We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) reaction at ω=0.439GeV and Q2=0.8(GeV/c)2 for missing momentum Pmiss≤355MeV/c. We have extracted the response functions RL+TT, RT, RLT, and the left-right asymmetry, ALT, for the 1p1/2 and the 1p3/2 states. The data are well described by relativistic distorted wave impulse approximation calculations. At large Pmiss, the structure observed in ALT indicates the existence of dynamical relativistic effects. (APS
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the O-16(e,e'p) reac...
We have measured the cross section for quasielastic 1p-shell proton knockout in the O-16(e,e'p) reac...
The authors have measured the cross section for quasielastic 1 {rho}-shell proton knockout in the (s...
Coincidence cross sections and the structure functions R{sub L+TT},#2; R{sub T} and R{sub LT} have b...
The physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed inves...
The physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed inves...
The physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed inves...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e′p) react...
We have measured the cross section for quasielastic 1p-shell proton knockout in the O-16(e,e'p) reac...
We have measured the cross section for quasielastic 1p-shell proton knockout in the O-16(e,e'p) reac...
The authors have measured the cross section for quasielastic 1 {rho}-shell proton knockout in the (s...
Coincidence cross sections and the structure functions R{sub L+TT},#2; R{sub T} and R{sub LT} have b...
The physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed inves...
The physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed inves...
The physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed inves...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...
PHASEThe physics program in Hall A at Jefferson Lab commenced in the summer of 1997 with a detailed ...