scholarly journals Finite-range effects in the two-dimensional repulsive Fermi polaron

2021 ◽  
Vol 103 (4) ◽  
Author(s):  
Raúl Bombín ◽  
Viktor Cikojević ◽  
Juan Sánchez-Baena ◽  
Jordi Boronat
2018 ◽  
Vol 108 (8) ◽  
pp. 1837-1849 ◽  
Author(s):  
Marcel Griesemer ◽  
Ulrich Linden

2019 ◽  
Vol 4 (1) ◽  
pp. 20 ◽  
Author(s):  
Andrea Tononi

We derive the two-dimensional equation of state for a bosonic system of ultracold atoms interacting with a finite-range effective interaction. Within a functional integration approach, we employ a hydrodynamic parameterization of the bosonic field to calculate the superfluid equations of motion and the zero-temperature pressure. The ultraviolet divergences, naturally arising from the finite-range interaction, are regularized with an improved dimensional regularization technique.


1992 ◽  
Vol 46 (24) ◽  
pp. 15726-15738 ◽  
Author(s):  
M. T. Béal-Monod ◽  
A. Theumann ◽  
G. Forgacs

The wind-tunnel corrections to the lift and moment acting on an aerofoil in a subsonic two-dimensional flow, and situated midway between tunnel walls containing porous sections are calculated. The tunnel walls are taken to be porous over only a finite range R , and solid else­where, and sealed jackets over the porous sections enable the pressures on the outsides of these sections to be controlled. The porous wall is assumed to be of such a construction that the component of velocity normal to it is proportional to the pressure drop across it. Infinite porosity and zero porosity correspond to free streamline and solid-wall boundaries respectively, which are thus included in the theory as special cases. This paper is complementary to an earlier contribution (Woods 1955 c ) in which only the ‘blockage’, or average velocity increment at the model caused by the tunnel walls, was studied.


2019 ◽  
Vol 216 (3) ◽  
pp. 661-743 ◽  
Author(s):  
Michael Aizenman ◽  
Hugo Duminil-Copin ◽  
Vincent Tassion ◽  
Simone Warzel

1982 ◽  
Vol 117 ◽  
pp. 171-185 ◽  
Author(s):  
P. G. Saffman ◽  
J. C. Schatzman

The stability of the finite-area Kármán ‘vortex street’ to two-dimensional disturbances is determined. It is shown that for vortices of finite size there exists a finite range of spacing ratio κ for which the array is stable to infinitesimal disturbances. As the vortex size approaches zero, the range narrows to zero width about the classical von Kármán value of 0·281.


1966 ◽  
Vol 24 ◽  
pp. 118-119
Author(s):  
Th. Schmidt-Kaler

I should like to give you a very condensed progress report on some spectrophotometric measurements of objective-prism spectra made in collaboration with H. Leicher at Bonn. The procedure used is almost completely automatic. The measurements are made with the help of a semi-automatic fully digitized registering microphotometer constructed by Hög-Hamburg. The reductions are carried out with the aid of a number of interconnected programmes written for the computer IBM 7090, beginning with the output of the photometer in the form of punched cards and ending with the printing-out of the final two-dimensional classifications.


1966 ◽  
Vol 24 ◽  
pp. 3-5
Author(s):  
W. W. Morgan

1. The definition of “normal” stars in spectral classification changes with time; at the time of the publication of theYerkes Spectral Atlasthe term “normal” was applied to stars whose spectra could be fitted smoothly into a two-dimensional array. Thus, at that time, weak-lined spectra (RR Lyrae and HD 140283) would have been considered peculiar. At the present time we would tend to classify such spectra as “normal”—in a more complicated classification scheme which would have a parameter varying with metallic-line intensity within a specific spectral subdivision.


1966 ◽  
Vol 25 ◽  
pp. 46-48 ◽  
Author(s):  
M. Lecar

“Dynamical mixing”, i.e. relaxation of a stellar phase space distribution through interaction with the mean gravitational field, is numerically investigated for a one-dimensional self-gravitating stellar gas. Qualitative results are presented in the form of a motion picture of the flow of phase points (representing homogeneous slabs of stars) in two-dimensional phase space.


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