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Update home authored by Bharath Hebbe Madhusudhana's avatar Bharath Hebbe Madhusudhana
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...@@ -7,7 +7,7 @@ We consider spinful Fermions on a lattice with L sites. The Hamiltonian we consi ...@@ -7,7 +7,7 @@ We consider spinful Fermions on a lattice with L sites. The Hamiltonian we consi
<a href="https://www.codecogs.com/eqnedit.php?latex=H=&space;J\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;\hat{c}_{i&plus;1,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;h.c&space;&plus;&space;\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;V_{i,&space;\sigma}&space;\hat{c}_{i,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;U&space;\sum_{i=1}^L&space;\hat{c}_{i,&space;\uparrow}^{\dagger}&space;\hat{c}_{i,&space;\uparrow}\hat{c}_{i,&space;\downarrow}^{\dagger}&space;\hat{c}_{i,&space;\downarrow}" target="_blank"><img src="https://latex.codecogs.com/gif.latex?H=&space;J\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;\hat{c}_{i&plus;1,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;h.c&space;&plus;&space;\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;V_{i,&space;\sigma}&space;\hat{c}_{i,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;U&space;\sum_{i=1}^L&space;\hat{c}_{i,&space;\uparrow}^{\dagger}&space;\hat{c}_{i,&space;\uparrow}\hat{c}_{i,&space;\downarrow}^{\dagger}&space;\hat{c}_{i,&space;\downarrow}" title="H= J\sum_{i=1, \sigma= \downarrow, \uparrow}^L \hat{c}_{i+1, \sigma}^{\dagger} \hat{c}_{i, \sigma} + h.c + \sum_{i=1, \sigma= \downarrow, \uparrow}^L V_{i, \sigma} \hat{c}_{i, \sigma}^{\dagger} \hat{c}_{i, \sigma} + U \sum_{i=1}^L \hat{c}_{i, \uparrow}^{\dagger} \hat{c}_{i, \uparrow}\hat{c}_{i, \downarrow}^{\dagger} \hat{c}_{i, \downarrow}" /></a> <a href="https://www.codecogs.com/eqnedit.php?latex=H=&space;J\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;\hat{c}_{i&plus;1,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;h.c&space;&plus;&space;\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;V_{i,&space;\sigma}&space;\hat{c}_{i,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;U&space;\sum_{i=1}^L&space;\hat{c}_{i,&space;\uparrow}^{\dagger}&space;\hat{c}_{i,&space;\uparrow}\hat{c}_{i,&space;\downarrow}^{\dagger}&space;\hat{c}_{i,&space;\downarrow}" target="_blank"><img src="https://latex.codecogs.com/gif.latex?H=&space;J\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;\hat{c}_{i&plus;1,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;h.c&space;&plus;&space;\sum_{i=1,&space;\sigma=&space;\downarrow,&space;\uparrow}^L&space;V_{i,&space;\sigma}&space;\hat{c}_{i,&space;\sigma}^{\dagger}&space;\hat{c}_{i,&space;\sigma}&space;&plus;&space;U&space;\sum_{i=1}^L&space;\hat{c}_{i,&space;\uparrow}^{\dagger}&space;\hat{c}_{i,&space;\uparrow}\hat{c}_{i,&space;\downarrow}^{\dagger}&space;\hat{c}_{i,&space;\downarrow}" title="H= J\sum_{i=1, \sigma= \downarrow, \uparrow}^L \hat{c}_{i+1, \sigma}^{\dagger} \hat{c}_{i, \sigma} + h.c + \sum_{i=1, \sigma= \downarrow, \uparrow}^L V_{i, \sigma} \hat{c}_{i, \sigma}^{\dagger} \hat{c}_{i, \sigma} + U \sum_{i=1}^L \hat{c}_{i, \uparrow}^{\dagger} \hat{c}_{i, \uparrow}\hat{c}_{i, \downarrow}^{\dagger} \hat{c}_{i, \downarrow}" /></a>
Although the general code Exact_Diagonalization.py' is designed for any onsite potential, in the script 'run_this_script.py' we use an on-site potential of the form <a href="https://www.codecogs.com/eqnedit.php?latex=V_{i,&space;\sigma}=&space;\Delta_{\sigma}(i-L/2)&space;&plus;&space;\alpha&space;(i-L/2)^2&space;&plus;&space;\delta_{r}&space;&plus;&space;\Delta_{aa}\cos(2\pi&space;\beta&space;i&space;&plus;&space;\phi_{aa}&space;)" target="_blank"><img src="https://latex.codecogs.com/gif.latex?V_{i,&space;\sigma}=&space;\Delta_{\sigma}(i-L/2)&space;&plus;&space;\alpha&space;(i-L/2)^2&space;&plus;&space;\delta_{r}&space;&plus;&space;\Delta_{aa}\cos(2\pi&space;\beta&space;i&space;&plus;&space;\phi_{aa}&space;)" title="V_{i, \sigma}= \Delta_{\sigma}(i-L/2) + \alpha (i-L/2)^2 + \delta_{r} + \Delta_{aa}\cos(2\pi \beta i + \phi_{aa} )" /></a>. Here, <a href="https://www.codecogs.com/eqnedit.php?latex=\delta_r&space;\in&space;[-\Delta_r,&space;\Delta_r]" target="_blank"><img src="https://latex.codecogs.com/gif.latex?\delta_r&space;\in&space;[-\Delta_r,&space;\Delta_r]" title="\delta_r \in [-\Delta_r, \Delta_r]" /></a> is a random onsite potential. Although the general code Exact_Diagonalization.py' is designed for any onsite potential, in the script 'run_this_script.py' we use an on-site potential of the form <a href="https://www.codecogs.com/eqnedit.php?latex=V_{i,&space;\sigma}=&space;\Delta_{\sigma}(i-L/2)&space;&plus;&space;\alpha&space;(i-L/2)^2&space;&plus;&space;\delta_{i}&space;&plus;&space;\Delta_{aa}\cos(2\pi&space;\beta&space;i&space;&plus;&space;\phi_{aa}&space;)" target="_blank"><img src="https://latex.codecogs.com/gif.latex?V_{i,&space;\sigma}=&space;\Delta_{\sigma}(i-L/2)&space;&plus;&space;\alpha&space;(i-L/2)^2&space;&plus;&space;\delta_{i}&space;&plus;&space;\Delta_{aa}\cos(2\pi&space;\beta&space;i&space;&plus;&space;\phi_{aa}&space;)" title="V_{i, \sigma}= \Delta_{\sigma}(i-L/2) + \alpha (i-L/2)^2 + \delta_{i} + \Delta_{aa}\cos(2\pi \beta i + \phi_{aa} )" /></a>. Here, <a href="https://www.codecogs.com/eqnedit.php?latex=\delta_i&space;\in&space;[-\Delta_r,&space;\Delta_r]" target="_blank"><img src="https://latex.codecogs.com/gif.latex?\delta_i&space;\in&space;[-\Delta_r,&space;\Delta_r]" title="\delta_i \in [-\Delta_r, \Delta_r]" /></a> is a random onsite potential.
Below is a decription of the variables that appear in secion 1 of the script 'run_this_script.py' Below is a decription of the variables that appear in secion 1 of the script 'run_this_script.py'
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