Still in Chapter 2 - field extensions. Then Chapter 3, for the idea of dimension (and a review of some linear algebra).
There are lots of parts to that problem - pretty much one per sentence. I'll put each part of the answer in a separate bullet below.
Let p be a prime. Since it's not easy to put a sqrt sign on this web page, I will write S for sqrt(p).
(a + bS)*(a' + b'S) = aa'+ bb'p + (ab' + a'b)SIf a, b, a' and b' are rational then so are (aa'+bb'p) and (ab'+a'b) so this product is in Q[S].
a + bS = a' + b'S (*)then a=a' and b=b'. Here's the proof. Equation (*) implies that
(a-a') + (b-b')S = 0which we know forces a-a'=0 and b-b'=0, hence a=a' and b=b'.
1 1 (a-bS) (a-bS)
------ = ----------- = -----
(a+bS) (a+bS)(a-bS) a2-b2p
Now I know what I need to know to write the proof going
forwards. Given z = a + bS, let t = a2-b2p. Then
t is not 0 (if it were then the prime p would = (a/b)2,
which is impossible). So let
w = (a/t) - (b/t)Swhich is clearly an element of R. I claim w is a multiplicative inverse of z. To prove the claim, just carry out the multiplication to see that wz=1. (I won't type it over again here. It has to work because of the preliminary algebra I did figuring out what w had to be.)
These are all short proofs in which every step must be justified. It's important to keep the notation clean, and to be sure to reason from what you are given to what you want. If you end your proof with something like "0=0" it isn't right. Be sure to use "=" only where you mean it, not as a synonym for "therefore".
Proof: Since 0+0=0 in V (the vector space) I know (from the meaning of "=") that
f*(0+0) = f*0Then
f*0 + f*0 = f*0 (Axiom 1)Now I know that the vector f*0 has an additive inverse in V; call it w. Then adding w to both sides of the previous equation and using the associative law for + on the left tells me
f*0 = 0which is what I wanted to show.
Proof. This is similar to the last one. Start with 0+0=0 in F. Then
0*v = (0+0)*v = 0*v + 0*v (Distributive law.)Let w be the additive inverse of 0*v in V and add it to both sides to reach the desired concusion.
Proof. This seems obvious and is easy to prove, once you understand what's tricky about it. Remember that there is really no such thing as subtraction in either F or V. (-f) is just the way we write the additive inverse of f in F, and -(f*V) is the way we write the additive inverse of (f*V) in V. To show that the vector on the left in the theorem is the additive inverse of f*V we need to show that when we add it to f*V we get 0:
(-f)*v + f*V = (-f + f)*v (distributive law) = 0*v (meaning of -f in field F) = 0 (previously proved)
Proof. Suppose f*v=0 but f !=0. Then since the scalars form a field, f has a multiplicative inverse g. Then v = 1*v = (g*f)*v = g*(f*v) = g*0 = 0, which is a contradiction. (In the preceding chain of equalities I used Axiom 4 for vector spaces, the associative law, and a fact I just proved.)
The double square brackets in F[[x]] is new notation. When R is a ring we write R[[x]] for the ring of "formal power series" in the variable x. That's the set of all expressions of the form a0 + a1x + a2x2 + ... where the coefficients ai come from the ring R. You add and multiply those objects using the usual rules for the arithmetic of exponents (which are ordinary integers) and the arithmetic of the ring R for adding and multiplying the coefficients.
The proof one way is easy. If f(x) has a 0 constant term then it looks like thisL
a1x + a2x2 + ...and there's clearly no power series you can multiply this by that will make all the terms but the constant term cancel. You will always be able to factor an x out of whatever you get. So there's nothing you can multiply this power series by and get just plain 1. So when f(x) has a zero constant term it does not have a multiplicative inverse.
The proof the other way is harder.
x2 - 2y2 = +-1 (*) n xn yn check 1 1 1 1 - 2*1 = -1 2 3 2 9 - 2*4 = 1 3 7 5 49 - 2*25 = -1Lewanda noted that the pattern seems to be
yn+1 = xn + yn xn+1 = xn + 2ynThis set of solutions to (*) isn't an accident. There's a conceptual way to see what's going on. The clue is in the arithmetic of the ring R = Z[sqrt(2)] - the set of all real numbers of the form a+b*sqrt(2) where a and b are ordinary integers. R is very far from being a field. Most of its members don't have multiplicative inverses. But some do.
Suppose xn and yn satisfy (*) and xn+1 and yn+1 are defined as above, and compute:
xn+12 - 2yn+12
= (xn + 2yn)2 - 2(xn + yn)2
= tedious formal algebra you all got right
= -(xn2 - 2yn2)
= -+1.
so xn+1 and yn+1 satisfy (*) too - with the
opposite sign. I know the first lines work, so this proof shows all
the succeeding lines work as well.
It's very important to note here that there's no +-1 until the end of
the chain of equalities. If I put it in the first line then all I am
doing is asserting what I am trying to prove!
We've essentially done this in problem 1 above. The best way to see it here is to note that when (x,y) solves * we have
(x + y sqrt(2))*(x - y sqrt(2)) = +11so that +-(x - y sqrt(2)) is the multiplicative inverse of (x+y*sqrt(2)). The converse is true too.
Suppose r has a multiplicative inverse - call it s. Then I will show that sn is the multiplicative inverse of rn. To do that I need to show that sn*rn = 1. But that's easy. Using the associative and commutative laws many times tells me that sup>n*rn = (r*s)n, but that's just 1n which equals 1.
Note that this proof uses no mumbo jumbo about negative exponents, nothing about 1/r = r-1. All that mumbo jumbo is only true once you've proved it, and we haven't.
Proof: When you multiply
(a + b sqrt(2)) * ( 1 + sqrt(2) ) = (a+2b) + (a+b)sqrt(2)you see that you get exactly the equations for computing xn+1 and yn+1 from xn and yn in the table.
x2 - dy2 = +-1 (**)(We've just studied the special case d=2.) See how far you can get with the cases d=3 and d=5. First look for one small solution, then use the strategy above to see how to generate the table.
For more information on this topic (probably more than you want to know), you can google "Pell's equation". Here's the first hit, from mathworld. It's pretty informative, particularly down toward the bottom of the page, at about equation (31). If you get that far, look at the smallest solution for d=61.