$\mathit CP$ VIOLATION PARAMETERS

sin$(2\beta )$

INSPIRE   PDGID:
S042BET
For a discussion of $\mathit CP$ violation, see the review on “$\mathit CP$ Violation” in the Reviews section. sin$(2\beta )$ is a measure of the $\mathit CP$-violating amplitude in the ${{\mathit B}_{{{d}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit K}_S^0}$ .
VALUE DOCUMENT ID TECN  COMMENT
$\bf{ 0.709 \pm0.011}$ OUR EVALUATION  $~~$(Produced by HFLAV)  See the ideogram below.
$\bf{ 0.708 \pm0.017}$ OUR AVERAGE  Error includes scale factor of 1.5.  See the ideogram below.
$0.724$ $\pm0.014$ 1
AAIJ
2024
LHCB ${{\mathit p}}{{\mathit p}}$ at 7, 8 and 13 TeV
$0.667$ $\pm0.023$ $\pm0.012$ 2
ADACHI
2012A
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$0.57$ $\pm0.58$ $\pm0.06$ 3
SATO
2012
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(5S)}}$
$0.69$ $\pm0.52$ $\pm0.08$ 4
AUBERT
2009AU
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$0.687$ $\pm0.028$ $\pm0.012$ 5
AUBERT
2009K
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$1.56$ $\pm0.42$ $\pm0.21$ 6
AUBERT
2004R
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$0.79$ ${}^{+0.41}_{-0.44}$ 7
AFFOLDER
2000C
CDF ${{\mathit p}}{{\overline{\mathit p}}}$ at $1.8$ TeV
$0.84$ ${}^{+0.82}_{-1.04}$ $\pm0.16$ 8
BARATE
2000Q
ALEP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Z}}$
$3.2$ ${}^{+1.8}_{-2.0}$ $\pm0.5$ 9
ACKERSTAFF
1998Z
OPAL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Z}}$
• • We do not use the following data for averages, fits, limits, etc. • •
$0.717$ $\pm0.013$ $\pm0.008$ 10, 11
AAIJ
2024
LHCB ${{\mathit p}}{{\mathit p}}$ at 13 TeV
$0.760$ $\pm0.034$ 10, 12
AAIJ
2017BN
LHCB ${{\mathit p}}{{\mathit p}}$ at 7, 8 TeV
$0.72$ $\pm0.09$ $\pm0.03$ 13
SAHOO
2008
BELL Repl. by ADACHI 2012A
$0.714$ $\pm0.032$ $\pm0.018$ 5
AUBERT
2007AY
BABR Repl. by AUBERT 2009K
$0.642$ $\pm0.031$ $\pm0.017$
CHEN
2007
BELL Repl. by ADACHI 2012A
$0.728$ $\pm0.056$ $\pm0.023$ 14
ABE
2005B
BELL Repl. by CHEN 2007
$0.722$ $\pm0.040$ $\pm0.023$ 15
AUBERT
2005F
BABR Repl. by AUBERT 2007AY
$0.99$ $\pm0.14$ $\pm0.06$ 16
ABE
2002U
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$0.719$ $\pm0.074$ $\pm0.035$ 17
ABE
2002Z
BELL Repl. by ABE 2005B
$0.59$ $\pm0.14$ $\pm0.05$ 18
AUBERT
2002N
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$0.741$ $\pm0.067$ $\pm0.034$ 19
AUBERT
2002P
BABR Repl. by AUBERT 2005F
$0.58$ ${}^{+0.32}_{-0.34}$ ${}^{+0.09}_{-0.10}$
ABASHIAN
2001
BELL Repl. by ABE 2001G
$0.99$ $\pm0.14$ $\pm0.06$ 20
ABE
2001G
BELL Repl. by ABE 2002Z
$0.34$ $\pm0.20$ $\pm0.05$
AUBERT
2001
BABR Repl. by AUBERT 2001B
$0.59$ $\pm0.14$ $\pm0.05$ 20
AUBERT
2001B
BABR Repl. by AUBERT 2002P
$1.8$ $\pm1.1$ $\pm0.3$ 21
ABE
1998U
CDF Repl. by AFFOLDER 2000C
1  A combination of this Run 2 result with the Run 1 result from AAIJ 2017BN is reported with a correlation coefficient of 0.40.
2  Measurement based on ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}_S^0}$ , ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit K}_S^0}$ , ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}_L^0}$ , and ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit \chi}_{{{c1}}}{(1P)}}{{\mathit K}_S^0}$ decays.
3  SATO 2012 uses 121 fb${}^{-1}$ data collected on ${{\mathit Y}{(5S)}}$ resonance. Uses the ''${{\mathit B}}−{{\mathit \pi}}$ tagging'' where ${{\mathit B}}{{\mathit \pi}^{+}}$ and ${{\mathit B}}{{\mathit \pi}^{-}}$ tagged ${{\mathit J / \psi}}{{\mathit K}_S^0}$ events are compared.
4  Uses Dalitz plot analysis of ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit K}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ decays and the first of two equivalent solutions.
5  Measurement based on ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}{{\mathit K}^{(*)0}}$ decays.
6  Measurement in which the ${{\mathit J / \psi}}$ decays to hadrons or to muons that do not satisfy the standard identification criteria.
7  AFFOLDER 2000C uses about 400 ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit K}_S^0}$ events. The production flavor of ${{\mathit B}^{0}}$ was determined using three tagging algorithms: a same-side tag, a jet-charge tag, and a soft-lepton tag.
8  BARATE 2000Q uses 23 candidates for ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit K}_S^0}$ decays. A combination of jet-charge, vertex-charge, and same-side tagging techniques were used to determine the ${{\mathit B}^{0}}$ production flavor.
9  ACKERSTAFF 1998Z uses 24 candidates for ${{\mathit B}_{{{d}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit K}_S^0}$ decay. A combination of jet-charge and vertex-charge techniques were used to tag the ${{\mathit B}_{{{d}}}^{0}}$ production flavor.
10  Measurement based on ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}_S^0}$ , ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit K}_S^0}$ with ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$, ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ and ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$.
11  AAIJ 2024 provides the correlation coefficient ${{\mathit \rho}}$ = 0.441 between the uncertainties of sin$(2\beta )$ and $\mathit C_{{{\mathit c}} {{\overline{\mathit c}}} {{\mathit K}^{(*)0}} }$ (${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}{{\mathit K}^{(*)0}}$ ) measurements.
12  AAIJ 2017BN provides the correlation coefficient ${{\mathit \rho}}$ = 0.42 between the uncertainties of sin$(2\beta )$ and cos $(2\beta )$ measurements.
13  Based on ${{\mathit B}^{0}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit K}_S^0}$ decays.
14  Measurement based on $152 \times 10^{6}{{\mathit B}}{{\overline{\mathit B}}}$ pairs.
15  Measurement based on $227 \times 10^{6}{{\mathit B}}{{\overline{\mathit B}}}$ pairs.
16  ABE 2002U result is based on the same analysis and data sample reported in ABE 2001G.
17  ABE 2002Z result is based on $85 \times 10^{6}{{\mathit B}}{{\overline{\mathit B}}}$ pairs.
18  AUBERT 2002N result based on the same analysis and data sample reported in AUBERT 2001B.
19  AUBERT 2002P result is based on $88 \times 10^{6}{{\mathit B}}{{\overline{\mathit B}}}$ pairs.
20  First observation of $\mathit CP$ violation in ${{\mathit B}^{0}}$ meson system.
21  ABE 1998U uses $198$ $\pm17$ ${{\mathit B}_{{{d}}}^{0}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit K}^{0}}$ events. The production flavor of ${{\mathit B}^{0}}$ was determined using the same side tagging technique.

           sin$(2\beta )$
Conservation Laws:
$\mathit CP$ VIOLATION OBSERVED
References