remark 24.11 The SI dimension of every object in this chapter

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remark 24.11: The SI dimension of every object in this chapter24.11proposition 24.10: The canonical form is symplectic and intrinsic24.10remark 22.5: Units22.5remark 24.35: What non-squeezing does and does not say about nature24.35remark 24.22: Liouville's theorem is the foundation of statistical mechanics24.22remark 24.27: Fixing a scale, so that a ``ball'' means something24.27definition 13.52: Differential; pushforward13.52definition 24.9: The canonical form on a cotangent bundle24.9lemma 13.107: Poincaré lemma13.107proof : ch:07-symplectic-geometry@proof-3proofequation 22.1: eq:ham-hamiltonian22.1equation 21.43: eq:lag-generalized-momentum21.43remark 22.36: The whole dynamics in one operation22.36remark 22.42: What the matrix form is for22.42theorem 24.16: The Hamiltonian flow preserves the symplectic form24.16theorem 24.31: Gromov's non-squeezing theorem24.31theorem 24.21: Liouville24.21equation 22.56: eq:ham-symplectic-matrix22.56definition 24.28: Ball and cylinder24.28definition 24.33: Symplectic capacity24.33

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depends_on The canonical form is symplectic and intrinsic declared parts/03-classical-mechanics/07-symplectic-geometry.tex:346
depends_on Units declared parts/03-classical-mechanics/07-symplectic-geometry.tex:346
depends_on What non-squeezing does and does not say about nature declared parts/03-classical-mechanics/07-symplectic-geometry.tex:1225
depends_on Liouville's theorem is the foundation of statistical mechanics declared parts/03-classical-mechanics/07-symplectic-geometry.tex:733
depends_on Fixing a scale, so that a ``ball'' means something declared parts/03-classical-mechanics/07-symplectic-geometry.tex:942