TheoremBase

Monotonicity of the oriented integral reduces to that of the Riemann integral of the restrictions; the matrix clauses test the integral against quadratic forms, which pass inside the integral by the factor rule, and symmetry follows from the transpose rule.

Proof

Real numbers are computed with as in The Real Numbers as a Type.

Proof of (i). If u=vu=v, then ∫uvf=0=∫uvg\int_{u}^{v}f=0=\int_{u}^{v}g by The Riemann Integral on a Closed Interval via Lower and Upper Integrals (vii). Let u<vu<v. By The Riemann Integral on a Closed Interval via Lower and Upper Integrals (viii) and The Riemann Integral on a Closed Interval via Lower and Upper Integrals (vi), [u,v]⊆E[u,v]\subseteq E, the restrictions f∣[u,v]f|_{[u,v]} and g∣[u,v]g|_{[u,v]} are bounded and integrable on [u,v][u,v], and ∫uvf=∫uvf∣[u,v]\int_{u}^{v}f=\int_{u}^{v}f|_{[u,v]} and ∫uvg=∫uvg∣[u,v]\int_{u}^{v}g=\int_{u}^{v}g|_{[u,v]}. For r∈[u,v]r\in[u,v], f∣[u,v](r)=f(r)≤g(r)=g∣[u,v](r)f|_{[u,v]}(r)=f(r)\le g(r)=g|_{[u,v]}(r), by Domains and Restrictions of Maps (iii). So Rules for the Riemann Integral: Sums, Scalar Multiples, Monotonicity, Bounds and Constants (iii), with uu, vv for aa, bb and f∣[u,v]f|_{[u,v]}, g∣[u,v]g|_{[u,v]} for ff, gg, gives ∫uvf≤∫uvg\int_{u}^{v}f\le\int_{u}^{v}g.

Quadratic forms of the integral. Let aa, bb, uu, vv, MM and NN be as in the statement. By Basic Facts about Intervals of the Real Line (v), [a,b][a,b] is an interval containing two distinct points; it is the interval II of Rules for the Riemann Integral of Vector- and Matrix-Valued Maps, with nn for pp and qq. By Rules for the Riemann Integral of Vector- and Matrix-Valued Maps (i), ∫uvM\int_{u}^{v}M and ∫uvN\int_{u}^{v}N are defined. Let ξ∈Rn\xi\in\mathbb{R}^{n}, and let fξ,gξ:[a,b]→Rf_{\xi},g_{\xi}:[a,b]\to\mathbb{R} be the maps r↦ξ⋅(M(r)ξ)r\mapsto\xi\cdot(M(r)\xi) and r↦ξ⋅(N(r)ξ)r\mapsto\xi\cdot(N(r)\xi) (Values, Restriction and Equality of a Map, and the Map u↦t(u)u\mapsto t(u) as a Defined Set Symbol (v)). By Rules for the Riemann Integral of Vector- and Matrix-Valued Maps (vi), first with ξ\xi for zz and MM for AA, the integral from uu to vv of r↦M(r)ξr\mapsto M(r)\xi is defined and equals (∫uvM)ξ\bigl(\int_{u}^{v}M\bigr)\xi; then, with ξ\xi for zz and r↦M(r)ξr\mapsto M(r)\xi for xx, the integral of fξf_{\xi} from uu to vv is defined and

∫uvfξ=ξ⋅∫uvM(r)ξ dr=ξ⋅((∫uvM)ξ).(1)\int_{u}^{v}f_{\xi}=\xi\cdot\int_{u}^{v}M(r)\xi\,dr=\xi\cdot\Bigl(\Bigl(\int_{u}^{v}M\Bigr)\xi\Bigr).\tag{1}

Likewise ∫uvgξ\int_{u}^{v}g_{\xi} is defined and equals ξ⋅((∫uvN)ξ)\xi\cdot\bigl(\bigl(\int_{u}^{v}N\bigr)\xi\bigr).

Proof of (ii). ∫uvM\int_{u}^{v}M is defined, as shown above. By Rules for the Riemann Integral of Vector- and Matrix-Valued Maps (vii), the integral from uu to vv of r↦M(r)⊤r\mapsto M(r)^{\top} is defined and equals (∫uvM)⊤\bigl(\int_{u}^{v}M\bigr)^{\top}. Since M(r)∈S(n)M(r)\in\mathcal{S}(n), M(r)⊤=M(r)M(r)^{\top}=M(r) for every r∈[a,b]r\in[a,b], by Euclidean Space and Real Matrices: Standing Notation (iv), so the map r↦M(r)⊤r\mapsto M(r)^{\top} is MM (Values, Restriction and Equality of a Map, and the Map u↦t(u)u\mapsto t(u) as a Defined Set Symbol (iv)). Hence (∫uvM)⊤=∫uvM\bigl(\int_{u}^{v}M\bigr)^{\top}=\int_{u}^{v}M, and ∫uvM\int_{u}^{v}M, a matrix in Mn(R)\mathcal{M}_{n}(\mathbb{R}) by Riemann Integral of a Vector-Valued or Matrix-Valued Map (iv), lies in S(n)\mathcal{S}(n) by Euclidean Space and Real Matrices: Standing Notation (iv).

Proof of (iii). Let ξ∈Rn\xi\in\mathbb{R}^{n}. For r∈[a,b]r\in[a,b] with u≤r≤vu\le r\le v, fξ(r)=ξ⋅(M(r)ξ)≥0f_{\xi}(r)=\xi\cdot(M(r)\xi)\ge0, by Positive Semidefinite and Positive Definite Real Matrices (i). By Rules for Oriented Riemann Integrals of Real-Valued Maps: Sums, Scalar Multiples, Constants, Continuous Maps, Additivity and Evaluation by an Antiderivative (iii), with [a,b][a,b] for EE and 00 for cc (if u<vu<v, then [u,v]⊆[a,b][u,v]\subseteq[a,b] by Basic Facts about Intervals of the Real Line (ii)), the integral from uu to vv of the constant map [a,b]→R[a,b]\to\mathbb{R} with value 00 is defined and equals (v−u)⋅0=0(v-u)\cdot0=0. So (i), with [a,b][a,b] for EE, this constant map for ff and fξf_{\xi} for gg, together with (1), gives 0≤∫uvfξ=ξ⋅((∫uvM)ξ)0\le\int_{u}^{v}f_{\xi}=\xi\cdot\bigl(\bigl(\int_{u}^{v}M\bigr)\xi\bigr). As ξ\xi was arbitrary and ∫uvM∈S(n)\int_{u}^{v}M\in\mathcal{S}(n) by (ii), ∫uvM\int_{u}^{v}M is positive semidefinite, by Positive Semidefinite and Positive Definite Real Matrices (i).

Proof of (iv). By (ii), applied to MM and to NN, ∫uvM\int_{u}^{v}M and ∫uvN\int_{u}^{v}N lie in S(n)\mathcal{S}(n). Let ξ∈Rn\xi\in\mathbb{R}^{n}. For r∈[a,b]r\in[a,b] with u≤r≤vu\le r\le v, M(r)⪯N(r)M(r)\preceq N(r) gives fξ(r)=ξ⋅(M(r)ξ)≤ξ⋅(N(r)ξ)=gξ(r)f_{\xi}(r)=\xi\cdot(M(r)\xi)\le\xi\cdot(N(r)\xi)=g_{\xi}(r), by The Positive Semidefinite Ordering on Symmetric Matrices (i). By (i), with [a,b][a,b] for EE and fξf_{\xi}, gξg_{\xi} for ff, gg, and by (1) and its analogue for NN,

ξ⋅((∫uvM)ξ)=∫uvfξ≤∫uvgξ=ξ⋅((∫uvN)ξ).\xi\cdot\Bigl(\Bigl(\int_{u}^{v}M\Bigr)\xi\Bigr)=\int_{u}^{v}f_{\xi}\le\int_{u}^{v}g_{\xi}=\xi\cdot\Bigl(\Bigl(\int_{u}^{v}N\Bigr)\xi\Bigr).

As ξ\xi was arbitrary, ∫uvM⪯∫uvN\int_{u}^{v}M\preceq\int_{u}^{v}N, by The Positive Semidefinite Ordering on Symmetric Matrices (i).

Citations

Loading…

Dependencies

Uses0

Loading…

Comments

Log in to comment.

Loading…