equation 5.162 eq:rep-special-orthogonal

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Supports

• depends_on definition 5.131 Isotropic Cartesian tensor ¶
  • depends_on definition A.672 The octahedral rotation group ¶
    • depends_on proposition A.673 Cubic tensors of rank four ¶
      • depends_on theorem A.675 Three constants for a cubic crystal, two for an isotropic solid ¶
        • depends_on remark A.676 The third cubic constant is measured, and it is not small ¶
  • depends_on lemma 5.132 Parity constraint ¶
    • depends_on theorem 5.133 Isotropic Cartesian tensors of rank at most four ¶
      • depends_on lemma A.742 Isotropic representation ¶
        • depends_on corollary A.743 Two scalar functions instead of a tensor field ¶
        • depends_on lemma A.747 The third-order structure functions ¶
        • depends_on lemma A.744 Vanishing of the pressure–velocity correlation ¶
      • depends_on lemma A.671 The three products are independent ¶
        • depends_on proposition A.673 Cubic tensors of rank four ¶ ↺
      • depends_on lemma 30.26 Isotropic Cartesian tensors of rank four ¶
        • depends_on phenomenon 30.28 Hooke's law ¶
      • depends_on remark A.677 The lower ranks, and why an isotropic solid is not piezoelectric ¶
      • depends_on remark 30.27 Two results this chapter borrows from Part II ¶
      • depends_on remark 13.7 What the classification is used for ¶
• depends_on lemma 5.132 Parity constraint ¶ ↺