Proving that ##T## is skew-symmetric, inner product is an integration.

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The discussion centers on proving that the operator T is skew-symmetric, defined by T(f)(x) = ∫₀ˣ f(t) dt, within the context of a real inner product space. The inner products are expressed as ⟨T(f), g⟩ = ∫₀¹ ∫₀ˣ f(t) dt g(t) dt and ⟨f, T(g)⟩ = ∫₀¹ f(t) ∫₀ˣ g(t) dt dt. By applying integration by parts, the participants derive that ⟨T(f), g⟩ simplifies to -⟨f, T(g)⟩, confirming the skew-symmetry of T. The discussion also emphasizes the importance of the zero integral condition for functions in the subspace V. Ultimately, the proof is completed by showing that both inner products yield equivalent results under the defined conditions.
Hall
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Homework Statement
Let ##C(0.1)## be the real linear space of all real functions continuous on ##[0,1]## with inner product
$$
\langle f , \rangle = \int_{0}^{1} f(t) ~g(t) dt $$
Let ##V## be the subspace of all ##f## such that
$$
\int_{0}^{1} f(t) dt = 0$$

Let ##T: V \to C(0,1)## be the integration operator defined by
$$
T (f(x)) = \int_{0}^{x} f(t) dt$$

Prove that ##T## is skew-symmetric.
Relevant Equations
##T## will be skew-symmetric if
$$
\langle T(f), g \rangle = - \langle f, T(g)\rangle$$
##\langle T(f), g \rangle = \int_{0}^{1} \int_{0}^{x} f(t) dt ~ g(t) dt##
As ##\int_{0}^{x} f(t) dt## will be a function in ##x##, therefore a constant w.r.t. ##dt##, we have
##\langle T(f), g \rangle = \int_{0}^{x} f(t) dt ~ \int_{0}^{1} g(t) dt##

##\langle f, T(g)\rangle = \int_{0}^{1} f(t) ~ \int_{0}^{x} g(t) dt~ dt##
By the same argument, we have
##\langle f, T(g)\rangle = \int_{0}^{1} f(t) dt \int_{0}^{x} g(t) dt##

(Can someone tell me why preview button no longer produces a preview?)

What do you think how can I prove ##T## to be skew-symmetric?
 
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Don't you need the complex conjugate in there somewhere?
 
PeroK said:
Don't you need the complex conjugate in there somewhere?
Where did you see complex numbers?
 
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Hall said:
Homework Statement:: Let ##C(0.1)## be the real linear space of all real functions continuous on ##[0,1]## with inner product
$$
\langle f , \rangle = \int_{0}^{1} f(t) ~g(t) dt $$
Let ##V## be the subspace of all ##f## such that
$$
\int_{0}^{1} f(t) dt = 0$$

Let ##T: V \to C(0,1)## be the integration operator defined by
$$
T (f(x)) = \int_{0}^{x} f(t) dt$$

This should be <br /> T(f)(x) = \int_0^x f(t)\,dt.

Prove that ##T## is skew-symmetric.
Relevant Equations:: ##T## will be skew-symmetric if
$$
\langle T(f), g \rangle = - \langle f, T(g)\rangle$$

##\langle T(f), g \rangle = \int_{0}^{1} \int_{0}^{x} f(t) dt ~ g(t) dt##
As ##\int_{0}^{x} f(t) dt## will be a function in ##x##, therefore a constant w.r.t. ##dt##, we have
##\langle T(f), g \rangle = \int_{0}^{x} f(t) dt ~ \int_{0}^{1} g(t) dt##

If t is the dummy variable for the inner product integration, then you need a different symbol for the dummy variable in the definition of T(f)(t). So <br /> T(f)(t) = \int_0^t f(s)\,ds and the inner product with g is <br /> \begin{split}<br /> \langle T(f),g \rangle &amp;= \int_0^1 T(f)(t)g(t)\,dt \\<br /> &amp;= \int_0^1 \int_0^t f(s)\,ds\,g(t)\,dt. \end{split}<br /> But it is simpler to define F = T(f) and note that F&#039; = f.
 
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fresh_42 said:
Where did you see complex numbers?
I forgot an inner product could be real!
 
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pasmith said:
This should be <br /> T(f)(x) = \int_0^x f(t)\,dt.
If t is the dummy variable for the inner product integration, then you need a different symbol for the dummy variable in the definition of T(f)(t). So <br /> T(f)(t) = \int_0^t f(s)\,ds and the inner product with g is <br /> \begin{split}<br /> \langle T(f),g \rangle &amp;= \int_0^1 T(f)(t)g(t)\,dt \\<br /> &amp;= \int_0^1 \int_0^t f(s)\,ds\,g(t)\,dt. \end{split}<br /> But it is simpler to define F = T(f) and note that F&#039; = f.
I could get only this far:
$$
\langle T(f), g \rangle = \int_{0}^{1} \int_{0}^{t} f(s) ds g(t) dt$$
$$
\langle T(f), g \rangle = \int_{0}^{1} F(t) g(t) $$
Using integration by parts,
$$
\langle T(f), g \rangle = F(t) \int g(t) \big|_{0}^{1} - \int_{0}^{1} f(t) \int g(t) dt ~dt$$
$$
\langle T(f), g \rangle = F(t) G(t) \big|_{0}^{1} - \int f(t) G(t) dt $$

$$
\langle f, T(g) \rangle = \int_{0}^{1} f(t) \int_{0}^{t} g(s) ds ~dt$$

$$
\langle f, T(g) \rangle= G(t) \int f(t) dt \big|_{0}^{1} - \int_{0}^{1} g(t) F(t) dt $$
$$
\langle f, T(g) \rangle= F(t)~G(t) \big|_{0}^{1} - \int_{0}^{1} g(t) F(t) dt$$
 
What do you know about F(0) = \int_0^0 f(t)\,dt and F(1) = \int_0^1 f(t)\,dt, given that f \in V?
 
I don't see that you used the given information that the domain of T is the set of functions whose integrals are zero.
Hall said:
Let ##V## be the subspace of all ##f## such that
$$\int_{0}^{1} f(t) dt = 0$$

Let ##T: V \to C(0,1)## be the integration operator defined by
$$
T (f(x)) = \int_{0}^{x} f(t) dt$$

Hall said:
(Can someone tell me why preview button no longer produces a preview?)
Preview works for me.
 
pasmith said:
What do you know about F(0) = \int_0^0 f(t)\,dt and F(1) = \int_0^1 f(t)\,dt, given that f \in V?
They are zero.

So, our expressions for inner product reduces:
$$
\langle T(f), g \rangle = - \int_{0}^{1} f(t) G(t) dt$$
And
$$
\langle f, T(g) \rangle = -\int_{0}^{1}g(t) F(t) dt$$
 
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Hall said:
They are zero.

So, our expressions for inner product reduces:
$$
\langle T(f), g \rangle = - \int_{0}^{1} f(t) G(t) dt$$
And
$$
\langle f, T(g) \rangle = -\int_{0}^{1}g(t) F(t) dt$$
I think I got it, applying integration by parts once to the first inner product:
$$
\langle T(f), g \rangle = - \int_{0}^{1} f(t) G(t) dt$$
$$
\langle T(f) , g \rangle=
- \left( G(t) F(t) \big|_{0}^{1} - \int_{0}^{1} F(t) g(t) dt \right)$$
Again the first term will be zero, and we are remaining with
$$
\langle T(f), g \rangle = \int_{0}^{1} F(t) g(t) dt$$

Thus, we have
$$
\langle T(f), g\rangle = - \langle f, T(g)\rangle$$
hence, proving T is skew-symmetric.
 
Last edited:
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