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NEAR OPTIMAL BOUNDS IN FREIMAN'S THEOREM

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<strong>IN</strong>HOMOGENEOUS QUADRATIC FORMS 133<br />

above. Define<br />

f ˜(g<br />

: qξ) = <br />

v∈X(qξ )<br />

f (gv). (36)<br />

The following is an analogue of [EMM2, Theorem 2.3] and will provide us with<br />

the upper bound required for the proof of Theorem 1.9. The proof of this theorem is<br />

the main technical part of this paper and will occupy the rest of this paper.<br />

<strong>THEOREM</strong> 4.1<br />

Let G, H, K, and {at} be as in Section 2 for the signature (2, 2) case. Let Qξ be a<br />

quadratic form of signature (2, 2) which is Diophantine. Let q ∈ SL4(R) and qξ be<br />

as above. Let ν be a continuous function on K. Then we have<br />

<br />

<br />

<br />

lim sup<br />

t→∞<br />

˜f (atk : qξ)ν(k) dk ≤ f ˆ(g)<br />

dµ(g)<br />

K<br />

G/ Ɣ<br />

K<br />

ν(k) dk, (37)<br />

where µ is the G-invariant probability measure on G/ Ɣ if the homogenous part, Q,<br />

is irrational and where the H ⋉R 4 -invariant probability measure on the closed orbit<br />

is H ⋉R 4 · qξ if Q is a rational form.<br />

Proof of Theorem 1.9<br />

Suppose that Qξ is as in the statement of Theorem 1.9. An argument like that<br />

of [EMM1, Sections 3.4, 3.5] combined with Theorem 4.1 gives: if 0 /∈ (a,b),<br />

then<br />

lim sup<br />

T →∞<br />

NQ,ξ,(a,b,T ) = lim sup ÑQ,ξ,(a,b,T ) ≤ λQ,(b − a)T<br />

T →∞<br />

2 . (38)<br />

This upper bound, combined with the lower bound obtained by Theorem 1.4, proves<br />

Theorem 1.9. <br />

The proof of Theorem 4.1 extensively utilizes results and ideas from [EMM1]<br />

and [EMM2], and we will try to use their terminology and notation for the convenience<br />

of the reader. We recall these theorems and terminology when we need them. Let us<br />

start with the following.<br />

<strong>THEOREM</strong> 4.2<br />

Let {at} and K be as in Theorem 4.1. Let be any lattice in R 4 . Then for i = 1, 3<br />

and any ε>0, we have<br />

<br />

sup αi(atk)<br />

t>0 K<br />

2−ε dk < ∞. (39)

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