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It is easy to see that the placement of (i) forms a regular p -gon; the difference
of the angles is all
4
n
= 2 p .Now k
p is assumed, the regular p -gon is always
completed.
One can see that in (ii), every pair of angles taken from the head forms a
diameter. Since k and p are odd, it does not occur that at the end a diameter is
left uncompleted.
Besides, it is seen that in (ii), each iteration with respect to j consists of
m
1 distinct diameters. What remains is to claim that any angle in (ii) does
not coincide with the angles in (i). Note that 2(( j 1) m + l ) ˀ
n
+ ˀ = 2(( j 1) m + l + pm ) ˀ
n
.
For l =1 , 2 ,
1) m + l + pm are indivisible
by m , which implies that none of the angles in (ii) has appeared in (i).
···
,m
1, both ( j
1) m + l and ( j
See Fig. 4 for the behavior of the strategy for n = 40, p =5,and k = 15. Together
with Lemma 4 , we have a corollary.
Corollary 1. For n divisible by six, C opt ( k )=0 holds if and only if 2
k
n
2 or k = n .
For the case that n is a prime number, we show that C opt ( k ) cannot be zero
unless k = n through algebraic arguments. Let
B := cos 2 ˀ
, cos 4 ˀ
,..., cos 2( n
,
n , sin 2 ˀ
n , sin 4 ˀ
1) ˀ
, sin 2( n
1) ˀ
n
n
n
n
2 as the
which is the set of the destinations other than (1 , 0). We here regard
R
complex plane. Then, the n
1 positions in B stand for the roots of the equation
z n = 1 except z = 1. Letting ʶ be cos 2 n + i sin 2 n , these positions are expressed
as ʶ,ʶ 2 ,...,ʶ n− 1 . The following lemma is a special case of Theorem 12.13 in [ 8 ],
where
Q
[ X ] denotes the set of polynomials of X with the coecients being
rational.
Lemma 5. ([ 8 ]) For n prime, every element in A :=
{
f ( ʶ )
|
f
Q
[ X ]
}
can be
uniquely expressed in a linear combination of ʶ,ʶ 2 ,...,ʶ n− 1 with a j Q
,
a 1 ʶ + a 2 ʶ 2 +
+ a n− 1 ʶ n− 1 .
···
Theorem 5. For n prime, C opt ( k )=0 holds if and only if k = n .
Proof. Apply Lemma 5 with the element to be expressed being 0. Then, the
lemma states that we have to set a 1 ,a 2 ,...,a n− 1 to all zero. Back in the context
of
R
2 , this fact implies that wherever we place k points with 1
k
n
1
at some positions in B , the center of mass does not come to the origin. This
is based on the observation that the linear combination for a j
0 , 1
∈{
k }
with
n− 1
j =1 a j = 1 represents the center of mass of the k points placed at k distinct
positions in B . By rotational symmetry, even if we use the position (1 , 0), we
know that any placement of n
1 or fewer points cannot let the center come to
the origin.
 
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