MHB Modules - Northott: Proposition 1

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SUMMARY

The discussion centers on Proposition 1 from D. G. Northcott's "Lessons on Rings, Modules and Multiplicities," specifically addressing the proof that for an R-module M, the equation $$0_Rx = 0_M$$ holds true. Participants explore the implications of $$0_R + 0_R = 0_R$$ and how it leads to the conclusion that $$0_Rx = 0_Ry = 0_M$$ for all elements x, y in M. The proof is confirmed through the additive properties of groups, demonstrating that the additive inverse of $$0_R x$$ leads to the conclusion that $$0_R x = 0_M$$ for any x in M.

PREREQUISITES
  • Understanding of R-modules and their definitions
  • Familiarity with group theory, particularly additive groups
  • Knowledge of the properties of zero elements in algebraic structures
  • Basic proficiency in mathematical proofs and logical reasoning
NEXT STEPS
  • Study the properties of R-modules in detail, focusing on zero elements
  • Explore group theory, specifically the role of identity and inverse elements
  • Learn about the implications of additive identities in algebraic structures
  • Review mathematical proof techniques, particularly in abstract algebra
USEFUL FOR

Mathematicians, students of abstract algebra, and anyone interested in the foundational concepts of modules and groups will benefit from this discussion.

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In D. G. Northcott's book: Lessons on Rings, Modules and Multiplicities, Proposition 1 reads as follows:View attachment 3453The first line of the above proof reads as follows:

"Since $$0_R + 0_R = 0_R$$, the definition of an R-module shows that

$$0_Rx = (0_R + 0_R)x = 0_Rx + 0_Rx,$$

whence $$0_Rx = 0_M$$, because $$M$$ is a group. ... ... "Now it seems highly plausible that

$$0_Rx = 0_Rx + 0_Rx$$

in the group $$M$$ leads to the conclusion that $$0_Rx = 0_M$$ ... ... BUT ... how do we know (prove) this? ...

Can someone help?

[NOTE:

Northcott seems to be saying that in a group M, for an element $$a$$:

$$a = a + a$$

$$\Longrightarrow a$$ is the identity

$$\Longrightarrow x + a = a + x = x$$ for all $$x \in M$$

... BUT ... how do we prove this? ]
 
Last edited:
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Peter said:
In D. G. Northcott's book: Lessons on Rings, Modules and Multiplicities, Proposition 1 reads as follows:View attachment 3453The first line of the above proof reads as follows:

"Since $$0_R + 0_R = 0_R$$, the definition of an R-module shows that

$$0_Rx = (0_R + 0_R)x = 0_Rx + 0_Rx,$$

whence $$0_Rx = 0_M$$, because $$M$$ is a group. ... ... "Now it seems highly plausible that

$$0_Rx = 0_Rx + 0_Rx$$

in the group $$M$$ leads to the conclusion that $$0_Rx = 0_M$$ ... ... BUT ... how do we know (prove) this? ...

Can someone help?

[NOTE:

Northcott seems to be saying that in a group M, for an element $$a$$:

$$a = a + a$$

$$\Longrightarrow a$$ is the identity

$$\Longrightarrow x + a = a + x = x$$ for all $$x \in M$$

... BUT ... how do we prove this? ]

... ... just been thinking about the above question ...

Now have another question ...

How do we know that $$0_Rx = 0_Ry$$ for $$x,y \in M$$

Help with the above question and the question in the first post would be appreciated ...

Peter
 
Fix $x\in M$. Since $M$ is a group under addition, $0_R x$ has an additive inverse, $-(0_R x)$. Add $-(0_R x)$ to both sides of the equation $0_R x = 0_R x + 0_R x$. The left hand side will be $0_M$, and the right hand side will be $(0_R x + 0_R x) + [-(0_R x)]$, which is the same as $0_R x + (0_R x + [-(0_R x)])$, by associativity of addition. This reduces to $0_R x + 0_M$, which equals $0_R x$. Thus, $0_R x = 0_M$. Since this holds for every $x\in M$, $0_R x = 0_R y = 0_M$ for all $x, y\in M$ (answering your second question).
 
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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