# Commutator of charges in QFT

• nrqed

#### nrqed

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Consider the SUSY charge

$$Q= \int d^3y~ \sigma^\mu \chi~ ~\partial_\mu \phi^\dagger~$$

The SUSY transformation of fields, let's say of the scalar field, can be found using the commutator

$$i [ \epsilon \cdot Q, \phi(x)] = \delta \phi(x)$$

using the equal time commutator

$$[\phi(\vec{x},t), \dot{\phi}^\dagger(\vec{y},t) ] = \delta^3(\vec{x} - \vec{y})$$

Everything works fine at the condition of assuming that the time in $$\phi^\dagger(y)$$ is equal to the time in in $$\phi(x)$$ .

However, I don't see why we need to assume this. The charge is time independent so we should be able to use whatever time we like to calculate the commutator. But if we pick a different time than the time of $$\phi(x)$$, we get zero for the transformation of the scalar field, which is incorrect.

So why do we need to set the two times equal?

Patrick

The reason for it is called the equal time commutator is simply that it is defined to be like that. At least that is the impression I have by reading 7 introductory books on QFT. Nothing deeper than "in the spirit of non Rel QM"...

But the reason for choosing equal time then is that one includes time dependence by Heisenberg picture, i.e we start with time INDEP. fields, and then have the commutator:
$$[\phi(\vec{x}), \dot{\phi}^\dagger(\vec{y}) ] = \delta^3(\vec{x} - \vec{y})$$

Then we add the time dependence of the fields, which are operators in QFT, by Heisenberg picture.

See e.g. page 41 in srednicki's textbook

http://www.physics.ucsb.edu/~mark/ms-qft-DRAFT.pdf

The reason for it is called the equal time commutator is simply that it is defined to be like that. At least that is the impression I have by reading 7 introductory books on QFT. Nothing deeper than "in the spirit of non Rel QM"...

But the reason for choosing equal time then is that one includes time dependence by Heisenberg picture, i.e we start with time INDEP. fields, and then have the commutator:
$$[\phi(\vec{x}), \dot{\phi}^\dagger(\vec{y}) ] = \delta^3(\vec{x} - \vec{y})$$

Then we add the time dependence of the fields, which are operators in QFT, by Heisenberg picture.

See e.g. page 41 in srednicki's textbook

http://www.physics.ucsb.edu/~mark/ms-qft-DRAFT.pdf

Hi Malawi Glenn,