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Measuring New-Physics Parameters in B Penguin Decays
High Energy Physics - Phenomenology · Submitted 15 Apr 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The knowledge of these parameters allows us to rule out many NP models and thus partially identify the new physics.
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The abstract, sentence by sentence
We examine new-physics (NP) effects in B decays with large b -> s penguin amplitudes. Decays involving b -> d penguins are assumed to be unaffected. We consider a model-independent parametrization of such NP. We argue that NP strong phases are negligible relative to those of the standard model. This allows us to describe the NP effects in terms of a small number of effective amplitudes A_NP^q (q=u,d,s,c) and corresponding weak phases Phi_q. We then consider pairs of neutral B decays which are related by flavour SU(3) in the standard model. One receives a large b -> s penguin component and has a NP contribution; the other has a b -> d penguin amplitude and is unaffected by NP. The time-dependent measurement of these two decays allows the {\it measurement} of the NP parameters A_NP^q and Phi_q. The knowledge of these parameters allows us to rule out many NP models and thus partially identify the new physics.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We examine new-physics (NP) effects in B decays with large b -> s penguin amplitudes. | contribution 0.80 | 0.82 | 0.05 | asserted 0.71 |
| s1 | Decays involving b -> d penguins are assumed to be unaffected. | limitation 0.42 | 0.16 | 0.03 | asserted 0.91 |
| s2 | We consider a model-independent parametrization of such NP. | method 0.64 | 0.82 | 0.03 | asserted 0.89 |
| s3 | We argue that NP strong phases are negligible relative to those of the standard model. | method 0.65 | 0.52 | 0.06 | asserted 0.94 |
| s4 | This allows us to describe the NP effects in terms of a small number of effective amplitudes A_NP^q (q=u,d,s,c) and corresponding weak phases Phi_q. | method 0.88 | 0.73 | 0.08 | asserted 0.93 |
| s5 | We then consider pairs of neutral B decays which are related by flavour SU(3) in the standard model. | method 0.85 | 0.71 | 0.02 | asserted 0.93 |
| s6 | One receives a large b -> s penguin component and has a NP contribution; the other has a b -> d penguin amplitude and is unaffected by NP. | method 0.90 | 0.23 | 0.07 | asserted 1.00 |
| s7 | The time-dependent measurement of these two decays allows the {\it measurement} of the NP parameters A_NP^q and Phi_q. | method 0.77 | 0.45 | 0.53 | asserted 0.98 |
| s8 | The knowledge of these parameters allows us to rule out many NP models and thus partially identify the new physics. | interpretation 0.97 | 0.33 | 0.70 | asserted 0.78 |
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The paper
Original abstract
We examine new-physics (NP) effects in B decays with large b -> s penguin amplitudes. Decays involving b -> d penguins are assumed to be unaffected. We consider a model-independent parametrization of such NP. We argue that NP strong phases are negligible relative to those of the standard model. This allows us to describe the NP effects in terms of a small number of effective amplitudes A_NP^q (q=u,d,s,c) and corresponding weak phases Phi_q. We then consider pairs of neutral B decays which are related by flavour SU(3) in the standard model. One receives a large b -> s penguin component and has a NP contribution; the other has a b -> d penguin amplitude and is unaffected by NP. The time-dependent measurement of these two decays allows the {\it measurement} of the NP parameters A_NP^q and Phi_q. The knowledge of these parameters allows us to rule out many NP models and thus partially identify the new physics.
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References
How the literature uses it
13 arXiv papers cite this in 15 sentences
Papers citing it · 11 sentences without a confident label
Cites it as support 3 papers
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Firstly, a large annihilation contribution to the $B→πK$ decays is an unexpected solution to the $B→πK$ puzzle, as the branching fractions do not favor a sizable annihilation amplitude [ref] which is also supported by model-independent $B→P P$ fits to available data [ref] .
A joint explanation of the $B\to \pi K$ puzzle and the $B \to K \nu \bar{\nu}$ excess · Addressing the B -> pi K puzzle with axion-like particles · 0.98
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The NP strong phases involve only the (constrained) NP operators, and are therefore small [ref] .
New Physics in b -> s mu+ mu-: CP-Violating Observables · CP-violating effects · 0.96
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We expect the strong phases associated with $T^ϕ$ and $C^ϕ$ to be very small [ref] as self-rescattering of these NP amplitudes is intrinsically feeble [ref] .
Flavor Violations in $B$-Mesons within Non-Minimal SU(5) · SU(5) diquark contributions to $$ · 0.98
Cites it as background 1 paper
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There has been a lot of discussion about the possibility of new physics in nonleptonic $B$-decays (for example [ref] ).
Penguin Loops for Nonleptonic B-Decays in the Standard Model: Is there a Penguin Puzzle? · Penguins Contributions from New Physics · 0.99
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