|
|
|
|
LEADER |
01957 am a22002413u 4500 |
001 |
94637 |
042 |
|
|
|a dc
|
100 |
1 |
0 |
|a Counts, Ian Thomas Hunt
|e author
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Physics
|e contributor
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Laboratory for Nuclear Science
|e contributor
|
100 |
1 |
0 |
|a Counts, Ian Thomas Hunt
|e contributor
|
100 |
1 |
0 |
|a Ilten, Philip James
|e contributor
|
100 |
1 |
0 |
|a Williams, M.
|e contributor
|
700 |
1 |
0 |
|a Ilten, Philip James
|e author
|
700 |
1 |
0 |
|a Williams, M.
|e author
|
245 |
0 |
0 |
|a Measurement of the CP-violating phase β in B[superscript 0] → [J over ψ π[superscript +] π[superscript -]] decays and limits on penguin effects
|
260 |
|
|
|b Elsevier,
|c 2015-02-19T17:04:09Z.
|
856 |
|
|
|z Get fulltext
|u http://hdl.handle.net/1721.1/94637
|
520 |
|
|
|a Time-dependent CP violation is measured in the [(-) over B][superscript 0] → [J over ψ]π[superscript +]π[superscript −] channel for each π[superscript +]π[superscript −] resonant final state using data collected with an integrated luminosity of 3.0 fb[superscript −1] in pp collisions using the LHCb detector. The final state with the largest rate, [J over ψρ][superscript 0](770), is used to measure the CP -violating angle 2β[superscript eff] to be (41.7±9.6[superscript +2.8][subscript -6.3])°. This result can be used to limit the size of penguin amplitude contributions to CP violation measurements in, for example, [(-) over B][superscript 0] [subscript s] → [J over ψϕ] decays. Assuming approximate SU(3) flavour symmetry and neglecting higher order diagrams, the shift in the CP-violating phase [subscript ϕs] is limited to be within the interval [−1.05°,+1.18°] at 95% confidence level. Changes to the limit due to SU(3) symmetry breaking effects are also discussed.
|
520 |
|
|
|a National Science Foundation (U.S.)
|
546 |
|
|
|a en_US
|
655 |
7 |
|
|a Article
|
773 |
|
|
|t Physics Letters B
|