裂隙
发表于 2025-3-25 05:01:30
Growth Theory of Digital EconomicsAs we have discussed in Sect. 1.2, flavour processes such as rare B decays are excellent probes of new physics at the electroweak scale and beyond, due to their strong suppression in the SM.
性冷淡
发表于 2025-3-25 11:11:50
Institutional Economics in the Digital EraAs we have seen in Sect. 2.4.2, the SM contribution to meson mixing arises at the 1-loop level and is both CKM and GIM suppressed. This makes these observables highly sensitive to new physics contributions (an issue which we will explore further in Chap. 7), and so a precise knowledge of the theoretical predictions is very important.
骇人
发表于 2025-3-25 14:26:46
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abracadabra
发表于 2025-3-25 17:26:25
Charming Dark Matter,As discussed in Sect. 1.3.1, dark matter has a long history, but the interactions of DM (outside of its gravitational influence) remain elusive, despite concerted efforts.
ostrish
发表于 2025-3-25 21:15:14
Charming New Physics in Rare , Decays and Mixing?,As we have discussed in Sect. 1.2, flavour processes such as rare B decays are excellent probes of new physics at the electroweak scale and beyond, due to their strong suppression in the SM.
栏杆
发表于 2025-3-26 02:01:24
Dimension-Six Matrix Elements from Sum Rules,As we have seen in Sect. 2.4.2, the SM contribution to meson mixing arises at the 1-loop level and is both CKM and GIM suppressed. This makes these observables highly sensitive to new physics contributions (an issue which we will explore further in Chap. 7), and so a precise knowledge of the theoretical predictions is very important.
法律的瑕疵
发表于 2025-3-26 06:08:17
One Constraint to Kill Them All?,As we have discussed in Sect. 1.3.4, there are many intriguing anomalies in the . quark sector, for which a variety of possible classes of new physics model have been proposed. However, any new .-coupling immediately gives tree-level contributions to . mixing, which is strongly constrained by experiment.
tendinitis
发表于 2025-3-26 11:26:53
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Eructation
发表于 2025-3-26 14:34:03
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Popcorn
发表于 2025-3-26 17:44:48
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