article03. 225KB Jun 04 2011 12:06:50 AM

Journal de Th´eorie des Nombres
de Bordeaux 19 (2007), 583–594

A generalization of Scholz’s reciprocity law
par Mark BUDDEN, Jeremiah EISENMENGER et Jonathan
KISH
´sume
´. Nous donnons une g´en´eralisation de la loi de r´eciprocit´e
Re
de Scholz fond´ee sur les sous-corps K2t−1 et K2t de Q(ζp ) de degr´es
2t−1 et 2t sur Q, respectivement. La d´emonstration utilise un
choix particulier d’´el´ement primitif pour K2t sur K2t−1 et est bas´ee
sur la division du polynˆome cyclotomique Φp (x) sur les sous-corps.
Abstract. We provide a generalization of Scholz’s reciprocity
law using the subfields K2t−1 and K2t of Q(ζp ), of degrees 2t−1
and 2t over Q, respectively. The proof requires a particular choice
of primitive element for K2t over K2t−1 and is based upon the
splitting of the cyclotomic polynomial Φp (x) over the subfields.

1. Introduction
In 1934, Scholz [12] proved a rational quartic reciprocity law via class

field theory. While the law still bears Scholz’s name, it was recently noted
by Lemmermeyer (see the notes at the end of Chapter 5 in [11]) that it
had been proved much earlier in 1839 by Sch¨
onemann [13]. Since then,
Scholz’s reciprocity law has been proved using many different methods (see
[3], [7], [10], and [14] for other proofs). The unfamiliar reader is referred
to Emma Lehmer’s expository article [9] for an overview of rational reciprocity laws and Williams, Hardy, and Friesen’s article [15] for a proof of
an all-encompassing rational quartic reciprocity law that was subsequently
simplified by Evans [4] and Lemmermeyer [10].
We begin by stating Scholz’s reciprocity law and an octic version of the
law proved by Buell and Williams √
[2]. We will need the following notations.
For a quadratic field extension Q( d) of Q, with squarefree positive d ∈ Z,
let εd denote the fundamental
unit and h(d) denote the class number. The

·
standard notation · will be used to denote the Legendre symbol. We will
also need to define the rational power residue symbol. Assume that a is an
integer such that (a, p) = 1 that satisfies

a
Manuscrit re¸cu le 21 juillet 2006.

p−1
n

≡1

(mod p)

584

Mark Budden, Jeremiah Eisenmenger, Jonathan Kish

for a rational prime p and a positive integer n. Then define the rational
symbol
 
p−1
a
≡ a 2n (mod p).

p 2n
 
This symbol takes on the same values as ap
, the 2nth power residue
Q(ζ2n )

symbol where p is any prime above p in Q(ζ2n ). For our purposes, n
will usually be a power of 2. It should also be noted that the Legendre
symbol is equivalent to our
 rational power residue symbol when n = 1. By
a
convention, we define p = 1 for all a such that (a, p) = 1.
1

Theorem 1.1 (Scholz’s Reciprocity
  Law).
  Let p ≡ q ≡ 1 (mod 4) be
p
distinct rational primes such that q = pq = 1. Then
   

   
εp
εq
q
p
=
=
.
q 4 p 4
q
p

In [1], Buell and Williams conjectured, and in [2] they proved, an octic reciprocity law of Scholz-type which we refer to below as Buell and
Williams’ reciprocity law. Although their law is more complicated to state,
it does provide insight into the potential formulation of a general rational
reciprocity law of Scholz-type.
Theorem 1.2 (Buell and Williams’ Reciprocity
  Law).
  Let p ≡ q ≡ 1
p

(mod 8) be distinct rational primes such that q = pq = 1. Then
4
4
    
εq
   
 εp
if N (εpq ) = −1
q
p
q 4 p 4
   
=
εq
q 8 p 8  (−1)h(pq)/4 εp
if N (εpq ) = 1
q

4


p

4


where N is the norm map for the extension Q( pq) over Q.

Buell and Williams succeed in providing a rational octic reciprocity law
involving the fundamental units of quadratic fields, but it loses some of
the simplicity of the statement of Scholz’s reciprocity law and requires the
introduction of class numbers. It seems more natural to use units from the
unique quartic subfield of Q(ζp ) when constructing such an octic law. This
was our motivation in the formulation of a general rational reciprocity law
similar to that of Scholz.
In Section 2, we describe a primitive element for the unique subfield
  K 2t
t
t
of Q(ζp ) satisfying [K2t : Q] = 2 , when p ≡ 1 (mod 2 ) and p2 t−2 =
2

1. Our choice of a primitive element involves a specific choice of a unit
×
. Section 3 provides the proof of a generalization of Scholz’s
η2t ∈ OK
2t−1
reciprocity law after giving a thorough description of the rational residue

Generalization of Scholz’s law

585

symbols used in the theorem. We show that whenever p ≡ q ≡ 1 (mod 2t )
are distinct primes with t ≥ 2 and
 
 
 
q
2
p
=

=
= 1,
q 2t−1
p 2t−1
p 2t−2

then

where β2t =

t
Q

k=2

   


q
β2t

p
=
q 2 t p 2t
λ 2t−1
k−2

η22k

×
∈ OK

2t−1

and λ ∈ OK2t−1 is any prime above q.

Our proof is based upon the splitting of the cyclotomic polynomial Φp (x)
over the fields
 in question. In the special case where t = 2, we note that
εp
η4 

λ =
q , resulting in the statement of Scholz’s reciprocity law.
Since our rational reciprocity law takes on a simpler octic form than Buell
and Williams’ reciprocity law, comparing the two results in an interesting
corollary. It is observed that if p ≡ q ≡ 1 (mod 8) are distinct primes
satisfying
 
 
q
p
=
= 1,
q 4
p 4
then
η  ε 
q
8
=
(−N (εpq ))h(pq)/4 ,

λ
p 4
where λ ∈ OK4 is any prime above q.
Acknowledgements The work contained here was partially supported by
two internal grants from Armstrong Atlantic State University. The authors
would like to thank Sungkon Chang for carefully reading a preliminary draft
of this manuscript and providing comments which cleaned up some of our
arguments and fixed an oversight in Section 3. Thanks are also due to the
referee for several comments that improved the exposition.
2. Subfields of Q(ζp)
When p is an odd rational prime,√it is well-known that the unique quadratic subfield of Q(ζp ) is K2 = Q( p∗ ) where p∗ = (−1)(p−1)/2 p. In this
section, we provide a useful description of 
thesubfield K2t of Q(ζp ) of degree 2t over Q when p ≡ 1 (mod 2t ) and

2
p 2t−2

= 1. We will need the

following variant of Gauss’s Lemma that is due to Emma Lehmer (see [8]
or Proposition 5.10 of [11]) which we state without proof.
 
Lemma 2.1. Let ℓ and q = 2mn + 1 be rational primes such that qℓ
=1
n
and let
A = {α1 , α2 , . . . , αm }

Mark Budden, Jeremiah Eisenmenger, Jonathan Kish

586

be a half-system of nth power residues. Then
ℓαj ≡ (−1)a(j) απ(j)

(mod q)

for some permutation π of {1, 2, . . . , m} and
 
m
X

µ
= (−1)
where µ =
a(i).
q 2n
i=1

 should be noted that Lemma 2.1 can be applied to the evaluation of
 It

q 2n for all 1 ≤ ℓ < q by using Dirichlet’s theorem on arithmetic progressions and the observation that the rational residue symbol is well-defined
on congruence classes modulo q. The statement of Scholz’s Reciprocity
Law utilizes the fundamental unit of K2 . Our general rational reciprocity
law will similarly require the units described in the following theorem.
t
Theorem
  2.2. Let p ≡ 1 (mod 2 ) be
that p2 t−2 = 1 and set
2

p−1
A2 t = 1 ≤ a ≤
2

and

B2t


p−1
= 1≤b≤
2

Then the element

a rational prime with t ≥ 2 such
 

a

p t−1 = 1
2

 
 

b
b

= −1 .
p t−2 = 1 and
p 2t−1
2

η2t =
is a unit in OK2t−1 .

Q 



b∈B2t

b − ζ −b
ζ2p
2p

a∈A2t

a − ζ −a
ζ2p
2p

Q 



Proof. Let p ≡ 1 (mod 2t ) be a prime such that

 

2
p 2t−2

= 1 (ie., 2 ∈

A2t ∪B2t ) and suppose that η2t is defined as in the statement of the theorem.
We begin by noting that ζ2p ∈ Q(ζp ). This is easily checked by observing
that Q(ζp ) ⊆ Q(ζ2p ) and that both fields have degree p − 1 over Q. One
can check that η2t ∈ Z[ζp ]× by computing the norm of η2t in Q(ζp ) and
noting that A2t and B2t have the same cardinality. Next, we show that
η2t ∈ OK2t−1 . To do this, we define the element

Q
ζpb − ζp−b
ηe2t =

b∈B2t

Q

a∈A2t

ζpa − ζp−a

.

Generalization of Scholz’s law

If

 

587

2
p 2t−1

ηe2t =

= 1, then 2a ≡ ±a′ (mod p), 2b ≡ ±b′ (mod p), and



Q  b′
Q  2b
Q
−b′
−2b
ζ2p − ζ2p
ζ2p − ζ2p
ζpb − ζp−b

b∈B2t

Q

a∈A2t

ζpa −

=

ζp−a

b∈B2t

Q 

a∈A2t

2a − ζ −2a
ζ2p
2p

=

 

b′ ∈B2t

Q 

a′ ∈A2t

a − ζ −a
ζ2p
2p




 = η2t .

Applying a similar argument to the case p2 t−1 = −1, we have that
2

η2t if 2 ∈ A2t
ηe2t =
η2−1
if 2 ∈ B2t .
t

Next, we show that ηe2t ∈ K2t−1 by showing that it is fixed under all aut−1
tomorphisms σr ∈ Gal(Q(ζp )/Q) with r ∈ (Z/pZ)×2 . For such residues,


we have ra ≡ ±a (mod p) and rb ≡ ±b (mod p), which gives


Q  b′
Q

ζp − ζp−b
ζprb − ζp−rb
σr (e
η2t ) =

b∈B2t

Q

a∈A2t

ζpra −

ζp−ra

 = (−1)µB2t +µA2t

b′ ∈B2t

Q 

a′ ∈A2t

ζpa′ − ζp−a



,

where µA2t (respectively, µB2t ) counts the number of negatives resulting
from ra ≡ −a′ (mod p) (respectively, rb ≡ −b′ (mod p)). By Lemma 2.1,
it follows that
 
r
σr (e
η2t ) =
ηe t .
p 2t 2
Thus, we see that ηe2t ∈ K2t−1 ∩ Z[ζp ] = OK t−1 . Similarly, it can be shown
2

that ηe2−1
t ∈ K2t−1 ∩ Z[ζp ] = OK t−1 and we conclude that
2

η

2t

, η2−1
t

∈ K2t−1 ∩ Z[ζp ] = OK t−1 ,
2

resulting in the claim of the theorem.



The description of η4 and the fact that
q


K4 = Q
η4 (−1)(p−1)/4 p

when p ≡ 1 (mod 4) was shown in Proposition 5.9 and the discussion in
Section 3.4 of Lemmermeyer’s book [11], where it was subsequently used to
prove Scholz’s Reciprocity Law. The following theorem includes a proof of
this claim along with its extension to describe the subfield K2t when t ≥ 3.
 
Theorem 2.3. If p ≡ 1 (mod 2t ) is prime with t ≥ 2 and p2 t−2 = 1,
2

then K2t = Q(α2t ), where

1/2 1/4

1/2t−1

α2t = η2t η2t−1 · · · η4

(−1)(p−1)/2

t+1

p(2

t−1 −1)/2t

Mark Budden, Jeremiah Eisenmenger, Jonathan Kish

588

and K2t is the unique subfield of Q(ζp ) satisfying [K2t : Q] = 2t .
Proof. We begin with the cases t = 2, 3 then proceed by induction on t.
Define


Y 
Y 
−a
−b
a
b
ζ2p
− ζ2p
ζ2p
− ζ2p
and
R 2t =
N 2t =
a∈A2t

b∈B2t

so that η2t =
and

N 2t
R 2t

for all t ≥ 2. First consider the case when p ≡ 1 (mod 4)

N42 R42

Y

=

b
(ζ2p

b∈B4

=

p−1
Y

k=1



!2

−k
k
(ζ2p
− ζ2p
)=
(p−1)/2

= (−1)

Y

−b
ζ2p
)

p−1
Y

k=1

a
(ζ2p

a∈A4



!2

−a
ζ2p
)

k
ζ2p
(1 − ζp−k )

NQ(ζp )/Q (1 − ζp ) = p.

Then the sign of N4 R4 is (−1)(p−1)/4 resulting in

N4 R4 = (−1)(p−1)/4 p1/2 .
Substituting N4 η4−1 = R4 , we have
N42 = η4 (−1)(p−1)/4 p1/2

=⇒

1/2

N4 = η4 (−1)(p−1)/8 p1/4 .

Since N4 6∈ K2 , but N4 ∈ Q(ζp ), and using the fact that Q(ζp ) is a cyclic
extension of Q, we see that K4 = K2 (N4 ) = Q(N4 ).
 Now
 for the t = 3 case
2
we assume p ≡ 1 (mod 8), in which case we have p = 1. Then

and

N42 R42 = N42 N82 R82 = p,

−1
N82 R82 = η4 (−1)(p−1)/4 p1/2
p = η4−1 (−1)(p−1)/4 p1/2 ,
−1/2

N8 R8 = η4
Using η8 =

N8
R8 ,

(−1)(p−1)/8 p1/4 .

we have
−1/2

N82 = η8 η4

(−1)(p−1)/8 p1/4 ,

and
1/2 −1/4

N8 = η8 η4

(−1)(p−1)/16 p1/8 .

We handle the remaining
cases by induction on t ≥ 3. Suppose that for
 
2
k
k > 3, p ≡ 1 (mod 2 ), p k−2 = 1, and
2

1/2

−1/4

−1/2k−2

N2k−1 = η2k−1 η2k−2 · · · η4

k

(−1)(p−1)/2 p1/2

k−1

Generalization of Scholz’s law

is a primitive element for K2k−1 . Using η2k−1 =
R2k−1 = N2k R2k =

N22k η2−1
k ,

589

N2k−1
R2k−1 ,

η2k =

N 2k
R 2k ,

and

we have

N22k = η2k R2k−1 = η2k N2k−1 η2−1
k−1 ,
−1/2k−2

−1/2

N22k = η2k η2k−1 · · · η4

k

(−1)(p−1)/2 p1/2

k−1

,

and
−1/2k−1

1/2 −1/4

N2k = η2k η2k−1 · · · η4

(−1)(p−1)/2

k+1

k

p1/2 .

Again applying the fact that Gal (Q(ζp )/Q) is cyclic we have that
K2k = K2k−1 (N2k ) = Q(N2k )
is the unique subfield of Q(ζp ) with [K2k : Q] = 2k . For our purposes, we
will need the following description of K2t . Note that the element
α2t =

t
Y

N 2j

j=2

is also a primitive element for K2t over K2t−1 and a simple inductive argument shows that
1/2 1/4

1/2t−1

α2t = η2t η2t−1 · · · η4

(−1)(p−1)/2

t+1

p(2

t−1 −1)/2t

for all t ≥ 2.


3. Generalized Scholz-type reciprocity law

Before describing the main result, we need to explain the meaning of the

×
, and
symbol λη 2t whenever p ≡ q ≡ 1 (mod 2t ), pq t−1 = 1, η ∈ OK
2t−1
2
λ ∈ OK2t−1 is any prime above q. In this case, q splits completely in OK2t−1
and we have
OK2t−1 /λOK2t−1 ∼
= Z/qZ.
Recall that if γ, δ ∈ OK2t−1 , we write
γ≡δ

(mod λ)

if and only if λ divides γ − δ (see Chapter 9, Section 2 of [5]). While this
definition makes sense for γ and δ in the ring of integers of integers of any
extension field of K2t−1 , every element of OK2t−1 can be identified with a
unique element from the set
{0, 1, . . . , q − 1}
since its elements are incongruent modulo λ and may therefore be used as
coset representatives in OK2t−1 /λOK2t−1 .

590

Mark Budden, Jeremiah Eisenmenger, Jonathan Kish

Let aλ ∈ {0, 1, . . . , q − 1} be the unique element (which depends upon
the choice of λ) such that
Whenever we have

η ≡ aλ
(q−1)/2t−1



(mod λ).
≡1

(mod q),

then one can define
 
η

(q−1)/2t
:=
(mod q).
≡ aλ
λ 2t
q 2t


Of course, the symbol λη 2t is only defined when λη 2t−1 = 1. This symbol
is well-defined, but we must not forget its dependence on λ.
Next, we state our rational reciprocity law using the rational symbols
defined above. The proof of the reciprocity law depends upon the splitting
of the cyclotomic polynomial Φp (x) over the subfields K2t−1 and K2t and
is modelled after the proof of quadratic reciprocity given after Proposition
3.4 in Lemmermeyer’s book [11].
Theorem 3.1. If p ≡ q ≡ 1 (mod 2t ) are distinct odd primes with t ≥ 2
and
 
 
 
q
2
p
=
=
= 1,
q 2t−1
p 2t−1
p 2t−2
then
   


p
q
β2t
=
q 2 t p 2t
λ 2t−1
t
Q 2k−2
×
η2k ∈ OK
and λ ∈ OK2t−1 is any prime above q.
where β2t =
t−1
2

k=2

Proof. Let p and q be primes satisfying the hypotheses of Theorem 3.1.
The minimal polynomial of ζp over K2t−1 is given by
Y
(x − ζpr ) ∈ OK2t−1 [x],
ϕ(x) =
r∈R2t−1

where

 

r
=1 .
R2t−1 = 1 ≤ r ≤ p − 1
p 2t−1
Factoring ϕ(x) over OK2t , we obtain ϕ(x) = ψ1 (x)ψ2 (x) where
Y
Y
(x − ζpn ),
(x − ζpr ) and ψ2 (x) =
ψ1 (x)


r∈R2t

n∈N2t

R2t is defined analogously to R2t−1 , and N2t = R2t−1 − R2t . Also define
the polynomial
ϑ(x) = ψ1 (x) − ψ2 (x) ∈ OK2t [x].

Generalization of Scholz’s law

591

Let σ denote the nontrivial automorphism in Gal(K2t /K2t−1 ), and note
that σ = σm |K2t where
σm ∈ Gal(Q(ζp )/K2t−1 ) ⊂ Gal(Q(ζp )/Q)
is the automorphism σm (ζp ) = ζpm with m ∈ N2t . It follows that
σ(ϑ(x)) = −ϑ(x)
and since K2t = K2t−1 (α2t ), we have
σ(α2t ϑ(x)) = α2t ϑ(x) ∈ OK2t−1 [x].
Thus, it is possible to write ϑ(x) = α2t φ(x) for some φ(x) ∈ OK2t−1 [x].
Following the discussion before Theorem 3.1, let λ denote any prime above
q in OK2t−1 . Consider the congruence
 
q
q
q
ϑ(xq ) (mod λ),
(3.1)
(ϑ(x)) = (ψ1 (x) − ψ2 (x)) ≡
p 2t
which is actually defined on the ring OK2t . On the other hand, we have
(ϑ(x))q ≡ α2q t (φ(x))q

(mod λ).

By an analogue of Fermat’s little theorem, whenever κ ∈ OK2t−1 ,
κq ≡ κN (λ)−1 κ ≡ κ

(mod λ),

where the norm map N is the norm of the field extension K2t−1 over Q.
Since φ(x) ∈ OK2t−1 [x], we have
(3.2)

q
(ϑ(x))q ≡ α2q−1
(mod λ)
t α2t φ(x )
t

t

≡ (α22t )(q−1)/2 ϑ(xq ) (mod λ).

Comparing (3.1) and (3.2) gives
 
q
t
t
(3.3)
ϑ(xq ) ≡ (α22t )(q−1)/2 ϑ(xq ) (mod λ).
p 2t
Next, we show that
ϑ(X) = ψ1 (X) − ψ2 (X) 6≡ 0

(mod λ).

By Kummer’s Theorem ([6], Theorem 7.4), the ideal generated by q in Z[ζp ]
decomposes in exactly the same way as Φp (X) decomposes in (Z/qZ)[X].
Since p and q are distinct primes, the ideal generated by q in Z[ζp ] is
unramified. If
ϕ(X) ≡ (ψ1 (X))2

(mod λ),

592

Mark Budden, Jeremiah Eisenmenger, Jonathan Kish

then we can pick {0, 1, . . . q −1} as coset representatives of OK2t−1 /λOK2t−1

= Z/qZ to obtain a square factor of Φp (X) in (Z/qZ)[X], contradicting the
observation that q does not ramify in Z[ζp ]. Thus, (3.3) simplifies to
 
q
t
t
≡ (α22t )(q−1)/2 (mod λ),
(3.4)
p 2t
and we note that α2t ∈ OK2t−1 , which can therefore be identified with an
element in {0, 1, . . . , q − 1}. The proof is completed by induction on t ≥ 2.
If t = 2, we have
 
 2 
q
η4 p
4 (q−1)/4
≡ (α4 )

(mod λ).
p 4
λ 4
Both residue symbols only take on the values ±1 so that we have
 2 
 
η  p
η   p 
η4 p
q
4
4
=
=
=
p 4
λ 4
λ 2 λ 4
λ 2 q 4

since λp 4 is independent of the choice of λ. Now suppose that the theorem
holds for t = k − 1 ≥ 2, p ≡ q ≡ 1 (mod 2k ), and
 
 
 
q
2
p
=
=
= 1.
q 2k−1
p 2k−1
p 2k−2
In particular, we have
 


 
q
β2k−1
p
=
= 1.
q 2k−1 p 2k−1
λ
2k−2
Then (3.4) gives
!
 


p
β22k p
q
β2k
2k (q−1)/2k
(mod λ).


≡ (α2k )
p 2k
λ
λ 2k−1 λ 2k
k
2
p
Again, the value of λ 2k is independent of the choice of λ and all of the
residue symbols only take on the values ±1, resulting in


   
p
q
β2k
=
.
q 2k p 2k
λ 2k−1
Finally, it should be noted that the symbol
!


k−2
 η k   β k−1 
η22k β2k−1
β2k
2
=
= 2
λ 2k−1
λ
λ
λ
2k−1
k−1
2

is defined by the inductive hypothesis, completing the proof of the theorem.


Generalization of Scholz’s law

593

Theorem 3.1 holds regardless of the choice of prime λ above q. Noting
that the left-hand side of the law is independent of λ, we see that the
residuacity of β2t only depends upon the prime q. Hence, we may write




β2t
β2t
=
,
q 2t−1
λ 2t−1

allowing us to interpret our law as a true rational reciprocity law.
When p ≡ 1 (mod 4), it is known that η4 = εhp for an odd integer h, and
a proof can be found in Proposition 3.24 of [11]. In particular, if
   
p
q
=
= 1,
q
p
then
     
εp
η4
β4
=
=
,
λ
λ
q
so that Theorem 3.1 results in Scholz’s reciprocity law. The octic case of
Theorem 3.1 states that if p ≡ 1 (mod 8) and
 
 
p
q
=
= 1,
q 4
p 4

then

 
   
η  η 
q
β8
p
4
8
.
=
=
q 8 p 8
λ 4
λ
λ 4
The separation of the last residue symbol is justified since η4 is a quadratic
residue by Scholz’s reciprocity law. Our law takes on a simpler form than
that of Buell and Williams and comparing the two octic laws results in the
following corollary.
Corollary 3.2. If p ≡ q ≡ 1 (mod 8) are distinct primes satisfying
 
 
p
q
=
= 1,
q 4
p 4

then


εq
=
(−N (εpq ))h(pq)/4 ,
λ
p 4
is any prime above q.
η 
8

where λ ∈ OK4



In conclusion, we note that Lemmermeyer commented at the end of [10]
that he had “generalized Scholz’s reciprocity law to all number fields with
odd class number in the strict sense.” Lemmermeyer’s generalization has
not been published, but has appeared in his online notes on class field towers. His generalization is quite different from ours and does not lend itself
to an easy comparison. Despite the differences in the two generalizations,
all of the work contained here was motivated by the techniques used by
Lemmermeyer [11] leading up to his proof of Scholz’s Reciprocity Law.

Mark Budden, Jeremiah Eisenmenger, Jonathan Kish

594

References
[1] D. Buell and K. Williams, Is There an Octic Reciprocity Law of Scholz Type?. Amer.
Math. Monthly 85 (1978), 483–484.
[2] D. Buell and K. Williams, An Octic Reciprocity Law of Scholz Type. Proc. Amer. Math.
Soc. 77 (1979), 315–318.
[3] D. Estes and G. Pall, Spinor Genera of Binary Quadratic Forms. J. Number Theory 5
(1973), 421–432.
[4] R. Evans, Residuacity of Primes. Rocky Mountain J. of Math. 19 (1989), 1069–1081.
[5] K. Ireland and M. Rosen, A Classical Introduction to Modern Number Theory. 2nd edition, Graduate Texts in Mathematics 84, Springer-Verlag, 1990.
[6] G. Janusz, Algebraic Number Fields. 2nd ed., Graduate Studies in Mathematics 7, American
Mathematical Society, Providence, RI, 1996.
[7] E. Lehmer, On the Quadratic Character of some Quadratic Surds. J. Reine Angew. Math.
250 (1971), 42–48.
[8] E. Lehmer, Generalizations of Gauss’ Lemma. Number Theory and Algebra, Academic
Press, New York, 1977, 187–194.
[9] E. Lehmer, Rational Reciprocity Laws. Amer. Math. Monthly 85 (1978), 467–472.
[10] F. Lemmermeyer, Rational Quartic Reciprocity. Acta Arith. 67 (1994), 387–390.
[11] F. Lemmermeyer, Reciprocity Laws. Springer Monographs in Mathematics, SpringerVerlag, Berlin, 2000.
¨
[12] A. Scholz, Uber
die L¨
osbarkeit der Gleichung t2 − Du2 = −4. Math. Z. 39 (1934), 95–111.
¨ nemann, Theorie der Symmetrischen Functionen der Wurzeln einer Gleichung.
[13] T. Scho
Allgemeine S¨
atze u
¨ber Congruenzen nebst einigen Anwendungen derselben. J. Reine Angew.
Math. 19 (1839), 289–308.
[14] K. Williams, On Scholz’s Reciprocity Law. Proc. Amer. Math. Soc. 64 No. 1 (1977), 45–46.
[15] “
K. Williams,
K. Hardy, and C. Friesen, On the Evaluation of the Legendre Symbol
√ ”
A+B
p

m

. Acta Arith. 45 (1985), 255–272.

Mark Budden
Department of Mathematics
Armstrong Atlantic State University
11935 Abercorn St.
Savannah, GA USA 31419
E-mail : Mark.Budden@armstrong.edu
URL: http://www.math.armstrong.edu/faculty/budden
Jeremiah Eisenmenger
Department of Mathematics
University of Florida
PO Box 118105
Gainesville, FL USA 32611-8105
E-mail : eisenmen@math.ufl.edu
Jonathan Kish
Department of Mathematics
University of Colorado at Boulder
Boulder, CO USA 80309
E-mail : jonathan.kish@colorado.edu

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