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In geometry and physics, spinors (pronounced "spinner"; /spɪnər/) are elements of a complex vector space that can be associated with Euclidean space. Spinors can be thought of as companion geometric objects to Euclidean space that, like Euclidean vectors, respond when the Euclidean space is subjected to a rotation. A spinor transforms linearly when the…
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| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Spinor | is a | complex 2-component column vector v | 0.90 | text |
| Spinor | is a | element of a finite-dimensional group representation of the spin group on which the center acts non-trivially.OverviewThere are essentially two frameworks for viewing the notion… | 0.90 | text |
| Spinor | is a | element of the vector space V | 0.90 | text |
| Spinor | is a | section of the full complex spinor bundle | 0.90 | text |
| Spinor | is a | spinor satisfying a reality condition | 0.90 | text |
| Spinor | is a | ordinary complex number | 0.90 | text |
| coordinate systems | instance of | construction of them that does not rely on arbitrary choices | 0.80 | text |
| Euclidean space with its standard dot product | instance of | with any vector space equipped with a quadratic form | 0.80 | text |
| or Minkowski space with its Lorentz metric | instance of | with any vector space equipped with a quadratic form | 0.80 | text |
| the Dirac equation | instance of | when the relevant spin representation admits one.Spinor fields enter physics through equations | 0.80 | text |
| the Weyl equation | instance of | when the relevant spin representation admits one.Spinor fields enter physics through equations | 0.80 | text |
| which are first-order differential equations on the spinor bundle | instance of | when the relevant spin representation admits one.Spinor fields enter physics through equations | 0.80 | text |
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