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  "body": "\n## Summary\n\nA left-invariant vector field on a [[Lie group|7JBRGCVJRB]] is a [[vector field|0299VCW1TH]] that is unchanged by every left translation.\nSuch a field is fixed by its value at the identity, so left-invariant vector fields correspond to tangent vectors at the identity.\nThey are closed under the [[Lie bracket of vector fields|68FGQEBD6J]].\nThis makes the tangent space at the identity a Lie algebra, the Lie algebra of the group.\n\n## Explanations\n\n### L1 human\n\nPick an arrow at the identity element of a Lie group.\nCarry it to every other point $g$ by multiplying on the left by $g$; you get an arrow at every point, all fitting together smoothly.\nOn the plane $\\R^2$ as an additive group, this gives the constant vector fields: the same arrow attached at every point.\nOn the circle group, it gives a field of arrows of the same length all pointing anticlockwise, or all clockwise.\n",
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