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Volumn 6, Issue 1-4, 1995, Pages 189-203

A model of voltage-dependent dielectric losses for ferroelectric MMIC devices

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EID: 7044245605     PISSN: 10584587     EISSN: 16078489     Source Type: Journal    
DOI: 10.1080/10584589508019364     Document Type: Article
Times cited : (42)

References (53)
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    • in press, January E. Fajii, Y. Uemoto, S. Hayashi, T. Nasu, Y. Shimada, A. McMillan, and C. A. Paz de Araujo, IEDM Cod., 14 Dec 1992
    • J. F. Scott, M. Azuma, C. A. Paz de Araujo, L. D. McMillan, M. C. Scott, and T. Roberts, Integrated Ferroelectrics (in press, January 1994); E. Fajii, Y. Uemoto, S. Hayashi, T. Nasu, Y. Shimada, A. McMillan, and C. A. Paz de Araujo, IEDM Cod., 14 Dec 1992.
    • (1994) Integrated Ferroelectrics
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    • in the particular case of strontium titanate the intrinsic anharmonic damping mechanism has been confirmed via hyper-Raman studies of frequency-dependent loss: V. N. Denisov, B. N. Mitwin, V. B. Podobedov, and J. F. Scott, J. Raman Spectr. 14, 276 (1983)
    • V. I. Gurevich and A. K. Tagantsev, Adv. Phys. 40, 719 (1991); in the particular case of strontium titanate the intrinsic anharmonic damping mechanism has been confirmed via hyper-Raman studies of frequency-dependent loss: V. N. Denisov, B. N. Mitwin, V. B. Podobedov, and J. F. Scott, J. Raman Spectr. 14, 276 (1983).
    • (1991) Adv. Phys. , vol.40 , pp. 719
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    • The most comprehensive discussion of the three- and four-phonon anbarmonic self-energies in perfect crystals is, edited by R. W. H. Stevenson (Plenum, New York
    • The most comprehensive discussion of the three- and four-phonon anbarmonic self-energies in perfect crystals is in R. A. Cowley, Phonons in Perfect Lattices and in Lattices with Point Imperfections, edited by R. W. H. Stevenson (Plenum, New York, 1966), pp.170-207.
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    • edited by N. Setter and E. L. Colla (Birkhausen Verlag, Basel, Under some circumstances in perovskite oxides, due to the detailed shape of phonon dispersion curves through the Brillouin zone, the dependence of tan d on susceptibility may be to the 5/2 power, rather than 3/2
    • A. K. Tagantsev, Ferroelectric Ceramics, edited by N. Setter and E. L. Colla (Birkhausen Verlag, Basel, 1993), pp. 127. Under some circumstances in perovskite oxides, due to the detailed shape of phonon dispersion curves through the Brillouin zone, the dependence of tan d on susceptibility may be to the 5/2 power, rather than 3/2.
    • (1993) Ferroelectric Ceramics , pp. 127
    • Tagantsev, A.K.1
  • 25
    • 0003694228 scopus 로고
    • The work of Gurevich and Tagantsev emphasizes dielectric loss; for a comprehensive review of the complementary topic of ultrasonic attenuation in dielectric crystals, see, (Academic Press, New York
    • The work of Gurevich and Tagantsev emphasizes dielectric loss; for a comprehensive review of the complementary topic of ultrasonic attenuation in dielectric crystals, see R. Truell, C. Elbaum, and B. B. Chick, Ultrasonic Methods in Solid State Physics (Academic Press, New York, 1969).
    • (1969) Ultrasonic Methods in Solid State Physics
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    • Greenville, SC, Sept 1, (IEEE, Piscataway, NJ, edited by S. T. Liu, 1993)
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    • (1992) Proc. ISAF
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    • The leakage current dependence upon field for BST films in the latter study is also verified for pure strontium titanate by, edited by A. I. Kingon, E. R. Myers, and B. Tuttle (Materials Research Society, Pittsburgh
    • The leakage current dependence upon field for BST films in the latter study is also verified for pure strontium titanate by S. Matsubara, S. Miyazaki, T. Sakuma, and Y. Miyasaka, Ferroelectric Thin Films II, edited by A. I. Kingon, E. R. Myers, and B. Tuttle (Materials Research Society, Pittsburgh, 1992), p.281.
    • (1992) Ferroelectric Thin Films II , pp. 281
    • Matsubara, S.1    Miyazaki, S.2    Sakuma, T.3    Miyasaka, Y.4
  • 29
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    • The onset of additional conduction mechanisms in pore strontium titanate films above 200 kV/cm is also confirmed by
    • The onset of additional conduction mechanisms in pore strontium titanate films above 200 kV/cm is also confirmed by R. Waser and M. Klee, Integ. Ferroelec. 2, 23 (1992).
    • (1992) Integ. Ferroelec. , vol.2 , pp. 23
    • Waser, R.1    Klee, M.2
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    • The role of oxygen vacancies and resulting Schottky barriers is developed
    • by S. Triebwasser, Phys. Rev. 118, 100 (1960)
    • The role of oxygen vacancies and resulting Schottky barriers is developed by W. Kanzig, Phys. Rev. 98, 549 (1955) and by S. Triebwasser, Phys. Rev. 118, 100 (1960).
    • (1955) Phys. Rev. , vol.98 , pp. 549
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    • K. Carl and K.-H. Hardtl, 17, 473 (1978)
    • For the role of ionic vacancies in perovskites see also Y. V. Prisedsky, V. I. Shishkovsky, and V. V. Klimov, Ferroelectrics 17, 465 (1978), and also K. Carl and K.-H. Hardtl, Ferroelectrics 17, 473 (1978).
    • (1978) Ferroelectrics , vol.17 , pp. 465
    • Prisedsky, Y.V.1    Shishkovsky, V.I.2    Klimov, V.V.3
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    • Bethlehem, PA (IEEE, Piscataway, NJ, H. Ouchi and S. Kawashima, Jpn. J. Appl. Phys. 24, Suppl. 24-2, 60 (1985)
    • K. Wakino, Proc. Int Symp. Applic. Ferroelectrics (ISAF ‘86), Bethlehem, PA (IEEE, Piscataway, NJ, 1986), p.97; H. Ouchi and S. Kawashima, Jpn. J. Appl. Phys. 24, Suppl. 24-2, 60 (1985).
    • (1986) Proc. Int Symp. Applic. Ferroelectrics (ISAF ‘86) , pp. 97
    • Wakino, K.1


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