Π”ΠΈΠΏΠ»ΠΎΠΌΡ‹, курсовыС, Ρ€Π΅Ρ„Π΅Ρ€Π°Ρ‚Ρ‹, ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒΠ½Ρ‹Π΅...
Брочная ΠΏΠΎΠΌΠΎΡ‰ΡŒ Π² ΡƒΡ‡Ρ‘Π±Π΅

ΠšΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Π΅ Ρ„Π°Π·ΠΎΠ²Ρ‹Π΅ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Ρ‹ ΠΈ Π½ΠΈΠ·ΠΊΠΎΡ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Π΅ свойства ΠΌΠ°Π³Π½Π΅Ρ‚ΠΈΠΊΠΎΠ² с Ρ†Π΅Π»Ρ‹ΠΌ спином ΠΈ большой ΠΎΠ΄Π½ΠΎΠΈΠΎΠ½Π½ΠΎΠΉ Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠΈΠ΅ΠΉ Ρ‚ΠΈΠΏΠ° «лСгкая ΠΏΠ»ΠΎΡΠΊΠΎΡΡ‚ΡŒΒ»

Π”ΠΈΡΡΠ΅Ρ€Ρ‚Π°Ρ†ΠΈΡΠŸΠΎΠΌΠΎΡ‰ΡŒ Π² Π½Π°ΠΏΠΈΡΠ°Π½ΠΈΠΈΠ£Π·Π½Π°Ρ‚ΡŒ ΡΡ‚ΠΎΠΈΠΌΠΎΡΡ‚ΡŒΠΌΠΎΠ΅ΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹

Ishida T., Nakamura T., Fujii Y. et al.- NMR Study of Field Induced 2-Step Phase Transition in Singlet-Ground-State Antiferromagnet CsFeBr3 // Progress of Theoretical Physics Supplement. 2002. — Vol. 145. — Pp. 134βˆ’137. Borner B., Visser B., Steigenberger U. et aiMagnetic excitations in the quasi one-dimensional antiferromagnetic singlet groundstate system CsFeBr3 // Physica B: Condensed Matter… Π§ΠΈΡ‚Π°Ρ‚ΡŒ Π΅Ρ‰Ρ‘ >

Π‘ΠΎΠ΄Π΅Ρ€ΠΆΠ°Π½ΠΈΠ΅

  • Π“Π»Π°Π²Π° I. Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅
    • 1. 1. ЦСль диссСртационной Ρ€Π°Π±ΠΎΡ‚Ρ‹
    • 1. 2. ΠšΡ€Π°Ρ‚ΠΊΠΎΠ΅ содСрТаниС диссСртации
  • Π“Π»Π°Π²Π° II. Π’Π΅Ρ…Π½ΠΈΠΊΠ° ΠΈ Π΅Ρ‘ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΡ€ΠΈ Π’ = О
    • 2. 1. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½ΠΈΠ΅ спиновых ΠΎΠΏΠ΅Ρ€Π°Ρ‚ΠΎΡ€ΠΎΠ²
    • 2. 2. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΈ
      • 2. 2. 1. Elementary excitation spectrum
      • 2. 2. 2. ЭнСргия основного состояния
    • 2. 3. ΠžΠ±ΡΡƒΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΈ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΠ΅ с ΠΏΡ€Π΅Π΄Ρ‹Π΄ΡƒΡ‰ΠΈΠΌΠΈ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌΠΈ ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚ΠΎΠΌ
      • 2. 3. 1. Π”Ρ€ΡƒΠ³ΠΈΠ΅ спиновыС прСдставлСния для S =
      • 2. 3. 2. Π”Ρ€ΡƒΠ³ΠΈΠ΅ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Ρ‹ ΠΊ Π²Ρ‹Ρ‡ΠΈΡΠ»Π΅Π½ΠΈΡŽ спСктра
      • 2. 3. 3. Π‘Ρ€Π°Π²Π½Π΅Π½ΠΈΠ΅ с Ρ‡ΠΈΡΠ»Π΅Π½Π½Ρ‹ΠΌΠΈ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌΠΈ
      • 2. 3. 4. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΊ NiCl2−4SC (NH2)
  • Π“Π»Π°Π²Π° III. ΠŸΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ Π² ΡƒΠΏΠΎΡ€ΡΠ΄ΠΎΡ‡Π΅Π½Π½ΡƒΡŽ Ρ„Π°Π·Ρƒ
    • 3. 1. ΠœΠΎΠ΄ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΡ Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΈ Π² ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠΌ ΠΏΠΎΠ»Π΅
    • 3. 2. Π’ = 0 and Н Ρ„
    • 3. 3. Π’Ρ„ 0 and Π― ~ НБ1 (0)
    • 3. 4. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΊ DTN.Β¦
  • Π“Π»Π°Π²Π° IV. Анализ скошСнной Π°Π½Ρ‚ΠΈΡ„Π΅Ρ€Ρ€ΠΎΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠΉ Ρ„Π°Π·Ρ‹ ΠΈ ΠΎΠΊΡ€Π΅ΡΡ‚ности поля насыщСния ΠΏΡ€ΠΈ Π’ =
    • 4. 1. Π‘ΠΏΠΈΠ½-Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ Π°Π½Π°Π»ΠΈΠ·
    • 4. 2. ΠžΠΊΡ€Π΅ΡΡ‚Π½ΠΎΡΡ‚ΡŒ поля насыщСния
    • 4. 3. ΠžΠ±ΡΡƒΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΈ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΊ DTN

ΠšΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Π΅ Ρ„Π°Π·ΠΎΠ²Ρ‹Π΅ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Ρ‹ ΠΈ Π½ΠΈΠ·ΠΊΠΎΡ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Π΅ свойства ΠΌΠ°Π³Π½Π΅Ρ‚ΠΈΠΊΠΎΠ² с Ρ†Π΅Π»Ρ‹ΠΌ спином ΠΈ большой ΠΎΠ΄Π½ΠΎΠΈΠΎΠ½Π½ΠΎΠΉ Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠΈΠ΅ΠΉ Ρ‚ΠΈΠΏΠ° «лСгкая ΠΏΠ»ΠΎΡΠΊΠΎΡΡ‚ΡŒΒ» (Ρ€Π΅Ρ„Π΅Ρ€Π°Ρ‚, курсовая, Π΄ΠΈΠΏΠ»ΠΎΠΌ, ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒΠ½Π°Ρ)

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ΠŸΠΎΠΊΠ°Π·Π°Ρ‚ΡŒ вСсь тСкст
Π—Π°ΠΏΠΎΠ»Π½ΠΈΡ‚ΡŒ Ρ„ΠΎΡ€ΠΌΡƒ Ρ‚Π΅ΠΊΡƒΡ‰Π΅ΠΉ Ρ€Π°Π±ΠΎΡ‚ΠΎΠΉ