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首页> 外文期刊>The journal of high energy physics >New N documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathcal{N} $$end{document} = (0 , 4) AdS 3 near-horizons in Type IIB
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New N documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathcal{N} $$end{document} = (0 , 4) AdS 3 near-horizons in Type IIB

机译:new <内联公式id =“IEQ1”> <替代方案> n DocumentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsidemargin} { - 69pt} begin {document} $$$ nath {document} =(0 4)ADS 3 IIB型近视

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A bstract We construct new families of N documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathcal{N} $$end{document} = (0 , 4) AdS_(3)× S ~(2)× S ? 2 documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ {ilde{S}}^2 $$end{document} × S ~(1)backgrounds fibred over a 2d Riemann surface in Type IIB string theory. These solutions are obtained by extracting the near-horizon limit of D3-brane box configurations, consisting of D3-D5-NS5 branes ending on D5′-NS5′ background branes. We relate our families of solutions to previous AdS_(3)× S ~(2)× CY_(2)and AdS_(3)× S ~(3)× S ~(2)solutions to Type IIA recently constructed in the literature. We construct explicit 2d quiver CFTs associated to the D3-brane box configurations, and check that the central charges match the holographic result. We extend our solutions to include D7-branes, and show that a subclass of these solutions can be interpreted in terms of D3-D5-NS5 defect branes embedded in a 5d fixed point theory. This is explicitly realised by linking our solutions to a 6d domain wall that asymptotes locally the AdS_(6)× S ~(2)× Σ_(2)solution T-dual to the Brandhuber-Oz vacuum.
机译:一个bstract我们构建ñ的DocumentClass的新家庭[12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {upgreek } setlength { oddsidemargin} { - 69pt} {开始文档} $$ mathcal {N} $$ {端文档} =(0,4)AdS_(3)×S〜(2)×S? 2 documentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsidemargin} {-69pt} begin {document} $$ { tilde {s}} ^ 2 $$ { tilde {s}} ^ 2 $$ end {document}×s〜(1)背景在IIB串理论中的2D riemann曲面上的纤维。这些解决方案通过提取D3- Brane箱配置的近地平线限制而获得,由结束于D5'-NS5'背景布朗的D3-D5-NS5 Branes。我们将我们的解决方案的家庭与以前的ADS_(3)×S〜(2)×CY_(2)和ADS_(3)×S〜(3)×S〜(2)解决方案达到文献中最近构建的IIa型。我们构建与D3-BRANE盒配置相关的显式2D Quiver CFT,并检查中央收费是否与全息结果匹配。我们将我们的解决方案扩展到包括D7-Branes,并表明这些解决方案的子类可以解释为嵌入在5D定点理论中的D3-D5-NS5缺陷斑块。通过将我们的解决方案链接到6D域墙上,将我们的解决方案与本地逐渐呈现ADS_(6)×S〜(2)×Σ_(2)解决方案T-Dual至Brandhuber-Oz真空的解决方案来明确实现。

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