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Results in Mathematics

On the Refinement of Cartan Decomposition: An Implicit Commutative Substructure in $$\mathfrak {su}(2^{n})$$

Moody T. Chu

Published Jul 19, 2025• 1 citation
Publisher

Abstract

Abstract The Cartan decomposition of a semisimple Lie algebra is pivotal in both theoretical exploration and practical application. It generalizes the classical spectral, polar, and singular value decompositions found in linear algebra. This paper explores an advanced refinement of the Cartan decomposition of $$\mathfrak {su}(2^{n})$$ su ( 2 n ) , arising from the parameterization of a Hamiltonian for quantum simulation. Specifically, given an AI-type Cartan decomposition $${\mathfrak {g}} = {\mathfrak {k}} \oplus {\mathfrak {p}}$$ g = k ⊕ p of any Lie subalgebra $${\mathfrak {g}}$$ g in $$\mathfrak {su}(2^{n})$$ su ( 2 n ) , where $${\mathfrak {p}} = \widetilde{{\mathfrak {p}}} \oplus {\mathfrak {h}}$$ p = p ~ ⊕ h and $${\mathfrak {h}}$$ h is the maximal abelian subalgebra in $${\mathfrak {p}}$$ p , it is revealed that both the subalgebra $${\mathfrak {k}}$$ k and the corresponding $$\widetilde{{\mathfrak {p}}}$$ p ~ (which is generally not a subalgebra) can further be partitioned, respectively, as the direct sums of equal-dimensional commutative Lie subalgebras. With respect to the involution $$\theta (g)=-g^{\top }$$ θ ( g ) = - g ⊤ , any Lie subalgebra $${\mathfrak {g}}$$ g in $$\mathfrak {su}(2^{n})$$ su ( 2 n ) with nondegenerate Cartan decomposition can thus be fully decomposed as the orthogonal direct sum of $${\mathfrak {h}}$$ h and pairs of commutative Lie subalgebras over $${\mathfrak {k}}$$ k and $$\widetilde{{\mathfrak {p}}}$$ p ~ , all of which, except $${\mathfrak {h}}$$ h , share the same dimension.

DOI
10.1007/s00025-025-02478-3

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On the Refinement of Cartan Decomposition: An Implicit Commutative Substructure in su(2n)\mathfrak {su}(2^{n})su(2n)
Abstract The Cartan decomposition of a semisimple Lie algebra is pivotal in both theoretical exploration and practical application. It generalizes the classical spectral, polar, and singular value decompositions found in linear algebra. This paper explores an advanced refinement of the Cartan decomposition of su(2n)\mathfrak {su}(2^{n})su(2n) su ( 2 n ) , arising from the parameterization of a Hamiltonian for quantum simulation. Specifically, given an AI-type Cartan decomposition g=k⊕p{\mathfrak {g}} = {\mathfrak {k}} \oplus {\mathfrak {p}}g=k⊕p g = k ⊕ p of any Lie subalgebra g{\mathfrak {g}}g g in su(2n)\mathfrak {su}(2^{n})su(2n) su ( 2 n ) , where p=p~⊕h{\mathfrak {p}} = \widetilde{{\mathfrak {p}}} \oplus {\mathfrak {h}}p=p​⊕h p = p ~ ⊕ h and h{\mathfrak {h}}h h is the maximal abelian subalgebra in p{\mathfrak {p}}p p , it is revealed that both the subalgebra k{\mathfrak {k}}k k and the corresponding p~\widetilde{{\mathfrak {p}}}p​ p ~ (which is generally not a subalgebra) can further be partitioned, respectively, as the direct sums of equal-dimensional commutative Lie subalgebras. With respect to the involution θ(g)=−g⊤\theta (g)=-g^{\top }θ(g)=−g⊤ θ ( g ) = - g ⊤ , any Lie subalgebra g{\mathfrak {g}}g g in su(2n)\mathfrak {su}(2^{n})su(2n) su ( 2 n ) with nondegenerate Cartan decomposition can thus be fully decomposed as the orthogonal direct sum of h{\mathfrak {h}}h h and pairs of commutative Lie subalgebras over k{\mathfrak {k}}k k and p~\widetilde{{\mathfrak {p}}}p​ p ~ , all of which, except h{\mathfrak {h}}h h , share the same dimension.
A scheme to perform the Cartan decomposition for the Lie algebra su(N) of arbitrary finite dimensions is introduced. The schme is based on two algebraic structures, the conjugate partition and the quotient algebra, that are easily generated by a Cartan subalgebra and generally exist in su(N). In particular, the Lie algebras su(2^p) and every su(2^{p-1} < N < 2^p) share the isomorphic structure of the quotient algebra. This structure enables an efficient algorithm for the recursive and exhaustive construction of Cartan decompositions. Further with the scheme, a unitary transformation in SU(N) can be recursively decomposed into a product of certain designated operators, e.g., local and nonlocal gates. Such a recursive decomposition of a transformation implies an evolution path on the manifold of the group.
This chapter discusses in detail the case of two-level systems and the associated Lie group. It gives an example of a general decomposition of SU(n), namely the decomposition into planar rotation, which is quite simple and can be obtained by straightforward computations. This decomposition gives a direct way to parametrize the special unitary group. The chapter presents the basics of Cartan decompositions of semisimple Lie groups. It gives some examples of applications of Lie group decompositions and introduces some notions of Lie group and Lie algebra theory. The chapter discusses Cartan decompositions of Lie groups. Cartan decompositions appear to be ubiquitous in quantum control and dynamics and in quantum information theory.
We study the von Neumann algebra \mathcal{M} = \{P,Q\}'' generated by two orthogonal projections on a separable Hilbert space. Using the Halmos direct integral decomposition in the sense of Dixmier and Takesaki, we show that \mathcal{M} decomposes into abelian parts and a measurable field of copies of M_2(\mathbb{C}). For \mu-almost every \theta \in \Theta, the self-adjoint part of the fiber M_2(\mathbb{C}), equipped with the commutator i[\cdot,\cdot], carries a three-dimensional real Lie algebra structure isomorphic to \mathfrak{su}(2). This provides a purely algebraic, fiberwise mechanism for the appearance of \mathfrak{su}(2) from minimal non-commutative data. We then consider a quantum dynamical semigroup in the standard GKSL form with noise operators P and Q. Using the Frigerio–Evans theorem, we prove that its fixed-point algebra is \{P,Q\}', which is always abelian. Consequently, \mathfrak{su}(2) does not appear in the fixed-point algebra; instead, dissipative dynamics induce a collapse from the non-commutative fiber structure to classical abelian observables. This work provides the rigorous mathematical foundation for the non-commutative projection framework developed in the author’s previous preprints and clarifies the distinction between algebraic generation and dissipative selection.
Quantum algorithms usually are described via quantum circuits representable as unitary operators. Synthesizing the unitary operators described mathematically in terms of the unitary operators recognizable as quantum circuits is essential. One such a challenge lies in the Hamiltonian simulation problem, where the matrix exponential of a large-scale skew-Hermitian matrix is to be computed. Most current techniques are prone to approximation errors, whereas the parametrization of the underlying Hamiltonian via the Cartan decomposition is more promising. To prepare for such a simulation, this work proposes to tackle the Cartan decomposition by means of the Lax dynamics. The advantages include not only that it is numerically feasible with no matrices involved, but also that this approach offers a genuine unitary synthesis within the integration errors. This work contributes to the theoretic and algorithmic foundations in three aspects: exploiting the quaternary representation of Hamiltonian subalgebras; describing a common mechanism for deriving the Lax dynamics; and providing a mathematical theory of convergence.
Recently, Vatan and Williams utilize a matrix decomposition of SU(2n)SU(2^n)SU(2n) introduced by Khaneja and Glaser to produce {\tt CNOT}-efficient circuits for arbitrary three-qubit unitary evolutions. In this note, we place the Khaneja Glaser Decomposition ({\tt KGD}) in context as a SU(2n)=KAKSU(2^n)=KAKSU(2n)=KAK decomposition by proving that its Cartan involution is type {\bf AIII}, given n≥3n \geq 3n≥3. The standard type {\bf AIII} involution produces the Cosine-Sine Decomposition (CSD), a well-known decomposition in numerical linear algebra which may be computed using mature, stable algorithms. In the course of our proof that the new decomposition is type {\bf AIII}, we further establish the following. Khaneja and Glaser allow for a particular degree of freedom, namely the choice of a commutative algebra a\mathfrak{a}a, in their construction. Let χ1n\chi_1^nχ1n​ be a {\tt SWAP} gate applied on qubits 111, nnn. Then χ1nvχ1n=k1  a  k2\chi_1^n v \chi_1^n=k_1\; a \; k_2χ1n​vχ1n​=k1​ak2​ is a KGD for $\mathfrak{a}=\mbox{span}_{\mathbb{R}} \{ \chi_1^n ( \ket{j}\bra{N-j-1} -\ket{N-j-1}\bra{j}) \chi_1^n \}$ if and only if v=(χ1nk1χ1n)(χ1naχ1n)(χ1nk2χ1n)v=(\chi_1^n k_1 \chi_1^n) (\chi_1^n a \chi_1^n)(\chi_1^n k_2 \chi_1^n)v=(χ1n​k1​χ1n​)(χ1n​aχ1n​)(χ1n​k2​χ1n​) is a CSD.
The KAK decomposition is a fundamental tool in Lie theory and quantum computing. Despite its widespread use, the mathematical foundations remain incomplete, particularly regarding the precise conditions for the decomposition and the characterization of equivalence classes under multiplication by elements of KKK. Here, we present a mathematical theory of the KAK decomposition for connected compact semisimple Lie groups and derive the decomposition for SU(4)\mathrm{SU}(4)SU(4). In particular, we clarify the relationship between various definitions of a Cartan decomposition in the literature and give a complete proof of a general KAK decomposition theorem. We then distinguish two distinct notions of KAK equivalence classes, double coset equivalence and projective equivalence, thereby addressing mathematical inconsistencies regarding KAK classification in the literature. Specifically, for SU(4)\mathrm{SU}(4)SU(4), we show that local equivalence classes under multiplication by SU(2)⊗SU(2)\mathrm{SU}(2)\otimes \mathrm{SU}(2)SU(2)⊗SU(2) are geometrically represented not by the usual "Weyl chamber" as claimed in the existing literature. Instead, the "Weyl chamber" is only recovered by the projective-local equivalence which disregards global phases. We develop a systematic theory for determining equivalence and uniqueness for both notions of equivalence. Our work establishes a rigorous Lie-theoretic foundation for the theory of quantum gates and circuits.