Stealthy hyperuniform disorder: A new route to controlling electric states and magnetic phase transition in correlated systems

fig2: fig2/k0.0 fig2/k0.5 fig2/k1.0 fig2/k1.5 k_param_: _param_ = k_c in each directory, two files - Sq structure factor (kx ky S) kx,ky: wave number, S: structure factor - k_param_-bonds rhobuses for the bonds (x y kind) x,y: coordinates, kind: alpha or beta bond fig3b: - results vertex fractions as a function of kc (kcut N1 N2 C0 dC0 C1 dC1 C2 dC2 C3 dC3) kcut: kc N1,N2: fractions of alpha and beta bonds C_i, dC_i: fractions of C_i vertex and their standard deviations - SQV vertex fractions for the constrainted SHU with kca=1.5 (N1 N2 C0 dC0 C1 dC1 C2 dC2 C3 dC3) - QC vertex fractions for the quasiperiodic system (C0 C1 C2 C3) fig4: - dos-_param_ Density of states for kc=_param_ (x y) x: energy, y: density of states - IPR-random IPR spectra for kca=0.0- IPR-hu IPR spectra for kca=1.5 (x y) x: energy, y: IPR spectra fig5: - K-bonds rhobuses for the bonds for the K pattern (x y kind) x,y: coordinates, kind: alpha or beta bond - Sq-K structure factor for the K pattern (kx ky S) kx,ky: wave number, S: structure factor - dos-K Density of states for the K pattern (x y) x: energy, y: density of states - IPR-K IPR spectra for the K pattern (x y) x: energy, y: IPR spectra fig6: - Density-h_param_ Magnetization distribution for the hyperuniform case (U=_param_)- Density-r_param_ Magnetization distribution for the random case (U=_param_) (x y) x: absolute value of magnetization y: its distribution fig7:- hyper Average magnetization for the hyperuniform case with kca=1.5- random Average magnetization for the random case- qc Average magnetization for the quasiperiodic case (x y fig8:- hyper IPR spectra for the hyperuniform case with kca=1.5- random IPR spectra for the random case (x y dy z dz) x: Coulomb interaction U y,dy: IPR_1 and its standard deviation z,dz: IPR_2 and its standard deviation - qc IPR spectra for the quasiperiodic case (x y z) x: Coulomb interaction U, y: IPR_1, z: IPR_2 fig9:- Mag-h1-2.8 triangles for the sites in the hyperuniform case- Mag-r1-2.8 triangles for the sites in the random case (x y z) x,y: coordinates z: local magnetization fig10: fig10/k1.5/k1.5-bonds rhobuses for the bonds (x y kind) x,y: coordinates, kind: alpha or beta bond fig10/k1.5/vSq-_param_ structure factor for the vertex C_param_ (kx ky S) kx,ky: wave number, S: structure factor fig10/vk1.5/vk1.5-bonds rhobuses for the bonds (x y kind) x,y: coordinates, kind: alpha or beta bond fig10/vk1.5/vSq-_param_ structure factor for the vertex C_param_ (kx ky S) kx,ky: wave number, S: structure factor fig11:- dos-v Density of states for the constrainted SHU (x y) x: energy, y: density of states- IPR-v IPR spectra for the constrainted SHU (x y) x: energy, y: IPR spectra- vhyper Average magnetization for the constrainted SHU case (x y dy) x: Couploub interaction, y,dy: magnetization and its standard deviation