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Is there a way to prove that the Kronecker delta $\delta_{ij}$ is indeed the only isotropic second order tensor (i.e. invariant under rotation), i.e. so we can write $T_{ij} = \lambda \delta_{ij}$ for some constant $\lambda$?

By rotational invariance I mean: $$ T_{ij} = T^\prime_{ij} = R_{ip} R_{jq} T_{pq}\text{,} $$ where the matrices $R_{ij}$ are orthogonal.

It is very straightforward to show that $\delta_{ij}$ is invariant, but how can I show that it is unique?

mSSM
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2 Answers2

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There is a simpler proof at http://www.damtp.cam.ac.uk/user/reh10/lectures/nst-mmii-chapter3.pdf, pg 61, that proceeds as follows

Starting with an isotrophic 2nd order tensor written in matrix form Tij, its coordinates are rotated 90 deg. around the 3 axis to get T'ij, then by comparing T'ij (which equals Tij as T is isotrophic) and Tij and concluding by inspection that T11 = T22, T13 = T23 = -T13 = 0, T31 = T32 = -T31 = 0, and then rotating the coordinates 90% about the 2 axis to conclude that T11 = T33 and T21 = T32 = 0 and T21 = T23 = 0.

That is, the proof is simplicity itself and is given in detail in the reference.

DrWill
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Step 1: Realize $T$ is diagonal. Let $$R_{kl}=\begin{cases} -1 & \text{if }k=l=j\\ \delta_{kl} & \text{otherwise}\\ \end{cases}$$ therefore $R$ is the reflection w.r.t to the hyperplane perpendicular to the j-th vector in the standard ordered basis. $$R=R^T\land R^2=I\Rightarrow R^TR=RR^T=I$$ Therefore: $$T_{ij}=\sum_{p,q}R_{ip}R_{jq}T_{pq}=R_{ii}R_{jj}T_{ij}\\ i\neq j\Rightarrow T_{ij}=-T_{ij}\Rightarrow T_{ij}=0$$


Step 2: Realize $T_{jj} = T_{11}$. Let $$P_{kl}=\begin{cases} \delta_{jl} & \text{if } k=1\\ \delta_{1l} & \text{if } k=j\\ \delta_{kl} & \text{otherwise} \end{cases}$$ therefore $P$ is the permutation matrix that interchanges the 1st and j-th rows on left multiplication. $$(P^TP)_{kl}=\sum_{m}P^T_{km}P_{ml}=\sum_{m}P_{mk}P_{ml}=\sum_{m\neq1,j}P_{mk}P_{ml}+\sum_{m=1,j}P_{mk}P_{ml}\\ =\sum_{m\neq1,j}\delta_{mk}\delta_{ml}+\delta_{jk}\delta_{jl}+\delta_{1k}\delta_{1l}=\sum_{m}\delta_{mk}\delta_{ml}=\delta_{kl}$$ Therefore: $$T_{jj}=\sum_{p,q}P_{jp}P_{jq}T_{pq}=\sum_{q}P_{jq}^2T_{qq}=\sum_{q}\delta_{1q}^2T_{qq}=\sum_{q}\delta_{1q}T_{qq}=T_{11}$$

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    wow, whole answer in math mode :D – MyUserIsThis Jun 06 '15 at 08:16
  • It is actually a horrible idea to compose your whole answer in math mode. It make it difficult to copy the text for some people (when you right click a formula a different menu pops up), screen readers will not work correctly (for visually-impaired people), on mobile devices the formulas with a big width are a pain, etc. Please consider writing only formulas in math mode. – Najib Idrissi Dec 17 '15 at 14:13
  • The very first argument: why do you assume that $R_{ij}$ has that form? – mSSM Mar 31 '16 at 11:05
  • @mSSM I don't assume every orthogonal R has that form. That R is a tensor which meets the criterion of orthogonality and which is designed in that specific way for the purpose of bringing out the diagonal nature of T. – Jack's wasted life Mar 31 '16 at 12:16
  • @Jack'swastedlife Why do we assume T is diagonal? – f_garcia May 20 '21 at 01:58
  • @FernandoGarciaCortez Step 1 proves T is diagonal, we don't have to assume anything. – Jack's wasted life May 27 '21 at 19:58