| 1. | In special relativity, all four tensors transform under Lorentz transformations.
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| 2. | That requirement leads to the Lorentz transformation for space and time.
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| 3. | These numbers can be double-checked using the Lorentz transformation.
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| 4. | A particular Minkowski diagram illustrates the result of a Lorentz transformation.
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| 5. | The Lorentz transformations on the other hand is a different topic.
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| 6. | This property is the defining property of a Lorentz transformation.
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| 7. | It has in addition a set of preferred transformations Lorentz transformations.
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| 8. | In particular, a Lorentz scalar is invariant under a Lorentz transformation.
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| 9. | This component can be found from an appropriate Lorentz transformation.
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| 10. | Correctly expresses the transformation of the electromagnetic field under the Lorentz transformation.
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