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        "quote": "Just as in the non-relativistic case, the space of solutions to the equation of motion provides a representation of the group of space-time symmetries of the theory. This group will now be the [<u class=\"concept-term\" data-concept-reference=\"concepts/lie-theory/poincare-group\" data-concept-identity=\"urn:uuid:b9250f96-c06a-4ae1-ab1f-8035202bea26\" data-concept-route=\"/concept-identities#concept-b9250f96-c06a-4ae1-ab1f-8035202bea26\" id=\"first-4c72e0fabfe1ab841067-en\">Poincaré group</u>](../../../../../concepts/lie-theory/poincare-group), a ten dimensional group which includes a four dimensional subgroup of translations in space-time, and a six dimensional subgroup (the Lorentz group), which combines spatial rotations and “boosts” (transformations mixing spatial and time coordinates). The representation of the Poincaré group on the solutions to the relativistic wave equation will in general be reducible. Irreducible such representations will be the objects corresponding to elementary particles. This chapter will deal with the Lorentz group itself, chapter 41 with its representations, and chapter 42 will move on to the Poincaré group and its representations.",
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