[1] W. Lenz : Physik. Z. 21, 613 (1920) ; E. Ising : Beitrag zur Theorie des Ferromagnetismus, Zeits. f. Physik A 31, 253 (1925). Ising模型.
[2] W. Heisenberg : Mehrkorperproblem und Resonanz in der Quantenmechanik, Zeits. f. Physik A 38, 411 (1926). Heisenberg模型 (交換相互作用).
[3] P. Zeeman : On the influence of magnetism on the nature of the light emitted by a substance, Phil. Mag. 43, 226 (1897). Zeeman効果.
[4] R. Peierls : On Ising's model of ferromagnetism, Proc. Cambidge Phil. Soc. 32, 477 (1936). Peierlsの議論.
[5] R. B. Griffiths : Peierls proof of spontaneous magnetization in a twodimensional Ising ferromagnet, Phys. Rev. 136, A437 (1964). 2次元Ising模型における自発磁化の存在証明.
[6] C. N. Yang and T. D. Lee : Statistical theory of equations of state and phase transitions. I. Theory of condensation, Phys. Rev. 87, 404 (1952) ; T. D. Lee and C. N. Yang : Statistical theory of equations of state and phase transitions. II. Lattice gas and Ising model, Phys. Rev. 87, 410 (1952). Lee-Yangゼロ, 格子気体模型.
[7] M. E. Fisher : The nature of critical points, Lectures in Theoretical Physics Vol. 7c, edited by W. E. Brittin (University of Colorado Press, 1965). Fisherゼロ.
[8] R. B. Griffiths : Spontaneous magnetization in idealized ferromagnets, Phys. Rev. 152, 240 (1966). 長距離秩序と自発磁化の関係.
[9] P. Weiss : L'hypoth`ese du champ moleculaire et la propriete ferromagnetique, J. Phys. Theor. Appl. 6, 661 (1907). 分子場近似.
[10] K. Husimi : Proc. Int. Conf. Theor. Phys. 531 (1953) ; H. N. V. Temperley : The Mayer theory of condensation tested against a simple model of the imperfect gas, Proc. Phys. Soc. A 67, 233 (1954). 伏見-Temperley模型.
[11] R. P. Feynman : Slow electrons in a polar crystal, Phys. Rev. 97, 660 (1955). 変分法を用いた電子系基底状態のエネルギー.
[12] J. W. Gibbs : Elementary principles in statistical mechanics (Cambridge University Press, 1902) ; N. N. Bogoliubov : Dokl. Akad. Nauk USSR 119, 244 (1958) [Soviet Phys. Doklady 3, 292 (1958)]. Gibbs-Bogoliubovの不等式.
[13] L. D. Landau : On the theory of phase transitions Part I, Sov. Phys. JETP 7, 19 (1937) ; On the theory of phase transitions Part II, Sov. Phys. JETP 7, 627 (1937). Landau理論.
[14] V. L. Ginzburg and L. D. Landau : On the theory of superconductivity, Sov. Phys. JETP 20, 1064 (1950). Ginzburg-Landau理論.
[15] L. S. Ornstein and F. Zernike : Proc. Acad. Sci. Amsterdam 17, 793 (1914). Ornstein-Zernike方程式.
[16] R. L. Stratonovich : Soviet Phys. Doklady 2, 416 (1958) ; J. Hubbard : Calculation of partition functions, Phys. Rev. Lett. 3, 77 (1959). Hubbard-Stratonovich変換.
[17] V. L. Ginzburg : Soviet Physics-Solid State 2, 1824 (1960). Ginzburgの基準.
[18] A. Nordsieck, W. E. Lamb Jr., G. E. Uhlenbeck : On the theory of cosmicray showers I The Furry model and the fluctuation problem, Physica 7, 344 (1940). マスター方程式.
[19] R. J. Glauber : Time-dependent statistics of the Ising model, J. Math. Phys. 4, 294 (1963). Glauber ダイナミクス. Ising模型の動的効果.
[20] P. Langevin : C. R. Acad. Sci. (Paris) 146, 530 (1908). Langevin方程式.
[21] A. Einstein : Uber die von der molekularkinetischen Theorie der Warme geforderte Bewegung von in ruhenden Flussigkeiten suspendierten Teilchen, Annalen der Physik 322, 549 (1905). Brown運動の理論.
[22] A. D. Fokker : Annalen der Physik 348, 810 (1914) ; M. Planck : Sitzungsber. Preuss. Akad. Wiss. Phys. Math. Kl. 23, 324 (1917). Fokker-Planck方程式.
[23] B. I. Halperin, P. C. Hohenberg, and S. K. Ma : Calculation of dynamic critical properties using Wilson's expansion methods, Phys. Rev. Lett. 29, 1548 (1972). 時間依存Ginzburg-Landau模型を用いたスピン系のLangevinダイナミクス.
[24] L. Onsager : Crystal statistics. I. A two-dimensional model with an orderdisorder transition, Phys. Rev. 65, 117 (1944). 2次元Ising模型の厳密解.
[25] H. A. Kramers and G. H. Wannier : Statistics of the two-dimensional ferromagnet. Part I, Phys. Rev. 60, 252 (1941). 2次元Ising模型の双対性.
[26] M. Kac and J. C. Ward : A combinatorial solution of the two-dimensional Ising model, Phys. Rev. 88, 1332 (1952). 2次元Ising模型の高温展開.
[27] C. N. Yang : The spontaneous magnetization of a two-dimensional Ising model, Phys. Rev. 85, 808 (1952). 2次元Ising模型の自発磁化.
[28] T. H. Berlin and M. Kac : The spherical model of a ferromagnet, Phys. Rev. 86, 821 (1952) ; H.E. Stanley : Spherical model as the limit of infinite spin dimensionality, Phys. Rev. 176, 718 (1968). 球形模型.
[29] G. S. Rushbrooke : On the thermodynamics of the critical region for the Ising problem, J. Chem. Phys. 39, 842 (1963). 臨界指数不等式.
[30] B. Widom : Equation of state in the neighborhood of the critical point, J. Chem. Phys. 43, 3898 (1965). スケーリング仮説.
[31] A. Z. Patashinskii and V. L. Pokrovskii : Behavior of ordered systems near the transition point, Sov. Phys. JETP 23, 292 (1966). スケーリング理論.
[32] L. P. Kadanoff : Scaling laws for Ising models near Tc, Physics 2, 263 (1966). 粗視化の方法, スケーリング理論. 著者のWebサイトからダウンロード可 (http://jfi.uchicago.edu/~leop/ の "Oldies But Goodies").
[33] R. B. Griffiths : Thermodynamic inequality near the critical point for ferromagnets and fluids, Phys. Rev. Lett. 14, 623 ; Ferromagnets and simple fluids near the critical point : some thermodynamic inequalities, J. Chem. Phys. 43, 1958 (1965). 臨界指数不等式.
[34] M. E. Fisher : Rigorous inequalities for critical-point correlation exponents, Phys. Rev. 180, 594 (1969). 臨界指数不等式.
[35] B. D. Josephson : Inequality for the specific heat I. Derivation, Proc. Phys. Soc. 92, 269 (1967) ; Inequality for the specific heat II. Application to critical phenomena, Proc. Phys. Soc. 92, 276 (1967). 臨界指数不等式.
[36] K. G. Wilson : Renormalization group and critical phenomena. I. Renormalization group and the Kadanoff scaling picture, Phys. Rev. B 4, 3174 (1971) ; Renormalization group and critical phenomena. II. Phase-space cell analysis of critical behavior, Phys. Rev. B 4, 3184 (1971). くりこみ群.
[37] G. H. Wannier : The statistical problem in cooperative phenomena, Rev. Mod. Phys. 17, 50 (1945). 2次元Ising模型の双対性.
[38] A. A. Migdal : Zh. Eksp. Teor. Fiz. 69, 810, 1457 (1975) ; L. P. Kadanoff : Notes on Migdal's recursion formulas, Ann. Phys. (N.Y.) 100, 359 (1976). Migdal-Kadanoff くりこみ群.
[39] K. G. Wilson and M. E. Fisher : Critical exponents in 3.99 dimensions, Phys. Rev. Lett. 28, 240 (1972). e展開.
[40] G. C. Wick : The Evaluation of the collision matrix, Phys. Rev. 80, 268 (1950) ; C. Bloch and C. de Dominicis : Un developpement du potentiel de Gibbs d'un systeme quantique compose d'un grand nombre de particules, Nucl. Phys. 7, 459 (1958). Wick/Bloch-de Dominicisの定理.
[41] R. P. Feynman : Space-time approach to quantum electrodynamics, Phys. Rev. 76, 769 (1949). Feynman ダイアグラム.
[42] J. C. Le Guillou and J. Zinn-Justin : Critical exponents from field theory, Phys. Rev. B 21, 3976 (1980). φ4模型の高次項計算.
[43] A. Pelissetto and E. Vicari : Critical phenomena and renormalization-group theory, Phys. Rep. 368, 549 (2002). さまざまな計算によって得られた臨界指数の値のまとめ.
[44] K. G. Wilson : Non-Lagrangian models of current algebra, Phys. Rev. 179, 1499 (1969) ; L. P. Kadanoff : Operator algebra and the determination of critical indices, Phys. Rev. Lett. 23, 1430 (1969). 演算子積展開.
[45] A. M. Polyakov : Conformal symmetry of critical fluctuations, JETP Lett. 12, 381 (1970). 共形不変性.
[46] A. A. Belavin, A. M. Polyakov, and A. B. Zamolodchikov : Infinite conformal symmetry in two-dimensional quantum field theory, Nucl. Phys. B 241, 333 (1984). 共形場理論.
[47] Y. Nambu : Quasi-particles and gauge invariance in the theory of superconductivity, Phys. Rev. 117, 648 (1960) ; J. Goldstone : Field theories with superconductor solutions, Nuovo Cimento 19, 154 (1961) ; J. Goldstone, A. Salam, and S. Weinberg : Broken symmetries, Phys. Rev. 127, 965 (1962). 南部-Goldstoneモード, Goldstoneの定理.
[48] N. D. Mermin and H. Wagner : Absence of ferromagnetism or antiferromagnetism in one- or two-dimensional isotropic Heisenberg models, Phys. Rev. Lett. 17, 1133 (1966) ; N. D. Mermin : Absence of ordering in certain classical systems, J. Math. Phys. 8, 1061 (1967) ; P. C. Hohenberg : Existence of long-range order in one and two dimensions, Phys. Rev. 158, 383 (1967). Mermin-Wagner-Hohenbergの定理.
[49] J. Frohlich, B. Simon, and T. Spencer : Infrared bounds, phase transitions and continuous symmetry breaking, Comm. Math. Phys. 50, 79 (1976) ; F. Dyson, E. H. Lieb, and B. Simon : Phase transitions in quantum spin systems with isotropic and nonisotropic interactions, J. Stat. Phys. 18, 335 (1978). 3次元以上Heisenberg模型の秩序相の存在証明.
[50] V. L. Berezinskii : Destruction of long-range order in one-dimensional and two-dimensional systems having a continuous symmetry group I. Classical systems, Sov. Phys. JETP 32, 493 (1971) ; Destruction of long-range order in one-dimensional and two-dimensional systems having a continuous symmetry group II. Quantum systems, Sov. Phys. JETP 34, 610 (1972) ; J. M. Kosterlitz and D. J. Thouless : Ordering, metastability and phase transitions in two-dimensional systems, J. Phys. C : Solid State Phys. 6, 1181 (1973). Berezinskii-Kosterlitz-Thouless転移.
[51] J. Villain : J. Phys. France 36, 581 (1975). Villain模型.
[52] J. B. Kogut : An introduction to lattics gauge theory and spin systems, Rev. Mod. Phys. 51, 659 (1979). スピン系の解説論文. Berezinskii-Kosterlitz-Thouless転移のくりこみ群.
[53] J. V. Jose, L. P. Kadanoff, S. Kirkpatrick, and D. R. Nelson : Renormalization, vortices, and symmetry-breaking perturbations in the two-dimensional planar model, Phys. Rev. B 16, 1217 (1977). Berezinskii-Kosterlitz-Thouless転移のくりこみ群.
[54] M. Gell-Mann and M. Levy : The axial vector current in beta decay, Nuovo Cimento 16, 705 (1960). 非線形シグマ模型.
[55] F. J. Wegner and A. Houghton : Renormalization group equation for critical phenomena, Phys.Rev.A8, 401 (1973) ; J. Polchinski : Renormalization and effective Lagrangians, Nucl. Phys. B 231, 269 (1984) ; C. Wetterich : Exact evolution for the effective potential, Phys. Lett. B 301, 90 (1993). 汎関数くりこみ群.
[56] E. C. G. Stueckelberg and A. Petermann : La normalisation des constantes dans la theorie des quanta, Helv. Phys. Acta 26, 499 (1953) ; M. Gell-Mann and F. E. Low : Quantum electrodynamics at small distances, Phys.Rev. 95, 1300 (1954) ; N. N. Bogoljubov and D. V. Shirkov : Charge renormalization group in quantum field theory, Nuovo Cimento 3, 845 (1956). 場の理論的くりこみ群.
[57] L. Y. Chen, N. Goldenfeld, and Y. Oono : Renormalization group theory for global asymptotic analysis, Phys. Rev. Lett. 73, 1311 (1994). 微分方程式のくりこみ群解析.
[58] T. Kunihiro : A geometrical formulation of the renormalization group method for global analysis, Prog. Theor. Phys. 94, 503 (1995). 微分方程式のくりこみ群解析と包絡線方程式.
[59] F. Bloch : Zur Theorie des Ferromagnetismus, Z. Physik 61, 206 (1930) ; G. Heller and H. A. Kramers : Ein klassisches Modell des Ferromagnetikums und seine nachtr¨agliche Quantisierung im Gebiete tiefer Temperaturen, Proc. Roy. Acad. Sci. Amsterdam 37, 378 (1934) ; P. W. Anderson : An approximate quantum theory of the antiferromagnetic ground state, Phys. Rev. 86, 694 (1952) ; R. Kubo : The spin-wave theory of antiferromagnetics, Phys. Rev. 87, 568 (1952). スピン波の理論.
[60] T. Holstein and H. Primakoff : Field dependence of the intrinsic domain magnetization of a ferromagnet, Phys. Rev. 58, 1098 (1940). Holstein-Primakoff変換.
[61] H. B. Nielsen and S. Chadha : On how to count Goldstone bosons, Nucl. Phys. B 105, 445 (1976). 南部-Goldstoneモードの数と分散の関係.
[62] H. Watanabe and H. Murayama : Unified description of Nambu-Goldstone bosons without Lorentz invariance, Phys. Rev. Lett. 108, 251602 (2012) ; Y. Hidaka : Counting rule for Nambu-Goldstone modes in nonrelativistic systems, Phys. Rev. Lett. 110, 091601 (2013). 南部-Goldstoneモードの数と生成子の数の関係.
[63] H. Wagner : Long-wavelength excitations and the Goldstone theorem in many-particle systems with "broken symmetries," Zeit. f. Physik 195, 273 (1966). スピン波のふるまいについて.
[64] T. Matsubara : A new approach to quantum-statistical mechanics, Prog. Theor. Phys. 14, 351 (1955). 虚時間形式による量子統計力学.
[65] H. F. Trotter : On the product of semi-groups of operators, Proc. Amer. Math. Soc. 10, 545 (1959) ; M. Suzuki : Relationship between d-dimensional quantal spin systems and (d+1) -dimensional Ising systems, Prog. Theor. Phys. 56, 1454 (1976). 鈴木-Trotter分解.
[66] P. Jordan and E. Wigner : Uber das Paulische Aquivalenzverbot, Zeits. f. Physik A 47, 631 (1928) ; E. Lieb, T. Schultz, and D. Mattis : Two soluble models of an antiferromagnetic chain, Ann. Phys. (N.Y.) 16, 407 (1961). Jordan-Wigner変換.
[67] J. Schwinger : On angular momentum (Harvard University, 1952) [in Quantum theory of angular momentum, edited by L. C. Biedenharn and H. Van Dam (Academic Press, 1965)]. Schwingerボソン.
[68] N. Metropolis, A. W. Rosenbluth, M. N. Rosenbluth, A. H. Teller, and E. Teller : Equation of state calculations by fast computing machines, J. Chem. Phys. 21, 1087 (1953) ; W. K. Hastings : Biometrika 57, 97 (1970). Metropolis-Hastingsアルゴリズム.
[69] M. Creutz : Microcanonical Monte Carlo simulation, Phys. Rev. Lett. 50, 1411 (1983). デーモンアルゴリズム.
[70] A. Kitaev : Anyons in an exactly solved model and beyond, Ann. Phys. 321, 2 (2006). Kitaev模型.