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1.
The superfluid transition temperature, Tc, is calculated from a scattering amplitude (constructed from the polarization potentials of Aldrich and Pines) which has been shown to yield agreement with experiment for transport properties. Our calculated values agree with experiment at all pressures up to 34 atm.  相似文献   

2.
K. Maki 《Physics letters. A》1973,46(3):173-174
Spin waves in the A phase of the superfluid 3He are studied within a microscopic model. It is shown that the spin wave mode with a phonon like dispersion and a gap exists through out the A phase.  相似文献   

3.
It is suggested that at a wave vector near the inverse average interparticle separation, the spectrum of a 3He atom in superfluid 4He has a roton like dip. The results of light scattering and transport measurements in liquid 3He-4He mixtures can thereby be reconciled.  相似文献   

4.
The Bose spectrum of superfluid solutions 3He4He is investigated in the case of p-pairing of Fermi particles. Both three-dimensional and two-dimensional models are considered. It is shown that the Bose-Fermi interaction changes the sound velocities in both subsystems. The other collective modes (17 in the 3D-model and 11 in the 2D-model) remain almost unchanged.  相似文献   

5.
The possibility of superfluidity of 3He in dilute solutions of 3He in liquid 4He is investigated, and the corresponding critical temperature is estimated. The results indicate S-state pairing, i.e., for small concentrations of 3He, the highest transition temperature is obtained for L = 0, but the obtained critical temperatures are very low.  相似文献   

6.
The contribution of the textures in the B-phase of superfluid 3He to the specific heat has been calculated. The specific heat is found to be divergent near Tc.  相似文献   

7.
J.W Serene  D Rainer 《Physics Reports》1983,101(4):221-311
We develop the quasiclassical theory for normal and superfluid liquid 3He using a systematic expansion in small parameters such as δ/EF, ?0?1/kF, etc., and paying particular attention to the high-energy renormalizations of the external pertubations and observables. We apply the general formalism to a number of more specific problems including the derivation of the non-linear quantum kinetic equation for normal 3He, the weak-coupling and strong-coupling free energies and static response functions for superfluid 3He, and the low-frequency and high-frequency dynamics of the superfluid phases. We also discuss extensions of the quasiclassical framework to cover strong short-ranged pertubations such as walls and ions, review recent phenomenological models for the quasiparticle scattering amplitude, and present a brief but self-contained derivation of the Keldysh perturbation theory for real-time Green's functions.  相似文献   

8.
We report the first measurements of the NMR frequency in 3He A and B under conditions where the net magnetization, M, is tipped far from its equilibrium direction along HO. In 3He A the frequency shift ω - γHO varies from the continuous wave value at tipping angle Φ = 0 to a negative shift at Φ = 180°. In 3He B no frequency shift is observed, however for Φ ? 100° a beat pattern is seen to develop in the free induction decay envelope.  相似文献   

9.
Transverse zero sound should propagate in superfluid 3He only in a rather narrow range below Tc.  相似文献   

10.
On the basis of the Hamiltonian technique equations describing hydrodynamics of anisotropic superfluid liquid 3HeA are obtained. The conservation laws are formulated. Expressions for dissipative terms are found.  相似文献   

11.
The spin contribution to the heat capacity and entropy of 3He has been singled out. With increasing T the spin entropy reaches a constant value, different from ln 2. The spin contribution ≈ ln T can be observed in the temperature dependence of the pressure.  相似文献   

12.
The quasiparticle interaction in liquid 3He is studied. It is shown that part of the interaction can be considered induced through the exchange of density and spin-density excitations. The coupling of these excitations to quasiparticles is shown to be given rigorously by the quasiparticle interaction itself in the long wavelength limit. The induced part of the interaction is then calculated by determining the density-density and spin-density-spin-density response functions assuming that the irreducible particle-hole vertex functions are frequency independent. The remainder of the interaction is shown to be given by a vertex function which does not have certain singularities and it is argued that it can be approximated by the Brueckner G-matrix. From the net interaction Landau parameters are extracted and compared with the experimentally known ones. Since the agreement was not satisfactory, the consequences of making a theory in terms of “paramagnons” is explored. This leads to much better numerical results, but the theory is less satisfactory. Consideration of the density-density response function arrived at here shows it to be similar to one proposed by Pines and Nozières [3, 24], who assumed a local relation between a density fluctuation and the potential it produces. We come to the conclusion that the numerical discrepancies between our calculated Landau parameters and the experimental ones probably arise from neglect of the exchange of two and more spin fluctuations. In the paper following this one, O. Sjöberg makes application of our theory to calculate the Landau parameters of nuclear matter. No “soft” excitations such as the spin fluctuations of liquid 3He exist in nuclear matter, and the theory appears to be quantitatively much better there, although some of the crucial Landau parameters are not directly measurable, and a direct check is not possible.  相似文献   

13.
Neutron inelastic scattering from 4He at T = 2.3 K shows that for Q ? 2 nm?1 “sound-wave” excitations propagate with the characteristics of ordinary or first sound while for Q ? 3 nm?1 they propagate with the characteristics of zero sound.  相似文献   

14.
The longitudinal relaxation time, T1, was measured in liquid 3He4He mixtures with molar concentrations of 3He of 0.12, 0.20 and 0.45 under saturated vapor pressure. λ-anomaly was clearly observed in the temperature dependence of T1.  相似文献   

15.
Existing second-sound velocity measurements are interpreted to imply an unexpectedly strong concentration dependence for the amplitude of ?s?.  相似文献   

16.
In this paper we present the first of two closely related studies devoted to the connection between the phenomenological hydrodynamics and microscopic theories of superfluid 3He. In this first part, we express in a systematical way all the phenomenological parameters appearing in the hydrodynamic equations in terms of microscopically well defined correlation functions. The method used for this purpose goes back to the work of Kadanoff and Martin on normal fluids and has recently been formulated in the framework of Mori's projector formalism by Forster. Apart from the assumptions about the structure of the superfluid phases of 3He and certain regularity assumptions about the collision-dominated part of the correlation functions, which have to be satisfied if the hydrodynamic limit exists at all, but which remain unproven, this part of our work is nearly exact. The only approximation made is the perturbative treatment of the very small magnetic dipole energy. The kO limit of various correlation functions is considered. Novel consequences of the directional long range order for the transverse momentum density correlation function of the A phase, which are unique to that phase, are obtained. The instantaneous reactive parameters of the system are expressed as equal time commutators and evaluated rigorously. Some reactive parameters, e.g. the one leading to “orbit waves” are shown to have a collisional part, which has not yet been evaluated in a microscopic theory. NMR is considered as the kO limit of spin wave resonances with an energy gap due to the magnetic dipole-dipole interaction at k = 0. The NMR linewidth is thereby fixed by the same transport parameter, which determines the spin wave damping in the theory where the gap is neglected. The relevant transport parameter is expressed along with all others by the rigorous Kubo formulae of the theory in which the magnetic dipole energy is neglected. The close analogy of the NMR linewidth parameter to transport parameters like the shear viscosity, which are measured in quite different experiments, is thereby elucidated. Further, approximate evaluations of the Kubo relations of these parameters, within a common microscopic approach will be given in a second related study.  相似文献   

17.
Equilibrium ferromagnetic ordering in liquid 3He at temperatures T ? 0.3 K due to long-wavelength spin fluctuations is predicted. The magnetocaloric effect and other thermodynamic properties of 3He↑ are discussed. The properties of 3He↑4He solutions are considered in the case of a restricted geometry.  相似文献   

18.
F.W. Nijhoff  H.W. Capel 《Physica A》1981,106(3):369-397
A rigorous expression is given for the free energy of a system of fermions in the presence of a magnetic field interacting via a pairing hamiltonian in the weak-coupling limit. Starting from this expression Landau expansions are derived in two special cases, i.e. the case of general l-wave pairing in zero field and the case of l = 1 pairing, which applies to liquid 3He, in non-zero field.  相似文献   

19.
Very long relaxation times τ were observed in our earlier specific heat measurements on liquid 3He/4He mixtures in two-phase-states near the tricritical temperature TO. It appear that 1/τ ∝ (TO ? T).  相似文献   

20.
The lifetime of electrons deposited on the liquid surface of 4He was measured. It is smaller than 8 μs at 0.5 K and, as is concluded from its temperature dependence, governed by the electronic mobility parallel to the superfluid surface.  相似文献   

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