Euclidean Rings - Rotman Example 3.76

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SUMMARY

This discussion focuses on Example 3.76 from Joseph J. Rotman's "A First Course in Abstract Algebra with Applications (Third Edition)", which illustrates the properties of Euclidean rings. The key point is that every field is a Euclidean ring, specifically addressing the conditions outlined in the definition. The participants clarify that for the second condition to hold, one should set \( q = gf^{-1} \) and \( r = 0 \), ensuring that the equation \( g = qf + r \) is satisfied for all \( g \in R \) and \( f \in R^{\times} \).

PREREQUISITES
  • Understanding of Euclidean rings and their definitions
  • Familiarity with fields and their properties
  • Basic knowledge of algebraic structures
  • Proficiency in manipulating algebraic equations
NEXT STEPS
  • Study the properties of Euclidean rings in greater detail
  • Explore the implications of fields being Euclidean rings
  • Learn about the role of the division algorithm in Euclidean rings
  • Investigate other examples of algebraic structures in Rotman's book
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Students of abstract algebra, mathematicians interested in algebraic structures, and educators teaching concepts related to Euclidean rings and fields.

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I am reading Joseph J. Rotman's book: A First Course in Abstract Algebra with Applications (Third Edition) ...

I am currently focused on Section 3.5 From Numbers to Polynomials ...

I need help with Example 3.76 ... ... the example concerns Euclidean rings and their defining characteristics so I am including the definition of a Euclidean ring in the relevant text shown below ... ...

The relevant text from Rotman's book is as follows:https://www.physicsforums.com/attachments/4649

View attachment 4648
I am trying to understand Example 3.76 which indicates that every field is a Euclidean ring ... ...

I can see that point (i) of the definition is satisfied with $$\partial$$ set identically to zero ...... BUT ... I fail to understand what Rotman is saying about how point (ii) is satisfied ... ...

In order for (ii) to be satisfied, for every $$g \in R$$ and every $$f \in R^{\times}$$ we have to find $$q, r \in R$$ such that:

$$g = qf + r$$ ... ... ... (*)

... BUT ...

Rotman says to set $$q = f^{-1}$$ and $$r = 0$$

but if we do this (*) above becomes

$$g = f f^{-1} + 0 = 1$$ ...

but $$g$$ may be any element of $$R$$ ... ?Can someone please explain what is going on ... that is, what Rotman means in this example ...

Hope someone can help ...

Peter
 
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Peter said:
Rotman says to set $$q = f^{-1}$$ and $$r = 0$$ but if we do this (*) above becomes $$g = f f^{-1} + 0 = 1$$ ... but $$g$$ may be any element of $$R$$ ... ?
You are right. The book should say: if $g\in R$ and $f\in R^{\times}$ set $q=gf^{-1}$ and $r=0.$ So, for all $g\in R$ and for all $f\in R^{\times}$ we verify $g=(\underbrace{gf^{-1}}_{q})\;f+\underbrace{0}_{r}.$
 
Fernando Revilla said:
You are right. The book should say: if $g\in R$ and $f\in R^{\times}$ set $q=gf^{-1}$ and $r=0.$ So, for all $g\in R$ and for all $f\in R^{\times}$ we verify $g=(\underbrace{gf^{-1}}_{q})\;f+\underbrace{0}_{r}.$

Thanks for that clarification Fernando ... I appreciate your help ...

Peter
 

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