9 Peripheral Channel Structure and Transfer-Operator Gaps
This chapter studies the peripheral spectrum of finite-dimensional quantum channels: the eigenvalues of unit modulus that survive the ergodic averaging of Chapter 8, following [ Wol12 , Chapter 6 ] . For a finite Kraus map, the peripheral eigenvalues form a finite cyclic group.
9.1 Peripheral eigenvalue group structure
This section proves a finite-Kraus specialization of the cyclicity conclusion in [ Wol12 , Theorem 6.6(1) ] : the peripheral eigenvalues form a finite cyclic group. It does not establish the bound on the group order in item (1), nor the conclusions in items (2)–(4). Wolf’s theorem assumes an irreducible positive unital Schwarz map, whereas the statement below assumes a Kraus representation and hence complete positivity. The remaining abstract Schwarz-map case is not included. The trace-preserving refinement that the order divides the bond dimension is proved in Theorem 9.2.2. The invertibility of peripheral eigenvectors and the product closure of the peripheral eigenvalues used below are proved in Section 9.8.
Let \(E\) be an irreducible unital Kraus map on \(M_{D}(\mathbb {C})\) with a positive-definite adjoint fixed point (trace-preservation is not required). Then there exist \(m \ge 1\) and a primitive \(m\)-th root of unity \(\gamma \) such that the peripheral eigenvalues of \(E\) are exactly \(\{ 1,\gamma ,\gamma ^2,\ldots ,\gamma ^{m-1}\} \).
Let \(S\) be the set of peripheral eigenvalues and let \(m=|S|\). Finiteness of \(S\) and \(1\in S\) give \(m{\gt}0\). Every element of \(S\) is a root of unity, while \(S\) is closed under products and powers. Hence \(\mu ^{-1}\) belongs to \(S\) whenever \(\mu \in S\). Multiplication by such a \(\mu \) therefore permutes \(S\). Since no element of \(S\) vanishes,
Cancelling the nonzero product gives \(\mu ^m=1\).
Let \(\gamma =\exp (2\pi i/m)\), a primitive \(m\)-th root of unity. The set \(S\) is contained in the set of all \(m\)-th roots of unity, and both sets have cardinality \(m\). Thus they are equal. Consequently every element of \(S\) is \(\gamma ^j\) for some \(0\leq j{\lt}m\), and power closure gives the reverse inclusion.
9.2 Peripheral spectral refinements
The trace-preserving refinements below and the cyclic decomposition and one-dimensionality results for the peripheral spectrum are generic finite-Kraus-map statements, with no tensor-network content; they are relocated here from the periodic-decomposition appendix, whose blocking and canonical-form arguments cite them across the chapter boundary.
Let \(\mathcal{E}_K\) be the Kraus map of a finite matrix family \(K\). Assume that \(\mathcal{E}_K\) is irreducible and unital and has a positive-definite adjoint fixed point. Then there exist \(m\geq 1\) and a primitive \(m\)-th root of unity \(\gamma \) such that the peripheral eigenvalues of \(\mathcal{E}_K\) are exactly \(\{ 1,\gamma ,\gamma ^2,\ldots ,\gamma ^{m-1}\} \).
The peripheral eigenvalues form a finite subgroup of \(\mathbb {C}^\times \): they contain \(1\), are nonzero, and are closed under multiplication and inversion. Every finite subgroup of \(\mathbb {C}^\times \) is cyclic. Choosing a generator \(\gamma \) gives the asserted primitive root and enumeration.
Let \(K\) be a finite matrix family on \(M_{D}(\mathbb {C})\) with Kraus map \(\mathcal{E}_K\). Assume that \(\mathcal{E}_K\) is irreducible, that \(K\) is unital and trace-preserving, and that the adjoint Kraus map has a positive-definite fixed point. Then there exist \(m\geq 1\) and a primitive \(m\)-th root of unity \(\gamma \) such that \(m\mid D\) and the peripheral eigenvalues of \(\mathcal{E}_K\) are exactly \(\{ 1,\gamma ,\gamma ^2,\ldots ,\gamma ^{m-1}\} \).
Apply Theorem 9.2.1 for the cyclic structure. Divisibility \(m\mid D\) follows from the cyclic decomposition: \(m\) mutually orthogonal projections summing to \(\mathbb {1}\) each have equal trace by trace preservation, so \(m\, \operatorname{tr}(P_0)=D\) with \(\operatorname{tr}(P_0)\in \mathbb {N}\).
Let \(K\) be a finite matrix family on \(M_{D}(\mathbb {C})\) with Kraus map \(\mathcal{E}_K\). Assume that \(\mathcal{E}_K\) is irreducible, that \(K\) is unital and trace-preserving, and that the adjoint Kraus map fixes a positive-definite matrix. Let \(\gamma \) be a primitive \(m\)-th root of unity such that the peripheral eigenvalues are exactly \(\{ \gamma ^k:k\in \{ 0,\ldots ,m{-}1\} \} \). Then \(m\mid D\).
The cyclic decomposition gives orthogonal projections \(P_0,\ldots ,P_{m-1}\) with \(\sum _kP_k=\mathbb {1}\) and \(E(P_{k+1})=P_k\). Trace preservation gives \(\operatorname{tr}(P_{k+1})=\operatorname{tr}(P_k)\) for every \(k\), hence
Since the trace of an orthogonal projection is an integer, \(m\mid D\).
9.2.1 Cyclic decomposition of irreducible finite Kraus maps
The construction — normalizing a peripheral eigenvalue to a unitary eigenvector, forming its discrete Fourier (cyclic) spectral projections, and the supporting corner-algebra apparatus (restriction to an invariant corner, corner rank, and the compression isometry \(PM_{D}(\mathbb {C})P\cong M_{n}(\mathbb {C})\)) — is given in Section 9.8.
Let \(K\) be a finite unital matrix family whose Kraus map is irreducible, and suppose the adjoint Kraus map fixes a positive-definite matrix. If the peripheral spectrum is generated by a primitive \(m\)-th root \(\gamma \), then there are a unitary \(U\) and orthogonal projections \(P_0,\ldots ,P_{m-1}\) summing to \(\mathbb {1}\) such that \(E_K(U^k)=\gamma ^kU^k\), \(U^m=\mathbb {1}\), \(U=\sum _{k=0}^{m-1}\gamma ^kP_k\), and \(E_K(P_{k+1})=P_k\).
Normalize an eigenvector for \(\gamma \) to a unitary \(U\). Its powers remain eigenvectors, and the Fourier projections of \(U\) give the stated cyclic decomposition.
Let \(K\) be a finite unital matrix family whose Kraus map is irreducible, and suppose that the adjoint Kraus map fixes a positive-definite matrix. For every peripheral eigenvalue \(\gamma \) of the transfer map, the \(\gamma \)-eigenspace is one-dimensional.
Given a peripheral unitary eigenvector \(U\) for \(\gamma \), the multiplicative-domain identity gives \(E(XU^\dagger )=XU^\dagger \) for any \(\gamma \)-eigenvector \(X\). By the scalar fixed-point lemma for irreducible unital maps, \(XU^\dagger =c\mathbb {1}\), hence \(X=cU\) and the eigenspace is one-dimensional.
9.3 Peripheral Channel Structure and Transfer-Operator Gaps: Supporting Results
This section collects the generic supporting results for finite-dimensional quantum channels behind the peripheral spectral theory of Section 9.2: an auxiliary trace identity and trace-positivity result, the Banach-algebra convergence fact behind the overlap-decay theorems, the rank-one Perron projection behind the primitive overlap limit, and the cyclic-decomposition machinery that removes peripheral periodicity.
9.4 Auxiliary trace identities
For any linear endomorphism \(T\) on \(M_{D_1\times D_2}(\mathbb {C})\), the operator trace expands as
where \(E_{pq}\in M_{D_1\times D_2}(\mathbb {C})\) has entry \(1\) in position \((p,q)\) and zero elsewhere.
The operator trace is \(\operatorname{Tr}(T)=\sum _{p,q}\operatorname{tr}(T(E_{pq})E_{qp})\), and \(\operatorname{tr}(ME_{qp})=M_{pq}\).
9.5 Auxiliary trace positivity
If \(A,B\geq 0\), then \(\operatorname{tr}(AB)\geq 0\).
Write \(B=U\Lambda U^\dagger \) with \(U\) unitary and \(\Lambda \) diagonal. Then
because \(U^\dagger AU\geq 0\) and \(\Lambda _{ii}\geq 0\) for every \(i\).
9.6 Spectral-radius decay and overlap limits
Let \(a\) be an element of a complex Banach algebra with \(\rho _{\operatorname{spec}}(a){\lt}1\). Then \(a^n\to 0\) as \(n\to \infty \).
Choose \(r\) with \(\rho _{\operatorname{spec}}(a){\lt}r{\lt}1\). The Gelfand formula \(\| a^n\| ^{1/n}\to \rho _{\operatorname{spec}}(a)\) gives \(\| a^n\| \leq r^n\) for all sufficiently large \(n\), and \(r^n\to 0\).
9.7 Rank-one Perron projection
and \(N:=E-P\) for the complementary part. The power decomposition (Theorem 2.12.2, Chapter 2) gives \(E^n=P+N^n\) for \(n\geq 1\).
The fixed-point projection \(P\) has operator trace \(\operatorname{Tr}(P)=1\).
\(P\) has the rank-one form \(P(X)=f(X)\rho \) for the linear functional \(f(X)=\operatorname{tr}(X)/\operatorname{tr}(\rho )\). The operator trace of a rank-one endomorphism \(X\mapsto f(X)\rho \) equals \(f(\rho )\), and \(f(\rho )=\operatorname{tr}(\rho )/\operatorname{tr}(\rho )=1\).
Let \(V\) be a nonzero finite-dimensional complex normed space. If every eigenvalue of an endomorphism \(F:V\to V\) satisfies \(|\lambda |{\lt}1\), then the spectral radius of \(F\) is strictly less than \(1\).
Let \(E:M_{D}(\mathbb {C})\to M_{D}(\mathbb {C})\) be an irreducible primitive channel, and let \(\rho \ne 0\) be a positive semidefinite fixed point. Then \(\operatorname{tr}(\rho )\ne 0\) and, for \(P=P_\rho \), \(\rho _{\operatorname{spec}}(E-P){\lt}1\).
Positive semidefiniteness and \(\rho \ne 0\) imply \(\operatorname{tr}(\rho )\ne 0\). Every eigenvalue of \(E-P\) has modulus strictly less than one by irreducibility and primitivity. Since \(M_{D}(\mathbb {C})\) is finite-dimensional, the maximum eigenvalue modulus equals the spectral radius.
9.8 Periodicity removal
This section proves the cyclic-decomposition machinery of Theorem 9.2.1.1 and the divisibility statements of Theorem 9.2.2 and Theorem 9.2.3: normalizing a peripheral eigenvector to a unitary, forming its discrete Fourier (cyclic) spectral projections, and tracking how the channel shifts the resulting corners.
Let \(E\) be an irreducible unital Kraus map on \(M_{D}(\mathbb {C})\) with a positive-definite adjoint fixed point. If \(X \ne 0\) satisfies \(E(X) = \mu X\) with \(|\mu | = 1\), then \(X\) is invertible.
By the Kadison–Schwarz inequality (3), the gap \(G=E(X^\dagger X)-E(X)^\dagger E(X)\) is positive semidefinite. Pairing \(G\) with the positive-definite adjoint fixed point and using \(E(X)=\mu X\) and \(|\mu |=1\) gives weighted trace zero, hence \(G=0\). Therefore \(E(X^\dagger X)=E(X)^\dagger E(X)=X^\dagger X\), so \(X^\dagger X\) is a nonzero positive semidefinite fixed point. Irreducibility upgrades it to a positive-definite, hence invertible, matrix, so \(\det (X)\ne 0\).
Let \(E\) be an irreducible unital Kraus map on \(M_{D}(\mathbb {C})\) with a positive-definite adjoint fixed point. If \(\mu , \nu \) are peripheral eigenvalues of \(E\), then so is \(\mu \nu \).
Take eigenvectors \(X\) and \(Y\) for \(\mu \) and \(\nu \), respectively. The Kadison–Schwarz equality at \(X\) places \(X\) in the multiplicative domain. Thus the right multiplicative identity (12) gives \(E(YX)=E(Y)E(X)=(\nu \mu )YX\). Since \(X\) and \(Y\) are invertible by Lemma 9.8.1, \(YX\ne 0\), and \(|\mu \nu |=1\).
If \(E\) is irreducible and unital, then every fixed point of \(E\) is a scalar multiple of \(\mathbb {1}\).
If \(E(X)=X\), then the Hermitian matrices \(X+X^\dagger \) and \(\mathrm{i}(X-X^\dagger )\) are also fixed by \(E\). The positive-semidefinite fixed-point uniqueness theorem gives \(X+X^\dagger =a\mathbb {1}\) and \(\mathrm{i}(X-X^\dagger )=b\mathbb {1}\), hence \(X=\frac{1}{2}(a-\mathrm{i}b)\mathbb {1}\).
For an irreducible unital Schwarz map with faithful adjoint fixed point, each peripheral eigenvalue admits a unitary eigenvector.
For an eigenvector \(X\) at a peripheral eigenvalue \(\gamma \), the Kadison–Schwarz equality gives \(E(X^\dagger X)=E(X)^\dagger E(X)=X^\dagger X\), so \(X^\dagger X\) is a nonzero positive semidefinite fixed point. Irreducible uniqueness of the positive semidefinite fixed point makes it a positive scalar \(c\mathbb {1}\); rescaling \(X\) by \(c^{-1/2}\) produces a unitary eigenvector.
If \(E(U)=\mu U\) with \(|\mu |=1\) and \(U\) unitary, then \(E(U^n)=\mu ^nU^n\) for every \(n\).
The Kadison–Schwarz equality at the unitary eigenvector places \(U\) in the multiplicative domain, so the right multiplicative identity (12) gives \(E(U^n)=E(U)^n=\mu ^nU^n\) by induction on \(n\).
Peripheral unitary eigenvectors can be normalized compatibly with the faithful fixed-point state.
Given a unitary eigenvector \(U\) for a primitive \(m\)-th root \(\gamma \), Lemma 9.8.5 gives \(E(U^m)=U^m\), a fixed point that is scalar by Lemma 9.8.3: \(U^m=\alpha \mathbb {1}\). Unitarity of \(U^m\) forces \(|\alpha |=1\); multiplying \(U\) by an \(m\)-th root \(\beta \) of \(\alpha ^{-1}\) produces \((\beta U)^m=1\) while preserving the eigenvector equation.
A primitive \(m\)-th peripheral root yields \(m\) orthogonal projections summing to \(\mathbb {1}\) and cyclically permuted by the channel.
Given a unitary \(U\) of order \(m\) with \(E(U)=\gamma U\) for a primitive \(m\)-th root \(\gamma \), the Fourier projections \(P_k:=m^{-1}\sum _{j=0}^{m-1}\overline\gamma ^{kj}U^j\) are mutually orthogonal and sum to \(\mathbb {1}\) by discrete Fourier orthogonality of the characters \(j\mapsto \gamma ^{kj}\); since \(E(U^j)=\gamma ^jU^j\) (Lemma 9.8.5), each Fourier mode is shifted by one step, giving \(E(P_{k+1})=P_k\).
Combining these lemmas proves Theorem 9.2.1.1: Lemma 9.8.6 supplies a unitary generator of exact order \(m\) for a primitive \(m\)-th peripheral root, and Lemma 9.8.7 builds the \(m\) Fourier projections out of its powers, using Lemma 9.8.5 to identify how the channel shifts them.
9.8.1 Cyclic corners and restricted primitivity
For an orthogonal projection \(P\) and linear map \(E\), the corner \(PM_{D}(\mathbb {C})P\) is preserved if \(E(PXP)=PE(PXP)P\) for every \(X\).
The corner subspace associated with \(P\) is \(\{ PXP:X\in M_{D}(\mathbb {C})\} \).
The restriction of \(E\) to an invariant corner \(PM_{D}(\mathbb {C})P\).
Irreducibility of the corner-restricted map.
The rank of an orthogonal projection \(P\in M_{D}(\mathbb {C})\), equivalently the dimension of its range.
Let \(P\in M_{D}(\mathbb {C})\) be an orthogonal projection of rank \(n\). The corner algebra \(PM_{D}(\mathbb {C})P\) is linearly isomorphic to the full matrix algebra \(M_{n}(\mathbb {C})\). The isomorphism is built from the spectral diagonalisation of \(P\) by conjugating the top-left \(n\times n\) block by the unitary diagonalising \(P\).
The rank of an orthogonal projection \(P\) equals its trace: \(n=\operatorname{tr}(P)\).
The eigenvalues of an orthogonal (Hermitian idempotent) projection are \(0\) or \(1\): the eigenvalues \(\lambda \) satisfy \(\lambda ^2=\lambda \) from \(P^2=P\). The trace is the sum of the eigenvalues, which counts the eigenvalue-\(1\) multiplicities, i.e. the rank \(n\).
Appropriate powers of the channel preserve each sector corner.
Induction on the exponent, using the left- and right-multiplicative domain identities on each sector projection \(P_k\), shows \(T^n(P_{k+n\bmod m}XP_{k+n\bmod m})=P_k\, T^n(X)\, P_k\); specializing to \(n=m\), where \(P_{k+m}=P_k\), gives that \(T^m\) preserves the corner \(P_kM_{D}(\mathbb {C})P_k\).
Let \(P\in M_{D}(\mathbb {C})\) be a nonzero idempotent and let \(E\) be a linear map on \(M_{D}(\mathbb {C})\) that preserves the corner \(PM_{D}(\mathbb {C})P\), is primitive, and fixes the corner projection, \(E(P)=P\). Then the restriction of \(E\) to the corner \(PM_{D}(\mathbb {C})P\) is again primitive.
The corner projection \(P\) lies in its own corner and is fixed by the restriction, so \(1\) is a peripheral eigenvalue of the restriction. Conversely, every eigenvalue of the restriction of unit modulus arises from a nonzero corner element \(X\) with \(E(X)=\mu X\); viewing \(X\) as an element of \(M_{D}(\mathbb {C})\) exhibits \(\mu \) as a peripheral eigenvalue of \(E\). Primitivity of \(E\) forces \(\mu =1\), so the peripheral spectrum of the restriction is exactly \(\{ 1\} \) and the restriction is primitive.
Let \(T\) be irreducible, let \(P_0,\ldots ,P_{m-1}\) be orthogonal projections summing to \(\mathbb {1}\) and cyclically permuted by \(T\), and suppose that every orthogonal projection \(Q\) with \(QP_k=P_kQ=Q\) that is invariant under the corner restriction of \(T^m\) to \(P_kM_{D}(\mathbb {C})P_k\) admits an orthogonal projection \(R\) invariant under \(T\) on the full algebra with \(Q=0\iff R=0\) and \(Q=P_k\iff R=\mathbb {1}\). Then, for every \(k\), the restriction of \(T^m\) to the corner \(P_kM_{D}(\mathbb {C})P_k\) is irreducible.
Let \(Q\) be an invariant projection for the corner restriction of \(T^m\) on \(P_kM_{D}(\mathbb {C})P_k\). The orbit-sum hypothesis supplies an ambient invariant projection \(R\) for \(T\) with \(Q=0\iff R=0\) and \(Q=P_k\iff R=\mathbb {1}\). Irreducibility of \(T\) forces \(R=0\) or \(R=\mathbb {1}\), hence \(Q=0\) or \(Q=P_k\) by the two biconditionals.
Each sector restriction is primitive.
Every peripheral eigenvalue of \(T\) is an \(m\)-th root of unity, so the peripheral spectrum of \(T^m\) is exactly \(\{ 1\} \); combined with \(T^m(P_k)=P_k\), Lemma 9.8.1.9 makes the corner restriction of \(T^m\) to \(P_kM_{D}(\mathbb {C})P_k\) primitive.
The channel raised to the period preserves every cyclic corner.
The same induction as in Lemma 9.8.1.8, with the cyclic shift \(k\mapsto k+1\) replaced by a permutation \(\sigma \) of the sector index set, shows that \(T^{\mathrm{ord}(\sigma )}\) preserves each corner \(P_kM_{D}(\mathbb {C})P_k\).
9.8.2 Group structure and divisibility
The product of two peripheral eigenvalues is peripheral.
Peripheral eigenvalues admit unitary eigenvectors (Lemma 9.8.4). If \(U_\alpha ,U_\beta \) are unitary eigenvectors for \(\alpha ,\beta \), the multiplicative-domain identity gives \(E(U_\alpha U_\beta )=E(U_\alpha )E(U_\beta )=\alpha \beta \, U_\alpha U_\beta \), and \(U_\alpha U_\beta \neq 0\) since both factors are unitary.
The inverse of a peripheral eigenvalue is peripheral.
For a unitary eigenvector \(U_\alpha \) with \(|\alpha |=1\), conjugating the eigenvector equation gives \(E(U_\alpha ^\dagger )=\overline\alpha \, U_\alpha ^\dagger =\alpha ^{-1}U_\alpha ^\dagger \), and \(U_\alpha ^\dagger \neq 0\).
Theorem 9.2.1.2 follows the same pattern: given a peripheral unitary eigenvector \(U\) for \(\gamma \) (Lemma 9.8.4), the multiplicative-domain identity gives \(E(XU^\dagger )=XU^\dagger \) for any \(\gamma \)-eigenvector \(X\), so the scalar fixed-point lemma for irreducible unital maps (Lemma 9.8.3) gives \(XU^\dagger =c\mathbb {1}\), hence \(X=cU\) and the eigenspace is one-dimensional.
The divisibility statements of Theorem 9.2.2 and Theorem 9.2.3 follow from Lemma 9.8.7 and Theorem 9.8.1.7: the \(m\) cyclic Fourier projections \(P_0,\ldots ,P_{m-1}\) sum to \(\mathbb {1}\) and are cyclically permuted by \(E\), so trace preservation gives \(\operatorname{tr}(P_{k+1})=\operatorname{tr}(P_k)\) for every \(k\), hence \(D=\operatorname{tr}(\mathbb {1})=\sum _{k=0}^{m-1}\operatorname{tr}(P_k)=m\, \operatorname{tr}(P_0)\). Since the trace of an orthogonal projection is a natural number (Theorem 9.8.1.7), \(m\mid D\).