When dealing with polynomials, it is sometimes useful to introduce the idea of
Symmetric Polynomials. A Symmetric Polynomial is simply a polynomial that has
the same result no matter the order in which the input variables are given. The
simplest example would be the product of three variables
and
.

. Swapping
the values of some of the variables with each other does not change the outcome. If
one tries to generate all symmetric polynomials with three variables, which sort of
satisfy a ”simplicity” rule (which for now is not well defined), then they might end
with such a result. 
, is often denoted as
or sometimes
. From this definition, you can
try to complete the listed elementary symmetric polynomials with a new one.

and
. It is often useful to represent symmetric equations using
elementary symmetric polynomials (more about this later).
Something that holds a specific point of interest is the expressions of the form
. For this specific problem there exists the Newton-Girard Formula for
Symmetric Polynomials. Define a function
in the following way.

.


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Consider a simple inequality.

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. We can prove this
by just substituting the definitions of
and
. 
and the same
, we assume
and get
the following. ![]() |
and
) are the most useful ones. Using
these inequalities along with basic usage of other common inequalities can
help solve a variety of different problems. One might notice that most of
the techniques somehow transform an equation or inequality into a form
involving purely elementary symmetric polynomials and can ask the question:
what if such a form does not exist? Happily, for us, there is a theorem called
the Fundamental Theorem of Symmetric Polynomials, which claims that
any symmetric polynomial can, in fact, be expressed as an expression using
elementary symmetric polynomials (the theorem applies to any number of
variables). The proof of this statement will also not be provided here due to its
complexity.
Say we have three systems of symmetric equations as the following.

, for example. First of all, transform the
equations using elementary symmetric polynomials. 
,
and from the third equation we can find
. 
using the
Newton-Girard Formula. 

. Do the same as last time: express the system using
elementary symmetric polynomials. 
and
. 
such that
are all roots of that polynomial. This
would be useful as from there we can immediately find the solution in the following
way. 
to be roots of a
polynomial
, simply let
. Expanding out the
expression, we get the following. ![]() |

. 
is to calculate
and
. 
. 
is unnecessary; one could replace all the calculations
by simply calculating
through
and
. In fact, what was
just described is yet another proof or perspective on the Newton-Girard
Formula. Obviously, in such cases, using the Newton-Girard Formula directly
is best. However, if you forgot, you could always remember it using this
trick.