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NEAR OPTIMAL BOUNDS IN FREIMAN'S THEOREM

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108 GUILLARMOU and TZOU<br />

where<br />

I1 =<br />

<br />

M0<br />

<br />

I2 = 2h<br />

V (a 2 + a 2 <br />

)dvg + 2<br />

M0<br />

<br />

V Re ae 2iψ/h<br />

<br />

s1<br />

h<br />

+ e −2iψ/h<br />

<br />

a0 + r1<br />

<br />

h<br />

M0<br />

V |a| 2 Re(e 2iψ/h )dvg, (19)<br />

+ b0<br />

<br />

+ b0 + a0 + s1 + r1<br />

h<br />

<br />

dvg. (20)<br />

Remark 5.2<br />

We observe from the last identity in Lemma 4.1.2 that r1/h in the expression I2 can<br />

be replaced by the term r12 satisfying 2ir12∂ψ = b up to an error which can go in<br />

the o(h) in (18), and similarly for the term s1/h, which can be replaced by a terms12<br />

independent of h.<br />

We apply the stationary phase to these two terms in Lemmas 5.3 and 5.4.<br />

LEMMA 5.3<br />

The estimate<br />

<br />

I2 = 2h<br />

M0<br />

V Re <br />

a(b0 + a0 +s12 +r12)dvg + o(h)<br />

holds true where r12, s12,r12 ands12 are independent of h.<br />

Proof<br />

We start with the following.<br />

LEMMA 5.4<br />

Let f ∈ L 1 (M0). Thenash → 0,<br />

<br />

M0<br />

e 2iψ/h f dvg = o(1).<br />

Proof<br />

Since C k (M0) is dense in L 1 (M0) for all k ∈ N, it suffices to prove the lemma for<br />

f ∈ C k (M0).Letɛ>0 be small, and choose a cutoff function χ which is identically<br />

equal to 1 on the boundary such that<br />

<br />

M0<br />

χ|f | dvg ≤ ɛ.

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