scholarly journals One-particle density matrix and momentum distribution function of one-dimensional anyon gases

2008 ◽  
Vol 2008 (06) ◽  
pp. P06005 ◽  
Author(s):  
Raoul Santachiara ◽  
Pasquale Calabrese
2020 ◽  
Vol 8 (4) ◽  
Author(s):  
Oleksandr Gamayun ◽  
Oleg Lychkovskiy ◽  
Mikhail Zvonarev

We investigate the momentum distribution function of a single distinguishable impurity particle which formed a polaron state in a gas of either free fermions or Tonks-Girardeau bosons in one spatial dimension. We obtain a Fredholm determinant representation of the distribution function for the Bethe ansatz solvable model of an impurity-gas \deltaδ-function interaction potential at zero temperature, in both repulsive and attractive regimes. We deduce from this representation the fourth power decay at a large momentum, and a weakly divergent (quasi-condensate) peak at a finite momentum. We also demonstrate that the momentum distribution function in the limiting case of infinitely strong interaction can be expressed through a correlation function of the one-dimensional impenetrable anyons.


2015 ◽  
Vol 11 (3) ◽  
pp. 3091-3098
Author(s):  
Nelson Nenuwe ◽  
John O. A. Idiodi

Critical exponents at  and   for the momentum distribution function are studied for one-dimensional Hubbard model in the presence of magnetic field, using conformal field theory (CFT) approach. Exponents at  and  are reproduced. Results at  is in contrast to earlier numerical prediction of 1, while at , the exponent is 49/8. The singularities at  and  appears to be weak and gradually degenerating into a smooth curve.


Author(s):  
Yahya Younesizadeh ◽  
Fayzollah Younesizadeh

In this work, we study the differential scattering cross-section (DSCS) in the first-order Born approximation. It is not difficult to show that the DSCS can be simplified in terms of the system response function. Also, the system response function has this property to be written in terms of the spectral function and the momentum distribution function in the impulse approximation (IA) scheme. Therefore, the DSCS in the IA scheme can be formulated in terms of the spectral function and the momentum distribution function. On the other hand, the DSCS for an electron off the [Formula: see text] and [Formula: see text] nuclei is calculated in the harmonic oscillator shell model. The obtained results are compared with the experimental data, too. The most important result derived from this study is that the calculated DSCS in terms of the spectral function has a high agreement with the experimental data at the low-energy transfer, while the obtained DSCS in terms of the momentum distribution function does not. Therefore, we conclude that the response of a many-fermion system to a probe particle in IA must be written in terms of the spectral function for getting accurate theoretical results in the field of collision. This is another important result of our study.


1992 ◽  
Vol 46 (21) ◽  
pp. 14313-14316 ◽  
Author(s):  
Rajiv R. P. Singh ◽  
Rodney L. Glenister

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