Abstract
AbstractIn this paper we consider the following problem: Given a Hamiltonian graph G, and a Hamiltonian cycle C of G, can we compute a second Hamiltonian cycle $$C^{\prime } \ne C$$
C
′
≠
C
of G, and if yes, how quickly? If the input graph G satisfies certain conditions (e.g. if every vertex of G is odd, or if the minimum degree is large enough), it is known that such a second Hamiltonian cycle always exists. Despite substantial efforts, no subexponential-time algorithm is known for this problem. In this paper we relax the problem of computing a second Hamiltonian cycle in two ways. First, we consider approximating the length of a second longest cycle on n-vertex graphs with minimum degree $$\delta $$
δ
and maximum degree $$\Delta $$
Δ
. We provide a linear-time algorithm for computing a cycle $$C^{\prime } \ne C$$
C
′
≠
C
of length at least $$n-4\alpha (\sqrt{n}+2\alpha )+8$$
n
-
4
α
(
n
+
2
α
)
+
8
, where $$\alpha = \frac{\Delta -2}{\delta -2}$$
α
=
Δ
-
2
δ
-
2
. This results provides a constructive proof of a recent result by Girão, Kittipassorn, and Narayanan in the regime of $$\frac{\Delta }{\delta } = o(\sqrt{n})$$
Δ
δ
=
o
(
n
)
. Our second relaxation of the problem is probabilistic. We propose a randomized algorithm which computes a second Hamiltonian cycle with high probability, given that the input graph G has a large enough minimum degree. More specifically, we prove that for every $$0<p\le 0.02$$
0
<
p
≤
0.02
, if the minimum degree of G is at least $$\frac{8}{p} \log \sqrt{8}n + 4$$
8
p
log
8
n
+
4
, then a second Hamiltonian cycle can be computed with probability at least $$1 - \frac{1}{n}\left( \frac{50}{p^4} + 1 \right) $$
1
-
1
n
50
p
4
+
1
in $$poly(n) \cdot 2^{4pn}$$
p
o
l
y
(
n
)
·
2
4
p
n
time. This result implies that, when the minimum degree $$\delta $$
δ
is sufficiently large, we can compute with high probability a second Hamiltonian cycle faster than any known deterministic algorithm. In particular, when $$\delta = \omega (\log n)$$
δ
=
ω
(
log
n
)
, our probabilistic algorithm works in $$2^{o(n)}$$
2
o
(
n
)
time.
Funder
Engineering and Physical Sciences Research Council
Publisher
Springer Science and Business Media LLC