scholarly journals Singlet Mott state simulating the bosonic Laughlin wave function

2014 ◽  
Vol 89 (4) ◽  
Author(s):  
Biao Lian ◽  
Shoucheng Zhang
1993 ◽  
Vol 07 (10) ◽  
pp. 679-687
Author(s):  
SHAOJIN QIN ◽  
ZHAOBIN SU ◽  
BINGSHEN WANG

We show that, up to a global phase freedom, the most probable distribution of electrons given by the maxima of modulus square of Laughlin wave function (LWF), which is known to be a wave function for an incompressible liquid state of fractional Hall effect, has a triangular lattice structure. We introduce the Gaussian approximation for the modulus square of LWF. We find that the radial distribution function calculated from the Gaussian approximation has a form close to that of LWF at ν = 1, 1/3 and close to a crystal-like behavior when ν becomes smaller. We interprete the underlying physics to be that in the incompressible liquid regime, the "hidden" triangular lattice is smeared away by the quantum phase fluctuation, and as a precursor for liquid-crystal transition when the filling ν decreases towards the crystallization regime, it might manifest itself to be a sort of correlated short-range ordered density fluctuation.


1995 ◽  
Vol 52 (19) ◽  
pp. 13742-13744 ◽  
Author(s):  
Prasanta K. Panigrahi ◽  
M. Sivakumar

2017 ◽  
Vol 19 (8) ◽  
pp. 083019
Author(s):  
Jiang-Min Zhang ◽  
Yu Liu

2004 ◽  
Vol 18 (20n21) ◽  
pp. 2771-2817 ◽  
Author(s):  
HONG-YI FAN

We review how to rely on the quantum entanglement idea of Einstein–Podolsky–Rosen and the developed Dirac's symbolic method to set up two kinds of entangled state representations for describing the motion and states of an electron in uniform magnetic field. The entangled states can be employed for conveniently expressing Landau wave function and Laughlin wave function with a fresh look. We analyze the entanglement involved in electron's coordinates (or momenta) eigenstates, and in the angular momentum-orbit radius entangled state. Various applications of these two representations, such as in developing angular momentum theory, squeezing mechanism, Wigner function and tomography theory for this system are presented. Thus the present review systematically summarizes a distinct approach for tackling this physical system.


2015 ◽  
Vol 92 (24) ◽  
Author(s):  
Benedikt Herwerth ◽  
Germán Sierra ◽  
Hong-Hao Tu ◽  
J. Ignacio Cirac ◽  
Anne E. B. Nielsen

2001 ◽  
Vol 15 (14) ◽  
pp. 463-472 ◽  
Author(s):  
HONGYI FAN ◽  
JINGXIAN LIN

Based on the gauge-invariant Wigner operator in <λ| representation (see Ref. 10), where the state |λ> can conveniently describe the motion of an electron in a uniform magnetic field, we provide an approach for identifying the corresponding state vector for Laughlin wave function and deriving the Wigner function (quasi-probability distribution) for the Laughlin state vector. The angular momentum-excited Laughlin state vectors are also obtained via <λ| representation.


1991 ◽  
Vol 06 (34) ◽  
pp. 3153-3162 ◽  
Author(s):  
STEFANO FORTE

We determine the path-integral for particles with fractional spin and statistics in the adiabatic limit, and we discuss the identification of the spin-changing term with a Berry phase. We show that the standard proof that the Laughlin wave function describes excitations with fractional statistics holds only on the basis of a tacit assumption of questionable validity.


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