Undergrad Understanding Extension Fields & Polynomials

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The discussion clarifies the concept of extension fields, particularly how the field ##F[x]/\langle p(x) \rangle##, where ##p(x)## is irreducible, serves as an extension of ##F##. While ##F## is not a direct subfield of this quotient, it can be viewed as isomorphic to a subfield through the canonical embedding ##\mu(a) = a + \langle p(x) \rangle##. This embedding allows for treating elements of the extension field more conveniently, similar to how complex numbers are represented. The conversation emphasizes the practicality of notation, suggesting that rigorous forms can be cumbersome and unnecessary. Overall, the simplification of notation enhances understanding and usability in mathematical discussions.
Mr Davis 97
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I am a little confused about terminology when it comes to extension fields. In my textbook, E is a field extension of F if F is a subfield of E. This is understandable. However, in proving that all polynomials have a zero in an extension field, ##F[x] / \langle p(x) \rangle##, where ##p(x)## is irreducible, is identified as an extension field of ##F##. But how does that match the definition of extension field given above? ##F## isn't a subfield of ##F[x] / \langle p(x) \rangle## at all, but rather isomorphic to a subfield by the isomorphism ##\mu (a) = a + \langle p(x) \rangle##, right?
 
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Yes.

Now ##F[x]/\langle p(x) \rangle## is an ##F-##vector space with a basis vector ##1##, so the embedding ##\mu## is a canonical one (maybe even natural) and ##F## can be considered as a subfield. Usually we also write the elements of ##E = F[x]/ \langle p(x) \rangle ## by Latin letters like ##v \in E## instead of ##[v]_{\langle p(x) \rangle }## and elements ##\mu(a)## as ##a## instead of ##a\cdot 1##. It is nothing gained by a rigorous notation here, so it's easier to drop all the extra ##\mu \, , \, [\,.\,]_{\langle p(x) \rangle} \, , \, \cdot 1 , \cdot x , \ldots , \cdot x^{\deg p -1}##.

It's similar to what we do with complex numbers: ##a + i\cdot b## is far more convenient than ##a\cdot 1 + b \cdot x## or ##\mu(a) + \mu(b)x## or even ##a \cdot [1]_{\langle x^2+1 \rangle} + b \cdot [x]_{\langle x^2+1 \rangle}##. As can be seen here, ##F=\mathbb{R}## would have be to mentioned additionally anyhow. Imagine we would always have to speak of representatives of cosets in ##\mathbb{R}[x]/{\langle x^2+1 \rangle}## instead of real numbers in ##\mathbb{C}##.
 
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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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