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We give a concise review of the empirical properties of liquid and solid 3He-~He mixtures and their phenomenological interpretation.The bulk of the paper is about dilute solutions of 3He in liquid 4He at temperatures well below the tricritical point, where the roton and phonon excitations are comparatively unimportant. We describe the thermodynamic properties in terms of the Landau-Pomeranchuk 3He quasiparticles and the effective interaction between them, introduced by Emery and Bardeen, Baym and Pines. The scattering amplitude, needed to fit the low temperature transport properties, and the effective interaction are related, provided the multiple virtual scattering calculated by Fu and Pethick is included. The multiple scattering should always be included, even for very small concentrations. We present the evidence for the velocity dependence of the effective interaction, and urge that this also be taken into account in the interpretation of experiments. We give a short description of spin-polarized liquid mixtures and of the possibility of pairing superfluidity in solutions of He in liquid 4He. The existence of supersaturated solutions may be a way to attain p-wave pairing at accessible temperatures. Because of phase separation, the concentration of 4He in dilute mixtures 4 3 473 Van der Boog, Husson, Disatnik and Kramers [104] Esel'son, Nosovitskaya, Pogorelov and Sobolev [105] Spin diffusion coefficient Candela, McAlister, Wei and Vermeulen [89] Gully and Mullin [93] Murdock, Mountfield and Corruccini [107] Fenner and Luszczynski [106] Mass diffusion constant Vvedenskii and Peshkov [108] and Pobel [111] Magnetic susceptibility (by NMR) Ahonen, Paalanen, Richardson and Takano [65] 3" m an. .,..I TABLE I. Continued o~ Specific heat Owers-Bradley, Main, Bowley, Batey and Church [46] Van der Zeeuw, Mudde and Van Beelen [112] Polturak and Rosenbaum [113] Greywall [114] Phase separation Nakaumra, Fuji, Shigi and Nagao [140] Osmotic pressure Van de Klundert, Bos, Van der Meij and Steffens [116] Normal density p. Sobolev, Esel'snn, Nosovitskaya and Pogorelov [67] Pogoreiov, Esel'son, Nosovitskaya and Sobolev [66] Speeds of first and second sound u t, u 2 and attenuation o/l, Rudavskii, Chagovets and Sheshin [ 118] Wiegers, Jochemsen, Kranenburg and Frossati [84] Adamenko, Rudavskii, Tsyganok and Chagovets [119] Chagovets, Rudavskii and Goncharov [121] Rudavskii and Chagovets [120] Grivor'ev, Dyumin, Dikina and Svatko [179] Rudavskii and Chagovets [103] Greywali and Paalanen [85] [91] Dyumin, Esel'son, Dikina and Kotenev [122] Van der Boog, Husson, Disatnik and Kramers [104] Greywall [124] Van der Boog, Husson and Kramers [123] de Voogt, de Haas, Weiber and Kramers [126] de Voogt and Kramers [127] Rockwell, Benjamin and Greytak [125] X = 0.44-2.6% X =0.6-0.85% X=3-5% X
We give a concise review of the empirical properties of liquid and solid 3He-~He mixtures and their phenomenological interpretation.The bulk of the paper is about dilute solutions of 3He in liquid 4He at temperatures well below the tricritical point, where the roton and phonon excitations are comparatively unimportant. We describe the thermodynamic properties in terms of the Landau-Pomeranchuk 3He quasiparticles and the effective interaction between them, introduced by Emery and Bardeen, Baym and Pines. The scattering amplitude, needed to fit the low temperature transport properties, and the effective interaction are related, provided the multiple virtual scattering calculated by Fu and Pethick is included. The multiple scattering should always be included, even for very small concentrations. We present the evidence for the velocity dependence of the effective interaction, and urge that this also be taken into account in the interpretation of experiments. We give a short description of spin-polarized liquid mixtures and of the possibility of pairing superfluidity in solutions of He in liquid 4He. The existence of supersaturated solutions may be a way to attain p-wave pairing at accessible temperatures. Because of phase separation, the concentration of 4He in dilute mixtures 4 3 473 Van der Boog, Husson, Disatnik and Kramers [104] Esel'son, Nosovitskaya, Pogorelov and Sobolev [105] Spin diffusion coefficient Candela, McAlister, Wei and Vermeulen [89] Gully and Mullin [93] Murdock, Mountfield and Corruccini [107] Fenner and Luszczynski [106] Mass diffusion constant Vvedenskii and Peshkov [108] and Pobel [111] Magnetic susceptibility (by NMR) Ahonen, Paalanen, Richardson and Takano [65] 3" m an. .,..I TABLE I. Continued o~ Specific heat Owers-Bradley, Main, Bowley, Batey and Church [46] Van der Zeeuw, Mudde and Van Beelen [112] Polturak and Rosenbaum [113] Greywall [114] Phase separation Nakaumra, Fuji, Shigi and Nagao [140] Osmotic pressure Van de Klundert, Bos, Van der Meij and Steffens [116] Normal density p. Sobolev, Esel'snn, Nosovitskaya and Pogorelov [67] Pogoreiov, Esel'son, Nosovitskaya and Sobolev [66] Speeds of first and second sound u t, u 2 and attenuation o/l, Rudavskii, Chagovets and Sheshin [ 118] Wiegers, Jochemsen, Kranenburg and Frossati [84] Adamenko, Rudavskii, Tsyganok and Chagovets [119] Chagovets, Rudavskii and Goncharov [121] Rudavskii and Chagovets [120] Grivor'ev, Dyumin, Dikina and Svatko [179] Rudavskii and Chagovets [103] Greywali and Paalanen [85] [91] Dyumin, Esel'son, Dikina and Kotenev [122] Van der Boog, Husson, Disatnik and Kramers [104] Greywall [124] Van der Boog, Husson and Kramers [123] de Voogt, de Haas, Weiber and Kramers [126] de Voogt and Kramers [127] Rockwell, Benjamin and Greytak [125] X = 0.44-2.6% X =0.6-0.85% X=3-5% X
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