<p>In this paper, we consider the multiplicity and asymptotics of standing waves for the energy critical half-wave, which are solutions to <Equation ID="Equ1"> <EquationNumber>(0.1)</EquationNumber> <EquationSource Format="TEX">\({{\sqrt{-\Delta} u}}=\lambda u+\mu{\vert u \vert}^{q-2}u+{\vert u \vert}^{2^{\ast}-2}u, \quad u \in H^{1/2}({\mathbb R}^{N}),\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mrow> <msqrt> <mo>−</mo> <mi mathvariant="normal">Δ</mi> </msqrt> <mi>u</mi> </mrow> </mrow> <mo>=</mo> <mi>λ</mi> <mi>u</mi> <mo>+</mo> <mi>μ</mi> <msup> <mrow> <mo fence="false" stretchy="false">|</mo> <mi>u</mi> <mo fence="false" stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo fence="false" stretchy="false">|</mo> <mi>u</mi> <mo fence="false" stretchy="false">|</mo> </mrow> <mrow> <msup> <mn>2</mn> <mrow> <mo>∗</mo> </mrow> </msup> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> <mspace width="1em" /> <mi>u</mi> <mo>∈</mo> <msup> <mi>H</mi> <mrow> <mn>1</mn> <mrow> <mo>/</mo> </mrow> <mn>2</mn> </mrow> </msup> <mo stretchy="false">(</mo> <msup> <mrow> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> </mrow> <mrow> <mi>N</mi> </mrow> </msup> <mo stretchy="false">)</mo> <mo>,</mo> </math></EquationSource> </Equation> under the constraint <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\int_{{\mathbb R}^{N}} u^{2}=a^{2}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mo>∫</mo> <mrow> <msup> <mrow> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> </mrow> <mrow> <mi>N</mi> </mrow> </msup> </mrow> </msub> <msup> <mi>u</mi> <mrow> <mn>2</mn> </mrow> </msup> <mo>=</mo> <msup> <mi>a</mi> <mrow> <mn>2</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, where <i>N</i> ≥ 2, <i>a</i> &gt; 0, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(q \in (2,2+{2 \over N}), 2^{\ast}={{2N} \over {N-1}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mn>2</mn> <mo>+</mo> <mrow> <mfrac> <mn>2</mn> <mi>N</mi> </mfrac> </mrow> <mo stretchy="false">)</mo> <mo>,</mo> <msup> <mn>2</mn> <mrow> <mo>∗</mo> </mrow> </msup> <mo>=</mo> <mrow> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>−</mo> <mn>1</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> and <i>λ</i> ∈ ℝ appears as a Lagrange multiplier. We show that (0.1) admits a ground state <i>u</i><sub><i>a</i></sub> and an excited state <i>v</i><sub><i>a</i></sub>, which are characterized by a local minimizer and a mountain-pass critical point of the corresponding energy functional. Several asymptotic properties of {<i>u</i><sub><i>a</i></sub>}, {<i>v</i><sub><i>a</i></sub>} are obtained and it is worth pointing out that we get a precise description of {<i>u</i><sub><i>a</i></sub>} as <i>a</i> → 0<sup>+</sup> without needing any uniqueness condition on the related limit problem. Finally, assuming local well-posedness, we prove that the set of ground states is stable under the half-wave evolution.</p>

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Multiplicity and asymptotics of standing waves for the energy critical half-wave

  • Xiao Luo,
  • Tao Yang,
  • Xiaolong Yang

摘要

In this paper, we consider the multiplicity and asymptotics of standing waves for the energy critical half-wave, which are solutions to (0.1) \({{\sqrt{-\Delta} u}}=\lambda u+\mu{\vert u \vert}^{q-2}u+{\vert u \vert}^{2^{\ast}-2}u, \quad u \in H^{1/2}({\mathbb R}^{N}),\) Δ u = λ u + μ | u | q 2 u + | u | 2 2 u , u H 1 / 2 ( R N ) , under the constraint \(\int_{{\mathbb R}^{N}} u^{2}=a^{2}\) R N u 2 = a 2 , where N ≥ 2, a > 0, \(q \in (2,2+{2 \over N}), 2^{\ast}={{2N} \over {N-1}}\) q ( 2 , 2 + 2 N ) , 2 = 2 N N 1 and λ ∈ ℝ appears as a Lagrange multiplier. We show that (0.1) admits a ground state ua and an excited state va, which are characterized by a local minimizer and a mountain-pass critical point of the corresponding energy functional. Several asymptotic properties of {ua}, {va} are obtained and it is worth pointing out that we get a precise description of {ua} as a → 0+ without needing any uniqueness condition on the related limit problem. Finally, assuming local well-posedness, we prove that the set of ground states is stable under the half-wave evolution.