizik Mühendisliği, Physics and Physics Engineering
  6. Anahtar Kelimeler: Faz geçişleri, Ferroelektrik, Modifikasyon, Phase transitions, Ferroelectrics, Modification
  7. Yıl: 1996
  8. Dil: Türkçe
  9. Üniversite: İstanbul Teknik Üniversitesi
  10. Enstitü: Fen Bilimleri Enstitüsü
  11. Ana Bilim Dalı: Belirtilmemiş.
  12. Bilim Dalı: Belirtilmemiş.
  13. Sayfa Sayısı: Belirtilmemiş.

Özet

Özet yok.

Özet (Çeviri)

T(K> Ps 62.5 65 67.5 70 72.5 75 (a) T(K) (b) Fig 5.Temperature dependence of Vs. a) The dots show the experimental data of HDDBACEEC crystal. The solid line is calculated from fitting of Eq(20) to the experimental data of HDDBACEEC [13] crystal, b) The dots show the experimental data of triglycine selenate [14] crystals. The solid line is calculated from fitting Eq(20) the experimental data of triglycine selenate crystal.g{P(tc)mtc)j:)=v(W'c) We then find that Tc = T0+(k + 3B2 /]6C)/ A Next define Td as the temperature at which the radical of Eq(17) vanishes Td = T0+(k + 3B2 1 AC) I A Then, the ferroelectric phase susceptibility becomes 2C X = 1 B2\\ + -[(T-Td)l(Tc-ldf^-ld)l(Tc-Td)Y where T <TC. For Td>Tc> T0 the phase transition prevents either phase from having a divergence. 5. Modification of The Levanyuk-Sannikov Model Now we consider the addition of the aP2îj2 + - if term in thermodynamic potential which is suggested by Levanyuk and Sannikov as given below: G = A(T-T0)P2 /2 + BP4 /4 + CP6 /6 + brj4 / 4-qVrj2 + a?2r/2 +-rj2 (18) Minimization of termodynamics potential Eq(18) with respect to jj and P gives that Tj2=-(2qP-2aP2-e) (19),2\.2 V b J b b p b b We fit Eq(20) to the experimental data of HDDBACEEC [13] crystal and triglycine selenate [14].T(K> Ps 62.5 65 67.5 70 72.5 75 (a) T(K) (b) Fig 5.Temperature dependence of Vs. a) The dots show the experimental data of HDDBACEEC crystal. The solid line is calculated from fitting of Eq(20) to the experimental data of HDDBACEEC [13] crystal, b) The dots show the experimental data of triglycine selenate [14] crystals. The solid line is calculated from fitting Eq(20) the experimental data of triglycine selenate crystal.g{P(tc)mtc)j:)=v(W'c) We then find that Tc = T0+(k + 3B2 /]6C)/ A Next define Td as the temperature at which the radical of Eq(17) vanishes Td = T0+(k + 3B2 1 AC) I A Then, the ferroelectric phase susceptibility becomes 2C X = 1 B2\\ + -[(T-Td)l(Tc-ldf^-ld)l(Tc-Td)Y where T <TC. For Td>Tc> T0 the phase transition prevents either phase from having a divergence. 5. Modification of The Levanyuk-Sannikov Model Now we consider the addition of the aP2îj2 + - if term in thermodynamic potential which is suggested by Levanyuk and Sannikov as given below: G = A(T-T0)P2 /2 + BP4 /4 + CP6 /6 + brj4 / 4-qVrj2 + a?2r/2 +-rj2 (18) Minimization of termodynamics potential Eq(18) with respect to jj and P gives that Tj2=-(2qP-2aP2-e) (19),2\.2 V b J b b p b b We fit Eq(20) to the experimental data of HDDBACEEC [13] crystal and triglycine selenate [14].T(K> Ps 62.5 65 67.5 70 72.5 75 (a) T(K) (b) Fig 5.Temperature dependence of Vs. a) The dots show the experimental data of HDDBACEEC crystal. The solid line is calculated from fitting of Eq(20) to the experimental data of HDDBACEEC [13] crystal, b) The dots show the experimental data of triglycine selenate [14] crystals. The solid line is calculated from fitting Eq(20) the experimental data of triglycine selenate crystal.g{P(tc)mtc)j:)=v(W'c) We then find that Tc = T0+(k + 3B2 /]6C)/ A Next define Td as the temperature at which the radical of Eq(17) vanishes Td = T0+(k + 3B2 1 AC) I A Then, the ferroelectric phase susceptibility becomes 2C X = 1 B2\\ + -[(T-Td)l(Tc-ldf^-ld)l(Tc-Td)Y where T <TC. For Td>Tc> T0 the phase transition prevents either phase from having a divergence. 5. Modification of The Levanyuk-Sannikov Model Now we consider the addition of the aP2îj2 + - if term in thermodynamic potential which is suggested by Levanyuk and Sannikov as given below: G = A(T-T0)P2 /2 + BP4 /4 + CP6 /6 + brj4 / 4-qVrj2 + a?2r/2 +-rj2 (18) Minimization of termodynamics potential Eq(18) with respect to jj and P gives that Tj2=-(2qP-2aP2-e) (19),2\.2 V b J b b p b b We fit Eq(20) to the experimental data of HDDBACEEC [13] crystal and triglycine selenate [14].T(K> Ps 62.5 65 67.5 70 72.5 75 (a) T(K) (b) Fig 5.Temperature dependence of Vs. a) The dots show the experimental data of HDDBACEEC crystal. The solid line is calculated from fitting of Eq(20) to the experimental data of HDDBACEEC [13] crystal, b) The dots show the experimental data of triglycine selenate [14] crystals. The solid line is calculated from fitting Eq(20) the experimental data of triglycine selenate crystal.g{P(tc)mtc)j:)=v(W'c) We then find that Tc = T0+(k + 3B2 /]6C)/ A Next define Td as the temperature at which the radical of Eq(17) vanishes Td = T0+(k + 3B2 1 AC) I A Then, the ferroelectric phase susceptibility becomes 2C X = 1 B2\\ + -[(T-Td)l(Tc-ldf^-ld)l(Tc-Td)Y where T <TC. For Td>Tc> T0 the phase transition prevents either phase from having a divergence. 5. Modification of The Levanyuk-Sannikov Model Now we consider the addition of the aP2îj2 + - if term in thermodynamic potential which is suggested by Levanyuk and Sannikov as given below: G = A(T-T0)P2 /2 + BP4 /4 + CP6 /6 + brj4 / 4-qVrj2 + a?2r/2 +-rj2 (18) Minimization of termodynamics potential Eq(18) with respect to jj and P gives that Tj2=-(2qP-2aP2-e) (19),2\.2 V b J b b p b b We fit Eq(20) to the experimental data of HDDBACEEC [13] crystal and triglycine selenate [14].T(K> Ps 62.5 65 67.5 70 72.5 75 (a) T(K) (b) Fig 5.Temperature dependence of Vs. a) The dots show the experimental data of HDDBACEEC crystal. The solid line is calculated from fitting of Eq(20) to the experimental data of HDDBACEEC [13] crystal, b) The dots show the experimental data of triglycine selenate [14] crystals. The solid line is calculated from fitting Eq(20) the experimental data of triglycine selenate crystal.

Benzer Tezler

  1. Amonyum sülfatın ferroelektrik faz geçişinin incelenmesi ve smektojenlerin mezomorf ve morfolojik özelliklerinin araştırılması

    Investigation of ferrielectric phase transition of ammonium sulphate and investigation of mesomorphic and morphologic properties of smectogenes

    SEVTAP YILDIZ

    Yüksek Lisans

    Türkçe

    Türkçe

    1997

    Fizik ve Fizik Mühendisliğiİstanbul Teknik Üniversitesi

    Fizik Mühendisliği Ana Bilim Dalı

    DOÇ. DR. SELAMİ SALİHOĞLU

  2. Sıvı kristallerde smetrik a-smetrik C* faz geçişinin klasik ve genelleştirilmiş landau modelleri ile incelenmesi

    Classical and extended landau models introduction

    SUMRU BELLİCİ

    Yüksek Lisans

    Türkçe

    Türkçe

    1997

    Fizik ve Fizik Mühendisliğiİstanbul Teknik Üniversitesi

    Fizik Mühendisliği Ana Bilim Dalı

    PROF. DR. HAMİT YURTSEVEN

  3. Sıvı kristallerde manyetik ve elektrik alan etkisi altında ACC* faz diyagramlarının incelenmesi

    Smectic ACC* phase diagrams in liquid crystals under the effect of magnetic and electric fields

    DİDEM SÜNBÜL

    Yüksek Lisans

    Türkçe

    Türkçe

    2000

    Fizik ve Fizik Mühendisliğiİstanbul Teknik Üniversitesi

    PROF.DR. HAMİT YURTSEVEN