Differences

This shows you the differences between two versions of the page.

Link to this comparison view

Next revisionBoth sides next revision
documentation:language_reference:functions:rotate [2016/10/09 21:51] – created Maurits W. Haverkortdocumentation:language_reference:functions:rotate [2016/10/10 09:41] – external edit 127.0.0.1
Line 1: Line 1:
 +====== Rotate ======
  
 +###
 +//Rotate(psi, rotmat)// or //Rotate(Opp, rotmat)// rotates the basis of a wave-function or operator.
 +###
 +
 +===== Input =====
 +
 +  * psi or Opp : Wavefunction or operator
 +  * rotmat : matrix of dimension NFermion+NBoson (table of tables) or real or complex numbers
 +
 +===== Output =====
 +
 +  * psi or Opp : Wavefunction or operator
 +
 +===== Example =====
 +
 +###
 +A small example:
 +###
 +
 +==== Input ====
 +<code Quanty Rotate.Quanty>
 +dofile("../definitions.Quanty")
 +
 +OpppxR = Chop(Rotate(Opppx,rotmat))
 +OpppyR = Chop(Rotate(Opppy,rotmat))
 +OpppzR = Chop(Rotate(Opppz,rotmat))
 +
 +print("The matrix rotating an operator on the basis of spherical harmonics with alternating spin to a basis of kubic harmonics with alternating spin for a p orbital is:")
 +print(rotmat)
 +print("The operator adding a potential to the px orbital on a basis of spherical harmonics is: ",Opppx)
 +print("The operator adding a potential to the px orbital on a basis of kubic harmonics is: ",OpppxR)
 +print("The operator adding a potential to the py orbital on a basis of spherical harmonics is: ",Opppy)
 +print("The operator adding a potential to the py orbital on a basis of kubic harmonics is: ",OpppyR)
 +print("The operator adding a potential to the pz orbital on a basis of spherical harmonics is: ",Opppz)
 +print("The operator adding a potential to the pz orbital on a basis of kubic harmonics is: ",OpppzR)
 +
 +psixdnR = Chop(Rotate(psixdn,rotmat))
 +psixupR = Chop(Rotate(psixup,rotmat))
 +psiydnR = Chop(Rotate(psiydn,rotmat))
 +psiyupR = Chop(Rotate(psiyup,rotmat))
 +psizdnR = Chop(Rotate(psizdn,rotmat))
 +psizupR = Chop(Rotate(psizup,rotmat))
 +
 +print("The px orbital with spin down on a basis of spherical harmonics is: ",psixdn)
 +print("The px orbital with spin down on a basis of kubic harmonics is: ",psixdnR)
 +print("The py orbital with spin down on a basis of spherical harmonics is: ",psiydn)
 +print("The py orbital with spin down on a basis of kubic harmonics is: ",psiydnR)
 +print("The pz orbital with spin down on a basis of spherical harmonics is: ",psizdn)
 +print("The pz orbital with spin down on a basis of kubic harmonics is: ",psizdnR)
 +
 +print("Counting the px orbital on a basis of spherical harmonics: ",psixdn *Opppx *psixdn)
 +print("Counting the px orbital on a basis of kubic     harmonics: ",psixdnR*OpppxR*psixdnR)
 +print("Counting the py orbital on a basis of spherical harmonics: ",psiydn *Opppy *psiydn)
 +print("Counting the py orbital on a basis of kubic     harmonics: ",psiydnR*OpppyR*psiydnR)
 +print("Counting the pz orbital on a basis of spherical harmonics: ",psizdn *Opppz *psizdn)
 +print("Counting the pz orbital on a basis of kubic     harmonics: ",psizdnR*OpppzR*psizdnR)
 +</code>
 +
 +==== Result ====
 +<file Quanty_Output Rotate.out>
 +The matrix rotating an operator on the basis of spherical harmonics with alternating spin to a basis of kubic harmonics with alternating spin for a p orbital is:
 +{ { 0.70710678118655 , 0 , 0 , 0 , -0.70710678118655 , 0 } , 
 +  { 0 , 0.70710678118655 , 0 , 0 , 0 , -0.70710678118655 } , 
 +  { (0 + 0.70710678118655 I) , 0 , 0 , 0 , (0 + 0.70710678118655 I) , 0 } , 
 +  { 0 , (0 + 0.70710678118655 I) , 0 , 0 , 0 , (0 + 0.70710678118655 I) } , 
 +  { 0 , 0 , 1 , 0 , 0 , 0 } , 
 +  { 0 , 0 , 0 , 1 , 0 , 0 } }
 +The operator adding a potential to the px orbital on a basis of spherical harmonics is:
 +Operator: Opp px
 +QComplex                  0 (Real==0 or Complex==1 or Mixed==2)
 +MaxLength        =          2 (largest number of product of lader operators)
 +NFermionic modes =          6 (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   2
 +QComplex      =          0 (Real==0 or Complex==1)
 +N                      8 (number of operators of length   2)
 +C  0 A  0 |  4.999999999999999E-01
 +C  1 A  1 |  4.999999999999999E-01
 +C  4 A  4 |  4.999999999999999E-01
 +C  5 A  5 |  4.999999999999999E-01
 +C  4 A  0 | -5.000000000000000E-01
 +C  5 A  1 | -5.000000000000000E-01
 +C  0 A  4 | -5.000000000000000E-01
 +C  1 A  5 | -5.000000000000000E-01
 +
 +
 +The operator adding a potential to the px orbital on a basis of kubic harmonics is:
 +Operator: Opp px
 +QComplex                  0 (Real==0 or Complex==1 or Mixed==2)
 +MaxLength        =          2 (largest number of product of lader operators)
 +NFermionic modes =          6 (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   2
 +QComplex      =          0 (Real==0 or Complex==1)
 +N                      2 (number of operators of length   2)
 +C  0 A  0 |  1.000000000000000E+00
 +C  1 A  1 |  1.000000000000000E+00
 +
 +
 +The operator adding a potential to the py orbital on a basis of spherical harmonics is:
 +Operator: Opp py
 +QComplex                  0 (Real==0 or Complex==1 or Mixed==2)
 +MaxLength        =          2 (largest number of product of lader operators)
 +NFermionic modes =          6 (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   2
 +QComplex      =          0 (Real==0 or Complex==1)
 +N                      8 (number of operators of length   2)
 +C  0 A  0 |  4.999999999999999E-01
 +C  1 A  1 |  4.999999999999999E-01
 +C  4 A  4 |  4.999999999999999E-01
 +C  5 A  5 |  4.999999999999999E-01
 +C  4 A  0 |  5.000000000000000E-01
 +C  5 A  1 |  5.000000000000000E-01
 +C  0 A  4 |  5.000000000000000E-01
 +C  1 A  5 |  5.000000000000000E-01
 +
 +
 +The operator adding a potential to the py orbital on a basis of kubic harmonics is:
 +Operator: Opp py
 +QComplex                  0 (Real==0 or Complex==1 or Mixed==2)
 +MaxLength        =          2 (largest number of product of lader operators)
 +NFermionic modes =          6 (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   2
 +QComplex      =          0 (Real==0 or Complex==1)
 +N                      2 (number of operators of length   2)
 +C  2 A  2 |  1.000000000000000E+00
 +C  3 A  3 |  1.000000000000000E+00
 +
 +
 +The operator adding a potential to the pz orbital on a basis of spherical harmonics is:
 +Operator: Opp pz
 +QComplex                  0 (Real==0 or Complex==1 or Mixed==2)
 +MaxLength        =          2 (largest number of product of lader operators)
 +NFermionic modes =          6 (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   2
 +QComplex      =          0 (Real==0 or Complex==1)
 +N                      2 (number of operators of length   2)
 +C  2 A  2 |  9.999999999999999E-01
 +C  3 A  3 |  9.999999999999999E-01
 +
 +
 +The operator adding a potential to the pz orbital on a basis of kubic harmonics is:
 +Operator: Opp pz
 +QComplex                  0 (Real==0 or Complex==1 or Mixed==2)
 +MaxLength        =          2 (largest number of product of lader operators)
 +NFermionic modes =          6 (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   2
 +QComplex      =          0 (Real==0 or Complex==1)
 +N                      2 (number of operators of length   2)
 +C  4 A  4 |  9.999999999999999E-01
 +C  5 A  5 |  9.999999999999999E-01
 +
 +
 +The px orbital with spin down on a basis of spherical harmonics is:
 +WaveFunction: Wave Function
 +QComplex                  0 (Real==0 or Complex==1)
 +N                =          2 (Number of basis functions used to discribe psi)
 +NFermionic modes =          6 (Number of fermions in the one particle basis)
 +NBosonic modes            0 (Number of bosons in the one particle basis)
 +
 +#      pre-factor         Determinant
 +     7.071067811865E-01       100000
 +    -7.071067811865E-01       000010
 +
 +
 +The px orbital with spin down on a basis of kubic harmonics is:
 +WaveFunction: Wave Function
 +QComplex                  0 (Real==0 or Complex==1)
 +N                =          1 (Number of basis functions used to discribe psi)
 +NFermionic modes =          6 (Number of fermions in the one particle basis)
 +NBosonic modes            0 (Number of bosons in the one particle basis)
 +
 +#      pre-factor         Determinant
 +     1.000000000000E+00       100000
 +
 +
 +The py orbital with spin down on a basis of spherical harmonics is:
 +WaveFunction: Wave Function
 +QComplex                  1 (Real==0 or Complex==1)
 +N                =          2 (Number of basis functions used to discribe psi)
 +NFermionic modes =          6 (Number of fermions in the one particle basis)
 +NBosonic modes            0 (Number of bosons in the one particle basis)
 +
 +#      pre-factor             +I  pre-factor         Determinant
 +     0.000000000000E+00         7.071067811865E-01       100000
 +     0.000000000000E+00         7.071067811865E-01       000010
 +
 +
 +The py orbital with spin down on a basis of kubic harmonics is:
 +WaveFunction: Wave Function
 +QComplex                  0 (Real==0 or Complex==1)
 +N                =          1 (Number of basis functions used to discribe psi)
 +NFermionic modes =          6 (Number of fermions in the one particle basis)
 +NBosonic modes            0 (Number of bosons in the one particle basis)
 +
 +#      pre-factor         Determinant
 +     1.000000000000E+00       001000
 +
 +
 +The pz orbital with spin down on a basis of spherical harmonics is:
 +WaveFunction: Wave Function
 +QComplex                  0 (Real==0 or Complex==1)
 +N                =          1 (Number of basis functions used to discribe psi)
 +NFermionic modes =          6 (Number of fermions in the one particle basis)
 +NBosonic modes            0 (Number of bosons in the one particle basis)
 +
 +#      pre-factor         Determinant
 +     1.000000000000E+00       001000
 +
 +
 +The pz orbital with spin down on a basis of kubic harmonics is:
 +WaveFunction: Wave Function
 +QComplex                  0 (Real==0 or Complex==1)
 +N                =          1 (Number of basis functions used to discribe psi)
 +NFermionic modes =          6 (Number of fermions in the one particle basis)
 +NBosonic modes            0 (Number of bosons in the one particle basis)
 +
 +#      pre-factor         Determinant
 +     1.000000000000E+00       000010
 +
 +
 +Counting the px orbital on a basis of spherical harmonics: 1
 +Counting the px orbital on a basis of kubic     harmonics: 1
 +Counting the py orbital on a basis of spherical harmonics: 1
 +Counting the py orbital on a basis of kubic     harmonics: 1
 +Counting the pz orbital on a basis of spherical harmonics: 1
 +Counting the pz orbital on a basis of kubic     harmonics: 1
 +</file>
 +
 +===== Table of contents =====
 +{{indexmenu>.#1}}
Print/export