MHB Module Over a Division Ring - Blyth Theorem 1.1, Part 4

Math Amateur
Gold Member
MHB
Messages
3,920
Reaction score
48
I am reading T. S. Blyth's book "Module Theory: An Approach to Linear Algebra" ... ... and am currently focussed on Chapter 1: Modules, Vector Spaces and Algebras ... ...

I need help with an aspect of Theorem 1.1 part 4 ...

Theorem 1.1 in Blyth reads as follows:View attachment 5838In the above text, in part 4 of the Theorem we read:" ... ... when $$R$$ is a division ring

(4) $$\lambda x = 0_M$$ implies $$\lambda = 0_R$$ or $$x = 0_M$$ ... ... "


Blyth proves that if $$R$$ is a division ring and $$\lambda x = 0_M$$ with $$\lambda \neq 0_R$$ then we have that $$x = 0_M$$ ... ...But ... ... Blyth does not show that if $$R$$ is a division ring and $$\lambda x = 0_M$$ with $$x \neq 0_M$$ then we have that $$\lambda = 0_R$$ ... ...Can someone please help me to prove this ...

Peter
 
Last edited:
Physics news on Phys.org
This is simple logic, Peter.
You want to prove: $s1: p\to (a\vee b)$
For some reason you have proven: $s2: (p\wedge \neg a)\to b$
And you want to know if $s1$ and $s2$ are equivalent: $s1\Leftrightarrow s2$
If so, you have proven $s1$, and you are ready

You know this rule: $r1: (x\to y)\Leftrightarrow (\neg x \vee y)$, we are going to use this

Ok, you have proven $s2$:
$$(p\wedge \neg a)\to b$$
by $r1$, this is equivalent with:
$$\neg(p\wedge \neg a) \vee b$$
which is equivalent with
$$\neg p \vee a \vee b$$
which is equivalent with
$$\neg p \vee (a \vee b)$$
by $r1$, this is equivalent with:
$$p\to (a\vee b)$$
And you are ready.

Therefore, you don't have to prove the second implication.
 
steenis said:
This is simple logic, Peter.
You want to prove: $s1: p\to (a\vee b)$
For some reason you have proven: $s2: (p\wedge \neg a)\to b$
And you want to know if $s1$ and $s2$ are equivalent: $s1\Leftrightarrow s2$
If so, you have proven $s1$, and you are ready

You know this rule: $r1: (x\to y)\Leftrightarrow (\neg x \vee y)$, we are going to use this

Ok, you have proven $s2$:
$$(p\wedge \neg a)\to b$$
by $r1$, this is equivalent with:
$$\neg(p\wedge \neg a) \vee b$$
which is equivalent with
$$\neg p \vee a \vee b$$
which is equivalent with
$$\neg p \vee (a \vee b)$$
by $r1$, this is equivalent with:
$$p\to (a\vee b)$$
And you are ready.

Therefore, you don't have to prove the second implication.
Thanks Steenis ... but it is going on towards 2.00am here in Tasmania ... truly is the edge of the world ...😊 ...

... will work through what you have said in the morning ...

... but thank you for your assistance ...

Peter
 
Thread 'How to define a vector field?'
Hello! In one book I saw that function ##V## of 3 variables ##V_x, V_y, V_z## (vector field in 3D) can be decomposed in a Taylor series without higher-order terms (partial derivative of second power and higher) at point ##(0,0,0)## such way: I think so: higher-order terms can be neglected because partial derivative of second power and higher are equal to 0. Is this true? And how to define vector field correctly for this case? (In the book I found nothing and my attempt was wrong...

Similar threads

  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
1
Views
1K
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
891
Replies
2
Views
1K