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Qmechanic
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Using the Hausdorff formula I can find the dilation operator at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right].\tag{1} $$$$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right]+\ldots.\tag{1} $$

But isn't the second term zero?

By definition $$D=-ix^\mu \partial_\mu, \qquad P_\mu=-i\partial_\mu\tag{2}$$ then:

$$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align}\tag{3} $$

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

Using the Hausdorff formula I can find the dilation operator at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right].\tag{1} $$

But isn't the second term zero?

By definition $$D=-ix^\mu \partial_\mu, \qquad P_\mu=-i\partial_\mu\tag{2}$$ then:

$$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align}\tag{3} $$

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

Using the Hausdorff formula I can find the dilation operator at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right]+\ldots.\tag{1} $$

But isn't the second term zero?

By definition $$D=-ix^\mu \partial_\mu, \qquad P_\mu=-i\partial_\mu\tag{2}$$ then:

$$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align}\tag{3} $$

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

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Qmechanic
  • 213.1k
  • 48
  • 590
  • 2.3k

Using the Hausdorff formula I can find the dilation opertoroperator at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right]. $$$$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right].\tag{1} $$

But isn't the second term zero?

By definition $D=-ix^\mu \partial_\mu$, $P_\mu=-i\partial_\mu$$$D=-ix^\mu \partial_\mu, \qquad P_\mu=-i\partial_\mu\tag{2}$$ then:

$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align} $$$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align}\tag{3} $$

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

Using the Hausdorff formula I can find the dilation opertor at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right]. $$

But isn't the second term zero?

By definition $D=-ix^\mu \partial_\mu$, $P_\mu=-i\partial_\mu$ then:

$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align} $

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

Using the Hausdorff formula I can find the dilation operator at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right].\tag{1} $$

But isn't the second term zero?

By definition $$D=-ix^\mu \partial_\mu, \qquad P_\mu=-i\partial_\mu\tag{2}$$ then:

$$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align}\tag{3} $$

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

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Qmechanic
  • 213.1k
  • 48
  • 590
  • 2.3k

Using the Hausdorff formula I can find the dilation opertor at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right] $$$$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right]. $$

But isn't the second term zero  ?

By definition $D=-ix^\mu \partial_\mu$, $P_\mu=-i\partial_\mu$ then:

$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align} $

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

Using the Hausdorff formula I can find the dilation opertor at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right] $$

But isn't the second term zero  ?

By definition $D=-ix^\mu \partial_\mu$, $P_\mu=-i\partial_\mu$ then:

$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align} $

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

Using the Hausdorff formula I can find the dilation opertor at all position: $$ e^{i x^\rho P_\rho} D e^{-i x^\rho P_\rho}=D+\left[D,-i x^\rho P_\rho\right]+\frac{1}{2}\left[\left[D,-i x^\rho P_\rho\right],-ix^\sigma P_\sigma\right]. $$

But isn't the second term zero?

By definition $D=-ix^\mu \partial_\mu$, $P_\mu=-i\partial_\mu$ then:

$\begin{align} \left[D,-i x^\rho P_\rho\right] &= [-ix^\mu\partial_\mu, -ix^\rho(-i\partial_\rho)] \\&= -ix^\mu\partial_\mu(-ix^\rho(-i\partial_\rho)) - -ix^\rho(-i\partial_\rho)(-ix^\mu\partial_\mu) \\ &= (-i)^3 x^\mu\partial_\mu(x^\rho(\partial_\rho)) - (-i)^3 x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &= i x^\mu\partial_\mu(x^\rho\partial_\rho) - i x^\rho\partial_\rho(x^\mu\partial_\mu)\\ &=0 \end{align} $

With renaming of indices, this is exactly the same. Very confused because this shouldn't be the case.

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