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Simple question from Peskin Schroeder |
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| Sep6-05, 03:14 AM | #1 |
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Simple question from Peskin Schroeder
Gentlemen,
Could you help me please, Im sure it is not even worthy of your attention, but anyway... In Peskin, Schroeder - from expresion [tex] <0|\phi(x)\phi(y)|0> [/tex] survives [tex] <0|a_p a_q^\dag|0> [/tex] so it creates one-particle state |q> at position y and another one-particle state | p> at postion x. But how do I intuitively see that causuality/propagation of particle between these positions is imbeded and considered in that expresion? And another question [tex] <0|\phi(x)|p>=.......e^ipx[/tex] formula 2.42 it's said that it is a position-space representation of the state |p> just as in NR QM <x|p>, so it should be projection of single-particle |p> state onto the <x| baisis and what vectors/basis that state is projected on? where is that <x| vectors in 2.42 P.S. Im sure i missed something very simple in understanding of above and that's why posting such "silly" questions Thanks in advance |
| Sep8-05, 01:45 AM | #2 |
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(1) I think the expresion [tex] <0|\phi(x)\phi(y)|0> [/tex]
survives [tex] <0|a_p a_q^\dag|0> [/tex] means: [tex] <0|a_p^\dag a_q^\dag|0> [/tex]=0 and [tex] <0|a_p a_q|0> [/tex]=0; only [tex] <0|a_p a_q^\dag|0> [/tex] survives, of course p and q are arbitary, not single p and single q. the final result will be an integral over all possible p or q. (2) [tex] <0|\phi(x)=<x|[/tex], this is a simple calculation. there is no special physical significance here, the author, I guess, just mentioned NR case to make the formula be easily understood. |
| Sep8-05, 03:56 AM | #3 |
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but [tex] <0|\phi(x)[/tex] it is a complex conjugation of [tex] \phi(x)|0>[/tex] (as u mentioned in QM forum). So [tex] <0|\phi(x)=\int{\frac{d^3 p}{(2\pi)^3}\frac{1}{2E_p}e^{ipx}<p|[/tex] but with [tex] <0|\phi(x)=<x|[/tex] Im confused <-How/why it's that? |
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