Add to ORKGThe measured specific heat of normal liquid 3He shows a plateau for 0.15<1 K; below 0.15 K and above 1 K, it rises linearly with temperature. However, the slope on the high-temperature side is very much reduced compared with the free-Fermi-gas value. We explain these features through a microscopic, thermal spin- and density-fluctuation model. The plateau is due to spin fluctuations which have a low characteristic energy in 3He. Because of the low compressibility, the density fluctuations are highly suppressed; this leads to a reduced slope for CV(T) for high temperatures
We explain the anomalous temperature dependence of spin diffusion in liquid 3↑ and 3--4He mixtures. ...
The normal liquid helium 3 one-body momentum distribution, n(k), at zero and finite temperature is e...
The random-phase-approximation (RPA) dynamical response of liquid 3 He at finite temperatures has ...
The measured specific heat of normal liquid 3He shows a plateau for 0.15<1 K; below 0.15 K and above...
The measured specific heat of normal liquid 3He shows a plateau for 0.15<T<1 K; below 0.15 K a...
In this thesis I study two separate topics in many-body physics. In the first part I consider many-...
In this thesis I study two separate topics in many-body physics. In the first part I consider many-...
173 p.Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1986.In this thesis I study two se...
173 p.Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1986.In this thesis I study two se...
Below 1 K the thermal expansion coefficient α of Al3Ce is negative and linearly approaches zero at 0...
The spin susceptibility of nearly ferromagnetic Fermi systems, e.g., liquid <SUP>3</SUP>He, Pd, Ni<S...
Below 1 K the thermal expansion coefficient α of Al3Ce is negative and linearly approaches zero at 0...
In this paper, we report on the calculation of the constant volume specific heat Cv of liquid helium...
In this letter, I remark that normal liquid 3He can be described as a set of two levels systems, whi...
In this letter, I remark that normal liquid 3He can be described as a set of two levels systems, whi...
We explain the anomalous temperature dependence of spin diffusion in liquid 3↑ and 3--4He mixtures. ...
The normal liquid helium 3 one-body momentum distribution, n(k), at zero and finite temperature is e...
The random-phase-approximation (RPA) dynamical response of liquid 3 He at finite temperatures has ...
The measured specific heat of normal liquid 3He shows a plateau for 0.15<1 K; below 0.15 K and above...
The measured specific heat of normal liquid 3He shows a plateau for 0.15<T<1 K; below 0.15 K a...
In this thesis I study two separate topics in many-body physics. In the first part I consider many-...
In this thesis I study two separate topics in many-body physics. In the first part I consider many-...
173 p.Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1986.In this thesis I study two se...
173 p.Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1986.In this thesis I study two se...
Below 1 K the thermal expansion coefficient α of Al3Ce is negative and linearly approaches zero at 0...
The spin susceptibility of nearly ferromagnetic Fermi systems, e.g., liquid <SUP>3</SUP>He, Pd, Ni<S...
Below 1 K the thermal expansion coefficient α of Al3Ce is negative and linearly approaches zero at 0...
In this paper, we report on the calculation of the constant volume specific heat Cv of liquid helium...
In this letter, I remark that normal liquid 3He can be described as a set of two levels systems, whi...
In this letter, I remark that normal liquid 3He can be described as a set of two levels systems, whi...
We explain the anomalous temperature dependence of spin diffusion in liquid 3↑ and 3--4He mixtures. ...
The normal liquid helium 3 one-body momentum distribution, n(k), at zero and finite temperature is e...
The random-phase-approximation (RPA) dynamical response of liquid 3 He at finite temperatures has ...