MHB Split Short Exact Sequences - Bland - Proposition 3.2.6

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The discussion revolves around understanding Proposition 3.2.6 from Paul E. Bland's "Rings and Their Modules," specifically the proof concerning the well-defined nature of the application \( g' \). The key point is that \( g' \) may not be well defined due to the non-injectivity of \( g \), necessitating proof that \( g'(y) \) remains consistent regardless of the choice of pre-image \( x \). The participants analyze how Bland demonstrates that the difference between two elements related to \( g \) lies in the intersection of the kernel and another module, ultimately leading to the conclusion that \( g' \) is indeed well defined. This clarification is crucial for understanding the implications of the exact sequences discussed in the section. The conversation reflects a deep engagement with the material and seeks to solidify comprehension of the proof's nuances.
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I am reading Paul E. Bland's book, "Rings and Their Modules".

I am trying to understand Section 3.2 on exact sequences in Mod_R and need help with the proof of Proposition 3.2.6.

Proposition 3.2.6 and its proof read as follows:View attachment 3609The part of the proof that perplexes me is the section of the proof that begins with the claim that $$g'$$ is well defined. That section of the proof reads as follows:https://www.physicsforums.com/attachments/3610Now Bland takes two elements from $$Ker f'$$, namely:

$$(x - f(f'(x)))$$ and $$(x - f(f'(x))) $$

and forms their difference (which must also belong to $$Ker f'$$ since $$Ker f'$$ is a submodule) thus forming:

$$(x - f(f'(x))) - (x - f(f'(x)))$$

which Bland shows is equal to

$$(x - x') - f(f'(x - x'))
$$Now he has already shown that $$(x - x') \in I am f$$ and certainly $$f(f'(x - x')) \in I am f$$ ... ...

So we have that:

$$(x - x') - f(f'(x - x')) \in Ker f' \cap I am f $$

and also we have

$$Ker f' \cap I am f = 0$$ since $$M = Ker f' \oplus I am f$$

... ...

BUT ... ...

... ... why does this prove that $$g'$$ is "well defined" ... indeed what does Bland mean by this?

Further to the question can someone please confirm that my analysis above is correct ... or better ... critique my analysis pointing out any questionable or inaccurate statements ...

Help will be appreciated ...

Peter
 
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Hi Peter,

Bland's has just constructed an application $g'$, that may not be well defined because he tooks a definition based in $g'(y)=...(x)$ with $g(x)=y$.

This definition may depend on $x$, because $g$ doesn't need to be injective.

So he needs to prove that if you choose $x,x'$ with $g(x)=g(x')=y$ then $g'(y)=...(x)=...(x')$. That is, it doesn't mind what g-pre-image you choose for the element $y$, $g'(y)$ will be the same.

Now what he tooks is two elements such that $g(x)=g(x')$, and compute
$...(x)-...(x')=(x-f(f'(x)))-(x'-f(f'(x')))$ and proves that this difference lay on $Ker f' \cap I am f=0$, so $(x-f(f'(x)))-(x'-f(f'(x')))=0$, then $...(x)=...(x')$ and $g'$ is well defined.
 
Fallen Angel said:
Hi Peter,

Bland's has just constructed an application $g'$, that may not be well defined because he tooks a definition based in $g'(y)=...(x)$ with $g(x)=y$.

This definition may depend on $x$, because $g$ doesn't need to be injective.

So he needs to prove that if you choose $x,x'$ with $g(x)=g(x')=y$ then $g'(y)=...(x)=...(x')$. That is, it doesn't mind what g-pre-image you choose for the element $y$, $g'(y)$ will be the same.

Now what he tooks is two elements such that $g(x)=g(x')$, and compute
$...(x)-...(x')=(x-f(f'(x)))-(x'-f(f'(x')))$ and proves that this difference lay on $Ker f' \cap I am f=0$, so $(x-f(f'(x)))-(x'-f(f'(x')))=0$, then $...(x)=...(x')$ and $g'$ is well defined.
Thanks for you help, Fallen Angel ... ...

Still reflecting on what you have written ...

Will get back to you soon on this matter ...

Thanks again,

Peter
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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