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For every \(\lambda _2\in \mathbb {C}\), define the associated correlation-length quantity by
For a nonzero subleading eigenvalue in the physical range \(0{\lt}|\lambda _2|{\lt}1\), this quantity is positive. If all subleading spectral values vanish and correlations therefore vanish after finitely many transfer steps, the total definition gives the limiting value \(\xi =0\).
For a matrix \(\rho \in M_{D}(\mathbb {C})\) and an auxiliary insertion \(X\in M_{D}(\mathbb {C})\), define
When \(\operatorname{tr}(\rho )=1\), this removes the trace component of \(X\rho \).
Fix an MPS tensor and a right fixed point of its transfer map. Write the tensor as \(A\) and the fixed point as \(\rho ^R\). Under the hypotheses of Theorem 5.3.2, that fixed point exists and is unique up to scaling; we normalize it so that \(\operatorname{tr}(\rho ^R)=1\). For an auxiliary-space insertion \(X\in M_{D}(\mathbb {C})\), define
The transfer map associated to a tensor \(A\) is the linear map \(\mathcal{E}_A : M_{D}(\mathbb {C}) \to M_{D}(\mathbb {C})\) defined by
Diagrammatically, the transfer map is the double-layer contraction
in which the upper node denotes \(A\), the lower node denotes \(A^\dagger \), and the physical index is summed over between them.
For auxiliary-space insertions \(X,Y\in M_{D}(\mathbb {C})\) and \(n\ge 0\), define
Equivalently, insert \(X\) at site \(0\), propagate by \(\mathcal{E}_A^n\), then insert \(Y\) and take the trace.
Suppose that \(\rho \) is a right fixed point of the transfer map, \(\mathcal{E}_A(\rho )=\rho \). Then, for every \(n\geq 0\),
When moreover \(\operatorname{tr}(\rho )=1\), the preceding lemma shows that \(Z_\rho (X)\) is traceless. The identity isolates the fixed-point contribution before the remaining transfer iterates are analysed.
For an injective trace-preserving MPS tensor, there exist \(C{\gt}0\) and \(\xi {\gt}0\) such that, for all \(n\ge 0\) and all traceless \(X\in M_{D}(\mathbb {C})\), i.e. \(\operatorname{tr}(X)=0\),
Traceless matrices lie in \(\ker P\), where \(P\) is the fixed-point projection (8). Since \(\mathcal{E}_A-P\) has spectral radius strictly less than \(1\), choose any \(r\) with \(\rho (\mathcal{E}_A-P){\lt}r{\lt}1\). The Gelfand formula then gives exponential decay with \(\xi =-1/\log r\). Choosing a rate strictly above the spectral radius is necessary in general because a Jordan block at the spectral radius can prevent a uniform bound proportional to \(\rho (\mathcal{E}_A-P)^n\).
If a constant \(C_{XY}\in \mathbb {R}\) and \(\lambda _2\in \mathbb {C}\) satisfy, for all \(n\ge 0\),
then the connected correlator satisfies that exponential decay bound. The source [ CPGSV21 , Section II.B.3 ] obtains this by combining the sum-of-exponentials expansion with the triangle inequality, while under the primitive or injective hypotheses stated in Chapter 6, the transfer-map gap results ensure that the subleading eigenvalues lie strictly inside the unit disk.
If coefficients \(c_j\in \mathbb {C}\) and eigenvalues \(\lambda _j\in \mathbb {C}\), for \(j=1,\ldots ,D^2-1\), satisfy, for all \(n\ge 0\),
then the connected correlator equals the stated sum of exponentials. The source [ CPGSV21 , Section II.B.3 ] states that the connected correlator is a sum of \(D^2-1\) pure exponentials, \(C(X,Y;n)=\sum _{j\ge 2}^{D^2}c_{XY}(j)\lambda _j^n\). This pure-exponential representation follows when the relevant subleading spectral data of the transfer map are diagonalizable. For a non-diagonalizable transfer map, nontrivial Jordan blocks can instead produce terms of the form \(n^k\lambda ^n\). Accordingly, the pure-exponential formula is retained here as an explicit interface hypothesis rather than asserted for every normal MPS.
Fix an injective, trace-preserving MPS tensor \(A\) with positive definite fixed point \(\rho \). Let
be the corresponding fixed-point projection. Then there exist \(C {\gt} 0\) and \(0 {\lt} \delta \le 1\) such that, for all \(n\ge 0\) and \(X\in M_{D}(\mathbb {C})\),
The transfer-map gap \(\delta \) exists by primitivity (the corresponding theorem in the companion quantum-channel volume [ LTC26 , “Complementary transfer-map gap for primitive maps” ] , the complementary transfer-map gap).
Let \(A\) be a normalized MPS tensor with a nonzero PSD fixed point \(\rho \) of the transfer map. If \(\rho _{\operatorname{spec}}(\mathcal{E}_A-P){\lt}1\), where \(P\) is the fixed-point projection, then \(O_{AA}(N)\to 1\) as \(N\to \infty \).
Assume \(D \ge 1\). Let \(A\) be an injective MPS tensor with \(\sum _i (A^i)^\dagger A^i = \mathbb {1}\). Then the transfer map \(\mathcal{E}_A\) has a unique positive semidefinite fixed point \(\rho \) up to scaling, and \(\rho \) is positive definite.