具有 4 阶交映自变的 K3 曲面

Pub Date : 2024-03-12 DOI:10.1002/mana.202300052
Benedetta Piroddi
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Having called <span></span><math>\n <semantics>\n <mover>\n <mi>Z</mi>\n <mo>∼</mo>\n </mover>\n <annotation>$\\tilde{Z}$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mover>\n <mi>Y</mi>\n <mo>∼</mo>\n </mover>\n <annotation>$\\tilde{Y}$</annotation>\n </semantics></math>, respectively, the minimal resolutions of the quotient surfaces <span></span><math>\n <semantics>\n <mrow>\n <mi>Z</mi>\n <mo>=</mo>\n <mi>X</mi>\n <mo>/</mo>\n <msup>\n <mi>τ</mi>\n <mn>2</mn>\n </msup>\n </mrow>\n <annotation>$Z=X/\\tau ^2$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <mi>Y</mi>\n <mo>=</mo>\n <mi>X</mi>\n <mo>/</mo>\n <mi>τ</mi>\n </mrow>\n <annotation>$Y=X/\\tau$</annotation>\n </semantics></math>, we also describe the maps induced in cohomology by the rational quotient maps <span></span><math>\n <semantics>\n <mrow>\n <mi>X</mi>\n <mo>→</mo>\n <mover>\n <mi>Z</mi>\n <mo>∼</mo>\n </mover>\n <mo>,</mo>\n <mspace></mspace>\n <mi>X</mi>\n <mo>→</mo>\n <mover>\n <mi>Y</mi>\n <mo>∼</mo>\n </mover>\n </mrow>\n <annotation>$X\\rightarrow \\tilde{Z},\\ X\\rightarrow \\tilde{Y}$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <mover>\n <mi>Y</mi>\n <mo>∼</mo>\n </mover>\n <mo>→</mo>\n <mover>\n <mi>Z</mi>\n <mo>∼</mo>\n </mover>\n </mrow>\n <annotation>$\\tilde{Y}\\rightarrow \\tilde{Z}$</annotation>\n </semantics></math>: With this knowledge, we are able to give a lattice-theoretic characterization of <span></span><math>\n <semantics>\n <mover>\n <mi>Z</mi>\n <mo>∼</mo>\n </mover>\n <annotation>$\\tilde{Z}$</annotation>\n </semantics></math>, and find the relation between the Néron–Severi lattices of <span></span><math>\n <semantics>\n <mrow>\n <mi>X</mi>\n <mo>,</mo>\n <mover>\n <mi>Z</mi>\n <mo>∼</mo>\n </mover>\n </mrow>\n <annotation>$X,\\tilde{Z}$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mover>\n <mi>Y</mi>\n <mo>∼</mo>\n </mover>\n <annotation>$\\tilde{Y}$</annotation>\n </semantics></math> in the projective case. 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Having called <span></span><math>\\n <semantics>\\n <mover>\\n <mi>Z</mi>\\n <mo>∼</mo>\\n </mover>\\n <annotation>$\\\\tilde{Z}$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mover>\\n <mi>Y</mi>\\n <mo>∼</mo>\\n </mover>\\n <annotation>$\\\\tilde{Y}$</annotation>\\n </semantics></math>, respectively, the minimal resolutions of the quotient surfaces <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>Z</mi>\\n <mo>=</mo>\\n <mi>X</mi>\\n <mo>/</mo>\\n <msup>\\n <mi>τ</mi>\\n <mn>2</mn>\\n </msup>\\n </mrow>\\n <annotation>$Z=X/\\\\tau ^2$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>Y</mi>\\n <mo>=</mo>\\n <mi>X</mi>\\n <mo>/</mo>\\n <mi>τ</mi>\\n </mrow>\\n <annotation>$Y=X/\\\\tau$</annotation>\\n </semantics></math>, we also describe the maps induced in cohomology by the rational quotient maps <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>X</mi>\\n <mo>→</mo>\\n <mover>\\n <mi>Z</mi>\\n <mo>∼</mo>\\n </mover>\\n <mo>,</mo>\\n <mspace></mspace>\\n <mi>X</mi>\\n <mo>→</mo>\\n <mover>\\n <mi>Y</mi>\\n <mo>∼</mo>\\n </mover>\\n </mrow>\\n <annotation>$X\\\\rightarrow \\\\tilde{Z},\\\\ X\\\\rightarrow \\\\tilde{Y}$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mrow>\\n <mover>\\n <mi>Y</mi>\\n <mo>∼</mo>\\n </mover>\\n <mo>→</mo>\\n <mover>\\n <mi>Z</mi>\\n <mo>∼</mo>\\n </mover>\\n </mrow>\\n <annotation>$\\\\tilde{Y}\\\\rightarrow \\\\tilde{Z}$</annotation>\\n </semantics></math>: With this knowledge, we are able to give a lattice-theoretic characterization of <span></span><math>\\n <semantics>\\n <mover>\\n <mi>Z</mi>\\n <mo>∼</mo>\\n </mover>\\n <annotation>$\\\\tilde{Z}$</annotation>\\n </semantics></math>, and find the relation between the Néron–Severi lattices of <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>X</mi>\\n <mo>,</mo>\\n <mover>\\n <mi>Z</mi>\\n <mo>∼</mo>\\n </mover>\\n </mrow>\\n <annotation>$X,\\\\tilde{Z}$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mover>\\n <mi>Y</mi>\\n <mo>∼</mo>\\n </mover>\\n <annotation>$\\\\tilde{Y}$</annotation>\\n </semantics></math> in the projective case. We also produce three different projective models for <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>X</mi>\\n <mo>,</mo>\\n <mover>\\n <mi>Z</mi>\\n <mo>∼</mo>\\n </mover>\\n </mrow>\\n <annotation>$X,\\\\tilde{Z}$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mover>\\n <mi>Y</mi>\\n <mo>∼</mo>\\n </mover>\\n <annotation>$\\\\tilde{Y}$</annotation>\\n </semantics></math>, each associated to a different polarization of degree 4 on <span></span><math>\\n <semantics>\\n <mi>X</mi>\\n <annotation>$X$</annotation>\\n </semantics></math>.</p>\",\"PeriodicalId\":0,\"journal\":{\"name\":\"\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0,\"publicationDate\":\"2024-03-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/mana.202300052\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/mana.202300052","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

摘要

给定 X$X$,一个允许 4 阶交映自变的 K3 曲面 τ$tau$,我们描述了 H2(X,Z)$H^2(X,\mathbb {Z})$ 上的等势 τ∗\$tau ^*$。我们把 Z∼$\tilde{Z}$ 和 Y∼$\tilde{Y}$ 分别称为商曲面 Z=X/τ2$Z=X/\tau ^2$ 和 Y=X/τ$Y=X/\tau$ 的最小解析、我们还描述了有理商映射 X→Z∼,X→Y∼$X\rightarrow \tilde{Z},\X\rightarrow \tilde{Y}$ 和 Y∼→Z∼$$\tilde{Y}\rightarrow \tilde{Z}$ 在同调中诱导的映射:有了这些知识,我们就能给出 Z∼$\tilde{Z}$ 的网格理论特征,并找到投影情况下 X,Z∼$X,\tilde{Z}$ 和 Y∼$\tilde{Y}$ 的内龙-塞维里网格之间的关系。我们还为 X,Z∼$X,\tilde{Z}$和 Y∼$\tilde{Y}$建立了三个不同的投影模型,每个模型都与 X$X$ 上不同的 4 度极化相关联。
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K3 surfaces with a symplectic automorphism of order 4

Given X $X$ , a K3 surface admitting a symplectic automorphism τ $\tau$ of order 4, we describe the isometry τ $\tau ^*$ on H 2 ( X , Z ) $H^2(X,\mathbb {Z})$ . Having called Z $\tilde{Z}$ and Y $\tilde{Y}$ , respectively, the minimal resolutions of the quotient surfaces Z = X / τ 2 $Z=X/\tau ^2$ and Y = X / τ $Y=X/\tau$ , we also describe the maps induced in cohomology by the rational quotient maps X Z , X Y $X\rightarrow \tilde{Z},\ X\rightarrow \tilde{Y}$ and Y Z $\tilde{Y}\rightarrow \tilde{Z}$ : With this knowledge, we are able to give a lattice-theoretic characterization of Z $\tilde{Z}$ , and find the relation between the Néron–Severi lattices of X , Z $X,\tilde{Z}$ and Y $\tilde{Y}$ in the projective case. We also produce three different projective models for X , Z $X,\tilde{Z}$ and Y $\tilde{Y}$ , each associated to a different polarization of degree 4 on X $X$ .

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