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        "quote": "> [!example] <a class=\"object-permalink\" href=\"#example-7-5\">例 7.5</a> \n>\n> 设 $( V , \\cdot )$ 为实内积空间，如 <a href=\"../chapter-05/01-real-inner-product-spaces#section-5-1\" class=\"cross-reference\" id=\"xref-02-multilinear-maps-and-tensors-9\" data-reference=\"section-5-1\">第 5.1 节</a>所述。由下式定义的映射 $g:V\\times V\\to\\mathbb R$\n>\n> $$\n> g (u, v) = u \\cdot v\n> $$\n>\n> 显然是双线性的，并且是一个2阶协变张量，称为内积的<u class=\"concept-term\" data-concept-identity=\"urn:uuid:ac724144-5a08-407a-a27a-796eb367a161\" data-concept-route=\"/concept-identities#concept-ac724144-5a08-407a-a27a-796eb367a161\" id=\"first-52084e4e3766521c7bd5-zh\">度量张量(metric tensor)</u>。内积的分量$g _ { i j } = e _ { i } \\cdot e _ { j } = g ( e _ { i } , e _ { j } )$是度量张量关于基$\\{ e _ { i } \\}$的分量\n>\n> $$\n> g = g _ {i j} \\varepsilon^ {i} \\otimes \\varepsilon^ {j},\n> $$\n>\n> 而两个向量的内积是\n>\n> $$\n> u \\cdot v = g (u, v) = g _ {i j} u ^ {i} v ^ {j}.\n> $$\n>\n> 度量张量是对称的，\n>\n> $$\n> g (u, v) = g (v, u).\n> $$",
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        "quote": "> [!example] <a class=\"object-permalink\" href=\"#example-7-5\">Example 7.5</a> \n>\n> Let $( V , \\cdot )$ be a real inner product space, as in <a href=\"../chapter-05/01-real-inner-product-spaces#section-5-1\" class=\"cross-reference\" id=\"xref-02-multilinear-maps-and-tensors-9\" data-reference=\"section-5-1\">Section 5.1</a>. The map $g:V\\times V\\to\\mathbb R$ defined by\n>\n> $$\n> g (u, v) = u \\cdot v\n> $$\n>\n> is obviously bilinear, and is a covariant tensor of degree 2 called the <u class=\"concept-term\" data-concept-identity=\"urn:uuid:ac724144-5a08-407a-a27a-796eb367a161\" data-concept-route=\"/concept-identities#concept-ac724144-5a08-407a-a27a-796eb367a161\" id=\"first-52084e4e3766521c7bd5-en\">metric tensor</u> of the inner product. The components $g _ { i j } = e _ { i } \\cdot e _ { j } = g ( e _ { i } , e _ { j } )$ of the inner product are the components of the metric tensor with respect to the basis $\\{ e _ { i } \\}$\n>\n> $$\n> g = g _ {i j} \\varepsilon^ {i} \\otimes \\varepsilon^ {j},\n> $$\n>\n> while the inner product of two vectors is\n>\n> $$\n> u \\cdot v = g (u, v) = g _ {i j} u ^ {i} v ^ {j}.\n> $$\n>\n> The metric tensor is symmetric,\n>\n> $$\n> g (u, v) = g (v, u).\n> $$",
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        "quote": "流形 $M$ 上类型为 (0, 2) 的张量场 $g$ 称为非奇异的，如果 $g _ { p } \\in T ^ { ( 0 , 2 ) }$ 在每一点 $p \\in M$ 处都是非奇异张量。一个 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:e262a216-77fe-4a42-9099-b3672c04584d\" data-concept-route=\"/concept-identities#concept-e262a216-77fe-4a42-9099-b3672c04584d\" id=\"first-ee5625c59c4d344be166-zh\">伪黎曼流形(pseudo-Riemannian manifold)</u> $( M , g )$ 由一个可微流形 $M$ 连同类型为 (0, 2) 的对称非奇异张量场 $g$ 组成，该张量场称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:ac724144-5a08-407a-a27a-796eb367a161\" data-concept-route=\"/concept-identities#concept-ac724144-5a08-407a-a27a-796eb367a161\">度量张量(metric tensor)</u>。这等价于在每一点 $p \\in M$ 处的切空间 $T _ { p } ( M )$ 上定义一个内积 $X _ { p } \\cdot Y _ { p } = g _ { p } ( X _ { p } , Y _ { p } )$（见第 5 章和第 7 章）。我们将假设 $g$ 是可微张量场，从而对于每一对光滑向量场 $X$、$Y \\in { \\mathcal { T } } ( M )$，其内积都是可微函数，",
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        "quote": "A tensor field $g$ of type (0, 2) on a manifold $M$ is said to be non-singular if $g _ { p } \\in T ^ { ( 0 , 2 ) }$ is a non-singular tensor at every point $p \\in M$ . A <u class=\"concept-term\" data-concept-identity=\"urn:uuid:e262a216-77fe-4a42-9099-b3672c04584d\" data-concept-route=\"/concept-identities#concept-e262a216-77fe-4a42-9099-b3672c04584d\" id=\"first-ee5625c59c4d344be166-en\">pseudo-Riemannian manifold</u> $( M , g )$ consists of a differentiable manifold $M$ together with a symmetric non-singular tensor field $g$ of type (0, 2), called a <u class=\"concept-term\" data-concept-identity=\"urn:uuid:ac724144-5a08-407a-a27a-796eb367a161\" data-concept-route=\"/concept-identities#concept-ac724144-5a08-407a-a27a-796eb367a161\">metric tensor</u>. This is equivalent to defining an inner produc $X _ { p } \\cdot Y _ { p } = g _ { p } ( X _ { p } , Y _ { p } )$ on the tangent space $T _ { p } ( M )$ at every point $p \\in M$ (see Chapters 5 and 7). We will assume $g$ is a differentiable tensor field, so that for every pair of smooth vector fields $X$, $Y \\in { \\mathcal { T } } ( M )$ the inner product is a differentiable function,",
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