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Measurement of Time-Dependent CP Asymmetry in B0->ccbar K(*)0 Decays

High Energy Physics - Experiment · Submitted 10 Feb 2009 · 19 references

Pith's verdict: A careful, statistics-limited update of sin2β from BABAR; the assumptions are stated, the systematics are broken out honestly, and the number is trustworthy.

T0 · AI review

How this review was made: An AI referee (selfhosted/deepseek-v4.1-flash) read the paper on November 11, 2026 and answered a fixed list of questions about it. T0 is the starting level every paper gets. The levels describe how deeply Pith has checked the paper, never the authors.

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  5. T4 Proof Those claims proved, and the proof checked by computer.

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arXiv ID0902.1708 (version 2)
Pith IDLFH5TX4C, Pith's permanent record of this paper and its review
Citationet al, the BABAR Collaboration: B. Aubert. "Measurement of Time-Dependent CP Asymmetry in B0->ccbar K(*)0 Decays." arXiv:0902.1708 (2009). https://pith.science/paper/LFH5TX4C
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Referee report
The paper

The paper claims

BABAR reports sin(2 beta) = 0.687 +/- 0.028 (stat) +/- 0.012 (syst) and C_f = 0.024 +/- 0.020 (stat) +/- 0.016 (syst) from B0 -> charmonium K(*)0 decays, consistent with Standard Model CP violation.

The reading

BABAR studied pairs of B mesons produced at the PEP-II electron-positron collider. One B meson was fully reconstructed in a final state containing a charmonium particle (J/psi, psi(2S), chi_c1, or eta_c) plus a K or K* meson. The other B meson was used to tag whether the reconstructed B was a particle or an antiparticle at the moment it decayed. Because B0 mesons can oscillate into their antiparticles, the decay rate as a function of the difference between the two decay times carries a characteristic oscillation. In the Standard Model, this oscillation has a phase tied to the angle beta of the Cabibbo-Kobayashi-Maskawa quark-mixing matrix. The collaboration fits the decay-time distributions of about 15,500 tagged signal candidates, using a much larger sample of flavor-specific B decays to calibrate how often the tagging is wrong and how well the decay-time difference is measured. The combined fit gives S_f = -eta_f sin(2 beta) = 0.687 +/- 0.028 (stat) +/- 0.012 (syst) and C_f = 0.024 +/- 0.020 (stat) +/- 0.016 (syst). The C_f value is consistent with zero, as expected when direct CP violation is negligible. The paper also reports the first observation of CP violation in the eta_c K_S mode, at 5.4 standard deviations including systematic uncertainties. The result is an updated and more precise version of the collaboration's earlier measurement, not a new theoretical framework.
Extended reading notes

Core claim

The combined fit to J/psi K_S, J/psi K_L, psi(2S) K_S, chi_c1 K_S, eta_c K_S, and J/psi K*0 yields -eta_f S_f = 0.687 +/- 0.028 (stat) +/- 0.012 (syst) and C_f = 0.024 +/- 0.020 (stat) +/- 0.016 (syst), with sin(2 beta) = 0.687 +/- 0.028 under the Standard Model assumption C_f = 0.

Load-bearing premise

The extraction of sin(2 beta) from S_f assumes that direct CP violation and CP violation in B0-B0bar mixing are negligible in b -> c cbar s decays, so that C_f = 0 and lambda_f = eta_f exp(-2 i beta). This is stated in Section I and is not tested by the fit. The measured C_f is consistent with zero, but its uncertainty is 0.020 (stat) and 0.016 (syst), so a nonzero C_f would shift the interpretation of S_f as sin(2 beta).

Original abstract

We present updated measurements of time-dependent CP asymmetries in fully reconstructed neutral B decays containing a charmonium meson. The measurements reported here use a data sample of (465+/-5) million Upsilon(4S)->BBbar decays collected with the Babar detector at the PEPII asymmetric energy e+e- storage rings operating at the SLAC National Accelerator Laboratory. The time-dependent CP asymmetry parameters measured from JpsiKs, JpsiKL, Psi(2S)Ks, Chi_c1Ks, eta_cKs and JpsiK*0 decays are: C_f = 0.024+/-0.020(stat)+/-0.016(syst) and -\eta_f S_f = 0.687+/-0.028(stat)+/-0.012(syst).

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 3,229 input tokens, $0.0001 reported.

What the abstract itself states, as probabilities: claims first 0.02 · states limitation 0.08 · human participants 0.02 · controlled comparison 0.04 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.08 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

We present updated measurements of time-dependent CP asymmetries in fully reconstructed neutral B decays containing a charmonium meson. The measurements reported here use a data sample of (465+/-5) million Upsilon(4S)->BBbar decays collected with the Babar detector at the PEPII asymmetric energy e+e- storage rings operating at the SLAC National Accelerator Laboratory. The time-dependent CP asymmetry parameters measured from JpsiKs, JpsiKL, Psi(2S)Ks, Chi_c1Ks, eta_cKs and JpsiK*0 decays are: C_f = 0.024+/-0.020(stat)+/-0.016(syst) and -\eta_f S_f = 0.687+/-0.028(stat)+/-0.012(syst).

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We present updated measurements of time-dependent CP asymmetries in fully reconstructed neutral B decays containing a charmonium meson. contribution 1.00 0.95 0.21 asserted 0.99
s1 The measurements reported here use a data sample of (465+/-5) million Upsilon(4S)->BBbar decays collected with the Babar detector at the PEPII asymmetric energy e+e- storage rings operating at the SLAC National Accelerator Laboratory. method 1.00 0.64 0.03 asserted 0.99
s2 The time-dependent CP asymmetry parameters measured from JpsiKs, JpsiKL, Psi(2S)Ks, Chi_c1Ks, eta_cKs and JpsiK*0 decays are: C_f = 0.024+/-0.020(stat)+/-0.016(syst) and -\eta_f S_f = 0.687+/-0.028(stat)+/-0.012(syst). result 1.00 0.97 0.80 asserted 1.00

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from observation or experiment 0.75.

What was examined, and what was not

sources read
  • arXiv listing abstract v2
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures
Figure 1. FIG. 1: Distributions for
Figure 2. shows the ∆t distributions and asymmetries in yields between events with B0 and B0 tags for the ηf = −1 and ηf = +1 samples as a function of ∆t, overlaid with the projection of the likelihood fit result
Figure 3. FIG. 3: Time-dependent asymmetry between unmixed and
Figure 4. FIG. 4: a) Number of

Figures reproduced from arXiv:0902.1708 by the authors.

References
How later papers used it

47 later papers cite it

Evidence: substantial. 44 of the citing papers share no author with it, and 23 of those carry a confident label from Pith's citation classifier.

Pith read 17 of the 55 citing sentences, choosing only those whose citation markers point at this paper alone, and wrote the paraphrases from them. The summary, the counts, the evidence level, the links and the quotes come from code; the summary counts the papers listed below. A later paper is listed under a label when Pith's citation classifier gives one of its sentences that label at probability 0.8 or more (0.95 for support), Pith's reading finds that the citing paper itself did it, and a second check confirms the paraphrase against the sentence. This section lists uses only. It does not list criticism or disagreement, so their absence here says nothing about how the paper has been received. Papers that share an author with this one are listed apart, under "By the same authors". A quote is the citing authors' own sentence, shown when their paper's licence is CC BY, CC BY-SA or CC0. JSON

Uses its method or tool 3 of 4 papers with this label · 2 by the same authors

By the same authors

Uses its data or values 1 of 17 papers with this label
How the literature uses it

43 arXiv papers cite this in 51 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers whose main result relates to this one's

Found among the papers closest to this one by title and main claim. Pith's classifier compared each pair's main results and a second model family confirmed the relation; checked against two further families, shown conflicts agreed 118 times in 120 and shown same results 218 times in 239. The quoted sentence is the other paper's main claim.

States the same result 1 paper

Papers citing it · 23 sentences without a confident label

Uses its method or tool 4 papers
  • The other pairings of reference and transformed transitions can be found in Refs. [ref] [ref] .] The standard flavour tagging techniques developed for the violation discovery measurement are used in order to select and mesons, and the selection of even and odd filter basis pairs, for $b→ccs$ transitions differ by a vs a in the final state (see for example [ref] ).

    Symmetry violations at BaBar · Other symmetry tests in meson decay · 0.83

  • The three other variables entering the BDT are the absolute value of the cosine of the angle between the direction and the collision axis, the zeroth-order momentum-weighted Legendre polynomial moment, and the absolute value of the output of another BDT used for “flavor tagging”, , for distinguishing from decays using inclusive properties of the decay of the other meson in the $→$ event [ref] .

    Evidence for $CP$ violation in $B^{+} \to K^{*}(892)^{+} \pi^{0}$ from a Dalitz plot analysis of $B^{+} \to K^{0}_{\rm S} \pi^{+} \pi^{0}$ decays · Event selection · 0.93

  • The three other variables entering the neural network are the absolute value of the cosine of the angle between the direction and the beam axis, the absolute value of the cosine of the angle between the thrust axis and the beam axis, and the absolute value of the output of a neural network used for “flavor tagging”, , for distinguishing from decays using inclusive properties of the decay of the other meson in the $→$ event [ref] .

    Observation of the rare decay B+->K+pi0pi0 and measurement of the quasi-two body contributions B+->K*(892)+pi0, B+->f0(980)K+ and B+->chic0K+ · Event reconstruction and selection · 0.93

Uses its data or values 16 papers
  • Using the results of [ref] and Eq. [ref] we get, at $2σ$, [equation]

    Subtleties in the BaBar measurement of time-reversal violation · Relevant data · 1.00

  • In our $B$ decay to $J/ΨK$, the CP-odd final state of [ref] can be approximated by [equation] and CP-even final state of [ref] can be approximated by [equation] where $Δm_B=0.463$ps$^-1$ is fixed [ref] , which are shown in Fig.[ref].

    Cartan's Supersymmetry and the violation of CP symmetry · Cartan's supersymmetry and weak interactions · 0.92

  • The factories were optimised for this measurement [ref] and determined [ref] $sin2β^B-fact = 0.682 ±0.019$, which is the most precise constraint on the UT (Figure [ref]).

    The CKM Parameters · INDIVIDUAL CONSTRAINTS · 0.99

Compares with it 4 papers
Cites it as background 4 papers

Discussion

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