of irreducible fractions rn A (0;1] whose denominators do not exceed x. We shall ... number theorem by extracting an intermediate error term occurring in the asymptotic formula for .... Lemma (Lehner-Newman's second sum formula). X. F(x)Ã1.
J. Math. Soc. Japan Vol. 52, No. 4, 2000
Some sums involving Farey fractions II To the memory of Professor Pan Cheng Dong By Shigeru Kanemitsu,*) Takako Kuzumaki and Masami Yoshimoto (Received July 12, 1999)
Abstract. Let Fx denote the Farey series of order x, i.e. the increasing sequence of irreducible fractions rn A
0; 1 whose denominators do not exceed x. We shall obtain P F
x z precise asymptotic formulae for the sum n1 rn for complex z and related sums, F
x ]Fx coinciding the summatory P function of Euler's function. In particular, we shall prove an asymptotic formula for rÿ1 with as good an estimate as for the prime n number theorem by extracting an intermediate error term occurring in the asymptotic formula for F
x.
1. Introduction and statement of results. For a variable x V 1, let Fx Fx denote the Farey series of order x (x integral part of x), i.e. the sequence of irreducible fractions A
0; 1 whose denominators U x, arranged in increasing order of magnitude: bn Fx rn
bn ; cn 1; 0 < bn U cn U x : cn
Supplementarily, we put r0 b0 =c0 0=1. P The number of rn 's in Fx with cn n is nk1;
k; n1 f
n, Euler's function. The P total number of rn 's in Fx is therefore F
x nUx f
n. Let Qx Qx denote all pairs
cn ; cn1 of denominators of consecutive Farey fractions rn bn =cn and rn1 bn1 =cn1 (with c0 1):
1
Qx f
cn ; cn1 j 0 U n U F
x ÿ 1g
(]Qx ]Fx F
x). E.g. Q3 f
1; 3;
3; 2;
2; 3;
3; 1g. In Part I [15] we considered the m-th power moments sm
x for m 2; 3 (Theorems 1 and 2) and revealed the connection between these and the (associated) error terms of Euler's function, where X
cn cn1 ÿm
m A N: sm
x
cn ; cn1 A Qx
In view of the basic relation bn1 cn ÿ bn cn1 1; 2000 Mathematics Subject Classi®cation. Primary 11B57; Secondary 11N37. Key Words and Phrases. Farey series, Euler's function, exponential sums * The ®rst author was supported in part by Grant-in-Aid for Scienti®c Research (C) (No. 11640051), the Japan Society for the Promotion of Science.
916
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
we have rn1 ÿ rn
cn cn1 ÿ1 , so that sm
x
F
xÿ1 X
rn1 ÿ rn m
n0
is indeed the m-th power moment of the di¨erence of consecutive Farey fractions. In particular, s1
x rF
x ÿ r0 1 ÿ 0 1. Rather surprisingly, our Theorems [15] as well as those of Hall-Tenenbaum [9] caught attention of physicists in connection with circle maps (Cvitanovic [4]). In this Part II our objective is twofold. The ®rst-half of the paper is a direct continuation as well as an improved generalization of results in Part I, and the secondhalf is the presentation of results in the unpublished MS of the ®rst author's former paper ( jointly with R. Sita Rama Chandra Rao and A. Siva Rama Sarma) which was once submitted to these volumes, but withdrawn for better organization, years ago; although preparation of the new MS has been suspended because of untimely death of Sita Rama Chandra Rao, the ®rst author's friend and collaborator, that withdrawn MS is now completely rewritten, incorporating new developments. Namely, Theorem 1 contains not only improvements of Theorems 1 and 2 of Part I by a factor of
log log x 4=3 but also rather precise asymptotic formulas for sm
x in the cases m 4 and m V 5. The proof goes on the similar lines as those of Theorems 1 and 2; however, we shall prove all the results at a stretch, i.e. new asymptotic formulas for sm
x for m V 4 as well as improvements, by modifying proofs of Part I and introducing new lemmas, and also as byproducts evaluate certain in®nite series. Then we proceed to give re®nements of the former paper (referred to above), namely improvements over MikolaÂs' results [22] concerning the asymptotic behavior of P F
x ÿa sums for a > 0 (for positive power sums, see [16]) and precise asymptotic n1 rn formulas for unsymmetric form of sm
x, i.e. X
cn ; cn1 A Qx
1 ; cna cn1
the special case a 2 of which constitutes an improvement of Hans and Dumir's results [10]. All these results rest on Lehner-Newman's ®rst sum formula [19]: Lemma (Lehner-Newman's ®rst sum formula [19]). For any complex-valued function f
u; v de®ned at least for positive integral arguments u, v, we have
2
sf
x :
F
xÿ1 X
f
cn ; cn1
n0
f
1; 1
X
r X
2UrUx
k1
k; r1
f f
k; r f
r; k ÿ f
k; r ÿ kg:
On the other hand, our Theorems 6 and 7 are based on Lehner-Newman's second sum formula:
917
Farey fractions
Lemma (Lehner-Newman's second sum formula). F
xÿ1 X
3
f
cn ; cn1
X
X
f
r; k:
rUx xÿr 0 being an absolute constant, is the reducing factor which appears in the prime number theorem
9
M
x :
X
m
n O
xd
x;
nUx
where m
n denotes the MoÈbius function. Let Bk
t denote the k-th Bernoulli polynomial and let Bk
t : Bk
t ÿ t denote the k-th periodic Bernoulli polynomial. De®ne X m
n x
10 : B1 U
x n n nUx
918
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
U
x is the main term of E
x, i.e.
11
E
x ÿxU
x O
xd
x;
and, as a basis of the second estimate in (5), U
x O
log2=3 x
log log x 4=3
12
is the hitherto best known estimate. The estimate of Saltykov used in Part I is erroneous and PeÂtermann [24] has con®rmed, after amending some errors in Saltykov's paper, that Saltykov's method yields only (12). Let dn denote the distance from the n-th division point n=
F
x of the unit interval to the n-th Farey point rn : d n rn ÿ
n ; F
x
n 1; 2; . . . ; F
x:
The celebrated Riemann hypothesis (RH) is equivalent in the ®rst place to one of the forms of the prime number theorem: RH , M
x O
x 1=2e ;
13
for every e > 0 (hereafter we always use e in this context). Franel's theorem [5], [18] asserts that the RH is equivalent to the mean square of dn :
14
RH ,
F
x X
dn2 O
xÿ1e :
n1
In what follows we always denote by s the complex variable with Rs s, and by m a ®xed integer V 2. De®ne X x
15 M nÿs : Ss
x n nUx Then it is well known that
16
Sÿ1
x F
x;
S0
x 1;
and that
17
RH
,
Ss
x O
x 1=2e ;
1 for some s with s V : 2
We are now in a position to state main results of the paper. P F
xÿ1 Theorem 1. As x ! y, we have for sm
x n0
cn cn1 ÿm
2 1 z 0
2 4U
x log x log x log x g ÿ O (i) s2
x z
2x 2 2 z
2 x3 x3
Farey fractions
919
2z
2 3 1 z 0
2
1 2 (ii) s3
x log x g ÿ ÿ 2z
2c2
x z
3x 3 z
2x 4 4 z
2 12U
x log x log x O x5 x5 2z
3 1 4z
2
1 8z
3c3
x (iii) s4
x z
4x 4 x 5 z
3 20 13 z 0
2
1
2 2 3z
2c2
x 3z
2z
3c2
x log x g ÿ ÿ 3z
2x 6 30 z
2 40U
x log x log x O ; x7 x7 and for m V 5 (iv) sm
x
2z
m ÿ 1 m
1 fz
m ÿ 2 2z 2
m ÿ 1cmÿ1
xg m m1 z
mx z
m ÿ 1x m
m 1 z
m ÿ 3
1
2 z
m ÿ 2cmÿ2
x z
m ÿ 1cmÿ2
x x m2 3z
m ÿ 2 35y 0 log x 1 O m3 ; 2z
2x m3 x
where U
x is de®ned by (10), g is Euler's constant, y 0 equals 0 or 1 according as m 5 or m V 6, and for s > 1 and r A N, y X m
n x
r
18 ; Br cs
x : s n n n1 which satis®es lim inf cs
r
x U
19
x!y
Br ; z
s
1
so that cs
x 2 0
1, x ! y, where Br denotes the r-th Bernoulli number. In the course of proof we shall obtain the identity j r y X mÿ2 X 2 m X j1 1; r mj1 k mÿjÿ1 j0 r2 k1
k; r1
which, combined with Lemmas 9, 11, yields a vast amount of identities. Corollary 1. We have the following evaluations ( ) y X r mÿ2 mÿ2 X X m j m j X 1 z
2m 1 2 (i) 2 mj1 k mÿjÿ1 r j1 j 1 j0 r1 k1 j0
920
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
(i)
y X mÿ2 r mÿ2 X X m j X m j 1 2 12 j 1 r1 k1 r mj1 k mÿjÿ1 j1 j0 j0
k; r1
(i)
2
mÿ3 m j X j0
j1
!
r y X X r1 k1
(
z
2m 1 2
(ii) 2
mÿ1
mÿ3 m j X j0
j1
2
!
!
j1
2
2m ÿ 1
ÿ
mÿ1
!
ÿ
2m 1
2m ÿ 2 mÿ1
!)
z
2m ÿ i ÿ 1z
i 1
1 r mÿjÿ1 k mj1
!
(
!
i1
r1 k1
2m ÿ 2
j1
2mÿ3 X
r y X X
mÿ3 m j X j0
mÿ2 m j X j0
2m ÿ 2
1 r mj1 k mÿjÿ1
z
m j 1z
m ÿ j ÿ 1 2m ÿ 2 mÿ1
2mÿ3 X
!
)
ÿ 1 z
2m
z
2m ÿ i ÿ 1z
i 1;
i1
where empty sums are understood to be 0. Remark 1. (i) is a new essential formula, of which
i is the relatively prime version and
i the reciprocal version, and so is Formula (ii), which has relatively prime and reciprocal version. Each of these has its relatively prime and reciprocal versions. E.g. the reciprocal version of
i ,
i , states that ! r y X mÿ3 m j X X 1 (i) 2 mj1 k mÿjÿ1 j 1 r1 k1 r j0
k; r1
12
mÿ2 m j X
!
j1 j0 ! X 2m ÿ 2 2mÿ3 mÿ1
ÿ
2m 1
2m ÿ 2 mÿ1
!
z
2m ÿ i ÿ 1z
i 1:
i1
Example. Let H and H denote functions in Lemma 10. Then y X r X 1 5 z
4; (i) H
3; 1 3 r k 4 r1 k1
921
Farey fractions
(ii) H
4; 2
r y X X 1 z
6 p6 2 2 ; z z
3 ÿ
3 ÿ 4k 2 2835 r 3 r1 k1
(iii) H
2; 4
r y X X r1
k1
k; r1
1 37 z 2
3 37 945z 2
3 ÿ ÿ ; r 2 k 4 12 z
6 12 p6
etc. Proof. By taking m 2 in (i) of Corollary 1, m 3 in
i of Corollary 1 and in r
i of Remark 1 we obtain the above identities.
The identities including (i) can be traced back to Nielsen's book on gamma function and are also later given by Williams (see [24] and references given there). Each of these has its relatively prime versions. E.g. H
3; 1 5=4 due to the ®rst author [14]; for (i) itself, see Matsuoka [21]. These evaluations do not seem possible to deduce from Apostol and Vu's consideration [2]. Remark 2. Those identities in Lemma 11 as well as those in Corollary 1 may be of particular interest in the light of recent investigations of Zagier [31]. For r1 ; . . . ; rl A N (l is called the depth) de®ne the multiple zeta-values z
r1 ; . . . ; rl
X
n r1 n1 >>nl >0 1
1 : nlrl
Question. Consider the numbers Zr : z
r
r A N as known. Then to what extent can one write all z
r1 ; . . . ; rl as polynomials in Z1 ; Z2 ; . . .? A partial answer has been given by himself. be the Z-span of all multiple zeta-values of weight Theorem (Zagier [31]). Let AU2 k k : r1 r2 , depth l U 2. Then AU2 k
kÿ3=2 X
Qz
2nz
k ÿ 2n
n0
kÿ1 dim 2
if 2 a k, while if 2jk, then QAU2 k
kÿ2 : QZk QZn Zkÿn space of dim 6 3UnUk=2 X
n odd
Lemma 11, (i), Example (i), (ii) are in conformity with this theorem with l 2, and k a 1, k 4, and k 6, respectively. For related topics, see Zagier [32] and Arakawa and Kaneko [1]. Corollary 2 (Maier [20]). For integers g, h V 0 de®ne sg; h sg; h
x :
F
xÿ1 X
dn g
dn1 h :
n1
922
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
Then s2; 0
s0; 2
F
xÿ1 X
dn2
n1
1 z0 log x s1; 1 log x g ÿ
2 O ; z
2x 2 x3 z and s2; 1
z
2 O
xÿ4 : 3z
3x 3
Franel's sum s2; 0 has been considered by several authors, the initiator being Franel, whose theorem (see Formula (14) above) is based on the Franel identity, which in turn has its genesis in the 3-term relation for the 2-dimensional Dedekind sums (for this and references, see [16]). Regarding power moments, we have Theorem 2. For 2 U g A N, F
x X
jdn j g W
x 1ÿg ;
n1
and on the RH, for 1 U g A R, F
x X
jdn j g O
x 2ÿ
3=2ge O
x 1ÿge :
n1
In particular, for Maier's sums with g A N, O
x 1ÿ2ge on the RH s2g; 0 1ÿ2g 2ÿ2g ; o
x unconditionally: W
x Theorem 3 (Re®nements of MikolaÂs' results). For Ra > 0, a 0 1 (i)
F
x X n1
rÿa n
z
ax a1 1 ÿ F
x
a 1z
a 1 a ÿ 1 (
1 z
aca
xx a ; Ra > 1 ÿ 0; 0 < Ra U 1; a 0 1 Oa
x maxfRaÿ1; 1g
log x y ;
where y y
a 1 or 0 according as Ra 2 or Ra 0 2, and (ii)
F
x X 1 1 z 0
2 F
x log x g ÿ ÿ O
x log 2 x r 2 z
2 n1 n x2 1 z0 log x g ÿ ÿ
2 ÿ xD
x ÿ gxU
x O
xd
x; 2z
2 2 z
923
Farey fractions
where D
x :
x x B1 log n n n
X m
n nUx
y X m
n n1
x x log O
d
x B1 n n n
O
log 2 x
trivially U
x log x O
log x 4=3
log log x 8=3 O
log x 5=3
log log x 4=3 : Although only the formula (ii) in Theorem 3 expresses the relation between the distribution of Farey points and the error term of the prime number theorem, it is possible to re®ne the formula in (i) in a similar way, with some additional e¨ects, to be carried out in detail elsewhere. On the other hand, if we extract the main term, we again get equivalent conditions to the RH in terms of negative powers of Farey fractions. Theorem 4. For s 60z
3 1 3 ÿ 3:4752 . . . ; 1 < l U l0 : z
3=2z
7=2 4 2 let f
t fl
t
1 ÿ zl
t
ÿzl
t 1; tl
where zl
t
y X n0
1
n t l
denotes the Hurwitz zeta-function, and let Ef
x
F
x X n1
f
rn ÿ F
x
1
f
t dt:
0
Then RH , Ef
x O
x
1=2e : This is a direct consequence of the modi®ed Theorem 4 of Yoshimoto [29]: Theorem 5. Let f A C 6 0; 1 satisfy (at least) one of the conditions that f
4 is of constant sign, in which case c 15=8; f
4 and f
6 are of the same constant sign, c 1; f
4 and f
6 are of opposite constant sign, c 7=8. For thus de®ned c, suppose f
924
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
satis®es the inequality j f 0
1 ÿ f 0
0j jf
3
1 ÿ f
3
0j
V
c z
3=2z
7=2 : 60 z
3
Then statement (E) of [29] holds, i.e. RH , Ef
x O
x
1=2e : Theorem 6 (Improved generalization of Hans and Dumir [10]). (i)
F
xÿ1 X n1
1 cn2 cn1
1 z0 U
x log x log x log x g 1 ÿ
2 O ; z
2x x2 x2 z (ii)
F
xÿ1 X r1
1 cn3 cn1
z
2 1 1 z0
1 2 log x g ÿ ÿ
2 2z
2c2
x z
3x 2z
2x 2 2 z U
x log x log x O ; x3 x3 (iii)
F
xÿ1 X r1
1 cn4 cn1
z
3 1
1
z
2 2z 2
3c3
x z
4x 2z
2x 2 1 7 z0
1
2 2 log x g ÿ ÿ
2 3z
2c2
x 3z
2z
3c2
x 3z
2x 3 6 z U
x log x log x O ; x4 x4
and for every integer a V 5 (iv)
F
xÿ1 X n1
1 cna cn1
z
a ÿ 1 1
1
z
a ÿ 2 2z 2
a ÿ 1caÿ1
x 2 z
ax 2z
a ÿ 1x
1
1
z
a ÿ 3 3z 2
a ÿ 2caÿ2
x 3 3z
a ÿ 2x
925
Farey fractions
2
3z
a ÿ 2z
a ÿ 1caÿ2
x y 0 log x 1 O 4 ; aÿ1
a ÿ 1z
2x x where y 0 is 1 or 0 according as a 5 or a V 6. In the course of proof we prove Lemma 11,
i , and hence (i) also. Theorem 7 (Re®nements over results of [14], which in turn are re®nements of Lehner and Newman's results [19]). (i) For non-negative reals a, b, F
xÿ1 X
b cna cn1 ca; b x ab2 ÿ
n0
p2
a b 2ca; b U
xx ab1 6 00
O
x ab1
log log x y ; where y 00 1 if 0 < b U 1=2 and 0 if either b 0 or b > 1=2, and ca; b
(ii)
F
xÿ1 X n0
6 1 G
1 aG
1 b ÿ 2 : p
1 a
1 b G
3 a b
1 12 log 2 2 log 2 1 U
x O 2 ; 2 2 cn cn1
cn cn1 p x x x
F
xÿ1 X n0
1 6 2
2 log 2 ÿ 1x
1 ÿ 2 log 2U
x O
1; cn cn1 p
and F
xÿ1 X n0
cn cn1 11 ÿ 12 log 2 3 xE
x x
11 ÿ 12 log 2 O
x 2 : 2 cn cn1 3p 6
As we deduce Corollary 1 in the course of proof of Theorem 1, we reprove Gupta's identity r y X X r1
k1
k; r1
r 2
r
1 3 ; k 4
which follows also from Apostol and Vu's consideration [2]. Indeed, de®ning 0
T
s; z
r y X X r1
k1
k; r1
1 r s k z
r
k
;
926
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
one has T 0
s; z
1 T
s; z; z
s z 1
where T
s; z is de®ned by (19) of [2]. Their Eq. (22) gives, for a 1, Gupta's identity above. Regarding Gupta's identity and generalizations thereof, we refer to an extensive work of Hata [11] which enables us to evaluate a large class of in®nite series in closed form, using Farey fractions, or rather the intervals between them. In regard to Theorem 1 we note the recent papers [6], [7] of Hall who considers the moments of length of Farey arcs. From the point of view of circle maps as well as the analogy with the di¨erence between zeros of the Riemann zeta-function on the critical line these may be of particular interest and may shed some new light. 2. Preliminaries. We collect basic lemmas some of which are of interest in their own right. Lemma 1 (Ishibashi-Kanemitsu [12], Lemmas 3 and 8). For any u A C de®ne Lu
x
X
nu
and Mu
x
X
n u log n;
nUx
nUx
where for n u e u log n with log n A R. Then for any l A N satisfying l > Ru 1 (if u A N U f0g, we take l u 1) we have 8 1 > < x u1 z
ÿu; u 0 ÿ1 u 1 (i) Lu
x > : log x g; u ÿ1 ! l X u
ÿ1 r Br
xx u1ÿr r rÿ1 r1 8 !
y > u > > <
ÿ1 l Bl
tt uÿl dt; u B N U f0g; l x > > > : 0; u A N U f0g; where the error term can also be estimated as O
xRuÿl , and (ii) Mu
x
8 1 > x u1 log x ÿ > > > > : 1 log 2 x g ; 1 2
1
u 1
2
x u1 ÿ z 0
ÿu; u 0 ÿ1
u ÿ1
927
Farey fractions
! 8 l X
ÿ1 r u > > > Br
x
log x j rÿ2
ux u1ÿr ; u B N > > r > rÿ1 > > r1 > > > > ! > u1 r rÿ1 > r1 > > > > > > > l X > u!
r ÿ u ÿ 2! > u > > Br
xx u1ÿr ; uAN
ÿ1 : r! ru2
8 > > >
ÿ1 l > >
y > > > u u!
l ÿ u ÿ 1! > :
ÿ1 Bl
tt uÿl dt; l! x
u A N U f0g;
where g1 is the ®rst generalized Euler constant de®ned by g1 lim
x!y
! 1 ÿ log 2 x ; n 2
X log n nUx
and
j rÿ2
u
8 rÿ2 X > 1 > > ; 2Ur A N > > > uÿh > h0 < 0; > > > > > > > :ÿ
r1
1 ; u1
r 0,
and the error term can be estimated as O
xRuÿl log x, respectively. Corollary. Let k A N be given. Then for any u A C and any l A N with l > Ru 1, we have Lu
x Lu; k
x
X
nu
nUx;
n; k1
8 X 1 f
k u1 > > m
d d u ; u 0 ÿ1 x z
ÿu > > > > > : f
k
log x a
k g; u ÿ1 k ! l X X u
ÿ1 r x rÿ1 u1ÿr O
xRuÿl sl
k; m
d Br d x r d rÿ1 r1 djk
928
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
where sl
n
X
d l;
djn
and a
k ÿ
X log p k X m
d k log d t
k ÿ log k; f
k djk d p ÿ 1 f
k pjn
with a
k denoting Davenport's function and t
k denoting the function in Lemma 5 below. Lemma 2 (Kanemitsu-Yoshimoto [16]). Let 0 < x U 1 and let f
t be de®ned at the points m=n
m; n 1, 1 U m U n U x. Then h
x; f :
X
rn Ux
x M
m Vx
n f
rn Vx
n; n nUx nUx X
X
where X k f Vx
n : n kUnx and denotes the Dirichlet convolution. Lemma 3 (Lemma 6 of [15]). For complex s we have X f
n log n nUx
n s1 8 1
s ÿ 1 log x 1 > > > 1ÿ ÿ sÿ1 ; s 0 1 > > x sÿ1 x <
s ÿ 1 2 z
2 > > > 1 > > log 2 x; s1 : 2z
2 8 z
sz 0
s 1 z 0
s 1 > > ÿ ; s 0 1; s > 0 ÿ > 2 > z
s 1
s ÿ 1 2 z
2 > z
s 1 > > > > < 00 0 1 z
2 1 z g
2 g ; s 1 > ÿ > 1 > > z z
2 8 z
s s2 > > > > > : 0; otherwise log x ÿs x H
x log x O : xs
Farey fractions
929
Corollary. s
x 1
H
t log t dt t s1 8 z
sz 0
s 1 z 0
s z
s s > > > ÿ ; ÿ > 2 2 > z
s 1 sz
s 1 z
s 1 >
s ÿ 1 z
2 > > > > ! > > 2 00 0 0 > 1 z
2z
2 ÿ 2z
2 z > > > g
2 g1 > > z z
2 > z
2 2 > < 1 z0 > > g ÿ 1 ÿ
2 ; > > > z
2 z > > > >
x > > > H
t > > dt; > s1 > > 1 t > > > : 0;
s > 0; s 0 1
s1 s0 s > ÿ ; s01 > > X f
n < z
s 1
s ÿ 1z
2x sÿ1 n s1 > 0 > nUx 1 z > > : log x g ÿ
2 ; s 1 z
2 z xÿs H
x O
xÿs ;
and
21
22 and
s
y
H
t z
s s ÿ dt s1 z
s 1
s ÿ 1z
2 1 t
y H
t 1 z0 g ÿ 1 ÿ
2 ; dt t2 z
2 z 1
y
x
x 1
H
t dt O
xÿs ; t s1
s>0
H
t dt O
xÿs ; t s1
s U 0:
s 0 1;
Lemma 5. De®ne the arithmetic function t
k by t
k : P and let T
x kUx t
k. Then we have as x ! y
P
djk
m
d =d
log
k=d,
930
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
x z 0
2 1 T
x ÿ D
x O
d
x log x ÿ 1 ÿ z
2 z
2 2 x z 0
2 log x ÿ 1 ÿ ÿ D
x O
1; z
2 z
2 where D
x is de®ned in Theorem 3. Proof. Rewriting the 2-dimensional sum into a double sum and noting that P f
n djn m
d
n=d, we may write
23
T
x S1 ÿ S2 ;
where S1
X f
n nUx
n
S2
log n;
X m
d log d: d ddUx
To treat S1 , we apply the re®nement of Pan Cheng Dong's (Pan Cheng Tung's) result [23] X f
n
nUx
n
log
x x O
d
x: n z
2
The left-hand side is
log x
X f
n
ÿ
X f
n
log n n n nUx x H
x ÿ S1 ; log x z
2 nUx
whence S1
x
log x ÿ 1 H
x log x O
d
x: z
2
Comparing (7) and (11), we have
24
H
x ÿU
x O
d
x;
whence
25
S1
x
log x ÿ 1 ÿ U
x log x O
d
x: z
2
On the other hand,
26
X m
d x
X m
d x
1 x ÿ ÿ B1 log d log d S2 d d d d 2 d dUx dUx X m
d x X m
d 1 X m
d log d ÿ log d: log d ÿ B1 x d2 2 dUx d d d dUx dUx
931
Farey fractions
Applying X m
d
27
dUx
d
X m
d
28
dUx
d2
log d ÿ1 O
d
x; z 0
2
d
x log d O ; x z
2 2
we conclude that
29
S2
z 0
2 z
2 2
x 1 log d O
d
x: B1 d d 2
X m
d
xÿ
dUx
Putting together, we conclude the assertion. For the sake of completeness, we give a proof of (24). Similarly to (27), (28), we have a form of the prime number theorem
30
X m
d
O
d
x;
X m
d
1 d
x O : z
2 x
dUx
31
dUx
d
d2
Hence X m
d X m
d X X m
d x 1 n d d d d ddUx dUx dUx dUx=d
X f
n nUx
ÿ
X m
d
dUx
d
ÿU
x x
x x 1 ÿ B1 d d 2
X m
d
dUx
d2
ÿ
1 X m
d 2 dUx d
x ÿ U
x O
d
x; z
2
and (24) follows.
r
As a well-known generalization of Euler's function (f
n J1
n), we introduce Jordan's totient function Jk
n
X djn
m
d
n k d
Q ( n k pjn
1 ÿ pÿk = the number of ordered sets of k positive integers such that the g.c.d. of them is relatively prime to n). Lemma 6. For complex s and k A R satisfying either (i) 2 U k < s ÿ 1 or (ii) s ÿ 1 U k U 0 it holds that
932
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
(i)
X
nÿs Jk
n
nUx
x kÿs1 z
s ÿ k
1 ck
xx kÿs
k ÿ s 1z
k 1 z
s 8 O
x 1ÿs log x; k2 > > > > > > > > < k ÿ s
2 ckÿ1
xx kÿsÿ1 O
x 1ÿs log y x; 2 < k U 3 2 > > > > > > > > : k ÿ s c
2
xx kÿsÿ1 O
x kÿ1ÿs ; 3 < k; 2 kÿ1
where y is 1 or 0 according as k 3 or not. In particular, for k V 2 x k1
1 ck
xx k Jk
n
k 1z
k 1 nUx
X
8 O
x log x; k2 > > > > > > > > < k
2 kÿ1 O
x log y x; 2 < k U 3 2 ckÿ1
xx > > > > > > > k
2 > : ckÿ1
xx kÿ1 O
x kÿ1 ; 3 < k: 2 (ii)
X
nÿs Jk
n O
x 1ÿs :
nUx
The special case of (i) gives an improvement of Jarden's formula [13]. Of course, in other cases, we can obtain asymptotic formulas. The case of s 1 reduces to Lemma 4. If e.g. 0 < s ÿ 1 U k < 1, then
X nUx
nÿs Jk
n
8 x kÿs1 z
s ÿ k > > > ; k ÿ s 0 ÿ1 > > z
s <
k ÿ s 1z
k 1 > > > 1 z 0
s > >
log x g ÿ 2 ; : z
s z
s
k ÿ s ÿ1
O
x 1ÿs : Lemma 7. For a, b A R, let S
a; b
x
y X r>x
Then for a > 1,
r
ÿa
r X
k1
k; r1
k ÿb :
933
Farey fractions
S
a; 1
x
32
y X
rÿa
r>x
r X 1 k k1
k; r1
1 1 z0 log x g ÿ
2
a ÿ 1z
2x aÿ1 aÿ1 z U
x log x a log x O ; x xa and for a > 1, b V 2
33
S
a;b
z
b 1 a
1
x z
bcb
x ÿ
a ÿ 1z
b 1x aÿ1 x a az
2 ! b 1ÿa
b ÿ 2b log x
2 O a2ÿa ; a1 az
bcbÿ1
x ÿ 2x
a 1z
2 x
where a 2=a and b 3=b. Proof. Since S
a; b
x
X
rÿa Lÿb
r
r>x
we substitute from Corollary to Lemma 1 to get 8 X t
r X f
r > > > g ; b1 > > r a1 < r>x r a r>x S
a; b
x > X > 1 X f
r > ÿaÿb > r J
r ÿ ; b01 z
b > b : b ÿ 1 r>x r ab r>x O
X s1
r r>x
r ab
!
:
Applying Lemmas 4±6 as well as Corollary to Lemma 3 to respective sums and the P 2 r trivial estimate nUx s1
n O
x completes the proof. Lemma 8. For 0 U j A Z let
m j Aj
x 2 j1
Then for m V 2 (i) sm
x 1 ÿ
mÿ2 X j0
Aj
x;
X x X r r2
k1
k; r1
1 r mj1 k mÿjÿ1
:
934
S. Kanemitsu, T. Kuzumaki and M. Yoshimoto
and (ii)
m j lim Aj
x 2 x!y j1
X y X r r2
1
k1
k; r1
r mj1 k mÿjÿ1
:
Proof. We apply Formula (2) with f
x; y
xyÿm to get mÿ1 X0 X m 1 0 sm
x 1 ÿ j 1 ÿ sm
x; m mÿj j r k
r ÿ k j1 P0 stands for the double sum extended over 2 U r U x, 1 U k U r with say, where
k; r 1. Now, putting for 0 U i U n ÿ 2, mi mÿiÿ1 X0 X ji ; Ci
x mi mÿjÿi k
r ÿ k j j1 r we see that Ci
x Ai
x Ci1
x: Since sm0
x C0
x and Cmÿ2
x Amÿ2
x, it follows from this that sm0
x
mÿ2 X
Aj
x;
j0
thereby proving our assertion.
r
Lemma 9 (Relatively prime version). Suppose f
tx; ty t a f
x; y for a < ÿ1. Then r y X X
f
k; r z
ÿa
r y X X r1
r1 k1
f
k; r;
k1
k; r1
the series converging simultaneously. Lemma 10 (Reciprocity relation). For s > maxf1; 2 ÿ Rzg, let H
s; z
y X
rÿs
r1
r X
k ÿz :
k1
Then (i) H
s; z H
z; s z
sz
z z
s z: Similarly, de®ning
H
s; z
y X r1
r
ÿs
r X
k1
k; r1
k ÿz
1 H
s; z z
s z
H satis®es
i with the right-hand side divided by z
s z.
Farey fractions
935
Lemma 11. Let a V 2 be an integer. Then y r aÿ2 X X 1X 1 z
a ÿ iz
i 1;
a 2z
a 1 ÿ (i) 2 r a k1 k r1 i1
or equivalently (i)
r aÿ2 y X X 1 X 1 1 a2ÿ z
a ÿ iz
i 1: 2 r a k1 k z
a 1 i1 r1
k; r1
For Lemmas 9, 10, 11 see Sita Rama Chandra Rao and Siva Rama Sarma [26], [27] and references thereof. The following Lemmas 12±14 are needed solely for the proof of the estimate for D
x in Theorem 3, (ii). Lemma 12 (Lemma 2, [15]). Let fan gy n1 be a complex sequence such that an K O
log n , K > 0 and suppose that X an O
xd
x: nUx
Then 2 x an O
xd
x n nUx X uniformly in x. Lemma 13. Let
1 1=3 ÿ4=3
log x
log log x : X 80000 Then for any Q, Q 0 satisfying Q U Q 0 U 2Q;
x 6=X U Q U Q 0 U x exp
ÿ
log x 1=2 ;
we have 0
Q X
x m
mc O
Q
log xÿ1 : m mQ This follows immediately from Wal®sz [28], Lemma 4.5.4. Lemma 14. For any a > 0 and an arithmetical function f
n we have X X X x f
n x x m
n f
n m
n M ÿ
34 x f n n m m ax
1 O r
x 1 ÿ r rUx log x ; O x X
F
xÿ1 X
cna cn1
n0
!
log x O ; x
and hence that F
xÿ1 X n0
cna cn1
aÿ1 X X 1 Liÿa
r: i1 r i1 r>x
Substituting from Lemma 7 completes the proof.
r
The proof of Theorem 7 rests on Lehner-Newman's second sum formula (only the ®rst formula in (ii) rests on the ®rst sum formula) and similar reasonings in this paper with frequent use of Corollary to Lemma 1. We shall not, however, give a proof of Theorem 7 as it requires another series of lemmas. We shall publish it as well as detailed proofs of (generalizations of ) some lemmas in §2 elsewhere. References [ 1 ] T. Arakawa and M. Kaneko, Multiple zeta values, poly-Bernoulli numbers, and related zeta functions, to appear. [ 2 ] T. M. Apostol and T. H. Vu, Dirichlet series related to the Riemann zeta function, J. Number Theory, 19 (1984), 85±102. [ 3 ] S. Chowla, Contributions to the analytic theory of numbers, Math. Z., 35 (1932), 279±299. [ 4 ] P. CvitanovicÂ, Circle maps: irrationally winding, From Number Theory to Physics, ed. by Waldschmidt et al., Springer Verlag 1992, 631±658. [ 5 ] J. Franel, Les suites de Farey et les probleÁms des nombres premiers, Nachr. Ges. Wiss. GoÈttingen, Math.-Phys. Kl. (1924), 198±201.
947
Farey fractions
[ 6 ] R. R. Hall, A note on Farey series, J. London Math. Soc. (2), 2 (1970), 139±148. [ 7 ] R. R. Hall, On consecutive Farey arcs, Acta Arith., 66 (1994), 1±9. [ 8 ] R. R. Hall, Franel integrals, Sieve Methods, Exponential Sums, and their Applications in Number Theory, ed. by G. R. H. Greaves, G. Harman and M. N. Huxley, Cambridge UP. 1997, 143±159. [ 9 ] R. R. Hall and G. Tenenbaum, On consecutive Farey series, Acta Arith., 44 (1984), 397±405. [10] R. J. Hans and V. C. Dumir, An interesting identity, Res. Bull. Panjab Univ. (N.S), 15 (1964/65), 353±356. [11] M. Hata, Farey fractions and sums over coprime pairs, Acta Arith., 70 (1995), 149±159. [12] M. Ishibashi and S. Kanemitsu, Fractional part sums and divisor functions I, Number Theory and Combinatorics, ed. by J. Akiyama et al., World Sci. 1985, 119±183. [13] M. Jarden, Roots of unity over large algebraic ®elds, Math. Ann., 213 (1975), 109±127. [14] S. Kanemitsu, On some sums involving Farey fractions, Math. J. Okayama Univ., 20 (1978), 101± 113. [15] S. Kanemitsu, R. Sita Rama Chandra Rao and A. Siva Rama Sarma, Some sums involving Farey fractions I, J. Math. Soc. Japan, 34 (1982), 125±142. [16] S. Kanemitsu and M. Yoshimoto, Farey series and the Riemann hypothesis, Acta Arith., 75 (1996), 351±374. [17] P. Kargaev and A. Zhigljavsky, Asymptotic distribution of the distance function to the Farey points, J. Number Theory, 65 (1997), 130±149. [18] E. Landau, Vorlesungen uÈber Zahlentheorie, 2nd ed. Chelsea 1969. [19] J. Lehner and M. Newman, Sums involving Farey fractions, Acta Arith., 15 (1968/69), 181±187. È sterreich. Akad. Wiss. Math. -Natur. Kl. Sit[20] W. Maier, Fareysche Folgen und Sektorengitter, O zungsber. II, 191 (1982), 141±156. [21] Y. Matsuoka, On the values of a certain Dirichlet series at rational integers, Tokyo J. Math., 5 (1982), 389±403. [22] M. MikolaÂs, Farey series and their connection with the prime number problem I, II, Acta Univ. Szeged. Sect. Sci. Math., 13 (1949), 93±117; 14 (1951/52), 5±21. [23] Pan Cheng-Tung, On s
n and f
n, Bull. Acad. Polon. Sci. Cl. III, 4 (1956), 637±638; Acta Sci. Natur. Univ. Pekinensis, No. 3 (1956), 302±322 (Chinese). [24] Y. -F. S. PeÂtermann, Private communication to the ®rst author, May 20, 1996. [25] S. S. Pillai and S. D. Chowla, On the error terms in some asymptotic formulae in the theory of numbers (I), J. London Math. Soc., 5 (1930), 95±101. [26] R. Sita Rama Chandra Rao and A. Siva Rama Sarma, Some identities involving the Riemann zeta function, Indian J. Pure Appl. Math., 10 (1979), 602±607. [27] R. Sita Rama Chandra Rao and A. Siva Rama Sarma, Two identities due to Ramanujan, ibid., 11 (1980), 1139±1140. [28] A. Wal®sz, Weylsche Exponentialsummen in der neueren Zahlentheorie, VEB Deutscher Verlag der Wissenschaften, Berlin, 1963. [29] M. Yoshimoto, Farey series and the Riemann hypothesis II, Acta Math. Hung., 78 (1998), 287±304. [30] M. Yoshimoto, Farey series and the Riemann hypothesis VI, (in preparation). [31] D. Zagier, Talk at Prof. Yoshida's seminar at Kyushu Univ., Apr. 1992. [32] D. Zagier, Values of zeta functions and applications, Progress in Math., 120 (1994), 497±512.
Shigeru Kanemitsu
Takako Kuzumaki
Department of Electrical Engineering University of Kinki, Iizuka Fukuoka 820-8555, Japan
Department of Electrical Engineering Faculty of Engineering Gifu University Gifu City 501-1193, Japan
Masami Yoshimoto Graduate School of Mathematics Kyushu University Fukuoka 812-8581, Japan