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documentation:language_reference:functions:blockbanddiagonalize [2018/06/21 15:14] – created Simon Heinzedocumentation:language_reference:functions:blockbanddiagonalize [2025/11/20 03:29] (current) – external edit 127.0.0.1
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-====== Blockbanddiagonalize ====== +====== BlockBandDiagonalize ======
 ### ###
-alligned paragraph text+The function //BlockBandDiagonalize()// can be used to reduce the number of basis (spin-)orbitals by making linear combinations of (spin-)orbitals, according to the tight-binding structure (hopping matrix elements) within the (spin-)orbitals. As a simple example to make the idea clear, consider the following 3-by-3 matrix: 
 +$$ M = \begin{pmatrix} 0 & 1 & 1 \\  1 & 1 & 0 \\ 1 & 0 & 1 \end{pmatrix} $$ 
 +Now, assuming that $M$ corresponds to a tight-binding Hamiltonian defined on some basis, we can linearly combine the second and third basis orbitals, such that we get a single orbital which mix with the first orbital via the matrix M. Consider the following unitary rotation matrix: 
 +$$ U = \begin{pmatrix} 1 & 0 & 0 \\  0 & \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \\ 0 & \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \end{pmatrix} $$ 
 +Now, transforming the matrix $ M $ using the unitary matrix $ U $ results in: 
 +$$ M' = U M U^{T} = \begin{pmatrix} 0 & \frac{1}{\sqrt{2}} & 0 \\   \frac{1}{\sqrt{2}} & 1 & 0 \\ 0 & 0 & 1 \end{pmatrix} $$ 
 +In the new representation, the first basis orbital only mixes with the second  
 +The basis orbital and not with the third one. 
 +The function //BlockBandDiagonalize()// can accept 3 types of objects as an arguments: [[documentation:language_reference:objects:tightbinding:start|Tight-binding object]], [[documentation:language_reference:objects:operator:start|Operator]], or [[documentation:language_reference:objects:matrix:start|Matrix]]. 
 ### ###
  
-===== Input =====+====== Input ====== 
 +Case 1: 
 +  * //matrix//: hermitian matrix 
 +  * //blockSize//: size of the block (as number) or list of vectors representing the starting states
  
-  * bla : Integer +Case 2: 
-  * bla2 : Real+  * //operator//: hermitian operator 
 +  * //wave function //: single wave function of list of wave functions
  
-===== Output =====+Case 3: 
 +  * //tightbindingObject//: tight binding object 
 +  * //startingBlock //: list of atoms with positions, shells and orbitals used as starting block
  
-  * bla : real 
  
-===== Example =====+//(Optional) Third argument (in all cases)//
  
-### +   *NTri : (//integer//) maximum number of blocks included (//default: $\infty$//) 
-description text + 
-###+   *NOrtho : (//integer//) maximum number of reorthogonalizations (//default: $\infty$//)
  
-==== Input ==== +  *ReOrthogonalize: (//boolean//) use additional Gran-Schmidt orthogonalization after the Löwdin orthogonalization (//default: true//)
-<code Quanty Example.Quanty> +
--- some example code +
-</code>+
  
-==== Result ==== +====== Output ====== 
-<file Quanty_Output> +case1: 
-text produced as output +   *//ResponseFunction//:Response Function in tri representation. 
-</file>+   *//matrix//: Transformation Matrix to transform the input matrix into the Block band diagonalized one. 
  
 ===== Table of contents ===== ===== Table of contents =====
 {{indexmenu>.#1}} {{indexmenu>.#1}}
  

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