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Introduction Associative Algebra Explicit Decomposition References On some Computational Method for the Explicit Forms of the Decompositions of Master Equations Takeo Kamizawa Department of Information Sciences, Tokyo University of Science,


  1. Introduction Associative Algebra Explicit Decomposition References On some Computational Method for the Explicit Forms of the Decompositions of Master Equations Takeo Kamizawa Department of Information Sciences, Tokyo University of Science, Noda, Japan 51 Symposium on Mathematical Physics, Toruń, Poland, 16-18 June, 2019

  2. Introduction Associative Algebra Explicit Decomposition References Introduction

  3. Introduction Associative Algebra Explicit Decomposition References Master Equations The dynamics of quantum systems are described by a certain type of equations. Let H S be a complex Hilbert space and S ( H S ) be the set of states: S ( H S ) = { ρ ∈ B ( H S ) | ρ ∗ = ρ, ρ ≥ 0 , tr ρ = 1 } . In a (closed) system, the dynamics on S ( H S ) is written as dt ρ t = − i d � [ H S ( t ) , ρ t ] , where H S ( t ) is the system Hamiltonian and I = R or I = [ 0 , ∞ ) .

  4. Introduction Associative Algebra Explicit Decomposition References Master Equations However, our system suffers from the noise from the environment in general. ⇒ Different formulae including the noise effect need be considered.

  5. Introduction Associative Algebra Explicit Decomposition References Master Equations In order to describe more general systems (open systems), consider the dynamics on S ( H S ) : d dt ρ t = L ( t ) ρ t , where L : I × S ( H S ) → S ( H S ) .

  6. Introduction Associative Algebra Explicit Decomposition References GKSL Equation A well-known type of equations for open systems is the GKSL equation: dt ρ t = − i [ H S , ρ t ] + 1 d � c k ([ F k ρ t , F ∗ k ] + [ F k , ρ t F ∗ k ]) , 2 k c k : scalar , F k ∈ B ( H S ) s.t. { F k } k ∪ { I } forms a basis of B ( H S ) .

  7. Introduction Associative Algebra Explicit Decomposition References Master Equations If dim H S < ∞ and we introduce the ’vectorisation’ method, we have the ’matrix representation’ of L ( t ) : ρ t = ˜ vec ˙ L ( t ) vec ρ t , ˜ L ( t ) ∈ M n 2 ( C ) .

  8. Introduction Associative Algebra Explicit Decomposition References Master Equations Especially, when dim H S = n = 1, the master equation has the form: d dt ρ t = ˜ ℓ ( t ) ρ t , which is a solvable system because it can be solved by the “separation of variables”.

  9. Introduction Associative Algebra Explicit Decomposition References Master Equations However, it can be difficult to ’exactly solve’ the master equation if n ≥ 2. The analysis becomes far difficult if n ≥ 5 (because the computation of the eigenvalues is difficult due to Abel-Ruffini theorem). ⇒ What can we do?

  10. Introduction Associative Algebra Explicit Decomposition References Decomposition of Master Equation Assume that the matrix form of ˜ L ( t ) has a ’block-diagonal’ form: � ˜ � L 1 ( t ) ˜ L ( t ) = . ˜ L 2 ( t ) Then, the total master equation can be considered as the union of independent systems: � ρ 1 , t = ˜ ˙ L 1 ( t ) ρ 1 , t ρ t = ˜ ˙ L ( t ) ρ t = ⇒ ρ 2 , t = ˜ ˙ L 2 ( t ) ρ 2 , t

  11. Introduction Associative Algebra Explicit Decomposition References Decomposition of Master Equation The sizes of ˜ L 1 , ˜ L 2 are strictly less than n 2 . ⇒ Reduction of the dimension ⇒ Simplification of analysis

  12. Introduction Associative Algebra Explicit Decomposition References Decomposition of Master Equation Next, assume that ˜ L ( t ) can be ’block-diagonalised’ by a constant P : � ˜ � L 1 ( t ) P − 1 ˜ L ( t ) P = . ˜ L 2 ( t ) Then, the transformed equation by ρ t = P ψ t is � ˜ � L 1 ( t ) ˙ ψ t = ψ t , ˜ L 2 ( t ) so again the total master equation can be considered as the union of independent systems.

  13. Introduction Associative Algebra Explicit Decomposition References Decomposition of Master Equation However, it is not always possible to reduce ˜ L ( t ) into a block-diagonal form. Question How to check if ˜ L ( t ) is block-diagonalisable? Question If block-diagonalisable, how to compute the ’explicit’ form of the decomposition?

  14. Introduction Associative Algebra Explicit Decomposition References Associative Algebra

  15. Introduction Associative Algebra Explicit Decomposition References Associative Algebra An (associative) algebra A is defined as a linear space over C which is closed under the multiplication with the associative law: A · ( B · C ) = ( A · B ) · C ( A , B , C ∈ A ) . N ∈ A is said to be nilpotent if ∃ j ∈ N such that N j = O . P ∈ A is said to be properly nilpotent if PA is nilpotent for all A ∈ A .

  16. Introduction Associative Algebra Explicit Decomposition References Associative Algebra rad A is the radical of A , which is the set of all properly nilpotent elements in A . A is semi-simple if rad A = { O } . A is simple if A has no non-trivial ideal in A .

  17. Introduction Associative Algebra Explicit Decomposition References Wedderburn Decomposition An important result was shown by Wedderburn: Theorem (Wedderburn’s theorem). If A is a finite-dimensional semi-simple algebra over C , there are simple algebras A k ( k = 1 , . . . , s ) such that s � A = A k , (1) k = 1 which is unique up to the order. J.H.M. Wedderburn. Proc. Lond. Math. Soc. S2-6 (1908), pp. 77–118. Yu.A. Drozd, V.V. Kirichenko. ’Finite Dimensional Algebras’, Springer, 2012.

  18. Introduction Associative Algebra Explicit Decomposition References Wedderburn Decomposition Relation between the Wedderburn decomposition and the block-diagonal reducibility is the following: ˜ L ( t ) : Generator of the master equation A : Algebra generated by ˜ L ( t ) ˜   L 1 ( t ) s ... � ⇒ ˜ A = A k ⇐ L ( t ) ≃     ˜ k = 1 L s ( t )

  19. Introduction Associative Algebra Explicit Decomposition References Burnside’s Theorem on Algebra For the block-diagonal reduction, s = 1 or s ≥ 2 is important. Theorem (Burnside’s theorem). The only irreducible subalgebra of M n ( C ) with n ≥ 2 is M n ( C ) itself. In other words, for an algebra A � M n ( C ) with n ≥ 2 , there exists a non-trivial A -invariant subspace. Thus, dim A < n 2 iff s ≥ 2. W. Burnside. Proc. Lond. Math. Soc. 2 (1905), pp. 369–387. Yu.A. Drozd, V.V. Kirichenko. ’Finite Dimensional Algebras’, Springer, 2012.

  20. Introduction Associative Algebra Explicit Decomposition References Block-Diagonal Reduction of Generator In order to test the block-diagonal reducibility of the generator L ( t ) , 1 Construct the algebra A generated by ˜ L ( t ) . 2 Construct a basis B of A . If dim B = n 2 , then ˜ L ( t ) cannot be block-diagonalised. If dim B < n 2 , then ˜ L ( t ) may be block-diagonalised. 3 Check if A is semi-simple or not. If A is semi-simple, then ˜ L ( t ) can be block-diagonalised. If A is not semi-simple, then ˜ L ( t ) cannot be block-diagonalised.

  21. Introduction Associative Algebra Explicit Decomposition References Discriminant of Algebra Question How can we check if A is semi-simple? ⇒ The discriminant of an algebra can do. Let A be the algebra generated by ˜ L ( t ) and B = { B 1 , . . . , B m } be a basis of A . Theorem The algebra A is semi-simple if and only if   · · · tr B 1 B 1 tr B 1 B m . . ... . . disc B A = det  � = 0 .   . .  tr B m B 1 · · · tr B m B m T. Kamizawa. Open Syst. Infor. Dyn. 24 (2017), 1750002. Y.A. Mitropolsky, A.K. Lopatin. ’Nonlinear Mechanics, Groups and Symmetry’. Springer, 2013.

  22. Introduction Associative Algebra Explicit Decomposition References Explicit Decomposition

  23. Introduction Associative Algebra Explicit Decomposition References Explicit Decomposition of Semi-Simple Algebras Question Once an algebra A is known to be semi-simple and reducible, how can we compute each simple algebra of the Wedderburn decomposition? ⇒ It is enough to compute the identity elements E 1 , . . . , E s of simple algebras A 1 , . . . , A s , respectively, because A k = E k A . W. Eberly. Comput. Complex. 1 (1991), pp. 183–210.

  24. Introduction Associative Algebra Explicit Decomposition References Centre of Algebra Moreover, it is enough to compute the identity elements of the ’centre’ of simple algebras. Let A be an algebra. The centre of A is defined by Z ( A ) = { A ∈ A | AB = BA ( ∀ B ∈ A ) } . The centre is a commutative algebra and E k ∈ Z ( A k ) .

  25. Introduction Associative Algebra Explicit Decomposition References Centre of Algebra Our algebra A is semi-simple: A ≃ A 1 ⊕ · · · ⊕ A s , and in this case, we have Z ( A ) ≃ Z ( A 1 ) ⊕ · · · ⊕ Z ( A s ) . An identity element E k of A k is an identity element of Z ( A k ) .

  26. Introduction Associative Algebra Explicit Decomposition References Splitting Element Question How can we obtain the identity elements? For the explicit decomposition, an element so-called the ’splitting element’ plays an important role.

  27. Introduction Associative Algebra Explicit Decomposition References Splitting Element Let A be an m -dimensional algebra over a number field F (finite extension of Q ). An element Q ∈ A is a splitting element if its minimal polynomial ψ Q over F is square-free (i.e. no multiple root) and deg ψ Q = m . W. Eberly. Comput. Complex. 1 (1991), pp. 183–210.

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