Physlib

Physlib.Mathematics.InnerProductSpace.Adjoint

Adjoint of a linear map

This module defines the adjoint of a linear map `f : E → F` where `E` and `F` carry the instances of `InnerProductSpace'` over a field `𝕜`.

This is a generalization of the usual adjoint defined on `InnerProductSpace` for continuous linear maps.

18 declarations

definition

Adjoint of a map f:E→Ff: E \to F

For a map f:E→Ff : E \to F between two inner product spaces EE and FF over a field k\mathbb{k}, the adjoint f†:F→Ef^\dagger : F \to E is defined as the unique map satisfying the property ⟨f(x),y⟩=⟨x,f†(y)⟩\langle f(x), y \rangle = \langle x, f^\dagger(y) \rangle for all x∈Ex \in E and y∈Fy \in F. If such a map exists (i.e., if ff has an adjoint), the definition returns that map; otherwise, it returns the zero map.

theorem

⟨x,f′(y)⟩=⟨f(x),y⟩\langle x, f'(y) \rangle = \langle f(x), y \rangle for the adjoint f′f'

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. If f:E→Ff: E \to F is a map and f′:F→Ef': F \to E is its adjoint (meaning they satisfy the `HasAdjoint` property), then for any x∈Ex \in E and y∈Fy \in F, the inner product satisfies ⟨x,f′(y)⟩=⟨f(x),y⟩\langle x, f'(y) \rangle = \langle f(x), y \rangle.

theorem

Existence of an Adjoint for Continuous Linear Maps between Complete Generalized Inner Product Spaces

Let EE and FF be generalized inner product spaces over a field k\mathbb{k} (where k\mathbb{k} is R\mathbb{R} or C\mathbb{C}). Suppose EE and FF are complete with respect to their respective norms. For any continuous linear map f:E→Ff : E \to F, there exists an adjoint map f†:F→Ef^\dagger : F \to E such that ⟨f(x),y⟩=⟨x,f†(y)⟩\langle f(x), y \rangle = \langle x, f^\dagger(y) \rangle for all x∈Ex \in E and y∈Fy \in F. Specifically, this adjoint is given by the composition: f†=fromL2∘(toL2∘f∘fromL2)†∘toL2f^\dagger = \text{fromL2} \circ (\text{toL2} \circ f \circ \text{fromL2})^\dagger \circ \text{toL2} where toL2\text{toL2} and fromL2\text{fromL2} are the continuous linear identity maps between the spaces equipped with their original norms and the same spaces equipped with the L2L_2 norm ∥x∥2=Re⟨x,x⟩\|x\|_2 = \sqrt{\text{Re} \langle x, x \rangle}, and (⋅)†(\cdot)^\dagger denotes the standard Hilbert space adjoint.

theorem

f†=fromL2∘(toL2∘f∘fromL2)†∘toL2f^\dagger = \text{fromL2} \circ (\text{toL2} \circ f \circ \text{fromL2})^\dagger \circ \text{toL2}

Let EE and FF be complete generalized inner product spaces over a field k\mathbb{k} (where k\mathbb{k} is R\mathbb{R} or C\mathbb{C}). For any continuous linear map f:E→Ff : E \to F, the adjoint f†:F→Ef^\dagger : F \to E is equal to the composition of maps: f†=fromL2∘(toL2∘f∘fromL2)†∘toL2f^\dagger = \text{fromL2} \circ (\text{toL2} \circ f \circ \text{fromL2})^\dagger \circ \text{toL2} where toL2\text{toL2} and fromL2\text{fromL2} are the continuous linear identity maps between the spaces equipped with their original norms and the same spaces equipped with the L2L_2 norm ∥x∥2=Re⟨x,x⟩\|x\|_2 = \sqrt{\text{Re} \langle x, x \rangle}, and the inner (⋅)†(\cdot)^\dagger denotes the standard Hilbert space adjoint of the map between these L2L_2 spaces.

theorem

The adjoint map f′f' satisfies f′(0)=0f'(0) = 0

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. If f′:F→Ef' : F \to E is an adjoint of a map f:E→Ff : E \to F (meaning they satisfy the adjoint relation with respect to the inner products on EE and FF), then the image of the zero vector under f′f' is zero, i.e., f′(0)=0f'(0) = 0.

theorem

If f′f' is an adjoint of ff, then f†=f′f^\dagger = f'

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. If a map f:E→Ff: E \to F has an adjoint f′:F→Ef': F \to E (meaning ⟨f(x),y⟩=⟨x,f′(y)⟩\langle f(x), y \rangle = \langle x, f'(y) \rangle for all x∈Ex \in E and y∈Fy \in F), then the adjoint operator applied to ff, denoted f†f^\dagger, is equal to f′f'.

theorem

If g′=f′g' = f' and g′g' is an adjoint of ff, then f′f' is also an adjoint of ff

Let EE and FF be inner product spaces over a field k\mathbb{k}. Let f:E→Ff : E \to F be a linear map. If g′:F→Eg' : F \to E is an adjoint of ff and g′=f′g' = f', then f′f' is also an adjoint of ff.

theorem

The identity map is its own adjoint

Let EE be a generalized inner product space over a field k\mathbb{k}. The identity map idE:E→E\text{id}_E : E \to E is its own adjoint. That is, the identity function has an adjoint, and that adjoint is also the identity function.

theorem

The adjoint of the zero map is the zero map

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. The zero map f:E→Ff : E \to F, defined by f(x)=0f(x) = 0 for all x∈Ex \in E, has an adjoint g:F→Eg : F \to E which is also the zero map, defined by g(y)=0g(y) = 0 for all y∈Fy \in F.

theorem

The adjoint of f∘gf \circ g is g′∘f′g' \circ f'

Let E,FE, F, and GG be generalized inner product spaces over a field k\mathbb{k}. If a map f:F→Gf: F \to G has an adjoint f′:G→Ff': G \to F and a map g:E→Fg: E \to F has an adjoint g′:F→Eg': F \to E, then the composition f∘gf \circ g has an adjoint given by the composition of the adjoints in reverse order, g′∘f′g' \circ f'.

theorem

The adjoint of x↦(f(x),g(x))x \mapsto (f(x), g(x)) is (y,z)↦f′(y)+g′(z)(y, z) \mapsto f'(y) + g'(z)

Let E,FE, F, and GG be generalized inner product spaces over a field k\mathbb{k}. If a map f:E→Ff: E \to F has an adjoint f′:F→Ef': F \to E and a map g:E→Gg: E \to G has an adjoint g′:G→Eg': G \to E, then the map E→F×GE \to F \times G defined by x↦(f(x),g(x))x \mapsto (f(x), g(x)) has an adjoint F×G→EF \times G \to E defined by (y,z)↦f′(y)+g′(z)(y, z) \mapsto f'(y) + g'(z). Here, the product space F×GF \times G is equipped with the standard product inner product ⟨(y1,z1),(y2,z2)⟩=⟨y1,y2⟩F+⟨z1,z2⟩G\langle (y_1, z_1), (y_2, z_2) \rangle = \langle y_1, y_2 \rangle_F + \langle z_1, z_2 \rangle_G.

theorem

The adjoint of x↦(f(x))1x \mapsto (f(x))_1 is y↦f′(y,0)y \mapsto f'(y, 0)

Let E,FE, F, and GG be generalized inner product spaces over a field k\mathbb{k}. If a map f:E→F×Gf: E \to F \times G has an adjoint f′:F×G→Ef': F \times G \to E, then the map from EE to FF defined by taking the first component of ff, x↦(f(x))1x \mapsto (f(x))_1, has an adjoint given by y↦f′(y,0)y \mapsto f'(y, 0).

theorem

The adjoint of x↦(f(x))2x \mapsto (f(x))_2 is z↦f′(0,z)z \mapsto f'(0, z)

Let E,F,E, F, and GG be generalized inner product spaces over a field k\mathbb{k}. If a map f:E→F×Gf: E \to F \times G has an adjoint f′:F×G→Ef': F \times G \to E, then the map x↦(f(x))2x \mapsto (f(x))_2 (the projection of ff onto the second component) has an adjoint given by z↦f′(0,z)z \mapsto f'(0, z).

theorem

The adjoint of −f-f is −f′-f'

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. If f:E→Ff: E \to F is a map that has an adjoint f′:F→Ef': F \to E, then the map defined by x↦−f(x)x \mapsto -f(x) has an adjoint defined by y↦−f′(y)y \mapsto -f'(y).

theorem

f+gf + g has adjoint f′+g′f' + g'

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. If f,g:E→Ff, g: E \to F are maps that have adjoints f′,g′:F→Ef', g': F \to E respectively, then the map f+gf + g (defined by x↦f(x)+g(x)x \mapsto f(x) + g(x)) has an adjoint given by f′+g′f' + g' (defined by y↦f′(y)+g′(y)y \mapsto f'(y) + g'(y)).

theorem

Adjoint of f−gf - g is f′−g′f' - g'

Let EE and FF be generalized inner product spaces over a field k\mathbb{k}. If the maps f,g:E→Ff, g: E \to F have adjoints f′,g′:F→Ef', g': F \to E respectively, then the map f−gf - g (defined by x↦f(x)−g(x)x \mapsto f(x) - g(x)) has an adjoint f′−g′f' - g' (defined by y↦f′(y)−g′(y)y \mapsto f'(y) - g'(y)).

theorem

The adjoint of c⋅fc \cdot f is cˉ⋅f′\bar{c} \cdot f'

Let EE and FF be generalized inner product spaces over a field k\mathbb{k} (where k\mathbb{k} is R\mathbb{R} or C\mathbb{C}). If a map f:E→Ff: E \to F has an adjoint f′:F→Ef': F \to E, then for any scalar c∈kc \in \mathbb{k}, the map x↦c⋅f(x)x \mapsto c \cdot f(x) has an adjoint given by y↦cˉ⋅f′(y)y \mapsto \bar{c} \cdot f'(y), where cˉ\bar{c} denotes the complex conjugate of cc.

theorem

Adjoint of x↦f(x)vx \mapsto f(x)v is y↦f′(⟨y,v⟩‾)y \mapsto f'(\overline{\langle y, v \rangle})

Let EE and FF be generalized inner product spaces over a field k\mathbb{k} (typically R\mathbb{R} or C\mathbb{C}). Let f:E→kf: E \to \mathbb{k} be a linear map and f′:k→Ef': \mathbb{k} \to E be its adjoint, such that ⟨f(x),s⟩k=⟨x,f′(s)⟩E\langle f(x), s \rangle_{\mathbb{k}} = \langle x, f'(s) \rangle_E for all x∈Ex \in E and s∈ks \in \mathbb{k}. For any vector v∈Fv \in F, the map g:E→Fg: E \to F defined by g(x)=f(x)vg(x) = f(x)v has an adjoint g′:F→Eg': F \to E given by g′(y)=f′(⟨y,v⟩‾)g'(y) = f'(\overline{\langle y, v \rangle}), where ⟨y,v⟩‾\overline{\langle y, v \rangle} denotes the complex conjugate of the inner product in FF.