Abstract
This chapter introduces and treats the topic of quantum feedback control on linear quantum systems. Two distinct approaches to feedback control of quantum systems are considered: measurement-based feedback control and coherent feedback control. For measurement-based feedback control, the notions of controlled Hudson–Parthasarathy QSDEs and controlled quantum filtering equations are introduced. Three control problems are formulated and solved: measurement-based linear quadratic Gaussian control, coherent linear quadratic Gaussian control, and coherent feedback \(H^{\infty }\) control. Examples are provided to illustrate each control method.
Section 5.2 contains materials reprinted from Automatica [12], with permission from Elsevier.
Section 5.3 and the associated appendices contain materials reprinted, with permission, from [34] \(\copyright \) 2008 IEEE.
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Notes
- 1.
We note that [12] suggested that a lower LQG cost of 4.444 can be attained by a classical linear controller by measuring \(y''\) with the setting \(\theta =0\) and \(\epsilon \approx 0.715\). This is incorrect and the discrepancy arose out of a coding error therein. However, this error does not negate the findings of [12]. In fact, it only strengthens the conclusion that there can exist a coherent quantum LQG controller which outperforms all classical LQG controllers for the same cost function and actuation structure.
- 2.
This map is distinct from the quantum conditional expectation used in quantum filtering theory.
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Appendices
Appendices
Appendix A: Proof of Theorem 5.2
The proof of Theorem 5.2 will use the following lemma.
Lemma 5.4
Consider a real symmetric matrix X and corresponding operator-valued quadratic form \(x^{\top } Xx\) for the system (5.54). Then the following statements are equivalent:
-
(i)
There exists a constant \(\lambda \ge 0\) such that \( \langle \rho ,x^{\top }Xx\rangle \le \lambda \) for all Gaussian states \(\rho \).
-
(ii)
The matrix X is negative semidefinite.
Proof
\((i) \Rightarrow (ii)\). To establish this part of the lemma, consider a Gaussian state \(\rho \) which has mean \(\bar{x}\) and covariance matrix \(Y=[\mathrm{Tr}(\rho x_ix_j)]\), with symmetrized covariance \(\nicefrac {1}{2}(Y+Y^{\top }) \ge 0\) and \(Y-Y^{\top } =2 \imath \mathbb {J}_n\). Then, we can write
Now for any constant \(\alpha > 0\), consider the inequality of part (i) where \(\rho \) is a Gaussian state with mean \(\alpha \bar{x}\) and covariance matrix Y. Then, it follows from the bound \( \langle \rho ,x^{\top }Xx\rangle \le \lambda \) and (5.88) that \( \alpha ^2 \bar{x}^{\top } X \bar{x} + \mathrm{Tr}[XY] \le \lambda \ \) for all \(\alpha > 0\). From this, it immediately follows that \(\bar{x}^{\top } X \bar{x} \le 0\). However, \(\bar{x}\) can be chosen arbitrarily. Hence, we can conclude that condition (ii) of the lemma is satisfied.
\((ii) \Rightarrow (i)\). Suppose that the matrix X is negative semidefinite and let \(\rho \) be any Gaussian state and suppose that \(\rho \) has mean \(\bar{x}\) and covariance matrix \(Y \ge 0\). Then, it follows from (5.88) that \( \langle \rho ,x^{\top } Xx\rangle = \bar{x}^{\top } X \bar{x} + \mathrm{Tr}[XY] \). However, \(X \le 0\), \(Y + Y^{\top } \ge 0\), and \(Y-Y^{\top } =2 \imath \mathbb {J}_n\) implies \(\bar{x}^{\top } X \bar{x} \le 0\), and \(\mathrm{Tr}[XY] = \nicefrac {1}{2}\mathrm{Tr}[X(Y+Y^{\top })] \le 0\). Hence, \(\langle \rho ,x^{\top } Xx\rangle \le 0\) and condition (ii) is satisfied with \(\lambda = 0\). \(\Box \)
Proof of Theorem 5.2. Let the system be dissipative with \(V(x )=x^{\top } X x\). By Itō’s rule, the product table (5.60), and the quantum stochastic differential equation (5.54), we have
where \(\lambda _0\) is given by (5.59). We now note that \( \langle V(x(t)) \rangle = \langle \rho , E_0 [ V(x(t)) ] \rangle , \) where \(E_t\) (\(t \ge 0\)) denotes the conditional expectation mapFootnote 2 with respect to the vacuum state \(|\Omega \rangle \) of the field (e.g., see [51, p. 215]), and \(\rho \) is an initial Gaussian state of the system. Combining this with the integral of (5.89) and (5.56) we find that
Let \(t \rightarrow 0\) to obtain
Here, x and \(\beta _w\) denote the initial conditions. An application of Lemma 5.4 implies (5.57). Also, (5.58) is a straightforward consequence of this inequality when \(\mathsf {R}\) is replaced by \(\mathsf {R}+\epsilon I\) where \(\epsilon > 0\).
To establish the converse part of the theorem, we first assume that (5.57) is satisfied. Then with \(V(x) = x^{\top }Xx\), it follows from (5.89) that
for all \(t > 0\) and all \(\beta _w(t)\). Hence, inequality (5.56) is satisfied with \(\lambda \) given by (5.59).
If matrix inequality (5.58) is satisfied, then it follows by similar reasoning that there exists an \(\epsilon > 0\) such that
Hence, inequality (5.56) is satisfied with \(\lambda =\lambda _0\) given by (5.59) and with \(\mathsf {R}\) replaced by \(\mathsf {R}+\epsilon I\). \(\Box \)
Appendix B: Proof of Lemma 5.2
The proof of Lemma 5.2 will use the following lemma.
Lemma 5.5
If S is a Hermitian matrix, then there is a real constant \(\alpha _0\) such that \(\alpha I + S \ge 0\) for all \(\alpha \ge \alpha _0\).
Proof
Since S is Hermitian, it has real eigenvalues and is diagonalizable. Hence, \(S=V^*EV\) for some real diagonal matrix E and orthogonal matrix V. Now let \(\alpha _0=-\lambda \), where \(\lambda \) is the smallest eigenvalue of S. The result follows since \(\alpha I + S=V^*(\alpha I + E)V\) while \(\alpha I +E \ge 0\) for all \(\alpha \ge \alpha _0\). \(\Box \)
Proof of Lemma 5.2. The main idea is to explicitly construct matrices \(R \in \mathbb {R}^{2n_K \times 2n_K}\), \(\mathsf {K} \in \mathbb {C}^{(n_{v_K}+n_y) \times 2n_K}\), \(B_{K1} \in \mathbb {R}^{2n_K \times 2n_{v_K}}\), and \(B_{K0} \in \mathbb {R}^{2n_u \times 2n_{v_K}}\), with \(n_{v_K} \ge n_u\), such that (see Chap. 2)
are satisfied. To this end, let \(Z=\frac{1}{2}\mathbb {J}_{n_K}^{-1}A=-\frac{1}{2}\mathbb {J}_{n_K} A\). We first construct matrices \(\mathsf {K}_{b2}\), \(\mathsf {K}_{b1}\), \(B_{K1,1}\), and \(B_{K1,2}\) according to the following procedure:
-
1.
Construct the matrix \(\mathsf {K}_{b2}\) according to (5.75).
-
2.
Construct a real symmetric \(2n_K \times 2n_K\) matrix \(W_1\) such that the matrix
$$\begin{aligned} W_2= & {} W_1 \\&\;+\imath \left( \frac{Z-Z^{\top }}{2}-\frac{1}{4}C_K^{\top }P_{n_u}^{\top }\left[ \begin{array}{cc} 0 &{} I \\ -I &{} 0 \end{array} \right] P_{n_u}C_K -\mathfrak {I}(\mathsf {K}_{b2}^*\mathsf {K}_{b2}) \right) , \end{aligned}$$is non-negative definite. It follows from Lemma 5.5 that such a matrix \(W_1\) always exists.
-
3.
Construct a matrix \(\mathsf {K}_{b1}\) such that \(\mathsf {K}_{b1}^* \mathsf {K}_{b1}=W_2\), where \(\mathsf {K}_{b1}\) has at least 1 row. This can be done, for example, using the singular value decomposition of \(W_2\) (in this case, \(\mathsf {K}_{b1}\) will have \(2n_K\) rows).
-
4.
Construct the matrices \(B_{K1,1}\) and \(B_{K1,2}\) according to Eqs. (5.74) and (5.76), respectively.
Let \(R=\frac{1}{2}(Z+Z^{\top })\). We now show that there exists an integer \(n_{v_K} \ge n_u\) such conditions (5.90)–(5.93) are satisfied with the matrix R as defined and with \(B_{K1}=[\begin{array}{cc} B_{K1,1}&B_{K1,2} \end{array}]\) and
First note that necessarily \(n_{v_K} \ge n_u+1 > n_u\) since \(B_{K1}\) has at least \(2n_{u}+2\) columns. Also, by virtue of our choice of \(\mathsf {K}_{b1}\), we have
and hence
Since \(R=\frac{Z+Z^{\top }}{2}\), we have \(R+\mathfrak {I}(\mathsf {K}^* \mathsf {K})=Z\). Therefore, (5.90) is satisfied.
Now, we observe that \( \imath \mathbb {J}_{n_K} B_K\mathrm{diag}_{n_y}(M^*)P_{n_y}^{\top }=[\begin{array}{cc} T&-T^\# \end{array}] \ \) for some \(2n_K \times n_y\) complex matrix T. But by taking the conjugate transpose of both sides of (5.75) which defined \(\mathsf {K}_{b2}\), we conclude that \(T=-\mathsf {K}_{b2}^*\). Hence,
From (5.74) which defined \(B_{K1,1}\), we obtain
Combining (5.76), (5.95) and (5.96) gives us
Therefore, (5.91) is also satisfied. Moreover, it is straightforward to verify (5.92) by substituting \(\mathsf {K}\) as defined by (5.94) into the right-hand side of (5.92). Finally, since \(n_{v_K} \ge n_u\), it follows that \([\begin{array}{cc} B_{K0}&0_{2n_u \times 2(n_{v_K}+n_y-n_u)} \end{array}]\) is precisely the right-hand side of (5.93). This completes the proof of Theorem 5.4. \(\Box \)
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Nurdin, H.I., Yamamoto, N. (2017). Feedback Control of Linear Dynamical Quantum Systems. In: Linear Dynamical Quantum Systems. Communications and Control Engineering. Springer, Cham. https://doi.org/10.1007/978-3-319-55201-9_5
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