Assume that we have α=a+bi, β=c+di, where a,b,c,d∈R.
α(β)=(a+bi)(c+di)=
(ac−bd)+(ad+bc)i.
β(α)=(c+di)(a+bi)=
(ca−db)+(cb+da)
We know that from the commutativity of addition that operations such as (ac−bd)+(ad+bc),(ca−db)+(cb+da) are equivalent . The same follows for ac,ca,bd,db, from the commutativity of multiplication.
Associativity:
(α+β)+λ=α+(β+λ),∀α,β,λ∈C.
α(βλ)=(αβ)λ,∀α,β,λ∈C.
Identity:
1λ=λ,∀λ∈C
Additive Inverse:
∀α∈C,∃!β∈C:α+β=0.
Multiplicative Inverse:
∀α∈C,∃!β:αβ=1,wherea=0
Distributive Property:
λ(α+β)=λ(α)+λ(β),∀α,β,λ∈C.
Additive Inverse:
Let α,β∈C:
Let −α denote the additive inverse of α, thus ∃!(−α), such that α+(−α)=0.
Subtraction of complex numbers is defined like so:
β−α=β+(−α).
Division is defined as: β/α=β(1/α).
Also, if we let α>0, then 1/α is the multiplicative inverse of a, such that α(1/α)=1
Notation: Throughout this book, we will use F, as a stand in for R,andC, as both of these are examples of fields. What this means, is that if we can prove a theorem holds for F, then we can prove that it holds for R,andC. The elements of some fields F, are referred to as scalars, which is a fancy term for number. For α∈F, we consider αm, to be the product of α with itself m times: am=m timesα⋅⋅⋅α. From this we can comfortably assume that:
Before we go into the definition of Rn and Cn, we should consider two important examples: The set R2, which can be thought of as a plane, and is the set of all ordered pairs of real numbers, and R3, the set of all points in 3-space:
R2={(x,y):x,y∈R}
R3={(x,y,z):x,y,z∈R}
In order to generalize these concepts to higher dimensions we need to use the concept of lists:
A list of length n, is an ordered collection of n elements: (x1…xn).
Two lists are equal iff they have the same number of elements in the same order.
Also, in order to define these higher dimensional analogues, we will use F which is equivalent to CorR.
Fn is the set of all lists of elements of F, where the lists are of length n.
We can't visualize Rn,wheren≥4, and the same also holds for Cn,wheren>1. However, while these lack physical geometric representations, we can still manipulate elements of Fn algebraically.
Addition in Fn is defined by adding the corresponding coordinates:
(x1…xn)+(y1…yn)=(x1+y1…xn+yn)
However, it is typically easier to replace these lists with the variable that is subscripted to represent an element of the list, and results in cleaner mathematics.
If x,y∈Fn,x+y=y+x, meaning commutativity extends to Fn.
Proof of Commutativity of Addition
Let x=(x1…xn), and let y=(y1…yn).
x+y=(x1…xn)+(y1…yn)=
(x1+y1…xn+yn)=
(y1+x1…yn+xn)=
This following line holds, due to the commutativity of addition in F.