Can the Displacement Operator Rotate a Photonic State in Phase Space?

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naima
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Hi PF

I read the definition of the displacement operator:
##D(\lambda) = e^{\lambda a^\dagger - \lambda ^* a}##
but i did not find how this operator can be implemented say in a cavity with a photonic state inside.
Could you give me links?
thanks.
 
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Danke Vanhees71
I read in this wiki
""...letting the unitary displacement operator D(α) operate..."
The problem is not to let it operate. The problem is to prepare a device which will enable an experimentalist to displace a sate by ##\alpha##
I read the external links at the end of the article but i did not find any device's
description. I think that it needs pulses but with which interaction?
 
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Mandel & Wolf (sect. 11.13, p568) give a derivation of the field produced by a time-dependent classical current, and show (iiuc) that it's a coherent state. As the current changes, the state changes continuously, but it's always a coherent state. I.e., changing the current is equivalent (in that case) to acting with a ##D(\alpha)##--like operator.
 
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Thanks
I found the same in another book (Gerry and Knight)
http://qiqo.hznu.edu.cn/upLoad/down/month_1406/201406231000574799.pdf
Skip to "generating a coherent state" p52
 
Suppose that, using a pulse during t, i displace the vacuum to a gaussian centered around a point P in the phase space. This point will rotate in this plane. At a given moment the gaussian will be centerd around -P. If i apply the same pulse will the atom return to its vacuum?
If yes how can we know when we have to light the atom ?Edit
As i have many copies of the ground state |g> i can vary the ##\Delta t## between two pulses and for which it returms to |g> and know the rotation period.
 
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