MeanFieldOperator

MeanFieldOperator($O$, $\rho$) creates the mean-field version of operator $O$ with the corresponding density matrix $\rho$. $rho$ stores the expectation values of $a^{\dagger}_{\tau}a^{\phantom{\dagger}}_{\tau'}$, a table of dimensions $NFermion$ by $NFermion$.

Any two particle parts of the operator will be replaced in mean-field, using the Hartree-Fock approximation by: \begin{eqnarray} a^{\dagger}_{i}a^{\dagger}_{j}a^{\phantom{\dagger}}_{k}a^{\phantom{\dagger}}_{l} &\to&\\ \nonumber &-& a^{\dagger}_{i}a^{\phantom{\dagger}}_{k} \langle a^{\dagger}_{j}a^{\phantom{\dagger}}_{l} \rangle \\ \nonumber &+& a^{\dagger}_{i}a^{\phantom{\dagger}}_{l} \langle a^{\dagger}_{j}a^{\phantom{\dagger}}_{k} \rangle \\ \nonumber &+& a^{\dagger}_{j}a^{\phantom{\dagger}}_{k} \langle a^{\dagger}_{i}a^{\phantom{\dagger}}_{l} \rangle \\ \nonumber &-& a^{\dagger}_{j}a^{\phantom{\dagger}}_{l} \langle a^{\dagger}_{i}a^{\phantom{\dagger}}_{k} \rangle \\ \nonumber &-& \langle a^{\dagger}_{i}a^{\phantom{\dagger}}_{l} \rangle \langle a^{\dagger}_{j}a^{\phantom{\dagger}}_{k} \rangle \\ \nonumber &+& \langle a^{\dagger}_{i}a^{\phantom{\dagger}}_{k} \rangle \langle a^{\dagger}_{j}a^{\phantom{\dagger}}_{l} \rangle \end{eqnarray}

If the option AddDFTSelfInteraction was set to true more terms are added to the Mean-Field Operator, namely \begin{equation} \sum_{m,n} U (\langle a^\dagger_m a^{\phantom{\dagger}}_n \rangle)^{T} a^\dagger_m a^{\phantom{\dagger}}_n \end{equation} where \begin{equation} U = \left( \frac{N_{Fermion} (N_{Fermion}-1)}{2} \right)^{-1} \sum_{m,n} \left( U_{m\,n\,n\,m} - U_{m\,n\,m\,n} \right) \end{equation} is the average interaction energy electrons have with one another.

• $O$ : Operator
• $rho$ : Matrix (Table of Table of length $O.NF$) of doubles
• Possible options are:

  • “AddDFTSelfInteraction” bool defining if the electron self-interaction is to be included. (Standard false)

• $O_{MF}$ The mean-field approximated operator

Example.Quanty

NF = 4
op = NewOperator("Number",NF,{1},{1},{0.1+I}) + NewOperator("U",NF,{0},{1},{5}) + 3
rho = {{0.7,0.3+I,0,0},{0.3-I,0.4,0,0},{0,0,0,0},{0,0,0,0}}
 
print("Full Operator:")
print(op)
print("\nDensity:")
print(rho)
print("\nMeanFieldOperator:")
print( MeanFieldOperator(op, rho) )
print("\nMeanFieldOperator with electron self-interaction:")
print( MeanFieldOperator(op, rho, {{"AddDFTSelfInteraction",true}}) )

Full Operator:
 
Operator: CrAn
QComplex         =          2 (Real==0 or Complex==1 or Mixed==2)
MaxLength        =          4 (largest number of product of lader operators)
NFermionic modes =          4 (Number of fermionic modes (site, spin, orbital, ...) in the one particle basis)
NBosonic modes   =          0 (Number of bosonic modes (phonon modes, ...) in the one particle basis)
 
Operator of Length   0
QComplex      =          0 (Real==0 or Complex==1)
N             =          1 (number of operators of length   0)
|  3.000000000000000E+00
 
Operator of Length   2
QComplex      =          1 (Real==0 or Complex==1)
N             =          1 (number of operators of length   2)
C  1 A  1 |  1.000000000000000E-01  1.000000000000000E+00
 
Operator of Length   4
QComplex      =          0 (Real==0 or Complex==1)
N             =          1 (number of operators of length   4)
C  1 C  0 A  1 A  0 | -5.000000000000000E+00
 
 
 
Density:
{ { 0.7 , (0.3 + 1 I) , 0 , 0 } , 
  { (0.3 - 1 I) , 0.4 , 0 , 0 } , 
  { 0 , 0 , 0 , 0 } , 
  { 0 , 0 , 0 , 0 } }
 
MeanFieldOperator:
 
Operator: 
QComplex         =          0 (Real==0 or Complex==1 or Mixed==2)
MaxLength        =          4 (largest number of product of lader operators)
NFermionic modes =          4 (Number of fermionic modes (site, spin, orbital, ...) in the one particle basis)
NBosonic modes   =          0 (Number of bosonic modes (phonon modes, ...) in the one particle basis)
 
Operator of Length   0
QComplex      =          0 (Real==0 or Complex==1)
N             =          1 (number of operators of length   0)
|  1.255000000000000E+01
 
Operator of Length   2
QComplex      =          1 (Real==0 or Complex==1)
N             =          4 (number of operators of length   2)
C  1 A  1 | -3.400000000000000E+00  1.000000000000000E+00
C  1 A  0 |  1.500000000000000E+00  5.000000000000000E+00
C  0 A  1 |  1.500000000000000E+00 -5.000000000000000E+00
C  0 A  0 | -2.000000000000000E+00  0.000000000000000E+00
 
 
 
MeanFieldOperator with electron self-interaction:
 
Operator: 
QComplex         =          0 (Real==0 or Complex==1 or Mixed==2)
MaxLength        =          4 (largest number of product of lader operators)
NFermionic modes =          4 (Number of fermionic modes (site, spin, orbital, ...) in the one particle basis)
NBosonic modes   =          0 (Number of bosonic modes (phonon modes, ...) in the one particle basis)
 
Operator of Length   0
QComplex      =          0 (Real==0 or Complex==1)
N             =          1 (number of operators of length   0)
|  1.255000000000000E+01
 
Operator of Length   2
QComplex      =          1 (Real==0 or Complex==1)
N             =          4 (number of operators of length   2)
C  1 A  1 | -3.066666666666666E+00  1.000000000000000E+00
C  1 A  0 |  1.500000000000000E+00  5.000000000000000E+00
C  0 A  1 |  1.500000000000000E+00 -5.000000000000000E+00
C  0 A  0 | -1.416666666666667E+00  0.000000000000000E+00