<p>We introduce and study invariant differential operators acting on the space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\cal{H}(\Omega)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="script">H</mi> </mrow> <mo class="MJX-tex-caligraphic" mathvariant="script" stretchy="false">(</mo> <mi mathvariant="script">Ω</mi> <mo class="MJX-tex-caligraphic" mathvariant="script" stretchy="false">)</mo> </math></EquationSource> </InlineEquation> of holomorphic functions on the complement <Equation ID="Equ1"> <EquationSource Format="TEX">\(\Omega=\{(z,w)\in \hat{\mathbb{C}}^{2}:z\cdot w \ne 1 \}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi mathvariant="normal">Ω</mi> <mo>=</mo> <mo fence="false" stretchy="false">{</mo> <mo stretchy="false">(</mo> <mi>z</mi> <mo>,</mo> <mi>w</mi> <mo stretchy="false">)</mo> <mo>∈</mo> <msup> <mrow> <mover> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>2</mn> </mrow> </msup> <mo>:</mo> <mi>z</mi> <mo>⋅</mo> <mi>w</mi> <mo>≠</mo> <mn>1</mn> <mo fence="false" stretchy="false">}</mo> </math></EquationSource> </Equation> of the “complexified unit circle” <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\{(z,w)\in \hat{\mathbb{C}}^{2}:z\cdot w = 1 \}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo fence="false" stretchy="false">{</mo> <mo stretchy="false">(</mo> <mi>z</mi> <mo>,</mo> <mi>w</mi> <mo stretchy="false">)</mo> <mo>∈</mo> <msup> <mrow> <mover> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>2</mn> </mrow> </msup> <mo>:</mo> <mi>z</mi> <mo>⋅</mo> <mi>w</mi> <mo>=</mo> <mn>1</mn> <mo fence="false" stretchy="false">}</mo> </math></EquationSource> </InlineEquation>. We obtain recursion identities, describe the behaviour under change of coordinates and find the generators of the corresponding operator algebra. We illustrate how this provides a unified framework for investigating conformally invariant differential operators on the unit disk <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathbb{D}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="double-struck">D</mi> </mrow> </math></EquationSource> </InlineEquation> and the Riemann sphere <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\hat{\mathbb{C}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> </math></EquationSource> </InlineEquation>, which have been studied by Peschl, Aharonov, Minda and many others, within their conjecturally natural habitat. We apply the machinery to a problem in deformation quantization by deriving explicit formulas for the canonical Wick-type star products on Ω, the unit disk <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbb{D}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="double-struck">D</mi> </mrow> </math></EquationSource> </InlineEquation> and the Riemann sphere <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\hat{\mathbb{C}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> in terms of such invariant differential operators. These formulas are given in the form of factorial series which depend holomorphically on a complex deformation parameter <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\bar{h}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mi>h</mi> <mo stretchy="false">¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> and lead to asymptotic expansions of the star products in powers of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\bar{h}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mi>h</mi> <mo stretchy="false">¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Peschl–Minda derivatives and convergent Wick star products on the disk, the sphere and beyond

  • Michael Heins,
  • Annika Moucha,
  • Oliver Roth,
  • Toshiyuki Sugawa

摘要

We introduce and study invariant differential operators acting on the space \(\cal{H}(\Omega)\) H ( Ω ) of holomorphic functions on the complement \(\Omega=\{(z,w)\in \hat{\mathbb{C}}^{2}:z\cdot w \ne 1 \}\) Ω = { ( z , w ) C ^ 2 : z w 1 } of the “complexified unit circle” \(\{(z,w)\in \hat{\mathbb{C}}^{2}:z\cdot w = 1 \}\) { ( z , w ) C ^ 2 : z w = 1 } . We obtain recursion identities, describe the behaviour under change of coordinates and find the generators of the corresponding operator algebra. We illustrate how this provides a unified framework for investigating conformally invariant differential operators on the unit disk \(\mathbb{D}\) D and the Riemann sphere \(\hat{\mathbb{C}}\) C ^ , which have been studied by Peschl, Aharonov, Minda and many others, within their conjecturally natural habitat. We apply the machinery to a problem in deformation quantization by deriving explicit formulas for the canonical Wick-type star products on Ω, the unit disk \(\mathbb{D}\) D and the Riemann sphere \(\hat{\mathbb{C}}\) C ^ in terms of such invariant differential operators. These formulas are given in the form of factorial series which depend holomorphically on a complex deformation parameter \(\bar{h}\) h ¯ and lead to asymptotic expansions of the star products in powers of \(\bar{h}\) h ¯ .