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The dispersion of3He quasiparticles in He II from neutron scattering
Authors:R Scherm  K Guckelsberger  A Szprynger  B Fåk
Affiliation:(1) Phys.-Tech. Bundesanstalt, 3300 Braunschweig, Germany;(2) W. Trzebiatowski Institute of Low Temperature and Structure Research, 50-950 Wroclaw, Poland;(3) CENG, DRFMC/SPSMS/MDN, 85X 38041 Grenoble-Cedex, France
Abstract:In an inelastic neutron scattering (INS) experiment on3He-4He mixtures one observes, besides the photon-roton mode which is barely modified by the admixture of3He, an additional excitation at lower energies which is interpreted as quasi-particle-hole excitations of a nearly free Fermi gas. We reanalyse INS data ofx 3=1% and 4.5% mixtures at various pressures to extract the mean energy 
$$\hat \omega _q $$
of the fermions. In the momentum range 9<q<17 nm–1 (above 2k F ) 
$$\hat \omega _q $$
follows very closely the relation 
$$\hat \omega _q $$
=A 2 q 2+A 4 q 4 at all concentrations, pressures and temperatures observed. In a 4.5% mixture (T F ap0.3 K), measurements were performed for temperatures in the range 0.07<T<0.9 K. We find bothA 2 andA 4 to be strongly temperature dependent. For the interpretation of thermodynamical properties, the single particle energy epsi k is parametrized as epsi k =epsio+1/(2ms*) ·k 2 · (1+gammak 2). Neglecting interactions between fermions, we calculate from the free-particle epsi k the scattering functionS(q, ohgr) and the mean value of the fermion peak energy ohgr q =int ohgrS 3(q, ohgr)dohgr/intS 3(q, ohgr)dohgr. We find that 
$$\hat \omega _q $$
follows closely epsi q , deviating at most by 10%. A comparison to the measuredA 2 andA 4 directly yieldsms* (x 3,p, T) and gamma(x 3,p, T). In the limitx 3=0,p=0 andT=0, the density and concentration dependence of the inertial mass is in excellent agreement with values found by Sherlock and Edwards. The temperature dependence of the specific heat data from Greywall and Owers-Bradleyet al. are well represented by our model atT<0,5 K.
Keywords:
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