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On the status of flavor anomalies Diego Guadagnoli LAPTh Annecy (France) Recap of flavor anomalies: b s LHCb and B factories measured several key b s and b c modes. Agreement with the SM is less than perfect. D. Guadagnoli,


  1. On the status of flavor anomalies Diego Guadagnoli LAPTh Annecy (France)

  2. Recap of flavor anomalies: b → s LHCb and B factories measured several key b → s and b → c modes. Agreement with the SM is less than perfect. D. Guadagnoli, Status of flavor anomalies

  3. Recap of flavor anomalies: b → s LHCb and B factories measured several key b → s and b → c modes. Agreement with the SM is less than perfect. + → K + μμ) [ 1,6 ] R K = BR ( B  = 0 . 7 4 5 ⋅( 1 ± 13% ) + → K + ee ) [ 1,6 ] BR ( B D. Guadagnoli, Status of flavor anomalies

  4. Recap of flavor anomalies: b → s LHCb and B factories measured several key b → s and b → c modes. Agreement with the SM is less than perfect.  the electron channel would be an + → K + μμ) [ 1,6 ] obvious culprit (brems + low stats). R K = BR ( B  = 0.745 ⋅( 1 ± 13% ) But disagreement is rather in muons + → K + ee ) [ 1,6 ] BR ( B  muons are among the most reliable objects within LHCb D. Guadagnoli, Status of flavor anomalies

  5. Recap of flavor anomalies: b → s LHCb and B factories measured several key b → s and b → c modes. Agreement with the SM is less than perfect.  the electron channel would be an + → K + μμ) [ 1,6 ] obvious culprit (brems + low stats). R K = BR ( B  = 0.745 ⋅( 1 ± 13% ) But disagreement is rather in muons + → K + ee ) [ 1,6 ] BR ( B  muons are among the most reliable objects within LHCb ➋ BR(B s → φ μμ): >3  below SM prediction. Same kinematical region m 2 μμ ∈ [1, 6 ] GeV 2 Initially found in 1/fb of LHCb data, then confirmed by a full Run-I analysis (3/fb) D. Guadagnoli, Status of flavor anomalies

  6. Recap of flavor anomalies: b → s LHCb and B factories measured several key b → s and b → c modes. Agreement with the SM is less than perfect.  the electron channel would be an + → K + μμ) [ 1,6 ] obvious culprit (brems + low stats). R K = BR ( B  = 0.745 ⋅( 1 ± 13% ) But disagreement is rather in muons + → K + ee ) [ 1,6 ] BR ( B  muons are among the most reliable objects within LHCb ➋ BR(B s → φ μμ): >3  below SM prediction. Same kinematical region m 2 μμ ∈ [1, 6 ] GeV 2 Initially found in 1/fb of LHCb data, then confirmed by a full Run-I analysis (3/fb)  B → K* μμ angular analysis: discrepancy in one combination of the angular expansion coefficients, known as P' 5 D. Guadagnoli, Status of flavor anomalies

  7.  B → K* μμ angular analysis: discrepancy in P' 5 arXiv:1604.04042 D. Guadagnoli, Status of flavor anomalies

  8.  B → K* μμ angular analysis: discrepancy in P' 5 arXiv:1604.04042 Effect is again in the same region: m 2 μμ ∈ [1, 6 ] GeV 2 D. Guadagnoli, Status of flavor anomalies

  9.  B → K* μμ angular analysis: discrepancy in P' 5 arXiv:1604.04042 Effect is again in the same region: m 2 μμ ∈ [1, 6 ] GeV 2 Compatibility between 1/fb and 3/fb LHCb analyses. D. Guadagnoli, Status of flavor anomalies

  10.  B → K* μμ angular analysis: discrepancy in P' 5 arXiv:1604.04042 Effect is again in the same region: m 2 μμ ∈ [1, 6 ] GeV 2 Compatibility between 1/fb and 3/fb LHCb analyses. Supported also by recent Belle analysis. D. Guadagnoli, Status of flavor anomalies

  11.  B → K* μμ angular analysis: discrepancy in P' 5 arXiv:1604.04042 μμ ∈ [1, 6 ] GeV 2 Effect is again in the same region: m 2 Compatibility between 1/fb and 3/fb LHCb analyses. Supported also by recent Belle analysis. Significance of the effect is debated. D. Guadagnoli, Status of flavor anomalies

  12. Recap of flavor anomalies: b → s LHCb and B factories measured several key b → s and b → c modes. Agreement with the SM is less than perfect.  the electron channel would be an + → K + μμ) [ 1,6 ] obvious culprit (brems + low stats). R K = BR ( B  = 0.745 ⋅( 1 ± 13% ) But disagreement is rather in muons + → K + ee ) [ 1,6 ] BR ( B  muons are among the most reliable objects within LHCb ➋ BR(B s → φ μμ): >3  below SM prediction. Same kinematical region m 2 μμ ∈ [1, 6 ] GeV 2 Initially found in 1/fb of LHCb data, then confirmed by a full Run-I analysis (3/fb)  B → K* μμ angular analysis: discrepancy in P' 5 Again same region m 2 μμ ∈ [1, 6 ] GeV 2 Compatibility between 1/fb and 3/fb LHCb analyses. Supported also by recent Belle analysis. Significance of the effect is debated. ⇒ There seems to be BSM LFNU ➊ (+ ➋ + ➌ ) and the effect is in µµ, not ee D. Guadagnoli, Status of flavor anomalies

  13. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D D. Guadagnoli, Status of flavor anomalies

  14. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16  ICHEP '16 updates D. Guadagnoli, Status of flavor anomalies

  15. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D First discrepancy found by BaBar in 2012 R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16 in both R(D) and R(D*)  ICHEP '16 updates D. Guadagnoli, Status of flavor anomalies

  16. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D First discrepancy found by BaBar in 2012 R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16 in both R(D) and R(D*)  2015: BaBar's R(D*) confirmed by LHCb   ICHEP '16 updates D. Guadagnoli, Status of flavor anomalies

  17. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D First discrepancy found by BaBar in 2012 R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16 in both R(D) and R(D*)  2015: BaBar's R(D*) confirmed by LHCb  2015: Belle finds a  more SM-like R(D*) (hadronic tau's)  ICHEP '16 updates D. Guadagnoli, Status of flavor anomalies

  18. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D First discrepancy found by BaBar in 2012 R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16 in both R(D) and R(D*)  2015: BaBar's R(D*) confirmed by LHCb  2015: Belle finds a  more SM-like R(D*) (hadronic tau's)  Early 2016: Belle also sees an R(D*) excess (semi-lep. tau's)  ICHEP '16 updates D. Guadagnoli, Status of flavor anomalies

  19. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D First discrepancy found by BaBar in 2012 R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16 in both R(D) and R(D*)  2015: BaBar's R(D*) confirmed by LHCb  2015: Belle finds a  more SM-like R(D*) (hadronic tau's)  Early 2016: Belle also sees an R(D*) excess (semi-lep. tau's)   Summer '16: SM-like R(D*) in new had.-tag Belle analysis ICHEP '16 updates D. Guadagnoli, Status of flavor anomalies

  20. Recap of flavor anomalies: b → c There are long-standing discrepancies in b → c transitions as well. ( * ) τ ν) ( * ) ) = BR ( B → D R ( D ( * ) ℓν) ( with ℓ= e, μ) BR ( B → D First discrepancy found by BaBar in 2012 R(D*) state-of-the-art adapted from Y. Sato, talk at ICHEP16 in both R(D) and R(D*)  2015: BaBar's R(D*) confirmed by LHCb  2015: Belle finds a  more SM-like R(D*) (hadronic tau's)  Early 2016: Belle also sees an R(D*) excess (semi-lep. tau's)   Summer '16: SM-like R(D*) in new had.-tag Belle analysis ICHEP '16 updates All in all: Simultaneous fit to R(D) & R(D*) about 4 σ away from SM D. Guadagnoli, Status of flavor anomalies

  21.  Each of the mentioned effects needs confirmation from Run II to be taken seriously D. Guadagnoli, Status of flavor anomalies

  22.  Each of the mentioned effects needs confirmation from Run II to be taken seriously  Yet, focusing for the moment on the b → s discrepancies Q1: Can we (easily) make theoretical sense of data? Q2: What are the most immediate signatures to expect ? D. Guadagnoli, Status of flavor anomalies

  23. Concerning Q2: most immediate signatures to expect D. Guadagnoli, Status of flavor anomalies

  24. Concerning Q2: most immediate signatures to expect Basic observation:  If R K is signaling LFNU at a non-SM level, we may also expect LFV at a non-SM level. D. Guadagnoli, Status of flavor anomalies

  25. Concerning Q2: most immediate signatures to expect Basic observation:  If R K is signaling LFNU at a non-SM level, we may also expect LFV at a non-SM level. In fact:  Consider a new, LFNU interaction above the EWSB scale, e.g. with ℓ Z' ℓ ℓ φ q new vector bosons: or leptoquarks: D. Guadagnoli, Status of flavor anomalies

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