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        "quote": "图 7.1：[<u class=\"concept-term\" data-concept-reference=\"concepts/topology/real-projective-line\" data-concept-identity=\"urn:uuid:ce618650-9f53-49e2-ab6f-718ffe06a89e\" data-concept-route=\"/concept-identities#concept-ce618650-9f53-49e2-ab6f-718ffe06a89e\" id=\"first-cdbf26767d2e19aff4dc-zh\">实射影直线(real projective line)</u>](../../../../../concepts/topology/real-projective-line.md) $\\mathbf{R}P^1$",
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        "quote": "Figure 7.1: The [<u class=\"concept-term\" data-concept-reference=\"concepts/topology/real-projective-line\" data-concept-identity=\"urn:uuid:ce618650-9f53-49e2-ab6f-718ffe06a89e\" data-concept-route=\"/concept-identities#concept-ce618650-9f53-49e2-ab6f-718ffe06a89e\" id=\"first-cdbf26767d2e19aff4dc-en\">real projective line</u>](../../../../../concepts/topology/real-projective-line.md) $\\mathbf{R}P^1$",
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        "quote": "每条这样的直线都与单位圆交于一对对跖点。因此，所有这类直线可以用一个半圆参数化，并把半圆两端视为同一点。这个空间称为[<u class=\"concept-term\" data-concept-reference=\"concepts/topology/real-projective-line\" data-concept-identity=\"urn:uuid:ce618650-9f53-49e2-ab6f-718ffe06a89e\" data-concept-route=\"/concept-identities#concept-ce618650-9f53-49e2-ab6f-718ffe06a89e\">实射影直线(real projective line)</u>](../../../../../concepts/topology/real-projective-line.md) $\\mathbf{R}P^1$。在更高维中，$\\mathbf{R}^n$ 内过原点的直线所成的空间称为[<u class=\"concept-term\" data-concept-reference=\"concepts/topology/real-projective-space\" data-concept-identity=\"urn:uuid:75e9bd12-9b58-4080-8f6c-d42cdf594c77\" data-concept-route=\"/concept-identities#concept-75e9bd12-9b58-4080-8f6c-d42cdf594c77\" id=\"first-6cbaf7163cfb07bdaad4-zh\">实射影空间(real projective space)</u>](../../../../../concepts/topology/real-projective-space.md) $\\mathbf{R}P^{n-1}$；它可以表示为 $\\mathbf{R}^n$ 中将对跖点视为同一点的单位球面。回顾[第 6.2.3 节](../chapter-06/02-spin-groups-in-three-and-four-dimensions#section-6-2-3)，$SO(3)$ 可与 $\\mathbf{R}P^3$ 等同。",
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        "quote": "Each such line intersects the unit circle at two antipodal points. Thus the set of lines can be parametrized by a semicircle with its two endpoints identified. This space is called the [<u class=\"concept-term\" data-concept-reference=\"concepts/topology/real-projective-line\" data-concept-identity=\"urn:uuid:ce618650-9f53-49e2-ab6f-718ffe06a89e\" data-concept-route=\"/concept-identities#concept-ce618650-9f53-49e2-ab6f-718ffe06a89e\">real projective line</u>](../../../../../concepts/topology/real-projective-line.md) $\\mathbf{R}P^1$. In higher dimensions, the space of lines through the origin in $\\mathbf{R}^n$ is the [<u class=\"concept-term\" data-concept-reference=\"concepts/topology/real-projective-space\" data-concept-identity=\"urn:uuid:75e9bd12-9b58-4080-8f6c-d42cdf594c77\" data-concept-route=\"/concept-identities#concept-75e9bd12-9b58-4080-8f6c-d42cdf594c77\" id=\"first-6cbaf7163cfb07bdaad4-en\">real projective space</u>](../../../../../concepts/topology/real-projective-space.md) $\\mathbf{R}P^{n-1}$; it can be represented by the unit sphere in $\\mathbf{R}^n$ with antipodal points identified. In particular, recall from [Section 6.2.3](../chapter-06/02-spin-groups-in-three-and-four-dimensions#section-6-2-3) that $SO(3)$ is identified with $\\mathbf{R}P^3$.",
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