MHB Ring Homomorphisms from Z to Z .... Lovett, Ex. 1, Section 5.4 .... ....

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The discussion centers on Exercise 1 from Section 5.4 of Stephen Lovett's "Abstract Algebra: Structures and Applications," focusing on ring homomorphisms from Z to Z. Two primary examples of homomorphisms are identified: the Zero Homomorphism, which maps all integers to zero, and the Identity Homomorphism, which maps each integer to itself. The challenge lies in rigorously proving that these are the only homomorphisms possible. A proposed approach involves showing that any other homomorphism must conform to these forms, leading to the conclusion that the only solutions are the Zero and Identity Homomorphisms. The discussion concludes with acknowledgment of the clarity gained from collaborative insights.
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I am reading Stephen Lovett's book, "Abstract Algebra: Structures and Applications" and am currently focused on Section 5.4 Ring Homomorphisms ...

I need some help with Exercise 1 of Section 5.4 ... ... ...

Exercise 1 reads as follows:View attachment 6452Relevant Definitions

A ring homomorphism is defined by Lovett as follows:https://www.physicsforums.com/attachments/6453Thoughts so far ... ...

One ring homomorphism, $$f_1 \ : \ \mathbb{Z} \rightarrow \mathbb{Z}$$ would be the Zero Homomorphism defined by $$f_1(r) = 0 \ \forall r \in \mathbb{Z}$$ ...

($$f_1$$ is clearly a homomorphism ... )

Another ring homomorphism $$f_2 \ : \ \mathbb{Z} \rightarrow \mathbb{Z}$$ would be the Identity Homomorphism defined by $$f_2(r) = r \ \forall r \in \mathbb{Z}$$ ...

($$f_2$$ is clearly a homomorphism ... )
Now presumably ... ... ? ... ... $$f_1$$ and $$f_2$$ are the only ring homomorphisms from $$\mathbb{Z} \rightarrow \mathbb{Z}$$ ... ... but how do we formally and rigorously show that there are no further homomorphisms ... ...

Hope that someone can help ...

Peter

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Have no tried the following idea ... but no luck ...Suppose $$\exists \ f_3 \ : \ \mathbb{Z} \rightarrow \mathbb{Z}$$ ... ... try to show no such $$f_3$$ exists ... at least no $$f_3$$ that is different from $$f_1 , f_2$$ exists ... ...Let $$f_3(2) = x $$ where $$x \in \mathbb{Z}$$ ...Then $$f_3(4) = f_3( 2 \cdot 2 ) = f_3( 2) f_3( 2) = x^2 $$
and
$$f_3(4) = f_3( 2 + 2) = f_3( 2) + f_3( 2) = x + x = 2x$$
Then we must have $$x^2 = 2x$$ ... ... ... (1)
I was hoping that there would be no integer solution to (1) ... but $$x = 0$$ satisfies ... so ... problems ..

Maybe a similar approach with different numbers will work ... ...

Can anyone comment on this type of approach ...

Peter
 
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Here's an outline of how I would do it.

First, $f(n+1) = f(n) + f(1)$. Use this to prove by induction that $f(n) = nf(1)$ for all positive $n$.

Next, $-n + n = 0$, so $f(-n) + f(n) = f(0) = 0$. Therefore $f(-n) = -f(n) = -nf(1)$. Thus $f(n) = nf(1)$ for all $n$, positive or negative.

Finally, $1^2 = 1$, so $\bigl(f(1)\bigr)^2 = f(1)$. It follows that $f(1)$ must be either $0$ or $1$. So $f(n)$ must be either $n\cdot0 = 0$ or $n\cdot1 = n$.
 
Opalg said:
Here's an outline of how I would do it.

First, $f(n+1) = f(n) + f(1)$. Use this to prove by induction that $f(n) = nf(1)$ for all positive $n$.

Next, $-n + n = 0$, so $f(-n) + f(n) = f(0) = 0$. Therefore $f(-n) = -f(n) = -nf(1)$. Thus $f(n) = nf(1)$ for all $n$, positive or negative.

Finally, $1^2 = 1$, so $\bigl(f(1)\bigr)^2 = f(1)$. It follows that $f(1)$ must be either $0$ or $1$. So $f(n)$ must be either $n\cdot0 = 0$ or $n\cdot1 = n$.
Thanks Opalg ...

Have the idea now ... very grateful for your help!

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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