Search for the decays B(c)+→μ+νμγ
Using proton-proton collision data collected by the LHCb experiment, this paper reports the first search for the radiative leptonic decays B+→μ+νμγ and Bc+→μ+νμγ at a hadron collider, finding no evidence for these processes and setting upper limits on their branching fractions.
Original authors: LHCb collaboration, R. Aaij, M. Abdelfatah, A. S. W. Abdelmotteleb, C. Abellan Beteta, F. Abudinén, T. Ackernley, A. A. Adefisoye, B. Adeva, M. Adinolfi, P. Adlarson, C. Agapopoulou, C. A. Aidala, S. Akar, K. Akiba, H. Al Saleh, P. Albicocco, J. Albrecht, R. Aleksiejunas, F. Alessio, P. Alvarez Cartelle, S. Amato, J. L. Amey, Y. Amhis, Z. Amos, L. An, L. Anderlini, M. Andersson, P. Andreola, M. Andreotti, S. Andres Estrada, A. Anelli, D. Ao, C. Arata, F. Archilli, Z. Areg, M. Argenton, S. Arguedas Cuendis, L. Arnone, M. Artuso, E. Aslanides, R. Ataíde Da Silva, M. Atzeni, B. Audurier, J. A. Authier, D. Bacher, I. Bachiller Perea, S. Bachmann, M. Bachmayer, J. J. Back, Z. B. Bai, V. Balagura, A. Balboni, W. Baldini, Z. Baldwin, L. Balzani, H. Bao, J. Baptista de Souza Leite, C. Barbero Pretel, M. Barbetti, I. R. Barbosa, R. J. Barlow, M. Barnyakov, S. Baron, S. Barsuk, W. Barter, J. Bartz, S. Bashir, B. Batsukh, P. B. Battista, A. Bavarchee, A. Bay, A. Beck, M. Becker, F. Bedeschi, I. B. Bediaga, N. A. Behling, S. Belin, A. Bellavista, I. Belyaev, G. Bencivenni, E. Ben-Haim, J. L. M. Berkey, R. Bernet, A. Bertolin, F. Betti, J. Bex, O. Bezshyyko, S. Bhattacharya, M. S. Bieker, N. V. Biesuz, A. Biolchini, M. Birch, F. C. R. Bishop, A. Bitadze, A. Bizzeti, T. Blake, F. Blanc, J. E. Blank, S. Blusk, J. A. Boelhauve, O. Boente Garcia, T. Boettcher, A. Bohare, C. Bolognani, R. B. Bonacci, A. Bordelius, F. Borgato, S. Borghi, M. Borsato, J. T. Borsuk, E. Bottalico, S. A. Bouchiba, M. Bovill, T. J. V. Bowcock, A. Boyer, C. Bozzi, J. D. Brandenburg, A. Brea Rodriguez, N. Breer, C. Breitfeld, J. Brodzicka, J. Brown, E. Buchanan, M. Burgos Marcos, C. Burr, C. Buti, J. S. Butter, J. Buytaert, W. Byczynski, S. Cadeddu, H. Cai, Y. Cai, Y. Cai, A. Caillet, R. Calabrese, L. Calefice, M. Calvi, M. Calvo Gomez, P. Camargo Magalhaes, J. I. Cambon Bouzas, P. Campana, A. Campomagnani, A. C. Campos, A. F. Campoverde Quezada, Y. Cao, S. Capelli, M. Caporale, L. Capriotti, R. Caravaca-Mora, A. Carbone, L. Carcedo Salgado, R. Cardinale, A. Cardini, P. Carniti, L. Carus, A. Casais Vidal, R. Caspary, G. Casse, M. Cattaneo, G. Cavallero, V. Cavallini, S. Celani, I. Celestino, S. Cesare, A. J. Chadwick, I. Chahrour, M. Charles, Ph. Charpentier, E. Chatzianagnostou, R. Cheaib, M. Chefdeville, C. Chen, J. Chen, S. Chen, Z. Chen, A. Chen Hu, M. Cherif, S. Chernyshenko, X. Chiotopoulos, G. Chizhik, V. Chobanova, A. Christakakis, M. Chrzaszcz, Y. Chu, V. Chulikov, P. Ciambrone, X. Cid Vidal, P. Cifra, P. E. L. Clarke, M. Clemencic, H. V. Cliff, J. Closier, C. Cocha Toapaxi, V. Coco, J. Cogan, E. Cogneras, L. Cojocariu, S. Collaviti, P. Collins, T. Colombo, M. Colonna, A. Comerma-Montells, L. Congedo, J. Connaughton, A. Contu, N. Cooke, G. Cordova, C. Coronel, I. Corredoira, A. Correia, G. Corti, G. C. Costantino, C. Cotirlan, J. Cottee Meldrum, B. Couturier, D. C. Craik, N. Crepet, M. Cruz Torres, M. Cubero Campos, E. Curras Rivera, R. Currie, C. L. Da Silva, X. Dai, J. Dalseno, C. D'Ambrosio, G. Darze, A. Davidson, J. E. Davies, O. De Aguiar Francisco, C. De Angelis, F. De Benedetti, J. de Boer, K. De Bruyn, S. De Capua, M. De Cian, U. De Freitas Carneiro Da Graca, F. De Gregorio, E. De Lucia, J. M. De Miranda, L. De Paula, E. De Santis, M. De Serio, P. De Simone, F. De Vellis, J. A. de Vries, F. Debernardis, D. Decamp, S. Dekkers, L. Del Buono, B. Delaney, J. Deng, O. Deschamps, F. Dettori, B. Dey, P. Di Nezza, S. Ding, Y. Ding, L. Dittmann, A. D. Docheva, A. Doheny, C. Dong, F. Dordei, J. Dorta Moreno, A. C. dos Reis, J. Dos Santos Oliveira, A. D. Dowling, L. Dreyfus, W. Duan, P. Duda, L. Dufour, V. Duk, P. Durante, M. M. Duras, J. M. Durham, O. D. Durmus, K. Duwe, A. Dziurda, S. Easo, E. Eckstein, U. Egede, S. Eisenhardt, E. Ejopu, L. Eklund, M. Elashri, D. Elizondo Blanco, J. Ellbracht, S. Ely, A. Ene, T. Evans, F. Fabiano, S. Faghih, L. N. Falcao, B. Fang, R. Fantechi, L. Fantini, M. Faria, K. Farmer, F. Fassin, D. 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Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer
Imagine the universe as a giant, high-speed particle collider, a cosmic pinball machine where scientists smash protons together at energies of 13 TeV to see what tiny, exotic pieces fly out. The LHCb experiment at CERN is like a super-precise camera set up to catch these fleeting moments. In this latest "snapshot" of 5.4 fb⁻¹ of data (a massive amount of collision history), the team went on a treasure hunt for two very specific, very rare types of decay: the B+ meson and the B+c meson turning into a muon, a neutrino, and a photon (a particle of light).
Think of these mesons as unstable, heavy "parent" particles that usually decay into predictable children. But the scientists were looking for a "ghost" decay where the parent vanishes, leaving behind a muon (a heavy cousin of the electron), a neutrino (a ghostly particle that barely interacts with anything), and a single flash of light. This specific decay is like a magician's trick: the parent disappears, and the only clues left are a heavy electron-like particle, a ghost, and a photon.
The Great Ghost Hunt
The team set up a sophisticated trap. Since neutrinos are invisible and fly away without leaving a trace, the scientists couldn't just look for the missing piece. Instead, they looked for a clever workaround: they waited for the photon to crash into the detector's material and split into an electron-positron pair. This gave them three tracks (the muon and the two electrons) to reconstruct the "crime scene" and figure out where the decay happened, even with the missing neutrino. They used powerful computer algorithms (like XGBoost, a type of artificial intelligence) to filter out the millions of "fake" events that looked similar but were just background noise.
The Result: No Treasure Found (Yet)
After sifting through the data, the result was a bit of a "bust," but a scientifically important one. The team found no evidence of an excess of these rare decays. In other words, they didn't find the treasure they were hunting for. The number of events they saw matched exactly what they expected from background noise.
Because they didn't find the particles, they couldn't measure how often this happens. Instead, they set a "ceiling" on how common it could possibly be. They are 90% confident that:
- The B+ meson decays this way less than 4.0 × 10⁻⁶ times (that's less than 4 times in a million).
- The B+c meson decays this way less than 1.6 × 10⁻³ times (that's less than 16 times in ten thousand).
These numbers are the strict upper limits. If the decay happens at all, it must be rarer than these limits.
Why This Matters
Even though they didn't find the decay, this is a huge deal for two reasons. First, this is the very first time anyone has looked for these specific decays at a hadron collider (a machine that smashes protons). Before this, only other types of experiments had tried, and they set slightly different limits. Second, this is the first time anyone has ever investigated the B+c → µ+νµγ decay.
The paper argues that finding this decay would be a golden ticket to understanding a mysterious property of the "light-cone distribution amplitude" (LCDA) of the B-meson. Think of the LCDA as a blueprint for how the tiny quarks inside the meson are moving. Scientists have a parameter called λB (lambda-B) that describes the typical momentum of the light quark inside, but nobody knows its exact value—it's estimated to be somewhere between 200 and 600 MeV. If they could measure this decay, they could pin down that blueprint. Since they didn't find it, they can't pin down the blueprint yet, but they have successfully ruled out the possibility that the decay is common.
The Bottom Line
The paper explicitly rules out the idea that these decays are happening frequently enough to be easily spotted with current data. It does not prove the decay exists, nor does it prove it doesn't exist; it simply says, "If it's happening, it's hiding very well, rarer than our current limits." The authors suggest that with the upgraded LHCb detector and more data in the future (Run 3), they might finally catch a glimpse of this elusive ghost. For now, the search continues, and the universe keeps its secrets a little tighter.
Technical Summary: Search for the decays B(c)+→μ+νμγ
Problem and Motivation
Precision tests of the Standard Model (SM) in the flavor sector are often limited by hadronic uncertainties, particularly the nonperturbative quantum chromodynamics (QCD) effects in B-meson decays. Within the QCD factorization approach, these dynamics are encoded in the B-meson light-cone distribution amplitude (LCDA). A critical parameter for exclusive B decay predictions is the first inverse moment of the leading-twist LCDA, λB, which characterizes the typical momentum of the light spectator quark. While theoretical estimates for λB range widely (200–600 MeV), the radiative leptonic decay B+→ℓ+νℓγ is considered the optimal channel to experimentally probe the B-meson LCDA and measure λB. For energetic photons, the decay amplitude factorizes, making the branching fraction proportional to 1/λB2 at leading power.
Despite its theoretical importance, the B+→ℓ+νℓγ decay remains unobserved due to its challenging final state (involving a neutrino and a photon) and a small predicted branching fraction of O(10−6). Previous searches by the BaBar and Belle collaborations have set upper limits but have not yet observed the signal. Furthermore, the radiative leptonic decay of the Bc+ meson (Bc+→μ+νμγ) has not been experimentally investigated to date, despite theoretical predictions suggesting a branching fraction between 2×10−5 and 8×10−5, enhanced by CKM matrix elements relative to the B+ decay.
Methodology
This analysis utilizes proton-proton collision data collected by the LHCb experiment at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4 fb−1 (2016–2018). The search targets the decays B+→μ+νμγ and Bc+→μ+νμγ.
- Reconstruction Strategy: Since the B-meson decay vertex cannot be reconstructed from a single charged track (the muon) alone, the analysis relies on photons converting into electron-positron pairs (γ→e+e−) within the vertex detector material. This provides three tracks (μ+,e+,e−) to reconstruct the B-decay vertex and suppress prompt background.
- Kinematic Variables: To compensate for the missing neutrino momentum, the corrected mass, mcorr(μ+γee), is used. The photon energy in the B-meson rest frame, Eγ∗, is calculated and required to be greater than 1 GeV.
- Background Suppression: Three multivariate classifiers (based on XGBoost and Gradient Boosted Decision Trees) are employed to separate signal from:
- Combinatorial background.
- Backgrounds where the converted photon originates from a neutral pion (π0) or eta (η) meson decay.
- Partially reconstructed backgrounds with additional charged tracks (e.g., B+→D0μ+νμ).
The selection retains approximately 22% of B+ signal and 8% of Bc+ signal while reducing background by ~98%.
- Normalization: Branching fractions are measured relative to the B0→K∗(892)0γ decay, which is reconstructed using converted photons to cancel systematic uncertainties related to photon conversion reconstruction.
- Background Modeling: The dominant backgrounds (π0 and η) are modeled using data-driven techniques. Candidates for μ+π0 and μ+η are reconstructed by combining the converted photon with an additional calorimeter photon (γcalo). An unbinned maximum-likelihood fit to the diphoton invariant mass determines the yields, and the sPlot technique is used to extract the mcorr distributions for these backgrounds. Misidentification backgrounds (e.g., hadrons misidentified as muons) are modeled using control samples with inverted particle identification (PID) requirements.
Key Contributions
- First Hadron Collider Search: This work presents the first search for B+→μ+νμγ at a hadron collider.
- First Bc+ Investigation: This constitutes the first experimental investigation of the Bc+→μ+νμγ decay.
- Methodological Innovation: The analysis demonstrates the feasibility of reconstructing radiative leptonic decays with missing neutrinos at the LHC by utilizing photon conversions to provide the necessary vertexing information.
- Efficiency Maps: The paper provides efficiency maps as a function of photon energy (Eγ∗) and helicity angle (cosθℓ), allowing for the reinterpretation of results under different theoretical models.
Results
No significant excess of events over the expected background is observed for either signal decay. The yields after bias correction are 32±24 for B+→μ+νμγ and 13−5+6 for Bc+→μ+νμγ. Consequently, upper limits on the branching fractions are set at the 90% confidence level (CL) for photons with Eγ∗>1 GeV:
- B(B+→μ+νμγ)<4.0×10−6
- B(Bc+→μ+νμγ)<1.6×10−3
The measured branching fractions are compatible with zero within 1.3 and 2.4 standard deviations for the B+ and Bc+ decays, respectively. The sensitivity for the B+ decay is comparable to the best previous results from the Belle collaboration.
Significance
This paper establishes the first experimental constraints on the Bc+→μ+νμγ decay and provides a competitive upper limit for the B+→μ+νμγ decay in a hadron collider environment. While the current limits do not yet probe the central values of the Standard Model predictions, the analysis validates the reconstruction technique required to measure these decays. The authors note that these searches are expected to benefit significantly from the increased luminosity and improved performance of the upgraded LHCb detector in Run 3, which will be crucial for eventually observing these decays and constraining the B-meson LCDA parameter λB.
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