The bilinear Hilbert transform BHT(f,g)(x)=p.v.∫Rf(x−t)g(x+t) dt/t\mathrm{BHT}(f,g)(x)=\mathrm{p.v.}\int_{\mathbb{R}} f(x-t)g(x+t)\,dt/t is known since Lacey and Thiele to map Lp1×Lp2L^{p_1}\times L^{p_2} boundedly into LpL^{p}, 1/p1+1/p2=1/p1/p_1+1/p_2=1/p, whenever 2/3<p<∞2/3<p<\infty and 1<p1,p2≤∞1<p_1,p_2\leq\infty. Whether the estimates extend to the remaining scaling range 1/2<p≤2/31/2<p\leq 2/3 — the lower boundary 1/21/2 being forced by the relation 1/p=1/p1+1/p21/p=1/p_1+1/p_2 with p1,p2≤∞p_1,p_2\leq\infty — has remained open since 1997. No proof is known for any exponent tuple in this range, and no counterexample with LpL^{p} inputs is known either: all known negative results concern larger operator classes or modified input spaces. The problem asks for a definitive resolution in either direction, including the endpoint p=2/3p=2/3, where only distributional estimates with double-logarithmic losses are available.

Background

The bilinear Hilbert transform is the bilinear singular integral

BHT(f1,f2)(x):=p.v.∫Rf1(x−t) f2(x+t) dtt,\mathrm{BHT}(f_1,f_2)(x):=\mathrm{p.v.}\int_{\mathbb{R}} f_1(x-t)\,f_2(x+t)\,\frac{dt}{t},

where p.v. denotes the Cauchy principal value. In Fourier coordinates it is the bilinear multiplier operator with symbol sgn⁡(ξ1−ξ2)\operatorname{sgn}(\xi_1-\xi_2):

BHT(f1,f2)(x)=∫R2sgn⁡(ξ1−ξ2) f^1(ξ1)f^2(ξ2) e2πix(ξ1+ξ2) dξ1dξ2.\mathrm{BHT}(f_1,f_2)(x)=\int_{\mathbb{R}^2}\operatorname{sgn}(\xi_1-\xi_2)\,\hat f_1(\xi_1)\hat f_2(\xi_2)\,e^{2\pi i x(\xi_1+\xi_2)}\,d\xi_1 d\xi_2.

The operator was introduced by A. P. Calderón in his study of the Cauchy integral along Lipschitz curves: the relevant commutators can be rewritten as averages of bilinear Hilbert transforms, and Calderón conjectured in the mid-1960s that BHT\mathrm{BHT} maps L2×L2L^2\times L^2 into L1L^1. The operator is modulation invariant — multiplying an input by e2πiξxe^{2\pi i \xi x} translates the output's Fourier support — which places it outside the classical Calderón–Zygmund theory of singular integrals (the framework that handles the ordinary Hilbert transform) and is the source of its difficulty. In two celebrated papers, Lacey and Thiele proved that BHT\mathrm{BHT} maps Lp1×Lp2L^{p_1}\times L^{p_2} boundedly into LpL^p whenever 1<p1,p2≤∞1<p_1,p_2\leq\infty, 1/p1+1/p2=1/p1/p_1+1/p_2=1/p, and 2/3<p<∞2/3<p<\infty (the case p>2p>2 in 1997, the general range in 1999), confirming Calderón's conjecture. Their proof created time-frequency analysis: inputs are decomposed into wave packets (functions localized simultaneously in time and frequency), and the sum is organized into trees (collections of wave packets whose frequency supports all lie inside that of one distinguished packet) whose contributions are controlled by orthogonality and combinatorial selection. The scaling relation 1/p=1/p1+1/p21/p=1/p_1+1/p_2 with p1,p2≤∞p_1,p_2\leq\infty forces p>1/2p>1/2, so 2/32/3 is not a natural barrier of the operator but a barrier of the current method; the conjectured truth is boundedness for all 1/2<p<∞1/2<p<\infty. The region of known boundedness is an open hexagon in the exponent simplex 1/p1+1/p2+1/p3=11/p_1+1/p_2+1/p_3=1 (where p3p_3 is the dual output exponent), whose six corners all correspond to hypothetical endpoint estimates L1×L2→L2/3L^1\times L^2\to L^{2/3} of some dual of BHT\mathrm{BHT}. Several adjacent facts delimit what any solution must overcome. First, Lacey (2000) showed that the threshold 2/32/3 is sharp, modulo endpoints, for the entire modulation-invariant model class: discrete model sums with arbitrary bounded coefficients — which is what generic tree-selection arguments actually bound — cannot be bounded below 2/32/3. Hence a positive result must exploit the specific structure of the symbol sgn⁡(ξ1−ξ2)\operatorname{sgn}(\xi_1-\xi_2), not merely modulation invariance. Second, at the endpoint p=2/3p=2/3 itself, Bilyk and Grafakos (2006) and Di Plinio and Thiele (2016) proved only distributional-type estimates with, respectively, single- and double-logarithmic losses; whether even the double logarithm can be removed (as it can for the quartile operator (the discrete Walsh-model analogue of BHT\mathrm{BHT}, built from dyadic step functions instead of Fourier waves), by Demeter and Di Plinio 2013) is open, and no strong or weak-type L2/3L^{2/3} bound is known. Third, no counterexample with LpL^p inputs exists: the negative results of Dai and Lu (2014) show failure only for Fourier–Lebesgue input spaces FLp′\mathcal{F}L^{p'} (functions whose Fourier transform lies in Lp′L^{p'}) with the other input in LpL^p, and Miyachi and Tomita (2017) showed unboundedness on products of Hardy spaces HpH^p with p≤1p\leq 1 (the Hardy scale is the standard LpL^p substitute below exponent 11, built from maximal averages rather than absolute values). Fourth, Dai and Lu proved that multipliers with symbols exponentially damped transversely to the singularity line {ξ1=ξ2}\{\xi_1=\xi_2\}, at any fixed damping strength δ>0\delta>0, are bounded in the full range 1/2<p<∞1/2<p<\infty, but with constants that blow up as δ→0\delta\to 0 whenever 1/2<p≤2/31/2<p\leq 2/3; passing to the undamped limit that recovers the true BHT\mathrm{BHT} symbol is exactly the open question. Subsequent work has confirmed rather than eroded the 2/32/3 barrier: Uraltsev and Warchalski (2022) proved uniform-in-parameter bounds for the family BHTβ\mathrm{BHT}_\beta exactly in p>2/3p>2/3 (the full range where uniform bounds can hold), and Fraccaroli, Saari, and Thiele (2024) extended uniform bounds to quasiconformally transformed symbols still only in the strict local L2L^2 range. For p<1p<1 the target LpL^p is quasi-Banach, so duality, convexity, and standard interpolation tools are unavailable — a structural source of difficulty for the lower part of the range.

Problem Statement

Determine whether the bilinear Hilbert transform

BHT(f1,f2)(x)=p.v.∫Rf1(x−t) f2(x+t) dtt\mathrm{BHT}(f_1,f_2)(x)=\mathrm{p.v.}\int_{\mathbb{R}} f_1(x-t)\,f_2(x+t)\,\frac{dt}{t}

extends to a bounded bilinear operator from Lp1(R)×Lp2(R)L^{p_1}(\mathbb{R})\times L^{p_2}(\mathbb{R}) into Lp(R)L^{p}(\mathbb{R}), where 1<p1,p2≤∞1<p_1,p_2\leq\infty and 1p=1p1+1p2\frac{1}{p}=\frac{1}{p_1}+\frac{1}{p_2}, for exponents in the remaining open range 12<p≤23\frac{1}{2}<p\leq\frac{2}{3}. A complete solution decides the dichotomy: either (i) a positive answer — a proof of boundedness for all exponent tuples in the stated range 12<p≤23\frac{1}{2}<p\leq\frac{2}{3}, including a strong- or weak-type bound at the endpoint p=23p=\frac{2}{3}; or (ii) a negative answer — an explicit construction of input functions in Lp1×Lp2L^{p_1}\times L^{p_2} demonstrating that the operator norm is infinite for some tuple with 12<p≤23\frac{1}{2}<p\leq\frac{2}{3}. Partial information such as estimates for damped approximating symbols (whose constants blow up as the damping tends to zero) or for Fourier–Lebesgue/Hardy input spaces does not resolve the question, which concerns the Lebesgue spaces themselves.

References

  1. Wei Dai and Guozhen Lu, "LpL^{p} estimates for the bilinear Hilbert transform for 1/2<p≤2/31/2<p\leq2/3: A counterexample and generalizations to non-smooth symbols", arXiv:1409.3875 (2014), https://arxiv.org/abs/1409.3875
  2. Michael Lacey and Christoph Thiele, "LpL^{p} estimates on the bilinear Hilbert transform for 2<p<∞2<p<\infty", Annals of Mathematics (2) 146 (1997), 693–724, DOI: 10.2307/2952458, https://doi.org/10.2307/2952458
  3. Michael Lacey and Christoph Thiele, "On Calderón's conjecture", Annals of Mathematics (2) 149 (1999), 475–496, DOI: 10.2307/120971, https://doi.org/10.2307/120971
  4. Michael T. Lacey, "The bilinear maximal functions map into LpL^{p} for 2/3<p≤12/3<p\leq 1", Annals of Mathematics (2) 151 (2000), 35–57, DOI: 10.2307/121111, https://doi.org/10.2307/121111
  5. Dmitriy Bilyk and Loukas Grafakos, "Distributional estimates for the bilinear Hilbert transform", Journal of Geometric Analysis 16 (2006), 563–584, DOI: 10.1007/BF02922131, https://doi.org/10.1007/BF02922131
  6. Ciprian Demeter and Francesco Di Plinio, "Endpoint bounds for the quartile operator", Journal of Fourier Analysis and Applications 19 (2013), 836–856, DOI: 10.1007/s00041-013-9275-4, https://doi.org/10.1007/s00041-013-9275-4
  7. Francesco Di Plinio and Christoph Thiele, "Endpoint bounds for the bilinear Hilbert transform", Transactions of the American Mathematical Society 368 (2016), 3931–3972, DOI: 10.1090/tran/6548, https://doi.org/10.1090/tran/6548
  8. Akihiko Miyachi and Naohito Tomita, "A remark on the unboundedness of the bilinear Hilbert transform on Hardy spaces", RIMS Kôkyûroku Bessatsu B65 (2017), 153–157, Zbl: 1390.42021, https://zbmath.org/6870707
  9. Gennady Uraltsev and Michał Warchalski, "The full range of uniform bounds for the bilinear Hilbert transform", arXiv:2205.09851 (2022), https://arxiv.org/abs/2205.09851
  10. Marco Fraccaroli, Olli Saari, and Christoph Thiele, "Uniform bounds for bilinear symbols with linear K-quasiconformally embedded singularity", Analysis & PDE 18 (2025), 2293–2323, DOI: 10.2140/apde.2025.18.2293 (preprint arXiv:2402.11661), https://doi.org/10.2140/apde.2025.18.2293
  11. Lars Becker and Polona Durcik, "The shifted bilinear Hilbert transform", arXiv:2603.20173 (2026), https://arxiv.org/abs/2603.20173