Kreyszig 2.6 Linear Operators

Problem 1. Show that the operators in sections 2.6-2, 2.6-3, and 2.6-4 are linear.

Solution:

To show that the operators in sections 2.6-2, 2.6-3, and 2.6-4 are linear, we need to verify that each operator satisfies the two linearity conditions for all vectors x,yx, y in the domain and all scalars a,ba, b in the field over which the vector space is defined:

  1. T(x+y)=T(x)+T(y)T(x + y) = T(x) + T(y) (additivity)

  2. T(ax)=aT(x)T(ax) = aT(x) (homogeneity)

Let's consider each operator in turn:

2.6-2 Identity Operator IxI_x: The identity operator IxI_x on a vector space XX is defined by Ix(x)=xI_x(x) = x for all xXx \in X.

  • For additivity, consider two vectors x,yXx, y \in X. We need to show that Ix(x+y)=Ix(x)+Ix(y)I_x(x + y) = I_x(x) + I_x(y). Indeed, Ix(x+y)=x+y=Ix(x)+Ix(y)I_x(x + y) = x + y = I_x(x) + I_x(y).

  • For homogeneity, consider a scalar aa and a vector xXx \in X. We need to show that Ix(ax)=aIx(x)I_x(ax) = aI_x(x). Indeed, Ix(ax)=ax=aIx(x)I_x(ax) = ax = aI_x(x).

2.6-3 Zero Operator 0x0_x: The zero operator 0x0_x on a vector space XX to another vector space YY is defined by 0x(x)=00_x(x) = 0 for all xXx \in X, where 00 is the zero vector in YY.

  • For additivity, consider two vectors x,yXx, y \in X. We have 0x(x+y)=0=0+0=0x(x)+0x(y)0_x(x + y) = 0 = 0 + 0 = 0_x(x) + 0_x(y).

  • For homogeneity, for any scalar aa and vector xinXx in X, 0x(ax)=0=a0=a0x(x)0_x(ax) = 0 = a \cdot 0 = a0_x(x).

2.6-4 Differentiation Operator DD: Let XX be the vector space of all polynomials on [a,b][a, b]. The differentiation operator DD is defined by D(T(x))=T(x)D(T(x)) = T'(x), where TT' denotes differentiation with respect to xx.

  • For additivity, let x(t)x(t) and y(t)y(t) be polynomials in XX. Then D(x(t)+y(t))=(x+y)(t)=x(t)+y((t)=D(x(t))+D(y(t))D(x(t) + y(t)) = (x + y)'(t) = x'(t) + y'((t) = D(x(t)) + D(y(t)).

  • For homogeneity, let aa be a scalar and x(t)x(t) be a polynomial in XX. Then D(ax(t))=(ax)(t)=ax(t)=aD(x(t))D(a \cdot x(t)) = (a \cdot x)'(t) = a \cdot x'(t) = a \cdot D(x(t)).

In all cases, the operators satisfy the linearity conditions, hence they are indeed linear operators.

\blacksquare


Problem 2. Show that the operators T1,T2,T3T_1, T_2, T_3, and T4T_4 from R2\mathbb{R}^2 into R2\mathbb{R}^2 defined by

  • T1(ξ1,ξ2)=(ξ1,0)T_1(\xi_1, \xi_2) = (\xi_1, 0)

  • T2(ξ1,ξ2)=(0,ξ2)T_2(\xi_1, \xi_2) = (0, \xi_2)

  • T3(ξ1,ξ2)=(ξ2,ξ1)T_3(\xi_1, \xi_2) = (\xi_2, \xi_1)

  • T4(ξ1,ξ2)=(γξ1,γξ2)T_4(\xi_1, \xi_2) = (\gamma\xi_1, \gamma\xi_2)

respectively, are linear, and interpret these operators geometrically.

Solution: To demonstrate the linearity of operators T1,T2,T3T_1, T_2, T_3, and T4T_4, we must verify that each operator satisfies the following properties for all vectors ξ,ηR2\xi, \eta \in \mathbb{R}^2 and all scalars aRa \in \mathbb{R}:

  1. Additivity: T(ξ+η)=T(ξ)+T(η)T(\xi + \eta) = T(\xi) + T(\eta)

  2. Homogeneity: T(aξ)=aT(ξ)T(a\xi) = aT(\xi)

For T1T_1:

  • Additivity: T1((ξ1+η1,ξ2+η2))=(ξ1+η1,0)=(ξ1,0)+(η1,0)=T1(ξ1,ξ2)+T1(η1,η2)T_1((\xi_1 + \eta_1, \xi_2 + \eta_2)) = (\xi_1 + \eta_1, 0) = (\xi_1, 0) + (\eta_1, 0) = T_1(\xi_1, \xi_2) + T_1(\eta_1, \eta_2)

  • Homogeneity: T1(a(ξ1,ξ2))=(aξ1,0)=a(ξ1,0)=aT1(ξ1,ξ2)T_1(a(\xi_1, \xi_2)) = (a\xi_1, 0) = a(\xi_1, 0) = aT_1(\xi_1, \xi_2)

For T2T_2, additivity and homogeneity can be shown similarly, with T2T_2 projecting any vector onto the y-axis.

For T3T_3:

  • Additivity: T3((ξ1+η1,ξ2+η2))=(ξ2+η2,ξ1+η1)=(ξ2,ξ1)+(η2,η1)=T3(ξ1,ξ2)+T3(η1,η2)T_3((\xi_1 + \eta_1, \xi_2 + \eta_2)) = (\xi_2 + \eta_2, \xi_1 + \eta_1) = (\xi_2, \xi_1) + (\eta_2, \eta_1) = T_3(\xi_1, \xi_2) + T_3(\eta_1, \eta_2)

  • Homogeneity: T3(a(ξ1,ξ2))=(aξ2,aξ1)=a(ξ2,ξ1)=aT3(ξ1,ξ2)T_3(a(\xi_1, \xi_2)) = (a\xi_2, a\xi_1) = a(\xi_2, \xi_1) = aT_3(\xi_1, \xi_2)

For T4T_4:

  • Additivity: T4((ξ1+η1,ξ2+η2))=(γ(ξ1+η1),γ(ξ2+η2))=(γξ1,γξ2)+(γη1,γη2)=T4(ξ1,ξ2)+T4(η1,η2)T_4((\xi_1 + \eta_1, \xi_2 + \eta_2)) = (\gamma(\xi_1 + \eta_1), \gamma(\xi_2 + \eta_2)) = (\gamma\xi_1, \gamma\xi_2) + (\gamma\eta_1, \gamma\eta_2) = T_4(\xi_1, \xi_2) + T_4(\eta_1, \eta_2)

  • Homogeneity: T4(a(ξ1,ξ2))=(aγξ1,aγξ2)=a(γξ1,γξ2)=aT4(ξ1,ξ2)T_4(a(\xi_1, \xi_2)) = (a\gamma\xi_1, a\gamma\xi_2) = a(\gamma\xi_1, \gamma\xi_2) = aT_4(\xi_1, \xi_2)

Geometric Interpretation:

  • T1T_1 and T2T_2 are projection operators onto the x-axis and y-axis respectively.

  • T3T_3 is a reflection operator across the line ξ1=ξ2\xi_1 = \xi_2.

\blacksquare


Problem 3. What are the domain, range, and null space of T1,T2,T3T_1, T_2, T_3 in Problem 2?

Solution:

To determine the domain, range, and null space of the linear operators T1,T2,T_1, T_2, and T3T_3, we consider their definitions from Problem 2.

For Operator T1T_1: T1(ξ1,ξ2)=(ξ1,0)T_1(\xi_1, \xi_2) = (\xi_1, 0)

  • Domain: The domain of T1T_1 is the entire R2\mathbb{R}^2.

  • Range: The range of T1T_1 is the x-axis, given by {(ξ1,0)ξ1R}\{(\xi_1, 0) \mid \xi_1 \in \mathbb{R}\}.

  • Null Space: The null space of T1T_1 is the set of all vectors that map to the zero vector under T1T_1, which is {(0,ξ2)ξ2R}\{(0, \xi_2) \mid \xi_2 \in \mathbb{R}\}.

For Operator T2T_2: T2(ξ1,ξ2)=(0,ξ2)T_2(\xi_1, \xi_2) = (0, \xi_2)

  • Domain: The domain of T2T_2 is the entire R2\mathbb{R}^2.

  • Range: The range of T2T_2 is the y-axis, described by {(0,ξ2)ξ2R}\{(0, \xi_2) \mid \xi_2 \in \mathbb{R}\}.

  • Null Space: The null space of T2T_2 includes all vectors that T2T_2 maps to the zero vector, which is {(ξ1,0)ξ1R}\{(\xi_1, 0) \mid \xi_1 \in \mathbb{R}\}.

For Operator T3T_3: T3(ξ1,ξ2)=(ξ2,ξ1)T_3(\xi_1, \xi_2) = (\xi_2, \xi_1)

  • Domain: The domain of T3T_3 is the entire R2\mathbb{R}^2.

  • Range: The range of T3T_3 is also R2\mathbb{R}^2 since any vector in R2\mathbb{R}^2 can be obtained by applying T3T_3 to some vector in R2\mathbb{R}^2.

  • Null Space: The null space of T3T_3 is the set of vectors that are mapped to the zero vector, which is only the zero vector itself {(0,0)}\{(0, 0)\}.

These operators' geometric interpretations relate to their ranges and null spaces, with T1T_1 and T2T_2 acting as projection operators onto the x-axis and y-axis, respectively, and T3T_3 mapping vectors onto the line ξ1=ξ2\xi_1 = \xi_2.

\blacksquare


Problem 4. What is the null space of T4T_4 in Problem 2? Of T1T_1 and T2T_2 in 2.6-7? Of TT in 2.6-4?

Solution:

Given the definitions of the operators T4T_4, T1T_1, and T2T_2 from the provided images, we can find their null spaces.

For Operator T4T_4 from 2.6-4 (Differentiation):

  • Definition: T4T_4 is defined on the vector space XX of all polynomials on [a,b][a, b] by T4(x(t))=x(t)T_4(x(t)) = x'(t), where the prime denotes differentiation with respect to tt.

  • Null Space: The null space of the differentiation operator consists of all polynomials x(t)x(t) such that x(t)=0x'(t) = 0. Thus, the null space of T4T_4 is the set of all constant polynomials on [a,b][a, b].

For Operator T1T_1 from 2.6-7 (Cross product with a fixed vector):

  • Definition: T1T_1 is defined on R3\mathbb{R}^3 by T1(x)=x×aT_1(\vec{x}) = \vec{x} \times \vec{a}, where a\vec{a} is a fixed vector in R3\mathbb{R}^3.

  • Null Space: The null space of T1T_1 includes all vectors x\vec{x} such that x×a=0\vec{x} \times \vec{a} = \vec{0}, which are the scalar multiples of a\vec{a} including the zero vector.

For Operator T2T_2 from 2.6-7 (Dot product with a fixed vector):

  • Definition: T2T_2 is defined on R3\mathbb{R}^3 by T2(x)=xaT_2(\vec{x}) = \vec{x} \cdot \vec{a}, where a=(ai)\vec{a} = (a_i) is a fixed vector in R3\mathbb{R}^3.

  • Null Space: The null space of T2T_2 consists of all vectors x\vec{x} that are orthogonal to a\vec{a}, which is the orthogonal complement of the vector a\vec{a} in R3\mathbb{R}^3.

The null spaces reflect the specific transformations these operators perform on their respective vector spaces.

\blacksquare


Problem 7. Determine if the operators T1T_1 and T3T_3 from Problem 2 commute.

Given:

  • T1(ξ1,ξ2)=(ξ1,0)T_1(\xi_1, \xi_2) = (\xi_1, 0)

  • T3(ξ1,ξ2)=(ξ2,ξ1)T_3(\xi_1, \xi_2) = (\xi_2, \xi_1)

Solution:

To check for commutativity, we calculate (T1T3)(ξ1,ξ2)(T_1T_3)(\xi_1, \xi_2) and (T3T1)(ξ1,ξ2)(T_3T_1)(\xi_1, \xi_2).

Applying T1T_1 followed by T3T_3:

  1. Apply T1T_1 to (ξ1,ξ2)(\xi_1, \xi_2):

    T1(ξ1,ξ2)=(ξ1,0)T_1(\xi_1, \xi_2) = (\xi_1, 0)

  2. Then apply T3T_3 to the result:

    T3(ξ1,0)=(0,ξ1)T_3(\xi_1, 0) = (0, \xi_1)

Applying T3T_3 followed by T1T_1:

  1. Apply T3T_3 to (ξ1,ξ2)(\xi_1, \xi_2):

    T3(ξ1,ξ2)=(ξ2,ξ1)T_3(\xi_1, \xi_2) = (\xi_2, \xi_1)

  2. Then apply T1T_1 to the result:

    T1(ξ2,ξ1)=(ξ2,0)T_1(\xi_2, \xi_1) = (\xi_2, 0)

Comparing Results:

  • T1T3T_1T_3 yields (0,ξ1)(0, \xi_1).

  • T3T1T_3T_1 yields (ξ2,0)(\xi_2, 0).

Since (0,ξ1)(ξ2,0)(0, \xi_1) \neq (\xi_2, 0) for arbitrary ξ1,ξ2\xi_1, \xi_2, we conclude that T1T_1 and T3T_3 do not commute.

Conclusion:

The operators T1T_1 and T3T_3 do not satisfy the commutativity property T1T3=T3T1T_1T_3 = T_3T_1 for all vectors in R2\mathbb{R}^2. Therefore, they are non-commutative.

\blacksquare


Problem 8. Represent the operators T1,T2,T3T_1, T_2, T_3, and T4T_4 from Problem 2 using 2×22 \times 2 matrices.

Given Operators:

  • T1(ξ1,ξ2)=(ξ1,0)T_1(\xi_1, \xi_2) = (\xi_1, 0)

  • T2(ξ1,ξ2)=(0,ξ2)T_2(\xi_1, \xi_2) = (0, \xi_2)

  • T3(ξ1,ξ2)=(ξ2,ξ1)T_3(\xi_1, \xi_2) = (\xi_2, \xi_1)

  • T4(ξ1,ξ2)=(γξ1,γξ2)T_4(\xi_1, \xi_2) = (\gamma\xi_1, \gamma\xi_2)

Matrix Representations:

  • For T1T_1:

    The matrix representation is: T1=[1000]T_1 = \begin{bmatrix} 1 & 0 \\ 0 & 0 \end{bmatrix}

  • For T2T_2:

    The matrix representation is: T2=[0001]T_2 = \begin{bmatrix} 0 & 0 \\ 0 & 1 \end{bmatrix}

  • For T3T_3:

    The matrix representation is: T3=[0110]T_3 = \begin{bmatrix} 0 & 1 \\ 1 & 0 \end{bmatrix}

  • For T4T_4:

    The matrix representation is: T4=[γ00γ]T_4 = \begin{bmatrix} \gamma & 0 \\ 0 & \gamma \end{bmatrix}

Conclusion:

Each operator from Problem 2 can be expressed as a 2×22 \times 2 matrix. These matrices transform vectors in R2\mathbb{R}^2 by linearly scaling and/or permuting their components as specified by the operators.

\blacksquare


Problem 9. Elaborate the condition in 2.6-10(a) regarding the existence of an inverse operator, T1T^{-1}, in the context of the null space of TT.

Theorem Interpretation: The theorem from section 2.6-10(a) can be restated in the context of the null space of TT as follows:

  • The inverse operator T1T^{-1} from R(T)\mathcal{R}(T) to D(T)\mathcal{D}(T) exists if and only if the only solution to Tx=0Tx = 0 is the trivial solution x=0x = 0. This is equivalent to saying that the null space of TT, denoted N(T)N(T) or ker(T)\text{ker}(T), consists solely of the zero vector.

Definitions:

  • Linear Operator: A mapping T:D(T)YT: \mathcal{D}(T) \rightarrow Y between vector spaces XX and YY, adhering to additivity (T(x+z)=T(x)+T(z)T(x + z) = T(x) + T(z)) and homogeneity (T(αx)=αT(x)T(\alpha x) = \alpha T(x)), for all x,zD(T)x, z \in \mathcal{D}(T) and scalars α\alpha.

  • Inverse Operator: T1:R(T)D(T)T^{-1}: \mathcal{R}(T) \rightarrow \mathcal{D}(T) is the reverse mapping such that T1(Tx)=xT^{-1}(Tx) = x for all xD(T)x \in \mathcal{D}(T) and T(T1y)=yT(T^{-1}y) = y for all yR(T)y \in \mathcal{R}(T).

  • Null Space: Denoted by N(T)N(T) or ker(T)\text{ker}(T), it is the set of vectors xD(T)x \in \mathcal{D}(T) where T(x)=0T(x) = 0.

In-Depth Analysis of Theorem 2.6-10(a):

This theorem posits that T1T^{-1} can only exist if Tx=0Tx = 0 strictly leads to x=0x = 0. Essentially, N(T)N(T) must be trivial—comprised solely of the zero vector. If N(T)N(T) included any non-zero vectors, TT could not be injective, as it would map distinct vectors to the same point (the zero vector in YY), contravening the bijective requirement for an inverse function.

Formulating the Condition for Inverse Existence:

The existence condition for T1T^{-1} relative to the null space of TT is that N(T)={0}N(T) = \{0\}. This reflects the injectivity of TT.

Examples:

  • For an Injective Operator: A matrix representation of TT as AA with no linearly dependent rows or columns ensures N(T)={0}N(T) = \{0\}, affirming the existence of T1T^{-1}.

  • For a Non-Injective Operator: Should TT be depicted by a matrix AA containing a zero row, N(T)N(T) would be non-trivial, housing non-zero vectors, thus negating the presence of T1T^{-1}.

Conclusion:

The theorem outlined in 2.6-10(a) underscores a pivotal tenet in linear algebra: the invertibility of a linear operator is inherently dependent on the exclusivity of the zero vector in its null space. An operator TT is invertible if and only if N(T)N(T) is trivial, serving as a vital criterion for TT's injectivity.

\blacksquare


Problem 10. Determine the existence of the inverse operator T1T^{-1} for the differentiation operator TT as defined in section 2.6-4.

Operator Definition:

The operator TT defined in section 2.6-4 is the differentiation operator acting on the vector space XX of all polynomials on the interval [a,b][a, b]. The action of TT is defined by T(x(t))=x(t)T(x(t)) = x'(t), where x(t)x'(t) denotes the derivative of x(t)x(t) with respect to tt.

Inverse Operator Existence Criteria:

An operator TT has an inverse T1T^{-1} if and only if TT is bijective, which means it is both injective (one-to-one) and surjective (onto).

Injectivity Analysis:

TT is injective if T(x)=T(y)T(x) = T(y) implies x=yx = y. For the differentiation operator, if x(t)=y(t)x'(t) = y'(t) for two polynomials x(t)x(t) and y(t)y(t), then x(t)x(t) and y(t)y(t) differ by at most a constant. Hence, for TT to be injective, we must restrict our attention to a subspace of XX where the constant of integration is fixed, for example by setting x(a)=0x(a) = 0 for all xXx \in X.

Surjectivity Analysis:

TT is surjective if for every function y(t)y(t) in the codomain, there exists an x(t)x(t) in the domain such that T(x)=yT(x) = y. The differentiation operator is surjective onto the space of all differentiable functions on [a,b][a, b] that can be expressed as the derivative of a polynomial, which is again the space of all polynomials on [a,b][a, b].

Existence of T1T^{-1}:

For the differentiation operator TT, an inverse would correspond to the integration operator. However, since integration includes a constant of integration, TT is not surjective onto XX, and therefore, its inverse T1T^{-1} does not exist as a map back into XX.

Conclusion:

The inverse T1T^{-1} of the differentiation operator TT as defined in 2.6-4 does not exist within the space of all polynomials on [a,b][a, b] because TT is not surjective onto XX. The differentiation operator, without additional constraints, does not have a unique inverse that maps back to the original polynomial space due to the constant of integration involved in the antiderivative.

\blacksquare

Counterexample Illustration:

Consider the differentiation operator TT on the space XX of polynomials over an interval [a,b][a, b]. We are given a function y(t)=ety(t) = e^t which is not a polynomial. Our goal is to find a polynomial x(t)x(t) such that x(t)=y(t)x'(t) = y(t).

Attempt to Find x(t)x(t):

The inverse operation to differentiation is integration. Thus, we integrate y(t)y(t) to find x(t)x(t):

x(t)=y(t)dt=etdt=et+C x(t) = \int y(t) dt = \int e^t dt = e^t + C

where CC represents the constant of integration.

Analysis:

The result of the integration, x(t)=et+Cx(t) = e^t + C, is not a polynomial. Hence, it does not reside in the space XX of polynomials on [a,b][a, b]. This shows that y(t)y(t), a non-polynomial function, does not have an antiderivative that is a polynomial in XX.

Conclusion:

Since the integration maps y(t)=ety(t) = e^t to a function outside the space of polynomials, it demonstrates that the differentiation operator TT is not surjective over the space XX. Consequently, TT does not have an inverse T1T^{-1} that maps back to XX. The function y(t)=ety(t) = e^t serves as a counterexample, indicating that there are functions in the codomain of TT for which no polynomial in XX is a pre-image, thereby confirming the non-existence of an inverse operator T1T^{-1} that returns to the original polynomial space XX.


Problem 11. Verify the linearity of the operator T:XXT: X \rightarrow X defined by T(x)=bxT(x) = bx for a fixed 2×22 \times 2 complex matrix bb, and determine the condition for the existence of the inverse operator T1T^{-1}.

Proof of Linearity: To demonstrate that TT is linear, it must satisfy additivity and homogeneity.

  • Additivity:

For any 2×22 \times 2 matrices xx and yy in XX:

T(x+y)=b(x+y)=bx+by=T(x)+T(y) T(x + y) = b(x + y) = bx + by = T(x) + T(y)
  • Homogeneity:

For any complex scalar α\alpha and matrix xx in XX:

T(αx)=b(αx)=αbx=αT(x) T(\alpha x) = b(\alpha x) = \alpha bx = \alpha T(x)

Since TT satisfies both properties, we conclude that TT is indeed a linear operator.

Condition for the Existence of T1T^{-1}: The inverse operator T1T^{-1} exists if and only if TT is bijective, which entails being both injective and surjective.

  • Injectivity:

TT is injective if T(x)=T(y)T(x) = T(y) implies x=yx = y. For TT, this condition holds if the matrix bb is invertible, i.e., det(b)0\text{det}(b) \neq 0.

  • Surjectivity:

TT is surjective if for every zz in XX, there exists an xx such that T(x)=zT(x) = z. This is true if bb is invertible, allowing us to solve x=b1zx = b^{-1}z for any zz.

Therefore, the inverse operator T1T^{-1} exists if and only if the matrix bb is invertible, characterized by a non-zero determinant, det(b)0\text{det}(b) \neq 0.

\blacksquare


Problem 12. Assess the surjectivity of the operator T:XXT: X \rightarrow X, defined by T(x)=bxT(x) = bx for a fixed matrix bb in XX, where XX is the vector space of all 2×22 \times 2 complex matrices, and bxbx denotes the standard product of matrices.

Surjectivity Definition:

An operator TT is said to be surjective if for every matrix zz in XX, there is a matrix xx in XX such that T(x)=zT(x) = z. Formally, this means that the equation bx=zbx = z has a solution for every matrix zz in XX.

Condition for Surjectivity:

The operator TT defined by matrix multiplication is surjective if and only if the matrix bb is invertible. This is equivalent to the requirement that det(b)0\text{det}(b) \neq 0. If bb is invertible, then for every matrix zz in XX, there exists a unique matrix x=b1zx = b^{-1}z that solves the equation bx=zbx = z, indicating that TT maps onto the entire space XX.

Conclusion:

Surjectivity of the operator TT hinges on the invertibility of the matrix bb. If bb is not invertible (i.e., det(b)=0\text{det}(b) = 0), not all matrices zz in XX will have a pre-image under TT, and thus TT will not be surjective. Conversely, if bb is invertible, TT is surjective, ensuring that the inverse operator T1T^{-1} exists and operates as T1(z)=b1zT^{-1}(z) = b^{-1}z for all zz in XX.

\blacksquare


Problem 13 Prove that if {x1,,xn}\{x_1, \ldots, x_n\} is a linearly independent set in D(T)\mathcal{D}(T), and T:D(T)YT: \mathcal{D}(T) \rightarrow Y is a linear operator with an inverse, then the set {Tx1,,Txn}\{Tx_1, \ldots, Tx_n\} is also linearly independent.

Proof:

Assume for contradiction that {Tx1,,Txn}\{Tx_1, \ldots, Tx_n\} is not linearly independent. Then there exist scalars c1,,cnc_1, \ldots, c_n, not all zero, such that:

c1Tx1++cnTxn=0. c_1 Tx_1 + \ldots + c_n Tx_n = 0.

Applying the inverse operator T1T^{-1} to both sides, and using the linearity of T1T^{-1}, we obtain:

c1T1(Tx1)++cnT1(Txn)=T1(0). c_1 T^{-1}(Tx_1) + \ldots + c_n T^{-1}(Tx_n) = T^{-1}(0).

Since T1TT^{-1}T is the identity operator on D(T)\mathcal{D}(T), we have T1(Txi)=xiT^{-1}(Tx_i) = x_i for all ii. Knowing that the identity operator maps 00 to 00, the equation simplifies to:

c1x1++cnxn=0. c_1 x_1 + \ldots + c_n x_n = 0.

This implies that c1,,cnc_1, \ldots, c_n must all be zero because {x1,,xn}\{x_1, \ldots, x_n\} is linearly independent, contradicting our assumption.

Conclusion:

Therefore, the set {Tx1,,Txn}\{Tx_1, \ldots, Tx_n\} must be linearly independent, under the condition that TT is invertible. This holds true due to the fundamental properties of linear transformations and their inverses in vector space theory.

\blacksquare


Problem 14. Prove that for a linear operator T:XYT: X \rightarrow Y with dimX=dimY=n\text{dim} X = \text{dim} Y = n, the range of TT, R(T)\mathcal{R}(T), is equal to YY if and only if the inverse operator T1T^{-1} exists.

Proof:

Forward Direction (R(T)=Y\mathcal{R}(T) = Y implies T1T^{-1} exists):

If R(T)=Y\mathcal{R}(T) = Y, then TT is surjective, meaning for every yYy \in Y, there exists at least one xXx \in X such that T(x)=yT(x) = y. Since dimX=dimY\text{dim} X = \text{dim} Y, TT is a surjective linear map between two finite-dimensional vector spaces of equal dimension, which implies TT is also injective. This is a consequence of the Rank-Nullity Theorem, which in this case implies that nullity(T)=0\text{nullity}(T) = 0 because rank(T)=dimY=n\text{rank}(T) = \text{dim} Y = n and rank(T)+nullity(T)=dimX\text{rank}(T) + \text{nullity}(T) = \text{dim} X.

Being both injective and surjective, TT is bijective, and therefore an inverse T1T^{-1} exists by definition.

Reverse Direction (T1T^{-1} exists implies R(T)=Y\mathcal{R}(T) = Y):

If T1T^{-1} exists, then by definition, TT is bijective, meaning it is both injective and surjective. The surjectivity of TT immediately gives us R(T)=Y\mathcal{R}(T) = Y, because for every yYy \in Y, the existence of T1T^{-1} guarantees an xXx \in X such that T(x)=yT(x) = y.

Conclusion:

The range of TT, R(T)\mathcal{R}(T), is equal to YY if and only if TT is bijective, and since TT is linear, this bijectivity is equivalent to the existence of an inverse T1T^{-1}. This holds true for finite-dimensional vector spaces XX and YY of equal dimension nn.

\blacksquare

Detailed Explanation of the Rank-Nullity Theorem in Context:

The Rank-Nullity Theorem is pivotal in understanding the relationship between the dimensions of a linear operator's range, null space, and domain. For a linear operator T:XYT: X \rightarrow Y with dimX=dimY=n\text{dim} X = \text{dim} Y = n, the theorem is expressed as:

rank(T)+nullity(T)=dimX \text{rank}(T) + \text{nullity}(T) = \text{dim} X

Here, rank(T)\text{rank}(T) represents the dimension of the range of TT (R(T)\mathcal{R}(T)), and nullity(T)\text{nullity}(T) signifies the dimension of the null space of TT (N(T)N(T)).

Application to the Given Problem:

  1. If R(T)=Y\mathcal{R}(T) = Y:

  • The rank of TT is the dimension of YY, hence rank(T)=dimY=n\text{rank}(T) = \text{dim} Y = n.

  • Applying the Rank-Nullity Theorem, and knowing dimX=n\text{dim} X = n, we deduce that nullity(T)=0\text{nullity}(T) = 0, which implies that TT is injective.

  • A linear operator that is injective and surjective is bijective, indicating the existence of an inverse T1T^{-1}.

  1. If T1T^{-1} Exists:

    • The existence of T1T^{-1} implies TT is bijective. Consequently, TT is injective, leading to nullity(T)=0\text{nullity}(T) = 0.

    • Since TT is also surjective, rank(T)=dimY=n\text{rank}(T) = \text{dim} Y = n.

    • The Rank-Nullity Theorem then confirms that rank(T)+nullity(T)=n\text{rank}(T) + \text{nullity}(T) = n, which equals dimX\text{dim} X, thus confirming that R(T)=Y\mathcal{R}(T) = Y.

Conclusion:

The Rank-Nullity Theorem in this scenario confirms that the linear operator TT is invertible if and only if it is surjective. When the domain and codomain are finite-dimensional vector spaces of equal dimension, surjectivity implies injectivity, which is integral to establishing the existence of an inverse operator T1T^{-1}.


Problem 15. We are tasked with proving that the range R(T)\mathcal{R}(T) of a linear operator TT defined on the vector space XX of all real-valued functions with derivatives of all orders is the entirety of XX. However, we must also demonstrate that the inverse T1T^{-1} does not exist. This is to be contrasted with Problem 14.

Showing that R(T)\mathcal{R}(T) is all of XX:

Any function y(t)y(t) in XX can be expressed as the derivative of another function in XX, as the space includes functions with derivatives of all orders. We can take an antiderivative of y(t)y(t) to find a function x(t)x(t) in XX whose derivative is y(t)y(t), that is, x(t)=y(t)x'(t) = y(t). Since the space of functions is closed under integration, this antiderivative x(t)x(t) is also in XX. This demonstrates that for every y(t)y(t) in XX, there exists an x(t)x(t) in XX such that T(x(t))=y(t)T(x(t)) = y(t), confirming that R(T)\mathcal{R}(T) is all of XX.

Showing that T1T^{-1} does not exist:

An inverse operator T1T^{-1} would map a function y(t)y(t) to a function x(t)x(t) such that T(x(t))=y(t)T(x(t)) = y(t). However, the process of taking an antiderivative is not unique due to the constant of integration. Hence, TT is not injective, as multiple functions in XX can map to the same function under TT. Since injectivity is a necessary condition for the existence of an inverse, T1T^{-1} does not exist.

Comparison with Problem 14 and Comments:

Problem 14 involves a finite-dimensional vector space, where surjectivity implies invertibility. In contrast, Problem 15 deals with an infinite-dimensional vector space of smooth functions, where surjectivity is not sufficient for invertibility. The non-uniqueness of the antiderivatives prevents TT from being injective, unlike in finite dimensions, where surjectivity implies injectivity due to the Rank-Nullity Theorem.

Conclusion:

Despite R(T)\mathcal{R}(T) covering all of XX, the non-uniqueness of the antiderivative, due to the constant of integration, prevents TT from being injective, thus precluding the existence of T1T^{-1}. This example underscores a significant distinction between linear operators in finite-dimensional spaces and those in infinite-dimensional spaces.