APPENDIX A
The lemmas below contain well-known results necessary for the further presentation.
Lemma A.1 [1]. Let X and Y be the solutions of the dual Lyapunov equations with a Hurwitz matrix A:
$${{A}^{{\text{T}}}}X + XA + W = 0\quad and\quad AY + Y{{A}^{{\text{T}}}} + V = 0.$$
Then
$$\operatorname{tr} (XV) = \operatorname{tr} (YW).$$
Lemma A.2 [10].
(1) Matrices A and B of compatible dimensions satisfy the relations
$${{\left\| {AB} \right\|}_{F}}\;\leqslant \;{{\left\| A \right\|}_{F}}\left\| B \right\|,$$
$$\left| {\operatorname{tr} AB} \right|\;\leqslant \;{{\left\| A \right\|}_{F}}{{\left\| B \right\|}_{F}},$$
$$\left\| A \right\|\;\leqslant \;{{\left\| A \right\|}_{F}},$$
$$AB + {{B}^{{\text{T}}}}{{A}^{{\text{T}}}}\;\leqslant \;\varepsilon A{{A}^{{\text{T}}}} + \frac{1}{\varepsilon }{{B}^{{\text{T}}}}B\quad for\;any\;\varepsilon > 0.$$
(2) Nonnegative definite matrices A and B satisfy the relations
$$0\;\leqslant \;{{\lambda }_{{\min }}}(A){{\lambda }_{{\max }}}(B)\;\leqslant \;{{\lambda }_{{\min }}}(A)\operatorname{tr} B\;\leqslant \;\operatorname{tr} AB\;\leqslant \;{{\lambda }_{{\max }}}(A)\operatorname{tr} B\;\leqslant \;\operatorname{tr} A\operatorname{tr} B.$$
Lemma A.3 [1]. The solution P of the Lyapunov equation
$$AP + P{{A}^{{\text{T}}}} + Q = 0$$
with a Hurwitz matrix A and Q \( \succ \) 0 obeys the bounds
$${{\lambda }_{{\max }}}(P)\; \geqslant \;\frac{{{{\lambda }_{{\min }}}(Q)}}{{2\sigma }},\quad {{\lambda }_{{\min }}}(P)\; \geqslant \;\frac{{{{\lambda }_{{\min }}}(Q)}}{{2\left\| A \right\|}},$$
where σ = \( - \mathop {\max }\limits_i \operatorname{Re} {{\lambda }_{i}}(A)\).
If Q = DDT and the pair (A, D) is controllable, then
$${{\lambda }_{{\max }}}(P)\; \geqslant \;\frac{{{{{\left\| {u{\kern 1pt} *{\kern 1pt} D} \right\|}}^{2}}}}{{2\sigma }} > 0,$$
where
$$u{\kern 1pt} *{\kern 1pt} A = \lambda u{\kern 1pt} *{\kern 1pt} ,\quad \operatorname{Re} \lambda = - \sigma ,\quad \left\| u \right\| = 1,$$
i.e., u is the left eigenvector of the matrix A corresponding to the eigenvalue λ of the matrix A with the greatest real part. The vector u and the number λ can be complex-valued; here, u* denotes the Hermitian conjugate.
APPENDIX B
Proof of Lemma 1. Indeed, if the matrix \({{\mathcal{A}}_{0}}\) + {\(\mathcal{A}\), k} is Hurwitz, then σ(\({{\mathcal{A}}_{0}}\) + {\(\mathcal{A}\), k}) > 0 and there exists the solution P \( \succcurlyeq \) 0 of the Lyapunov equation (10) for 0 < α < 2σ(\({{\mathcal{A}}_{0}}\) + {\(\mathcal{A}\), k}). Thus, the function f(k, α) > 0 is well-defined and f(k) > 0 by Theorem 1. The proof of Lemma 1 is complete.
Proof of Lemma 2. The optimization problem has the form
$$\min f(k,\alpha ),\quad f(k,\alpha ) = \operatorname{tr} P{{\left( {C\;0} \right)}^{{\text{T}}}}\left( {C\;0} \right) + \rho {{\left| k \right|}^{2}}$$
subject to the constraint described by the Lyapunov equation
$$\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k\} + \frac{\alpha }{2}I} \right)P + P{{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}} + \frac{1}{\alpha }\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}^{{\text{T}}}} = 0.$$
To differentiate with respect to k, we add the increment Δk and denote the corresponding increment of P by ΔP:
$$\begin{gathered} \left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k + \Delta k\} + \frac{\alpha }{2}I} \right)(P + \Delta P) \\ + \;(P + \Delta P){{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k + \Delta k\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}} + \frac{1}{\alpha }\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}^{{\text{T}}}} = 0. \\ \end{gathered} $$
Let us apply linearization and subtract this and the previous equations to obtain
$$\begin{gathered} \left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k\} + \frac{\alpha }{2}I} \right)\Delta P + \Delta P{{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}} \\ + \;\{ \mathcal{A},\Delta k\} P + P{{\{ \mathcal{A},\Delta k\} }^{{\text{T}}}} = 0. \\ \end{gathered} $$
(B.1)
The increment of f(k) is calculated by linearizing the corresponding terms:
$$\begin{gathered} \Delta f(k) = \operatorname{tr} (P + \Delta P){{\left( {C\;0} \right)}^{{\text{T}}}}\left( {C\;0} \right) + \rho {{\left| {k + \Delta k} \right|}^{2}} \\ - \;\left( {\operatorname{tr} P{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + \rho {{{\left| k \right|}}^{2}}} \right) = \operatorname{tr} \Delta P{{\left( {C\;0} \right)}^{{\text{T}}}}\left( {C\;0} \right) + 2\rho {{k}^{{\text{T}}}}\Delta k. \\ \end{gathered} $$
Consider Eq. (14), dual to (B.1). Due to Lemma A.1, from Eqs. (B.1) and (14) it follows that
$$\Delta f(k) = 2\operatorname{tr} Y\{ \mathcal{A},\Delta k\} P + 2\rho {{k}^{{\text{T}}}}\Delta k.$$
Thus,
$$df(k) = 2\operatorname{tr} PY\sum\limits_{i = 1}^2 {{{\mathcal{A}}_{i}}d{{k}_{i}}} + 2\rho \sum\limits_{i = 1}^2 {{{k}_{i}}d{{k}_{i}},} $$
which leads to (12).
The validity of (13) is demonstrated by analogy with ([1], Lemma 1). The proof of Lemma 2 is complete.
Proof of Lemma 3. The value \(\left( {\nabla _{{kk}}^{2}f(k)e,e} \right)\) is calculated by differentiating ∇k f(k) in the direction e ∈ \({{\mathbb{R}}^{2}}\). For this purpose, linearizing the corresponding terms and using the convenient notation
$$[\operatorname{tr} PY\mathcal{A}] = \left( \begin{gathered} \operatorname{tr} PY{{\mathcal{A}}_{1}} \\ \operatorname{tr} PY{{\mathcal{A}}_{2}} \\ \end{gathered} \right),$$
we calculate the increment of ∇k f(k) in the direction e:
$$\frac{1}{2}\Delta {{\nabla }_{k}}f(k)e = \rho (k + \delta e) + [\operatorname{tr} (P + \Delta P)(Y - \Delta Y)\mathcal{A}] - (\rho k + [\operatorname{tr} PY\mathcal{A}])$$
$$ = \rho (k + \delta e) + [\operatorname{tr} (P + \delta P{\kern 1pt} '(k)e)(Y + \delta Y{\kern 1pt} '(k)e)\mathcal{A}] - (\rho k + [\operatorname{tr} PY\mathcal{A}])$$
$$ = \delta (\rho e + [\operatorname{tr} (PY{\kern 1pt} '(k)e + P{\kern 1pt} '(k)eY)\mathcal{A}]),$$
where
$$\Delta P = P(k + \delta e) - P(k) = \delta P{\kern 1pt} '(k)e,$$
$$\Delta Y = Y(k + \delta e) - Y(k) = \delta Y{\kern 1pt} '(k)e.$$
Thus, with P ' = P '(k)e and Y ' = Y '(k)e, we have
$$\frac{1}{2}\left( {\nabla _{{kk}}^{2}f(k)e,\,\,e} \right) = (\rho e + [\operatorname{tr} (PY{\kern 1pt} '\; + P{\kern 1pt} '{\kern 1pt} Y)\mathcal{A}],\,\,e).$$
Furthermore, P = P(k) is the solution of Eq. (17). We write it in increments in the direction e:
$$\begin{gathered} \left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k + \delta e\} + \frac{\alpha }{2}I} \right)(P + \delta P{\kern 1pt} ') \\ + \;(P + \delta P{\kern 1pt} '){{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k + \delta e\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}} + \frac{1}{\alpha }\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}^{{\text{T}}}} = 0 \\ \end{gathered} $$
or
$$\begin{gathered} \left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k\} + \frac{\alpha }{2}I} \right)(P + \delta P{\kern 1pt} ') + (P + \delta P{\kern 1pt} '){{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}} \\ + \;\delta \left( {\{ \mathcal{A},\,\,e\} P + P{{{\{ \mathcal{A},\,\,e\} }}^{{\text{T}}}}} \right) + \frac{1}{\alpha }\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}^{{\text{T}}}} = 0. \\ \end{gathered} $$
Subtracting Eq. (17) from this expression gives Eq. (16).
Similarly, Y = Y(k) is the solution of the Lyapunov equation (14). We write it in increments in the direction e:
$$\begin{gathered} {{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k + \delta e\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}}(Y + \delta Y{\kern 1pt} ') \\ + \;(Y + \delta Y{\kern 1pt} ')\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k + \delta e\} + \frac{\alpha }{2}I} \right) + {{\left( {C\;0} \right)}^{{\text{T}}}}\left( {C\;0} \right) = 0 \\ \end{gathered} $$
or
$$\begin{gathered} {{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}}(Y + \delta Y{\kern 1pt} ') + (Y + \delta Y{\kern 1pt} ')\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k + \delta e\} + \frac{\alpha }{2}I} \right) \\ + \;\delta \left( {{{{\{ \mathcal{A},\,\,e\} }}^{{\text{T}}}}Y + Y\{ \mathcal{A},e\} } \right) + {{\left( {C\;0} \right)}^{{\text{T}}}}\left( {C\;0} \right) = 0. \\ \end{gathered} $$
Subtracting Eq. (14) from this expression yields
$${{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k\} + \frac{\alpha }{2}I} \right)}^{{\text{T}}}}Y + Y{\kern 1pt} '\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k\} + \frac{\alpha }{2}I} \right) + {{\{ \mathcal{A},\,\,e\} }^{{\text{T}}}}Y + Y\{ \mathcal{A},\,\,e\} = 0.$$
(B.2)
From (16) and (B.2) it follows that
$$\operatorname{tr} P{\kern 1pt} '{\kern 1pt} Y\{ \mathcal{A},\,\,e\} = \operatorname{tr} PY{\kern 1pt} '\{ \mathcal{A},\,\,e\} ,$$
so
$$\frac{1}{2}\left( {\nabla _{{kk}}^{2}f(k)e,\,\,e} \right) = \rho (e,\,\,e) + ([\operatorname{tr} (PY{\kern 1pt} '\; + P{\kern 1pt} '{\kern 1pt} Y)\mathcal{A}],\,\,e) = \rho (e,\,\,e) + 2\operatorname{tr} P{\kern 1pt} '{\kern 1pt} Y\{ \mathcal{A},\,\,e\} .$$
The proof of Lemma 3 is complete.
Proof of Lemma 4. Consider a sequence of stabilizing controllers {kj} ∈ \(\mathcal{S}\) such that kj → k ∈ \(\partial \mathcal{S}\), i.e., σ(\({{\mathcal{A}}_{0}}\) + {\(\mathcal{A}\), k}) = 0. In other words, for any ε > 0 there exists a number N = N(ε) such that
$$\left| {\sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} ) - \sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,k\} )} \right| = \sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} ) < \epsilon $$
for all j \( \geqslant \) N(\(\epsilon \)).
Let Pj be the solution of the Lyapunov equation (10) associated with the controller kj:
$$\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right){{P}_{j}} + {{P}_{j}}{{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right)}^{{\text{T}}}} + \frac{1}{{{{\alpha }_{j}}}}\left[ {\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}}^{{\text{T}}}} + {{\varepsilon }_{2}}I} \right] = 0.$$
Also, let Yj be the solution of the dual Lyapunov equation
$${{\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right)}^{{\text{T}}}}{{Y}_{j}} + {{Y}_{j}}\left( {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right) + {{\left( {C\;0} \right)}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I = 0.$$
Using Lemma A.3, we have
$$f({{k}_{j}}) = \operatorname{tr} {{P}_{j}}\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right) + \rho {{\left| {{{k}_{j}}} \right|}^{2}}\; \geqslant \;\operatorname{tr} {{P}_{j}}\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right)$$
$$ = \operatorname{tr} {{Y}_{j}}\frac{1}{{{{\alpha }_{j}}}}\left[ {\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}}^{{\text{T}}}} + {{\varepsilon }_{2}}I} \right]\; \geqslant \;\frac{1}{{{{\alpha }_{j}}}}{{\lambda }_{{\min }}}({{Y}_{j}})\operatorname{tr} \left[ {\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}}^{{\text{T}}}} + {{\varepsilon }_{2}}I} \right]$$
$$ \geqslant \;\frac{1}{{{{\alpha }_{j}}}}{{\lambda }_{{\min }}}({{Y}_{j}})\left\| {{\kern 1pt} \left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){\kern 1pt} } \right\|_{F}^{2}\; \geqslant \;\frac{1}{{{{\alpha }_{j}}}}\frac{{{{\lambda }_{{\min }}}\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right)}}{{2\left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right\|}}\left\| D \right\|_{F}^{2}$$
$$ \geqslant \;\frac{{{{\varepsilon }_{1}}}}{{4\sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},{{k}_{j}}\} )\left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right\|}}\left\| D \right\|_{F}^{2}$$
$$ \geqslant \;\frac{{{{\varepsilon }_{1}}}}{{4\epsilon \left( {\left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},{{k}_{j}}\} } \right\| + \epsilon } \right)}}\left\| D \right\|_{F}^{2}\xrightarrow[{\epsilon \to 0}]{} + \infty $$
since
$$0 < {{\alpha }_{j}} < 2\sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},{{k}_{j}}\} )$$
and
$$\left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} + \frac{{{{\alpha }_{j}}}}{2}I} \right\|\;\leqslant \;\left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} {\kern 1pt} } \right\| + \frac{{{{\alpha }_{j}}}}{2} < \left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} {\kern 1pt} } \right\| + \sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},\,\,{{k}_{j}}\} ).$$
On the other hand,
$$f({{k}_{j}}) = \operatorname{tr} {{P}_{j}}\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right) + \rho {{\left| {{{k}_{j}}} \right|}^{2}}\; \geqslant \;\rho {{\left| {{{k}_{j}}} \right|}^{2}}\xrightarrow[{\left| {{{k}_{j}}} \right| \to + \infty }]{} + \infty .$$
The proof of Lemma 4 is complete.
Proof of Corollary 2. The function f(k) has a minimum point on the set \({{\mathcal{S}}_{0}}\) (as a continuous function on a compact set), but the set \({{\mathcal{S}}_{0}}\) shares no points with the boundary \(\mathcal{S}\) due to (18). Finally, the function f(k) is differentiable on \({{\mathcal{S}}_{0}}\) by Lemma 2, which concludes the proof of Corollary 2.
Proof of Lemma 5. Applying Lemma A.2 to (15) gives
$$\frac{1}{2}\left\| {\nabla _{{kk}}^{2}f(k)} \right\| = \frac{1}{2}\mathop {\sup }\limits_{\left| e \right| = 1} \left| {\left( {\nabla _{{kk}}^{2}f(k)e,e} \right)} \right|\;\leqslant \;\mathop {\sup }\limits_{\left| e \right| = 1} \rho (e,e) + 2\mathop {\sup }\limits_{\left| e \right| = 1} \left| {\operatorname{tr} P{\kern 1pt} '{\kern 1pt} Y\{ \mathcal{A},e\} } \right|$$
$$ = \rho + 2\mathop {\sup }\limits_{\left| e \right| = 1} {{\left\| {P{\kern 1pt} '{\kern 1pt} } \right\|}_{F}}{{\left\| {Y\{ \mathcal{A},e\} } \right\|}_{F}}\;\leqslant \;\rho + 2{{\left\| {P{\kern 1pt} '{\kern 1pt} } \right\|}_{F}}\mathop {\sup }\limits_{\left| e \right| = 1} \left\| Y \right\|{{\left\| {\{ \mathcal{A},e\} } \right\|}_{F}}$$
$$\leqslant \;\rho + 2\sqrt 2 {{\left\| {P{\kern 1pt} '{\kern 1pt} } \right\|}_{F}}\left\| Y \right\|\mathop {\max }\limits_i {{\left\| {{{\mathcal{A}}_{i}}} \right\|}_{F}}$$
since
$${{\left\| {\{ \mathcal{A},\,\,e\} } \right\|}_{F}} = {{\left\| {\sum\limits_i {{{\mathcal{A}}_{i}}{{e}_{i}}} } \right\|}_{F}}\;\leqslant \;\sum\limits_i {{{{\left\| {{{\mathcal{A}}_{i}}} \right\|}}_{F}}\left| {{{e}_{i}}} \right|} \;\leqslant \;\mathop {\max }\limits_i {{\left\| {{{\mathcal{A}}_{i}}} \right\|}_{F}}{{\left| e \right|}_{1}}\;\leqslant \;\sqrt 2 \mathop {\max }\limits_i {{\left\| {{{\mathcal{A}}_{i}}} \right\|}_{F}}\left| e \right|.$$
Thus, it is necessary to estimate from above the value
$$\rho + 2\sqrt 2 \mathop {\max }\limits_i {{\left\| {{{\mathcal{A}}_{i}}} \right\|}_{F}}{{\left\| {P{\kern 1pt} '{\kern 1pt} } \right\|}_{F}}\left\| Y \right\|.$$
For ||Y || we have the upper bound
$$\begin{gathered} \frac{{{{\varepsilon }_{2}}}}{\alpha }\left\| Y \right\|\;\leqslant \;\frac{1}{\alpha }{{\lambda }_{{\min }}}\left[ {\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}}^{{\text{T}}}} + {{\varepsilon }_{2}}I} \right]\operatorname{tr} Y\;\leqslant \;\operatorname{tr} Y\frac{1}{\alpha }\left[ {\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}}^{{\text{T}}}} + {{\varepsilon }_{2}}I} \right] \\ = \operatorname{tr} P\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right) = f(k) - \rho {{\left| k \right|}^{2}}\;\leqslant \;f(k)\;\leqslant \;f({{k}_{0}}) \\ \end{gathered} $$
and consequently,
$$\left\| Y \right\|\;\leqslant \;\frac{\alpha }{{{{\varepsilon }_{2}}}}f({{k}_{0}}).$$
(B.3)
An upper bound for α is established as follows:
$$\alpha < 2\sigma ({{\mathcal{A}}_{0}} + \{ \mathcal{A},k\} )\;\leqslant \;2\left\| {{{\mathcal{A}}_{0}} + \{ \mathcal{A},k\} } \right\|$$
$$\leqslant \;2\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \sum\limits_i {\left\| {{{\mathcal{A}}_{i}}} \right\|\left| {{{k}_{i}}} \right|} } \right)\;\leqslant \;2\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|{{{\left| k \right|}}_{1}}} \right)$$
$$\leqslant \;2\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|\sqrt 2 \left| k \right|} \right)\;\leqslant \;2\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|\sqrt {\frac{2}{\rho }f(k)} } \right)$$
$$\leqslant \;2\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|\sqrt {\frac{2}{\rho }f({{k}_{0}})} } \right),$$
so
$$\left\| Y \right\|\;\leqslant \;\frac{2}{{{{\varepsilon }_{2}}}}\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|\sqrt {\frac{2}{\rho }f({{k}_{0}})} } \right)f({{k}_{0}}).$$
Now, let us estimate ||P || from above:
$$\begin{gathered} {{\varepsilon }_{1}}\left\| P \right\|\;\leqslant \;{{\lambda }_{{\min }}}\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right)\left\| P \right\| \hfill \\ \leqslant \;\operatorname{tr} P\left( {{{{\left( {C\;0} \right)}}^{{\text{T}}}}\left( {C\;0} \right) + {{\varepsilon }_{1}}I} \right) = f(k) - \rho {{\left| k \right|}^{2}}\;\leqslant \;f(k)\;\leqslant \;f({{k}_{0}}), \hfill \\ \end{gathered} $$
which yields
$$\left\| P \right\|\;\leqslant \;\frac{{f({{k}_{0}})}}{{{{\varepsilon }_{1}}}}.$$
It remains to estimate from above the value ||P ' ||F. In view of Lemma A.2,
$${{\lambda }_{{\max }}}\left( {\{ \mathcal{A},\,\,e\} P + P{{{\{ \mathcal{A},\,\,e\} }}^{{\text{T}}}}} \right) = \left\| {\{ \mathcal{A},\,\,e\} P + P{{{\{ \mathcal{A},\,\,e\} }}^{{\text{T}}}}} \right\|\;\leqslant \;\left\| {{{P}^{2}} + \{ \mathcal{A},\,\,e\} {{{\{ \mathcal{A},\,\,e\} }}^{{\text{T}}}}} \right\|$$
$$\leqslant \;{{\left\| P \right\|}^{2}} + {{\left\| {\{ \mathcal{A},\,\,e\} } \right\|}^{2}}\;\leqslant \;\frac{{{{f}^{2}}({{k}_{0}})}}{{\varepsilon _{1}^{2}}} + 2\mathop {\max }\limits_i {{\left\| {{{\mathcal{A}}_{i}}} \right\|}^{2}}\;\leqslant \;\xi \frac{{{{\varepsilon }_{2}}}}{\alpha }\;\leqslant \;\xi \frac{1}{\alpha }{{\lambda }_{{\min }}}\left[ {\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right){{{\left( \begin{gathered} D \\ 0 \\ \end{gathered} \right)}}^{{\text{T}}}} + {{\varepsilon }_{2}}I} \right]$$
for
$$\xi = \frac{\alpha }{{{{\varepsilon }_{2}}}}\left( {\frac{{{{f}^{2}}({{k}_{0}})}}{{\varepsilon _{1}^{2}}} + 2\mathop {\max }\limits_i {{{\left\| {{{\mathcal{A}}_{i}}} \right\|}}^{2}}} \right).$$
Therefore, the solution P ' of the Lyapunov equation (16) satisfies the inequality
$$\begin{gathered} P' \preccurlyeq \xi P \preccurlyeq \frac{\alpha }{{{{\varepsilon }_{2}}}}\left( {\frac{{{{f}^{2}}({{k}_{0}})}}{{\varepsilon _{1}^{2}}} + 2\mathop {\max }\limits_i {{{\left\| {{{\mathcal{A}}_{i}}} \right\|}}^{2}}} \right)\frac{{f({{k}_{0}})}}{{{{\varepsilon }_{1}}}}I \\ \preccurlyeq \frac{{2f({{k}_{0}})}}{{{{\varepsilon }_{1}}{{\varepsilon }_{2}}}}\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|\sqrt {\frac{2}{\rho }f({{k}_{0}})} } \right)\left( {\frac{{{{f}^{2}}({{k}_{0}})}}{{\varepsilon _{1}^{2}}} + 2\mathop {\max }\limits_i {{{\left\| {{{\mathcal{A}}_{i}}} \right\|}}^{2}}} \right)I. \\ \end{gathered} $$
Hence, it follows that
$${{\left\| {P{\kern 1pt} '{\kern 1pt} } \right\|}_{F}}\;\leqslant \;\frac{{2\sqrt n f({{k}_{0}})}}{{{{\varepsilon }_{1}}{{\varepsilon }_{2}}}}\left( {\left\| {{{\mathcal{A}}_{0}}} \right\| + \mathop {\max }\limits_i \left\| {{{\mathcal{A}}_{i}}} \right\|\sqrt {\frac{2}{\rho }f({{k}_{0}})} } \right)\left( {\frac{{{{f}^{2}}({{k}_{0}})}}{{\varepsilon _{1}^{2}}} + 2\mathop {\max }\limits_i {{{\left\| {{{\mathcal{A}}_{i}}} \right\|}}^{2}}} \right).$$
(B.4)
Considering the bounds (B.3) and (B.4), we arrive at the relation (19). The proof of Lemma 5 is complete.