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On the Exact Evaluation of the Face-Centred Cubic Lattice Green Function
Authors:
G S Joyce
R T Delves
Affiliation:
(1) Centre for Mathematical Sciences (CMS), Arunapuram P.O., Pala, 686574 Pala Campus, India;(2) 34 Panchi Batti Chauraha, Jodhpur, 342 011, Ratananda, India;(3) United Nations Vienna International Centre Space Application Programme, 1400 Wien, Austria;
Abstract:
The mathematical properties of the lattice Green function
Open image in new window
w=
w
1
+i
w
2
lies in a complex plane which is cut from
w
=?1 to
w
=3, and {
?
1
,
?
2
,
?
3
} is a set of integers with
?
1
+
?
2
+
?
3
equal to an even integer. In particular, it is proved that
G
(2
n
,0,0;
w
), where
n
=0,1,2,…, is a solution of a fourth-order linear differential equation of the Fuchsian type with four regular singular points at
w
=?1,0,3 and ∞. It is also shown that
G
(2
n
,0,0;
w
) satisfies a five-term recurrence relation with respect to the integer variable
n
. The limiting function
$G^{-}(2n,0,0;w_1)\equiv\lim_{\epsilon\rightarrow0+}G(2n,0,0;w_1-\mathrm{i}\epsilon) =G_{\mathrm{R}}(2n,0,0;w_1)+\mathrm{i}G_{\mathrm {I}}(2n,0,0;w_1) ,\nonumber $
where
w
1
∈(?1,3), is evaluated exactly in terms of
2
F
1
hypergeometric functions and the special cases
G
?
(2
n
,0,0;0),
G
?
(2
n
,0,0;1) and
G
(2
n
,0,0;3) are analysed using singular value theory. More generally, it is demonstrated that
G
(
?
1
,
?
2
,
?
3
;
w
) can be written in the form
Open image in new window
Open image in new window
ξ,
K
(
k
?
) and
E
(
k
?
) are complete elliptic integrals of the first and second kind, respectively, with
$k_{-}^2\equiv k_{-}^2(w)={1\over2}- {2\over w} \biggl(1+{1\over w} \biggr)^{-{3\over2}}- {1\over2} \biggl(1-{1\over w} \biggr ) \biggl(1+{1\over w} \biggr)^{-{3\over2}} \biggl(1-{3\over w} \biggr)^{1\over2}\nonumber $
and the parameter
ξ
is defined as
$\xi\equiv\xi(w)= \biggl(1+\sqrt{1-{3\over w}} \,\biggr)^{-1} \biggl(-1+\sqrt{1+{1\over w}} \,\biggr) .\nonumber $
This result is valid for
all
values of
w
which lie in the cut plane. The asymptotic behaviour of
G
?
(2
n
,0,0;
w
1
) and
G
(2
n
,0,0;
w
1
) as
n
→∞ is also determined. In the final section of the paper a new
2
F
1
product form for the
anisotropic
face-centred cubic lattice Green function is given.
Keywords:
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