MHB Unstructured Sets and Monoid Morphisms in Category Theory

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SUMMARY

This discussion centers on the understanding of monoid morphisms within the context of category theory, specifically referencing "An Introduction to Category Theory" by Harold Simmonds. The key points include the definition of a monoid morphism, which requires that for all elements \( r, s \in R \), the conditions \( \phi(r \star s) = \phi(r) \star \phi(s) \) and \( \phi(1) = 1 \) must hold. Participants clarify that Simmonds is describing the properties of monoid morphisms rather than defining why monoids constitute a category. The discussion also emphasizes the importance of recognizing overloaded symbols in mathematical definitions.

PREREQUISITES
  • Understanding of monoids and their properties
  • Familiarity with category theory concepts
  • Knowledge of morphisms in algebraic structures
  • Basic mathematical notation and operations
NEXT STEPS
  • Study the definition of categories in "An Introduction to Category Theory" by Harold Simmonds
  • Learn about monoid structures in "Category Theory" (Second Edition) by Steve Awodey
  • Explore the concept of overloaded symbols in mathematical contexts
  • Investigate the properties of the category Mon and its objects and arrows
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Mathematicians, students of category theory, and anyone interested in the formal properties of algebraic structures and their morphisms.

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I am reading the book: "An Introduction to Category Theory" by Harold Simmonds and am currently focused on Section 1.2: Categories of Unstructured Sets ...

I need some help in order to fully understand Example 1.2.1 on page 9 ... ...

Example 1.2.1 reads as follows:
View attachment 8336
In the above example we read the following: " ... ... A monoid morphism

$$R \stackrel{ \phi }{ \longrightarrow } S$$

between two monoids is a function that respects the furnishings, that is

$$\phi ( r \star s ) = \phi (r) \star \phi (s)$$ and $$\phi (1) = 1$$

for all $$r,s \in R$$. (Notice that we have overloaded the operation symbol and the unit symbol ... ... )

... ... "
My question is as follows:Where in the definition of a category does it follow that we must have $$\phi ( r \star s ) = \phi (r) \star \phi (s)$$ and $$\phi (1) = 1$$ for all $$r,s \in R$$ ...

and further ... ...

what does Simmons mean when he writes "Notice that we have overloaded the operation symbol and the unit symbol ... ... " ? Help will be appreciated ...

Peter***EDIT*** Oh! Reading the section again, maybe Simmons is not indicating why monoids are a category ... but simply describing a monoid morphism ... s that correct?====================================================================================The above post refers to the definition of a category ... so I think MHB readers would benefit from having access to Simmons' definition of a category ... so I am providing access to the same ... as follows:
View attachment 8337
View attachment 8338
https://www.physicsforums.com/attachments/8339
https://www.physicsforums.com/attachments/8340Hope that helps ...

Peter
 
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Peter said:
Reading the section again, maybe Simmons is not indicating why monoids are a category ... but simply describing a monoid morphism
Exactly. Definitions of categories of algebraic structures usually don't mention elements of those structures: individual monoid elements, vectors and so on. Instead categories are defined in terms of appropriate morphisms, i.e., maps that commute with the operations of the structure at hand.

Peter said:
what does Simmons mean when he writes "Notice that we have overloaded the operation symbol and the unit symbol ... ... " ?
In the definition of morphism we have two monoids: $R$ and $S$. Yet operations in both of them are denoted by $\star$, and units in both of them are denoted by 1. Overloading (at least in programming) is precisely this: when the same identifier denotes different things in different contexts. Formally one has to write $\phi(r\star_R s)=\phi(r)\star_S\phi(s)$ and $\phi(1_R)=1_S$ where $\star_R$ and $1_R$ are the operation and unit of $R$ and $\star_S$ and $1_S$ are the operation and unit of $S$.

It's an interesting technical problem in automated reasoning to implement overloading in this context. Fortunately, with the technique called "type classes", which originated in Haskell programming language, this is possible. This allows writing $\phi(r\star s)=\phi(r)\star\phi(s)$ without additional annotations, and the computer is able to figure out that the first $\star$ means $\star_R$ while the second one means $\star_S$.

Do we have an off-topic tag on this forum?
 
In addition to the last post

Simmons is indeed describing the properties of a monoid here

But the highlight of this section is the definition of the category Mon

Can you now, using what you have learned about monoids, decribe the objects, arrows, identity arrows, and the composition rule of Mon ?

Later, in exanple 1.5.1, you will learn that one monoid M, can be viewed as a category too
 
steenis said:
In addition to the last post

Simmons is indeed describing the properties of a monoid here

But the highlight of this section is the definition of the category Mon

Can you now, using what you have learned about monoids, decribe the objects, arrows, identity arrows, and the composition rule of Mon ?

Later, in exanple 1.5.1, you will learn that one monoid M, can be viewed as a category too
Thanks to Evgeny and Steenis for their help ...

Note that I found sections on monoids in the following two books:

(1) Category Theory (Second Edition) by Steve Awodey ... ... Section 1.4, Example 13

(2) Conceptual Mathematics: A First Introduction to Categories (Second Edition) ... ... Session 13: Monoids I am studying the material on monoids in the above two publications ...

Thanks again,

Peter
 
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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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