MHB Help with D&K Lemma 2.2.7 (Hadamard) Proof: Qs on Continuity of \phi_a

Click For Summary
The discussion focuses on the continuity of the operator-valued function φ_a and its implications for the differentiability of a function f at a point a, as presented in Duistermaat and Kolk's Lemma 2.2.7. It is established that φ_a is continuous at a if the limit of the operator distance between φ_a(x) and φ_a(a) approaches zero as x approaches a. The proof involves demonstrating that the limit condition holds for all vectors y in R^n, which aligns with the definition of strong operator continuity. Additionally, it is shown that if f is differentiable at a, then it is also continuous at that point, as the limit of f(x) equals f(a) when evaluated at the differentiable point. This connection highlights the relationship between differentiability and continuity in the context of the lemma.
Math Amateur
Gold Member
MHB
Messages
3,920
Reaction score
48
I am reading "Multidimensional Real Analysis I: Differentiation" by J. J. Duistermaat and J. A. C. Kolk ...

I am focused on Chapter 2: Differentiation ... ...

I need help with another aspect of the proof of Lemma 2.2.7 (Hadamard...) ... ...

Duistermaat and Kolk's Lemma 2.2.7 and its proof read as follows:https://www.physicsforums.com/attachments/7837
https://www.physicsforums.com/attachments/7838
Near to the end of the above text D&K write the following:

" ... ... A direct computation gives $$\| \epsilon_a(h) h^t \|_{ Eucl } = \| \epsilon_a(h) \| \| h \|$$, hence$$\lim_{ h \rightarrow 0 } \frac{ \| \epsilon_a(h) h^t \|_{ Eucl } }{ \| h \|^2 } = \lim_{ h \rightarrow 0 } \frac{ \| \epsilon_a(h) \| }{ \| h \| } = 0 $$This shows that $$\phi_a$$ is continuous at $$a$$. ... ... "

My questions are as follows:

Question 1

... how/why does the above show that $$\phi_a$$ is continuous at $$a$$. ... ...?

Can someone please demonstrate explicitly, formally and rigorously that $$\phi_a$$ is continuous at $$a$$. ... ...?Question 2

How/why does the proof of Hadamard's Lemma 2.2.7 imply that $$f$$ is continuous at $$a$$ if $$f$$ is differentiable at $$a$$ ... ?
Help will be much appreciated ... ...

Peter==========================================================================================

NOTE:

The start of D&K's section on differentiable mappings may help readers of the above post understand the context and notation of the post ... so I am providing the same as follows:
View attachment 7839
View attachment 7840
The start of D&K's section on linear mappings may also help readers of the above post understand the context and notation of the post ... so I am providing the same as follows:

View attachment 7841
View attachment 7842
View attachment 7843
Hope the above helps readers understand the context and notation of the post ...

Peter
 
Last edited:
Physics news on Phys.org
Hi, Peter.

Peter said:
Question 1

... how/why does the above show that $$\phi_a$$ is continuous at $$a$$. ... ...?

Can someone please demonstrate explicitly, formally and rigorously that $$\phi_a$$ is continuous at $$a$$. ... ...?

This question is perhaps a little deeper than it seems initially. The subtlety lies in the fact that $\phi_{a}(x)$ is an operator-valued function; i.e., for each $x$, $\phi_{a}(x)$ is a linear operator.

Step 1: Understanding Continuity
When the authors say "$\phi_{a}$ is continuous at $a$," what they mean is the operators $\phi_{a}(x)$ and $\phi_{a}(a)$ can be made arbitrarily close for $x$ sufficiently close to $a$ (i.e., the "distance" from $\phi_{a}(x)$ to $\phi_{a}(a)$ vanishes in the limit as $x\rightarrow a$). Symbolically what we want to show is that
$$\lim_{x\rightarrow a}\phi_{a}(x)=\phi_{a}(a)$$
Note that, at least symbolically, this is exactly the same notion as continuity in the case of a real-valued function of a single variable; i.e., $f$ is continuous at $a$ means
$$\lim_{x\rightarrow a}f(x)=f(a).$$
Step 2: Understanding Operator Norms
This begs the question: How do we measure the distance between operators? Depending on the context, there are several ways one can define a norm on a space of functions (this is not unlike your previous posts where you asked about different norms on $\mathbb{R}^{n}$). In the case of your post, the authors are (implicitly) using a notion known as "strong (operator) continuity," where, by definition,
$$\lim_{x\rightarrow a}\phi_{a}(x)=\phi_{a}(a)$$
provided
$$\lim_{x\rightarrow a}\|\phi_{a}(x)y-\phi_{a}(a)y\|=0,\qquad\forall y\in\mathbb{R}^{n},$$
where the norm above is the norm in $\mathbb{R}^{p}$ (which makes sense because $\phi_{a}(x)$ and $\phi_{a}(a)$ are operators taking elements of $\mathbb{R}^{n}$ into $\mathbb{R}^{p}$). Note that this condition which defines the meaning of the limit is the reason the authors need to introduce a $y$ in the equation
$$\phi_{a}(x)y=Df(a)y+\cdots$$
Step 3: Answering Your Question
From what was discussed in Step 2, we must show
$$\lim_{x\rightarrow a}\|\phi_{a}(x)y-\phi_{a}(a)y\|=0,\qquad\forall y\in\mathbb{R}^{n}.$$
Note that, by the authors' definition of $\phi_{a}(x)$, $\phi_{a}(a)=Df(a)$. Looking at the equation
$$\phi_{a}(x)y=Df(a)y+\cdots,$$
we see $\phi_{a}(x)-\phi_{a}(a)=\phi_{a}(x)-Df(a)=\cdots,$ so when the authors show
$$\lim_{h\rightarrow 0}\frac{\|\epsilon_{a}(h)h^{t}\|}{\|h\|^{2}}=0,$$
they are really proving
$$\lim_{x\rightarrow a}\|\phi_{a}(x)y-\phi_{a}(a)y\|=0,\qquad\forall y\in\mathbb{R}^{n},$$
which is precisely what we want to establish when proving $\phi_{a}(x)$ is continuous at $a$.

Peter said:
Question 2
How/why does the proof of Hadamard's Lemma 2.2.7 imply that $$f$$ is continuous at $$a$$ if $$f$$ is differentiable at $$a$$ ... ?

To prove that $f$ is continuous at $a$, we want to show that
$$\lim_{x\rightarrow a}f(x)=f(a),$$
where we note that $f$ is a function, not an operator, so we don't need to introduce $y$ as we did previously. From the above we know
$$\lim_{x\rightarrow a}\phi_{a}(x)=\phi_{a}(a)=Df(a),$$
so
$$\lim_{x\rightarrow a} f(x)=\lim_{x\rightarrow a} f(a)+\lim_{x\rightarrow a}\phi_{a}(x)(x-a)=f(a)+Df(a)(a-a)=f(a),$$
as desired.
 
GJA said:
Hi, Peter.
This question is perhaps a little deeper than it seems initially. The subtlety lies in the fact that $\phi_{a}(x)$ is an operator-valued function; i.e., for each $x$, $\phi_{a}(x)$ is a linear operator.

Step 1: Understanding Continuity
When the authors say "$\phi_{a}$ is continuous at $a$," what they mean is the operators $\phi_{a}(x)$ and $\phi_{a}(a)$ can be made arbitrarily close for $x$ sufficiently close to $a$ (i.e., the "distance" from $\phi_{a}(x)$ to $\phi_{a}(a)$ vanishes in the limit as $x\rightarrow a$). Symbolically what we want to show is that
$$\lim_{x\rightarrow a}\phi_{a}(x)=\phi_{a}(a)$$
Note that, at least symbolically, this is exactly the same notion as continuity in the case of a real-valued function of a single variable; i.e., $f$ is continuous at $a$ means
$$\lim_{x\rightarrow a}f(x)=f(a).$$
Step 2: Understanding Operator Norms
This begs the question: How do we measure the distance between operators? Depending on the context, there are several ways one can define a norm on a space of functions (this is not unlike your previous posts where you asked about different norms on $\mathbb{R}^{n}$). In the case of your post, the authors are (implicitly) using a notion known as "strong (operator) continuity," where, by definition,
$$\lim_{x\rightarrow a}\phi_{a}(x)=\phi_{a}(a)$$
provided
$$\lim_{x\rightarrow a}\|\phi_{a}(x)y-\phi_{a}(a)y\|=0,\qquad\forall y\in\mathbb{R}^{n},$$
where the norm above is the norm in $\mathbb{R}^{p}$ (which makes sense because $\phi_{a}(x)$ and $\phi_{a}(a)$ are operators taking elements of $\mathbb{R}^{n}$ into $\mathbb{R}^{p}$). Note that this condition which defines the meaning of the limit is the reason the authors need to introduce a $y$ in the equation
$$\phi_{a}(x)y=Df(a)y+\cdots$$
Step 3: Answering Your Question
From what was discussed in Step 2, we must show
$$\lim_{x\rightarrow a}\|\phi_{a}(x)y-\phi_{a}(a)y\|=0,\qquad\forall y\in\mathbb{R}^{n}.$$
Note that, by the authors' definition of $\phi_{a}(x)$, $\phi_{a}(a)=Df(a)$. Looking at the equation
$$\phi_{a}(x)y=Df(a)y+\cdots,$$
we see $\phi_{a}(x)-\phi_{a}(a)=\phi_{a}(x)-Df(a)=\cdots,$ so when the authors show
$$\lim_{h\rightarrow 0}\frac{\|\epsilon_{a}(h)h^{t}\|}{\|h\|^{2}}=0,$$
they are really proving
$$\lim_{x\rightarrow a}\|\phi_{a}(x)y-\phi_{a}(a)y\|=0,\qquad\forall y\in\mathbb{R}^{n},$$
which is precisely what we want to establish when proving $\phi_{a}(x)$ is continuous at $a$.
To prove that $f$ is continuous at $a$, we want to show that
$$\lim_{x\rightarrow a}f(x)=f(a),$$
where we note that $f$ is a function, not an operator, so we don't need to introduce $y$ as we did previously. From the above we know
$$\lim_{x\rightarrow a}\phi_{a}(x)=\phi_{a}(a)=Df(a),$$
so
$$\lim_{x\rightarrow a} f(x)=\lim_{x\rightarrow a} f(a)+\lim_{x\rightarrow a}\phi_{a}(x)(x-a)=f(a)+Df(a)(a-a)=f(a),$$
as desired.
Thanks GJA ... that was really helpful ...

Still reflecting on what you have said ...

Thanks again ...

Peter
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K