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| Tags: angular, between, exchange, momentum, particle, question, relation, symmetry |
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#1
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I have a problem understanding a point in the book "particle physics"
by B.R.Martin and G.shaw. The question is as following. A pair of pion_plus-pion_minus is supposed to be in a state of definite orbital angular momentum L . Now we apply charge conjugation operator on this state which exchanges the two particles. According the book, the resultant state vector is just (-1)^L times the original state vector, "BECAUSE interchanging the pion_plus and pion_minus reverses their relative position vector in the spatial wavefuction". I just can not understand this "BECAUSE"! Could some one show me the detail of the deduction. Thank you so much! |
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#2
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wrote in message
oups.com... I have a problem understanding a point in the book "particle physics" by B.R.Martin and G.shaw. The question is as following. A pair of pion_plus-pion_minus is supposed to be in a state of definite orbital angular momentum L . Now we apply charge conjugation operator on this state which exchanges the two particles. According the book, the resultant state vector is just (-1)^L times the original state vector, "BECAUSE interchanging the pion_plus and pion_minus reverses their relative position vector in the spatial wavefuction". I just can not understand this "BECAUSE"! Could some one show me the detail of the deduction. Thank you so much! The wave function for odd L is anti-symmetric: psi( x ) = - psi( - x ) psi( x1, x2 ) = - psi( x2, x1 ) [Old Man] |
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