139] AN INTRODUCTORY MEMOIR UPON QUANTICS. 229
15. Suppose now that $ is a covariant of ©, then the operation performed
upon any covariant of U gives rise to a covariant of the system
m m'
(*3fc y. y',-- •)•••)>
(f> •••$«, y, • ••)> (%', y, •••$#', y', •••)> &c -
To prove this it is to be in the first instance noticed, that as regards (£, 77, y,...), &c.
we have = ?/3|, &c. Hence considering {xd y }, &c. as referring to the quantic JJ,
the operation % {xd y \ — xd y will be equivalent to [xdy\ + — xd y , and therefore every
covariant of the system must be reduced to zero by each of the operations
59 = {xdy} + ydg — xd y .
This being the case, we have
59. = 59<b + 59 ($),
. 59 = 3>59 + <3? (59),
equations which it is obvious may be replaced by
59. = iDd? + yd$ (<E>),
$>. 59 = 3>59 + <I> {{xdy}),
and consequently (in virtue of the theorem) by
59. <f> = 59$ + yds (3>),
d?. 59 = $59 + \yd^ (d>);
and we have therefore
59.3> — 4>. 59 = — ({?70^} — yd$) (<I>) ;
or, since 4> is a covariant of ©, we have 59 • d> = <E>. 59. And since every covariant
of the system is reduced to zero by the operation 59, and therefore by the operation
d>. 59, such covariant will also be reduced to zero by the operation 59. d>, or what is
the same thing, the covariant operated on by d>, is reduced to zero by the operation
59 and is therefore a co variant, i.e. d> operating upon a covariant gives a covariant.
16. In the case of a quantic such as U —
m m
(*&&, y\x, y')...\
we may instead of the new sets (£, y), (£', y)... employ the sets (y, — x), (y',—x'), &c.
The operative quantic © is in this case defined by the equation © U = 0, and if
be, as before, any covariant of ©, then d> operating upon a covariant of U will give
a covariant of JJ. The proof is nearly the same as in the preceding case; we have
instead of the equation d> ({xdy}) = (d>) the analogous equation
{{xdy}) = - {xdy} (d>),
where on the left-hand side [xd y ] refers to JJ, but on the right-hand side [xd y } refers
to ©, and instead of 5® = {xdy\ + yd% — xd y we have simply 59 = {xd y } — xd y .