Tensor Products - Example 8 - Dummit and Foote - Section 10.4, page 370

Thus, in summary, Dummit and Foote Section 10.4 discusses the tensor product of modules, specifically the tensor product of the quotient ring $R/I$ and a left R-module N. They provide an example (Example (8) on page 366) that illustrates how to view the quotient ring $R/I$ as an (R/I, R)-bimodule and use it to define a left $R/I$-module structure on the tensor product. They also explain how the ideal I acts trivially in this case, and provide a universal mapping property for the tensor product. Finally, they use the example to demonstrate how to transform and justify the expression (r mod I) tensor n
  • #1
Math Amateur
Gold Member
MHB
3,998
48
I am reading Dummit and Foote Section 10.4: Tensor Products of Modules.

I would appreciate some help in understanding Example (8) on page 366 concerning viewing the quotient ring \(\displaystyle R/I \) as an \(\displaystyle (R/I, R) \)-bimodule.

Example (8) D&F page 370 reads as follows: (see attachment)

-------------------------------------------------------------------------------

"Let \(\displaystyle R\) be a ring (not necessarily commutative). Let \(\displaystyle I\) be a two-sided ideal in \(\displaystyle R\), and let \(\displaystyle N\) be a left \(\displaystyle R\)-module. Then, as previously mentioned, \(\displaystyle R/I\) is an \(\displaystyle (R/I, R)\)-bimodule, so the tensor product is a left \(\displaystyle R/I \) module. ... ... ...

... ... The tensor product is generated as an abelian group by simple tensors

\(\displaystyle (r \ mod \ I ) \otimes n = r(1 \otimes n) \text{ for } r \in R \text{ and } n \in N \) ... ... ... ... (1)

viewing the \(\displaystyle R/I\) module tensor product as an \(\displaystyle R\)-module on which \(\displaystyle I\) acts trivially" (?)

... ... ...

----------------------------------------------------------------------------

I am seeking help in order to understand how and why

\(\displaystyle (r \ mod \ I ) \otimes n = r(1 \otimes n) \text{ for } r \in R \text{ and } n \in N \) ... ... ... ... (1)

is the case, and also what D&F mean by "viewing the \(\displaystyle R/I\) module tensor product as an \(\displaystyle R\)-module on which \(\displaystyle I\) acts trivially"
My understanding of how the LHS of (1) may be transformed into something like the RHS is as follows:

Following D&F page 367 (see attachment) after the definition of the standard \(\displaystyle R\)-module structure we read (approximately) the following:

For a situation where \(\displaystyle N\) is a left \(\displaystyle R\)-module and \(\displaystyle M\) is an \(\displaystyle (S, R)\)-bimodule, we have that the \(\displaystyle (S, R)\)-bimodule structure of \(\displaystyle M\) implies that

\(\displaystyle s( \sum_{Finite} m_i \otimes n_i ) = \sum_{Finite} s m_i \otimes n_i \) ... ... ... (10.8)

gives a well-defined action of S on \(\displaystyle M \otimes_R N \) as a left S-module.

Rewriting (10.8) for a simple or elementary tensor (and switching LHS and RHS) we have:

\(\displaystyle sm \otimes n = s(m \otimes n) \) ... ... ... ... (10.8)'Now, in Example 8 we have:

\(\displaystyle N\) is a left \(\displaystyle R\)-module

and

\(\displaystyle M\) = \(\displaystyle R/I \) is an \(\displaystyle (R/I, R)\)-bimodule

and

\(\displaystyle R/I \otimes_R N \) is a left \(\displaystyle R/I\)-moduleThus in Example 8 we have:

\(\displaystyle (r \ mod \ I ) \otimes n = (r \ mod \ I ) \cdot 1_{R/I} \otimes n \)

and so applying (10.8)' we get

\(\displaystyle ( r \ mod \ I ) \otimes n = ((r \ mod \ I ) \cdot 1_{R/I}) \otimes n = (r \ mod \ I )( 1_{R/I} \otimes n) \) ... ... ... ... (2)

Can someone please confirm (or otherwise) that the above is correct?

Assuming I am correct in what I have done so far, then can someone help me with how we get from (2) to relation (1)?

... ... and, of course, how do we justify the steps from (2) to (1)?


Would appreciate help with the above.

Peter
 
Last edited:
Physics news on Phys.org
  • #2
First let's examine the statement:

"...$R/I$ tensor product as an $R$-module on which $I$ acts trivially."

We have a simple tensor, say:

$(r + I) \otimes n$.

If $x \in I$, then $x + I = 0 + I = I$, whence:

$(x + I)((r + I) \otimes n = [(x + I)(r + I)] \otimes n$

$= [(0 + I)(r + I)] \otimes n = (0r + I) \otimes n$

$=0_{R/I} \otimes n = 0$.

This is what is meant by "$I$ acts trivially", it induces a 0-map.

Recall that for any ring homomorphism $f: R \to S$ we can define an $S$-module $M$ as an $R$-module, by setting:

$rm = f(r)m$, and the fact that $f$ is a ring homomorphism automatically assures us the module axioms will be satisfied.

There is nothing "out of the ordinary" using the ring homomorphism $R \to R/I$.

So our $R$-action on $R/I \otimes_R N$ is given by:

$r(r' + I)\otimes n = [(r + I)(r' + I)]\otimes n = (rr' + I)\otimes n$.

If $r = x \in I$ this becomes:

$(xr' + I) \otimes n = (0 + I)\otimes n = 0$, since $xr' \in I$ (since $I$ is an ideal).

Given $r \in R$ it is also clear that:

$r + I = r1_R + I = r(1_R + I) = r(1_{R/I})$

Hence we have:

$r \text{ mod } I\otimes n = r(1_{R/I} \otimes n)$.

(Dummit and Foote really ought to be clear about "which 1" they are using, since we have 2 different rings floating around).

Note that they replace "bilinear" with "balanced map" which is the "corresponding idea" to a bilinear map when the $R$-action is on "two different sides", and $R$ is not necessarily commutative (such maps are also called "middle linear").

The universal mapping property of the tensor product actually applies most generally to $R$-balanced maps, and the $R$-bilinear maps most often given as examples are "special cases".
 
  • #3
Deveno said:
First let's examine the statement:

"...$R/I$ tensor product as an $R$-module on which $I$ acts trivially."

We have a simple tensor, say:

$(r + I) \otimes n$.

If $x \in I$, then $x + I = 0 + I = I$, whence:

$(x + I)((r + I) \otimes n = [(x + I)(r + I)] \otimes n$

$= [(0 + I)(r + I)] \otimes n = (0r + I) \otimes n$

$=0_{R/I} \otimes n = 0$.

This is what is meant by "$I$ acts trivially", it induces a 0-map.

Recall that for any ring homomorphism $f: R \to S$ we can define an $S$-module $M$ as an $R$-module, by setting:

$rm = f(r)m$, and the fact that $f$ is a ring homomorphism automatically assures us the module axioms will be satisfied.

There is nothing "out of the ordinary" using the ring homomorphism $R \to R/I$.

So our $R$-action on $R/I \otimes_R N$ is given by:

$r(r' + I)\otimes n = [(r + I)(r' + I)]\otimes n = (rr' + I)\otimes n$.

If $r = x \in I$ this becomes:

$(xr' + I) \otimes n = (0 + I)\otimes n = 0$, since $xr' \in I$ (since $I$ is an ideal).

Given $r \in R$ it is also clear that:

$r + I = r1_R + I = r(1_R + I) = r(1_{R/I})$

Hence we have:

$r \text{ mod } I\otimes n = r(1_{R/I} \otimes n)$.

(Dummit and Foote really ought to be clear about "which 1" they are using, since we have 2 different rings floating around).

Note that they replace "bilinear" with "balanced map" which is the "corresponding idea" to a bilinear map when the $R$-action is on "two different sides", and $R$ is not necessarily commutative (such maps are also called "middle linear").

The universal mapping property of the tensor product actually applies most generally to $R$-balanced maps, and the $R$-bilinear maps most often given as examples are "special cases".

Thanks for the help, Deveno.

Just a minor clarification:

You write:

"Given $r \in R$ it is also clear that:

\(\displaystyle r + I = r1_R + I = r(1_R + I) = r(1_{R/I}) \)

I am uncertain regarding how you justify the step:

\(\displaystyle r1_R + I = r(1_R + I) = r(1_{R/I}) \)

I can see that \(\displaystyle r 1_R + I = (r +I)(1_R + I) \) but I am unsure from there ... unless we are replacing r with r + I ... ?

Can you please explain/clarify?

Another, but I suspect related issue ... I find it disconcerting when you write:

\(\displaystyle r(r' + I)\otimes n = [(r + I)(r' + I)]\otimes n \)

since in (2), if we interpret it literally we have r = r +I, which seems a little weird ...

Can you clarify ...

... ... Maybe it has something to do with notational complexities surrounding the definition of the action ... but anyway, as I said, I find it disconcerting since r may become r + 1 or vice versa at various points in the argument ... hope you can help ..

Peter
 
Last edited:
  • #4
The expression:

$r(1 + I)$

comes from the NATURAL $R$-action of $R/I$ as an $R$-module, which is the NATURAL action of $R$ on an $S$-module $M$ when we have a homomorphism $f:R \to S$.

This doesn't make sense "in rings" but it DOES make sense in MODULES. So if we want to "mix and match" ring structures, modules are a natural setting. We do need some type of homomorphism connecting them, or else we cannot guarantee our "hybrid structure" will be well-behaved (in this case, we usually resort to the "default ring" $\Bbb Z$ where we always have some kind of compatibility).
 
  • #5
Deveno said:
The expression:

$r(1 + I)$

comes from the NATURAL $R$-action of $R/I$ as an $R$-module, which is the NATURAL action of $R$ on an $S$-module $M$ when we have a homomorphism $f:R \to S$.

This doesn't make sense "in rings" but it DOES make sense in MODULES. So if we want to "mix and match" ring structures, modules are a natural setting. We do need some type of homomorphism connecting them, or else we cannot guarantee our "hybrid structure" will be well-behaved (in this case, we usually resort to the "default ring" $\Bbb Z$ where we always have some kind of compatibility).

Thanks Deveno ... but, I am not following you ... my apologies I am probably being somewhat slow ... sorry ...

To try to follow your remark:

""$r(1 + I)$

comes from the NATURAL $R$-action of $R/I$ as an $R$-module... ..." I went to D&F's definition of a left R-module on page 337 ... following D&F we have ...

The (natural ?) R-action of R on M = R/I (that is a map

\(\displaystyle R \times R/I \to R/I \)) denoted by

\(\displaystyle rm = r(r' + I) \) where \(\displaystyle r, r' \in R \) and \(\displaystyle m = r' + I \in R/I \) ... ... "

so wouldn't the R-action of R/I as a left R-module be

\(\displaystyle rm = r(r' + I) \)?

Can you help?

I suspect I am missing something ... and also suspect I need to bring in the mapping \(\displaystyle f: R \to S \), but unsure ...

PeterPS - EDIT

I suspect I need to carefully reflect on the remarks in D&F's Examples (1) and (2) on page 366, which I am now engaged upon in an attempt to clarify things ...
 
  • #6
Peter said:
Thanks Deveno ... but, I am not following you ... my apologies I am probably being somewhat slow ... sorry ...

To try to follow your remark:

""$r(1 + I)$

comes from the NATURAL $R$-action of $R/I$ as an $R$-module... ..." I went to D&F's definition of a left R-module on page 337 ... following D&F we have ...

The (natural ?) R-action of R on M = R/I (that is a map

\(\displaystyle R \times R/I \to R/I \)) denoted by

\(\displaystyle rm = r(r' + I) \) where \(\displaystyle r, r' \in R \) and \(\displaystyle m = r' + I \in R/I \) ... ... "

so wouldn't the R-action of R/I as a left R-module be

\(\displaystyle rm = r(r' + I) \)?

Can you help?

I suspect I am missing something ... and also suspect I need to bring in the mapping \(\displaystyle f: R \to S \), but unsure ...

PeterPS - EDIT

I suspect I need to carefully reflect on the remarks in D&F's Examples (1) and (2) on page 366, which I am now engaged upon in an attempt to clarify things ...

You're almost there. That is indeed the natural action, but clearly any element:

$r + I = (r + I)(1 + I)$, and $(r + I)(1 + I)$ is the "actual" action of:

$r$ on $(1 + I)$.

So in considering acting on elements $r \text{ mod } I\otimes n$, we just have to consider an $R$ action on $1 \text{ mod } I\otimes n$, and only $r \in R - I$ actually "do anything" (the elements of $I$ have trivial action, that is: annihilate).

*******

$R/I$ is not, by itself, an $R$-module, we need to DEFINE:

$r(r'+I)$.

But the definition:

$r(r'+I) = rr'+I$ is "natural" and satisfies all the usual axioms:

$r[(r'+I) + (r''+I)] = r[(r'+r'')+I] = r(r'+r'') + I = (rr'+rr'') + I$

$= [(rr') + I] + [(rr'') + I] = r(r' + I) + r(r'' + I)$ and

$(r + r')(r'' + I) = (r + r')r'' + I = (rr' + rr'') + I$

$= (rr' + I) + (rr'' + I) = r(r'' + I) + r'(r'' + I)$, as well as:

$r(r'(r''+I)) = r[(r'r'') + I] = r(r'r'') + I = (rr')r" + I = (rr')(r'' + I)$, and:

$1_R(r + I) = (1_Rr) + I = r + I$.
 

Related to Tensor Products - Example 8 - Dummit and Foote - Section 10.4, page 370

1. What is a tensor product?

A tensor product is a mathematical operation that combines two vector spaces to create a new vector space. It is denoted by the symbol ⊗ and is used to represent linear transformations between vector spaces.

2. How is the tensor product defined in Example 8 in Dummit and Foote?

In Example 8 in Dummit and Foote, the tensor product is defined as the set of all formal sums of the form ∑(aᵢ⊗bᵢ) where aᵢ and bᵢ are elements of two given vector spaces. This set is then equipped with a specific addition and scalar multiplication operation to make it a vector space.

3. What is the purpose of using tensor products?

The purpose of using tensor products is to extend the notion of linear transformations to more general situations. It allows for the study of multilinear maps, which are functions that take multiple vectors as inputs and produce a single output.

4. How is the tensor product related to the direct sum of vector spaces?

The tensor product is closely related to the direct sum of vector spaces. In fact, the direct sum can be seen as a special case of the tensor product, where the vector spaces being combined are finite-dimensional. In general, the tensor product allows for the combination of vector spaces of any dimension.

5. Are there any practical applications of tensor products?

Yes, tensor products have many practical applications in various fields such as physics, engineering, and computer science. In physics, tensor products are used to represent physical quantities with multiple components, such as force or velocity. In engineering, they are used to model complex systems and in computer science, they are used in machine learning and data analysis.

Similar threads

  • Linear and Abstract Algebra
Replies
8
Views
2K
  • Linear and Abstract Algebra
Replies
7
Views
2K
  • Linear and Abstract Algebra
Replies
4
Views
1K
  • Linear and Abstract Algebra
Replies
3
Views
2K
  • Linear and Abstract Algebra
Replies
3
Views
2K
  • Linear and Abstract Algebra
Replies
7
Views
2K
  • Linear and Abstract Algebra
Replies
4
Views
2K
  • Linear and Abstract Algebra
Replies
1
Views
1K
  • Linear and Abstract Algebra
Replies
16
Views
3K
  • Linear and Abstract Algebra
Replies
7
Views
2K
Back
Top