Showing 321 - 340 results of 27,009 for search '(( 50 ((((teer decrease) OR (nn decrease))) OR (a decrease)) ) OR ( 3d point decrease ))', query time: 0.96s Refine Results
  1. 321

    Relationship between Differential Hepatic microRNA Expression and Decreased Hepatic Cytochrome P450 3A Activity in Cirrhosis by Raj Vuppalanchi (458660)

    Published 2013
    “…<div><p>Background and Aim</p><p>Liver cirrhosis is associated with decreased hepatic cytochrome P4503A (CYP3A) activity but the pathogenesis of this phenomenon is not well elucidated. …”
  2. 322

    Dispersion relation for the Hamiltonian hat{mathcal {H}}_0 of the π-flux cubic lattice model for different values of the parameter <em>a</em> (from top to bottom, <em>a</em> = 0, 0... by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  3. 323

    Dispersion relation for the tight-binding Hamiltonian hat{mathcal {H}}_0 on the π-flux square lattice model by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
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    Gap Δ versus <em>U</em> at <em>T</em> = 0 for different values of the interpolating parameter <em>a</em> and at half-filling (<em>n</em> = 1) by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  10. 330

    Critical temperature <em>T<sub>c</sub></em> (in units of <em>t</em>) for different values of the interpolating parameter <em>a</em> at half-filling (from top to bottom, <em>a</em>... by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  11. 331

    Anisotropic honeycomb lattice with a magnetic field: this model allows us to interpolate between the honeycomb lattice and the π-flux square lattice model by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  12. 332

    Density of states for the Hamiltonian on the π-flux cubic lattice model for different values of the anisotropy parameter <em>a</em> (from top to bottom, <em>a</em> = 0, 0.5, 1) by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  13. 333

    Critical interaction <em>U<sub>c</sub></em> for different values of the anisotropy parameter <em>a</em> for the π-flux cubic lattice model at half-filling by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  14. 334

    Critical value <em>U<sub>c</sub></em> versus the interpolating parameter <em>a</em> at <em>T</em> = 0 and half-filling (as in figure 5) by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  15. 335

    Critical temperature <em>T<sub>c</sub></em> for different values of the anisotropy parameter <em>a</em> for the π-flux cubic lattice model at half-filling (from top to bottom, <em>... by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
  16. 336

    Gap Δ versus <em>U</em> for different values of the anisotropy parameter <em>a</em> for the π-flux cubic lattice model at half-filling (from top to bottom, <em>a</em> = 0, 0.05, 0.... by G Mazzucchi (557358)

    Published 2013
    “…The reason for such a choice is that the π-flux cubic lattice displays Dirac points and that decreasing the hopping coefficient in a spatial direction (say, <em>t<sub>z</sub></em>), these Dirac points are unaltered: it is then possible to study the 3D–2D interpolation towards the π-flux square lattice. …”
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