Literature DB >> 26877543

Future flavour physics experiments.

Neville Harnew1.   

Abstract

The current status of flavour physics and the prospects for present and future experiments will be reviewed. Measurements in B-physics, in which sensitive probes of new physics are the CKM angle γ, the Bs mixing phase ϕs, and the branching ratios of the rare decays B(s)0→μ+μ- , will be highlighted. Topics in charm and kaon physics, in which the measurements of ACP and the branching ratios of the rare decays K→πνν¯ are key measurements, will be discussed. Finally the complementarity of the future heavy flavour experiments, the LHCb upgrade and Belle-II, will be summarised.

Entities:  

Keywords:  Belle‐II; CP‐violation; Flavour physics; LHCb; charm‐τ factory; rare decays

Year:  2015        PMID： 26877543      PMCID： PMC4737432          DOI： 10.1002/andp.201500230

Source DB:  PubMed          Journal:  Ann Phys        ISSN： 0003-3804


Introduction

Flavour physics holds the key to some of today's most important issues in particle physics, namely the indirect search for dark matter and the mechanism of CP‐violation. In the quark sector, the CKM matrix describes CP‐violation in the Standard Model (SM) but gives rise to too small a level of asymmetry to explain the observed dominance of matter over antimatter in the Universe. In particular, (non)‐consistency tests of the CKM mechanism provide an excellent framework to discover sources of New Physics (NP). We know that sources of NP must exist, but as yet there is no knowledge of the effects or the scale in the quark sector. The absence to date of NP signals at ATLAS and CMS makes a strong argument to pursue searches in heavy flavour decays via rare processes, such as flavour‐changing neutral currents (FCNCs). These are accessed via box and loop (penguin) decay processes which allow a probe of masses significantly beyond the kinematic limit 1. History has shown that such indirect searches provide a powerful discovery tool for such high masses. There are several key observables that will be the focus of future experimental measurements which will be discussed below. To demonstrate consistency of the CKM mechanism, measurements of the CP angle γ will need to be significantly improved. The weak phase in the system, , and in the charm system indicate CP‐violating effects in the SM which are expected to be very small, and where future experiments will probe down to SM expectations. These experiments will also improve the precision of and allow checks on lepton universality, including the decay . The branching ratios of , the parameter in and the rare kaon decay are measurements in which large NP effects can be expected.

The B physics programme

The experiments

LHCb and the LHCb Upgrade

The LHCb detector 2 is a single‐arm forward spectrometer designed to study CP violation in B‐hadron decays at the LHC. LHCb covers a polar angular aperture between approximately 10 and 300 mrad (250 mrad) in the bending (non‐bending) plane and exploits the sharply peaked forward‐backward production cross section. Up to 2018, LHCb will have accumulated ∼8 fb−1 of integrated luminosity, and beyond this the data‐doubling time becomes prohibitive. A compelling physics case has been made for improved precision and extra sensitivity to the rarest decay modes. The LHCb detector will therefore be upgraded in the long shutdown (LS2) of the LHC during 2018‐20 3. The subdetector readout electronics will be upgraded to a 40 MHz rate and all trigger decisions will be made in software, giving significant efficiency improvements. The detector will also be upgraded to run at a luminosity of up to 2 × 1033  cm−2s−1, a factor of 5 increase. A combination of these improvements will allow around an order of magnitude increase in precision compared to where we stand today.

KEKB and Belle‐II

KEKB collides 7 GeV on 4 GeV and runs mainly on the with a possibility to run on the . Both the KEKB accelerator and the Belle detector 4 are undergoing a major upgrade with the aim to start physics data‐taking in 2017‐2018 at a peak luminosity of ∼1036  cm−2s−1, approximately 40 times higher than its predecessor. The expectation is that Belle‐II will accumulate 50 ab−1 in ∼5 years giving approximately 50 times the current Belle data. Whilst LHCb has the benefit of the raw data rate, Belle‐II has several significant advantages. Firstly collisions benefit from a relatively clean environment and also the 's are produced in a quantum correlated state. The trigger is very efficient and the tagging efficiency is high with respect to a machine (about × 15). Another significant advantage over LHCb is the excellent reconstruction of neutrals: and neutrinos via missing energy. The physics programme of Belle‐II is broad, giving flavour‐physics measurements which are unique, but also complementary to LHCb. A description of the Belle‐II physics programme can be found in Ref. 5.

A consistent picture of CKM measurements

Imposing unitarity constraints on the CKM matrix gives the condition , which can be represented by the so‐called “unitarity triangle” when plotted in the complex plane. A consistency test of the SM requires that many different fits to the unitary triangle all result in a common apex and, if not, this will indicate additional amplitudes from NP. The current constraints on the parameters of the unitarity triangle are shown in Fig. 1 6. Whilst there is good general consistency with the CKM parametrization, the current measurements are dominated by box or loop processes. The measurements solely from tree processes still have large uncertainties, in particular from the left side of the triangle and the angle γ.
Figure 1

The experimental constraints on the sides and angles of the unitarity triangle from the CKMfitter group 6, represented on an Argand diagram. The base of the triangle is aligned along the real axis (), and is conventionally normalized to unity. The height of the apex of the triangle is plotted on the imaginary axis (). The experimental constraints on the three angles, α (light blue), β (violet) and γ (grey) are given by 95% confidence level (CL) bands. The darker blue band shows the 68% CL for β. Constraints on the triangle sides from measurements of (dark green) and the and mixing frequencies ( and respectively) are shown by the orange band at 95% CL. The 95% confidence constraint from measurements of indirect CP violation in the kaon system, the parameter (light green), is also shown. The dashed red region shows the 68% CL for the combination, which constrains the apex of the triangle.

The experimental constraints on the sides and angles of the unitarity triangle from the CKMfitter group 6, represented on an Argand diagram. The base of the triangle is aligned along the real axis (), and is conventionally normalized to unity. The height of the apex of the triangle is plotted on the imaginary axis (). The experimental constraints on the three angles, α (light blue), β (violet) and γ (grey) are given by 95% confidence level (CL) bands. The darker blue band shows the 68% CL for β. Constraints on the triangle sides from measurements of (dark green) and the and mixing frequencies ( and respectively) are shown by the orange band at 95% CL. The 95% confidence constraint from measurements of indirect CP violation in the kaon system, the parameter (light green), is also shown. The dashed red region shows the 68% CL for the combination, which constrains the apex of the triangle. It is important to measure γ with high statistical power in a variety of complementary channels to compare tree (SM dominated) and loop (sensitive to NP) diagrams. As an example of tree‐dominated processes, the evaluation of γ via the family of decays gives extremely small theoretical uncertainty 7. Hence measurements of these modes determine the “Standard Model” value of γ. LHCb's current best measurement of γ is from a combination of results from and decays which gives γ to be 72.6° with a confidence interval at the 68% level of  8. This is already a more significant measurement than BaBar and Belle combined, but still has large uncertainties. In the future, the statistical reach in γ of the LHCb upgrade will be ∼1% 9. The corresponding measurement for Belle‐II is expected to be ∼2‐3% 5. To keep systematic uncertainty at or below those levels requires an exceptionally good understanding of detector effects. For the triangle left side, the measurement of in semileptonic B decays has for several years had an internal inconsistency between the exclusive measurement and the inclusive measurement  10, namely (inclusive) and (exclusive). Similar effects have also been seen in the inclusive and exclusive measurements of  10, with (inclusive) and (exclusive). The significance is enticing, but not yet enough to confirm NP, and more measurements and lattice calculation improvements are necessary. LHCb has recently entered the game by measuring in decays to be  11. This measurement is 3.5 σ below the inclusive measurement and agrees well with the current exclusive average. Hence future measurements of and will resolve these discrepancies and can potentially provide exciting indications of NP. Inclusive measurements of from Belle‐II at the few percent level will be possible.

and

The decay is a loop process with a branching ratio (BR) of in the SM 12. This decay is extremely rare due to the absence of tree‐level FCNCs, helicity suppression and CKM‐matrix suppression. The decay is similarly suppressed and has a BR approximately 30 less,  13. The decays can be strongly enhanced in NP models, and are especially sensitive to high parameter space in the minimal supersymmetric model (MSSM) 14, where the rates go as . Searches over 30 years have given approximately an order of magnitude improvement every ∼5 years. Data from CMS 15 and LHCb 16 have been combined 17 and the resulting di‐muon mass measurement is shown in Fig. 2. The peaks show and excesses in the and channels, respectively. These measurements are consistent with SM expectations, although the larger than expected BR for the B 0 decay is intriguing.
Figure 2

Combined CMS and LHCb di‐muon mass combination for  17.

Combined CMS and LHCb di‐muon mass combination for  17. The LHCb upgrade and CMS experiments will continue to measure the ratio of BRs () with unrivaled precision. An ambitious goal of these experiments will be to search for other leptonic decays, for example , a channel which is much harder experimentally, but more sensitive to models incorporating extensions of the Higgs sector.

Angular analyses of

The rare decay is a FCNC process that proceeds via loop and box amplitudes in the SM. In extensions of the SM, contributions from new particles can modify the angular distributions of the decay products. The current world‐best measurements are made by LHCb 18 and good agreement has been found with SM parameterizations in most observables. However a local discrepancy from theoretical calculations 19 has been observed as a function of di‐muon effective mass squared (q 2) for one of the observables, the so‐called parameter. This result has been confirmed by recent analysis of the full data sample 20, shown in Fig. 3, demonstrating a tension with the SM prediction at a level of 2.9σ in each of the   GeV2 and GeV2 bins. A naïve combination of these deviations, based on a probability with two degrees of freedom and assuming the SM predictions in the two bins are uncorrelated, yields a local tension of 3.7σ. This is an interesting result that could be a hint of NP; however improved measurements are needed from both the LHCb upgrade and Belle‐II. Better theoretical QCD calculations with improved uncertainties are also required.
Figure 3

The parameter of the LHCb angular analysis of  20 compared to SM expectations 19.

The parameter of the LHCb angular analysis of  20 compared to SM expectations 19.

Lepton universality in B decays

Lepton universality dictates that the and decays should have same BR to within a factor 10−3; however the ratio of the BRs is sensitive to lepton flavour‐violating NP contributions. LHCb measures to be (stat) ±0.036 (syst), with hints of a deficit of compared to the expectation 21, currently a 2.6 σ tension. The expected precision from both Belle‐II and the LHCb upgrade will improve the errors by an order of magnitude and hence will resolve this issue. There is also an excess measured by the BaBar collaboration of decays relative to , where ℓ is a muon or electron. The measurements, and , exceed the SM expectations by 2.0 σ and 2.7 σ, respectively 22. The ratios are sensitive to NP contributions from a charged Higgs boson and, taken together, these results disagree with SM expectations at the 3.4 σ level, although the excess cannot be explained by a charged Higgs boson within the type II two‐Higgs‐doublet model 23. A recent Belle result lies between the SM expectation and the measurement from BaBar and is compatible with both 24. Belle‐II and possibly future LHCb results will be able to resolve this issue.

CP violation in mixing

The D0 experiment has observed an anomalous di‐muon asymmetry indicating CP violation in mixing 25, the so‐called measurement. is the difference of the numbers of decaying into and , divided by the sum, integrated over the lifetime. The D0 result of , observed in 6.1 fb−1 of data, differs by 3.2 σ from the SM prediction. This result has not yet been confirmed or refuted by separate measurements in the B 0 and systems from the BaBar 26 and LHCb 27 experiments. Much improved measurements are required from the LHCb upgrade and Belle‐II. The mixing process introduces a small CP‐violating weak phase whose predicted value in the SM,  rad, is theoretically very clean 28. However could be much larger than the SM prediction if NP contributes to transitions. This phase can be measured in the tree decay process through the interference of the direct decay with the decay involving mixing. A compilation of results from hadron collider experiments is shown in Fig. 4 29. Here the constraints are dominated by the LHCb result, rad 30, but with important contributions from ATLAS and CMS.
Figure 4

Contours of allowed regions in the plane of from LHCb, ATLAS, CMS and the Tevatron experiments29. is the width difference between eigenstates.

Contours of allowed regions in the plane of from LHCb, ATLAS, CMS and the Tevatron experiments29. is the width difference between eigenstates. Deviations from SM predictions can also be expected in the FCNC decay which again involves the interference of direct and mixing amplitudes. The upper limit of CP violation expected in the SM is ∼2% 31, hence the observation of any significant CP violation in is a signature for NP. LHCb's current measurement for in the channel in 3 fb−1 of data is  rad 32, hence the large errors mean that no CP violation of significance can yet be observed. However the LHCb upgrade will bring the precision on this down to ∼0.02 rad 9, to the same level as the current theoretical uncertainty.

Charm physics

The LHCb and Belle‐II experiments plan a full programme of charm physics measurements. Charm is produced from decays of b quarks and directly from gluon‐gluon fusion interactions in LHCb and from the continuum in Belle‐II. A dedicated experiment running at the IHEP charm‐factory, BES III 35, has already collected an unprecedented data sample on the , ψ(2S), ψ(3770) and ψ(4040) resonances. The experiment will also run at the tau‐pair threshold for a new precision tau mass measurement. Looking towards the future, BES III plans to collect data at centre‐of‐mass energies of 4260 MeV and 4360 MeV to conduct spectroscopic studies of the “XYZ” states 36, and also run at 4170 MeV in order to study the meson. BES III is scheduled to collect data for around another eight to ten years.

CP violation in charm mixing

An important and topical area in charm physics is the search for CP violation. CP‐violating effects are predicted to be very small in the SM, with a theoretical expectation of up to a few  33. LHCb has recently made measurements of charm mixing and CP violation in the parameter = % 34, where is the difference in D 0 and decaying into final state f, divided by the sum. Whilst no CP violation is yet observed, there is still much scope for NP effects. Improvements are also needed in the precision of which the LHCb upgrade and Belle‐II will provide. At the required level of precision, several complementary measurements will be required to resolve NP from SM contributions.

experiments

The current holy grail in kaon physics is the measurement of the BRs of the super‐rare decays and , which are suppressed by the CKM coupling and are very sensitive to contributions from physics beyond the SM. The SM predictions for these BRs are and , respectively 37 . The next‐generation experiments will measure these decays for the first time. The decay will be measured by NA62 38, a dedicated experiment at CERN which has now started running. The measurement is a major experimental challenge since the final state has two neutrinos and only one detectable particle. The aim is to collect 100 events at the SM BR during 2015‐16, with <10 events background. The KOTO experiment 39 at J‐PARC will measure the very challenging decay. Approximately 100 hours of data have been taken which has achieved similar sensitivity to the current limit of at 90% confidence from the KEK‐E391a experiment 40 . The next KOTO run is expected in 2015 and should improve the limit by a factor of ∼20, and then onwards towards the SM sensitivity.

Possible future facilities

Future circular colliders

The HL‐LHC will deliver more luminosity than the upgraded LHCb can take, but will nevertheless provide the world's most abundant source of b and c hadrons. Hence there remains the possibility of a dedicated flavour experiment beyond the LHCb upgrade. A study of the FCC programme at CERN, the Future Circular Collider, is ongoing 41. Possible modes of operation of the FCC are the collisions of (which includes a Higgs factory, TeraZ running on the Z 0 pole, OkuW at the threshold, the MegaTop top factory), or heavy ions. The option is in principle especially interesting for flavour physics. TeraZ gives Z events in 1 year, hence huge samples can be recorded in and . By way of example, TeraZ can deliver more than 20k events giving a precision on the SM BR; NP models can change the BR by large factors. Conversely, flavour physics options at the ILC/CLIC and a μ‐collider seem to be rather marginal to their respective programmes since they concentrate on high‐energy running where the cross‐sections for b and c production are small. At any future machine, the cross‐section increases slowly beyond  TeV up to 100 TeV and all SM physics is boosted into the forward region. This does not preclude flavour physics measurements, but it may become harder to argue for a dedicated experiment.

Future τ‐charm factories

There are several proposals for a next generation τ‐charm factory, to go beyond the lifespan of BES‐III. A facility at the Budker Institute of Nuclear Physics (BINP) in Russia 42 is in principle approved but the funding (400M Euros plus the detector) is unclear. This machine will operate at total energies from 2 to 5 GeV with an unprecedented luminosity of 1035 cm−2s−1 and with longitudinal polarization of the electrons. The major physics aims will be measurement of CP‐violation in the decays of charmed particles and a hunt for NP in the decay of the tau lepton, for example flavour violation. Other options being considered are for τ‐charm factories at the Cabibbo Laboratory, Italy 43 and HIEPAF, China 44. These machines aim for = 2‐7 GeV and peak luminosities ∼1035cm−2s−1. Physics programmes primarily focus on QCD and hadronic physics with some unique potential for charm and (polarised) τ physics.

Summary

The future of the flavour physics programme has been presented. In the medium term, the LHCb experiment is performing a high‐statistics study of CP violation with unprecedented precision, providing a sensitive test of the SM and physics beyond. These measurements are complemented in certain important channels by ATLAS and CMS. During the next 5 years the Belle‐II experiment and the LHCb upgrade will come online, each improving precision by at least a factor 10 from where we are today. These experiments are competing yet complementary, with their relative performance of key measurements summarized in Table 1. Some measurements will be unique to each experiment whereas others allow cross‐checks. The table is subjective both in terms of performance and specified observables; a selection of key measurements could equally have included and in B 0 etc.
Table 1

A subjective comparison of key measurements in flavour physics. ✓✓ represents world‐leading, ✓ represents high potential, but less precise, ? represents to be determined.

LHCb UpgradeBelle‐IIATLAS/CMS
CKM angle γ✓✓✓✓
Bs weak phase ϕs ✓✓✓
|Vub| ✓ ?✓✓
B(s)0→μ+μ− ✓✓✓✓
ΔACP ✓✓✓
D(*)τν ✓ ?✓✓
P5′ ✓✓✓✓✓
B0→τν¯ ✓✓
Flavour violation in τ decay✓✓✓✓
A subjective comparison of key measurements in flavour physics. ✓✓ represents world‐leading, ✓ represents high potential, but less precise, ? represents to be determined. In summary, many NP scenarios predict discoveries in flavour physics, which gives it an interesting and exciting future. Proposed upgrades of current experiments and the construction of new facilities will extend the flavour physics programme for many years to come.
  10 in total

1.  Observation of a charged charmoniumlike structure in e+ e- → π+ π- J/ψ at sqrt[s] = 4.26  GeV.

Authors:  M Ablikim; M N Achasov; X C Ai; O Albayrak; D J Ambrose; F F An; Q An; J Z Bai; R Baldini Ferroli; Y Ban; J Becker; J V Bennett; M Bertani; J M Bian; E Boger; O Bondarenko; I Boyko; R A Briere; V Bytev; H Cai; X Cai; O Cakir; A Calcaterra; G F Cao; S A Cetin; J F Chang; G Chelkov; G Chen; H S Chen; J C Chen; M L Chen; S J Chen; X Chen; Y B Chen; H P Cheng; Y P Chu; D Cronin-Hennessy; H L Dai; J P Dai; D Dedovich; Z Y Deng; A Denig; I Denysenko; M Destefanis; W M Ding; Y Ding; L Y Dong; M Y Dong; S X Du; J Fang; S S Fang; L Fava; C Q Feng; P Friedel; C D Fu; J L Fu; O Fuks; Q Gao; Y Gao; C Geng; K Goetzen; W X Gong; W Gradl; M Greco; M H Gu; Y T Gu; Y H Guan; A Q Guo; L B Guo; T Guo; Y P Guo; Y L Han; F A Harris; K L He; M He; Z Y He; T Held; Y K Heng; Z L Hou; C Hu; H M Hu; J F Hu; T Hu; G M Huang; G S Huang; J S Huang; L Huang; X T Huang; Y Huang; Y P Huang; T Hussain; C S Ji; Q Ji; Q P Ji; X B Ji; X L Ji; L L Jiang; X S Jiang; J B Jiao; Z Jiao; D P Jin; S Jin; F F Jing; N Kalantar-Nayestanaki; M Kavatsyuk; B Kopf; M Kornicer; W Kühn; W Lai; J S Lange; M Lara; P Larin; M Leyhe; C H Li; Cheng Li; Cui Li; D M Li; F Li; G Li; H B Li; J C Li; K Li; Lei Li; Q J Li; S L Li; W D Li; W G Li; X L Li; X N Li; X Q Li; X R Li; Z B Li; H Liang; Y F Liang; Y T Liang; G R Liao; X T Liao; D Lin; B J Liu; C L Liu; C X Liu; F H Liu; Fang Liu; Feng Liu; H Liu; H B Liu; H H Liu; H M Liu; H W Liu; J P Liu; K Liu; K Y Liu; Kai Liu; P L Liu; Q Liu; S B Liu; X Liu; Y B Liu; Z A Liu; Zhiqiang Liu; Zhiqing Liu; H Loehner; X C Lou; G R Lu; H J Lu; J G Lu; Q W Lu; X R Lu; Y P Lu; C L Luo; M X Luo; T Luo; X L Luo; M Lv; C L Ma; F C Ma; H L Ma; Q M Ma; S Ma; T Ma; X Y Ma; F E Maas; M Maggiora; Q A Malik; Y J Mao; Z P Mao; J G Messchendorp; J Min; T J Min; R E Mitchell; X H Mo; Y J Mo; H Moeini; C Morales Morales; K Moriya; N Yu Muchnoi; H Muramatsu; Y Nefedov; C Nicholson; I B Nikolaev; Z Ning; S L Olsen; Q Ouyang; S Pacetti; J W Park; M Pelizaeus; H P Peng; K Peters; J L Ping; R G Ping; R Poling; E Prencipe; M Qi; S Qian; C F Qiao; L Q Qin; X S Qin; Y Qin; Z H Qin; J F Qiu; K H Rashid; G Rong; X D Ruan; A Sarantsev; B D Schaefer; M Shao; C P Shen; X Y Shen; H Y Sheng; M R Shepherd; W M Song; X Y Song; S Spataro; B Spruck; D H Sun; G X Sun; J F Sun; S S Sun; Y J Sun; Y Z Sun; Z J Sun; Z T Sun; C J Tang; X Tang; I Tapan; E H Thorndike; D Toth; M Ullrich; I Uman; G S Varner; B Q Wang; D Wang; D Y Wang; K Wang; L L Wang; L S Wang; M Wang; P Wang; P L Wang; Q J Wang; S G Wang; X F Wang; X L Wang; Y D Wang; Y F Wang; Y Q Wang; Z Wang; Z G Wang; Z Y Wang; D H Wei; J B Wei; P Weidenkaff; Q G Wen; S P Wen; M Werner; U Wiedner; L H Wu; N Wu; S X Wu; W Wu; Z Wu; L G Xia; Y X Xia; Z J Xiao; Y G Xie; Q L Xiu; G F Xu; G M Xu; Q J Xu; Q N Xu; X P Xu; Z R Xu; F Xue; Z Xue; L Yan; W B Yan; Y H Yan; H X Yang; Y Yang; Y X Yang; H Ye; M Ye; M H Ye; B X Yu; C X Yu; H W Yu; J S Yu; S P Yu; C Z Yuan; Y Yuan; A A Zafar; A Zallo; S L Zang; Y Zeng; B X Zhang; B Y Zhang; C Zhang; C C Zhang; D H Zhang; H H Zhang; H Y Zhang; J Q Zhang; J W Zhang; J Y Zhang; J Z Zhang; LiLi Zhang; R Zhang; S H Zhang; X J Zhang; X Y Zhang; Y Zhang; Y H Zhang; Z P Zhang; Z Y Zhang; Zhenghao Zhang; G Zhao; H S Zhao; J W Zhao; K X Zhao; Lei Zhao; Ling Zhao; M G Zhao; Q Zhao; S J Zhao; T C Zhao; X H Zhao; Y B Zhao; Z G Zhao; A Zhemchugov; B Zheng; J P Zheng; Y H Zheng; B Zhong; L Zhou; X Zhou; X K Zhou; X R Zhou; C Zhu; K Zhu; K J Zhu; S H Zhu; X L Zhu; Y C Zhu; Y M Zhu; Y S Zhu; Z A Zhu; J Zhuang; B S Zou; J H Zou
Journal:  Phys Rev Lett       Date:  2013-06-17       Impact factor: 9.161

2.  Measurement of form-factor-independent observables in the decay B0→K(*0)μ(+)μ(-).

Authors:  R Aaij; B Adeva; M Adinolfi; C Adrover; A Affolder; Z Ajaltouni; J Albrecht; F Alessio; M Alexander; S Ali; G Alkhazov; P Alvarez Cartelle; A A Alves; S Amato; S Amerio; Y Amhis; L Anderlini; J Anderson; R Andreassen; J E Andrews; R B Appleby; O Aquines Gutierrez; F Archilli; A Artamonov; M Artuso; E Aslanides; G Auriemma; M Baalouch; S Bachmann; J J Back; C Baesso; V Balagura; W Baldini; R J Barlow; C Barschel; S Barsuk; W Barter; Th Bauer; A Bay; J Beddow; F Bedeschi; I Bediaga; S Belogurov; K Belous; I Belyaev; E Ben-Haim; G Bencivenni; S Benson; J Benton; A Berezhnoy; R Bernet; M-O Bettler; M van Beuzekom; A Bien; S Bifani; T Bird; A Bizzeti; P M Bjørnstad; T Blake; F Blanc; J Blouw; S Blusk; V Bocci; A Bondar; N Bondar; W Bonivento; S Borghi; A Borgia; T J V Bowcock; E Bowen; C Bozzi; T Brambach; J van den Brand; J Bressieux; D Brett; M Britsch; T Britton; N H Brook; H Brown; I Burducea; A Bursche; G Busetto; J Buytaert; S Cadeddu; O Callot; M Calvi; M Calvo Gomez; A Camboni; P Campana; D Campora Perez; A Carbone; G Carboni; R Cardinale; A Cardini; H Carranza-Mejia; L Carson; K Carvalho Akiba; G Casse; L Castillo Garcia; M Cattaneo; Ch Cauet; R Cenci; M Charles; Ph Charpentier; P Chen; N Chiapolini; M Chrzaszcz; K Ciba; X Cid Vidal; G Ciezarek; P E L Clarke; M Clemencic; H V Cliff; J Closier; C Coca; V Coco; J Cogan; E Cogneras; P Collins; A Comerma-Montells; A Contu; A Cook; M Coombes; S Coquereau; G Corti; B Couturier; G A Cowan; D C Craik; S Cunliffe; R Currie; C D'Ambrosio; P David; P N Y David; A Davis; I De Bonis; K De Bruyn; S De Capua; M De Cian; J M De Miranda; L De Paula; W De Silva; P De Simone; D Decamp; M Deckenhoff; L Del Buono; N Déléage; D Derkach; O Deschamps; F Dettori; A Di Canto; H Dijkstra; M Dogaru; S Donleavy; F Dordei; A Dosil Suárez; D Dossett; A Dovbnya; F Dupertuis; P Durante; R Dzhelyadin; A Dziurda; A Dzyuba; S Easo; U Egede; V Egorychev; S Eidelman; D van Eijk; S Eisenhardt; U Eitschberger; R Ekelhof; L Eklund; I El Rifai; Ch Elsasser; A Falabella; C Färber; G Fardell; C Farinelli; S Farry; D Ferguson; V Fernandez Albor; F Ferreira Rodrigues; M Ferro-Luzzi; S Filippov; M Fiore; C Fitzpatrick; M Fontana; F Fontanelli; R Forty; O Francisco; M Frank; C Frei; M Frosini; S Furcas; E Furfaro; A Gallas Torreira; D Galli; M Gandelman; P Gandini; Y Gao; J Garofoli; P Garosi; J Garra Tico; L Garrido; C Gaspar; R Gauld; E Gersabeck; M Gersabeck; T Gershon; Ph Ghez; V Gibson; L Giubega; V V Gligorov; C Göbel; D Golubkov; A Golutvin; A Gomes; P Gorbounov; H Gordon; C Gotti; M Grabalosa Gándara; R Graciani Diaz; L A Granado Cardoso; E Graugés; G Graziani; A Grecu; E Greening; S Gregson; P Griffith; O Grünberg; B Gui; E Gushchin; Yu Guz; T Gys; C Hadjivasiliou; G Haefeli; C Haen; S C Haines; S Hall; B Hamilton; T Hampson; S Hansmann-Menzemer; N Harnew; S T Harnew; J Harrison; T Hartmann; J He; T Head; V Heijne; K Hennessy; P Henrard; J A Hernando Morata; E van Herwijnen; M Hess; A Hicheur; E Hicks; D Hill; M Hoballah; C Hombach; P Hopchev; W Hulsbergen; P Hunt; T Huse; N Hussain; D Hutchcroft; D Hynds; V Iakovenko; M Idzik; P Ilten; R Jacobsson; A Jaeger; E Jans; P Jaton; A Jawahery; F Jing; M John; D Johnson; C R Jones; C Joram; B Jost; M Kaballo; S Kandybei; W Kanso; M Karacson; T M Karbach; I R Kenyon; T Ketel; A Keune; B Khanji; O Kochebina; I Komarov; R F Koopman; P Koppenburg; M Korolev; A Kozlinskiy; L Kravchuk; K Kreplin; M Kreps; G Krocker; P Krokovny; F Kruse; M Kucharczyk; V Kudryavtsev; K Kurek; T Kvaratskheliya; V N La Thi; D Lacarrere; G Lafferty; A Lai; D Lambert; R W Lambert; E Lanciotti; G Lanfranchi; C Langenbruch; T Latham; C Lazzeroni; R Le Gac; J van Leerdam; J-P Lees; R Lefèvre; A Leflat; J Lefrançois; S Leo; O Leroy; T Lesiak; B Leverington; Y Li; L Li Gioi; M Liles; R Lindner; C Linn; B Liu; G Liu; S Lohn; I Longstaff; J H Lopes; N Lopez-March; H Lu; D Lucchesi; J Luisier; H Luo; F Machefert; I V Machikhiliyan; F Maciuc; O Maev; S Malde; G Manca; G Mancinelli; J Maratas; U Marconi; P Marino; R Märki; J Marks; G Martellotti; A Martens; A Martín Sánchez; M Martinelli; D Martinez Santos; D Martins Tostes; A Martynov; A Massafferri; R Matev; Z Mathe; C Matteuzzi; E Maurice; A Mazurov; J McCarthy; A McNab; R McNulty; B McSkelly; B Meadows; F Meier; M Meissner; M Merk; D A Milanes; M-N Minard; J Molina Rodriguez; S Monteil; D Moran; P Morawski; A Mordà; M J Morello; R Mountain; I Mous; F Muheim; K Müller; R Muresan; B Muryn; B Muster; P Naik; T Nakada; R Nandakumar; I Nasteva; M Needham; S Neubert; N Neufeld; A D Nguyen; T D Nguyen; C Nguyen-Mau; M Nicol; V Niess; R Niet; N Nikitin; T Nikodem; A Nomerotski; A Novoselov; A Oblakowska-Mucha; V Obraztsov; S Oggero; S Ogilvy; O Okhrimenko; R Oldeman; M Orlandea; J M Otalora Goicochea; P Owen; A Oyanguren; B K Pal; A Palano; T Palczewski; M Palutan; J Panman; A Papanestis; M Pappagallo; C Parkes; C J Parkinson; G Passaleva; G D Patel; M Patel; G N Patrick; C Patrignani; C Pavel-Nicorescu; A Pazos Alvarez; A Pellegrino; G Penso; M Pepe Altarelli; S Perazzini; E Perez Trigo; A Pérez-Calero Yzquierdo; P Perret; M Perrin-Terrin; L Pescatore; E Pesen; K Petridis; A Petrolini; A Phan; E Picatoste Olloqui; B Pietrzyk; T Pilař; D Pinci; S Playfer; M Plo Casasus; F Polci; G Polok; A Poluektov; E Polycarpo; A Popov; D Popov; B Popovici; C Potterat; A Powell; J Prisciandaro; A Pritchard; C Prouve; V Pugatch; A Puig Navarro; G Punzi; W Qian; J H Rademacker; B Rakotomiaramanana; M S Rangel; I Raniuk; N Rauschmayr; G Raven; S Redford; M M Reid; A C dos Reis; S Ricciardi; A Richards; K Rinnert; V Rives Molina; D A Roa Romero; P Robbe; D A Roberts; E Rodrigues; P Rodriguez Perez; S Roiser; V Romanovsky; A Romero Vidal; J Rouvinet; T Ruf; F Ruffini; H Ruiz; P Ruiz Valls; G Sabatino; J J Saborido Silva; N Sagidova; P Sail; B Saitta; V Salustino Guimaraes; B Sanmartin Sedes; M Sannino; R Santacesaria; C Santamarina Rios; E Santovetti; M Sapunov; A Sarti; C Satriano; A Satta; M Savrie; D Savrina; P Schaack; M Schiller; H Schindler; M Schlupp; M Schmelling; B Schmidt; O Schneider; A Schopper; M-H Schune; R Schwemmer; B Sciascia; A Sciubba; M Seco; A Semennikov; K Senderowska; I Sepp; N Serra; J Serrano; P Seyfert; M Shapkin; I Shapoval; P Shatalov; Y Shcheglov; T Shears; L Shekhtman; O Shevchenko; V Shevchenko; A Shires; R Silva Coutinho; M Sirendi; T Skwarnicki; N A Smith; E Smith; J Smith; M Smith; M D Sokoloff; F J P Soler; F Soomro; D Souza; B Souza De Paula; B Spaan; A Sparkes; P Spradlin; F Stagni; S Stahl; O Steinkamp; S Stevenson; S Stoica; S Stone; B Storaci; M Straticiuc; U Straumann; V K Subbiah; L Sun; S Swientek; V Syropoulos; M Szczekowski; P Szczypka; T Szumlak; S T'Jampens; M Teklishyn; E Teodorescu; F Teubert; C Thomas; E Thomas; J van Tilburg; V Tisserand; M Tobin; S Tolk; D Tonelli; S Topp-Joergensen; N Torr; E Tournefier; S Tourneur; M T Tran; M Tresch; A Tsaregorodtsev; P Tsopelas; N Tuning; M Ubeda Garcia; A Ukleja; D Urner; A Ustyuzhanin; U Uwer; V Vagnoni; G Valenti; A Vallier; M Van Dijk; R Vazquez Gomez; P Vazquez Regueiro; C Vázquez Sierra; S Vecchi; J J Velthuis; M Veltri; G Veneziano; M Vesterinen; B Viaud; D Vieira; X Vilasis-Cardona; A Vollhardt; D Volyanskyy; D Voong; A Vorobyev; V Vorobyev; C Voß; H Voss; R Waldi; C Wallace; R Wallace; S Wandernoth; J Wang; D R Ward; N K Watson; A D Webber; D Websdale; M Whitehead; J Wicht; J Wiechczynski; D Wiedner; L Wiggers; G Wilkinson; M P Williams; M Williams; F F Wilson; J Wimberley; J Wishahi; W Wislicki; M Witek; S A Wotton; S Wright; S Wu; K Wyllie; Y Xie; Z Xing; Z Yang; R Young; X Yuan; O Yushchenko; M Zangoli; M Zavertyaev; F Zhang; L Zhang; W C Zhang; Y Zhang; A Zhelezov; A Zhokhov; L Zhong; A Zvyagin
Journal:  Phys Rev Lett       Date:  2013-11-04       Impact factor: 9.161

3.  Test of lepton universality using b+ → K+ℓ+ℓ- decays.

Authors:  R Aaij; B Adeva; M Adinolfi; A Affolder; Z Ajaltouni; S Akar; J Albrecht; F Alessio; M Alexander; S Ali; G Alkhazov; P Alvarez Cartelle; A A Alves; S Amato; S Amerio; Y Amhis; L An; L Anderlini; J Anderson; R Andreassen; M Andreotti; J E Andrews; R B Appleby; O Aquines Gutierrez; F Archilli; A Artamonov; M Artuso; E Aslanides; G Auriemma; M Baalouch; S Bachmann; J J Back; A Badalov; V Balagura; W Baldini; R J Barlow; C Barschel; S Barsuk; W Barter; V Batozskaya; V Battista; A Bay; L Beaucourt; J Beddow; F Bedeschi; I Bediaga; S Belogurov; K Belous; I Belyaev; E Ben-Haim; G Bencivenni; S Benson; J Benton; A Berezhnoy; R Bernet; M-O Bettler; M van Beuzekom; A Bien; S Bifani; T Bird; A Bizzeti; P M Bjørnstad; T Blake; F Blanc; J Blouw; S Blusk; V Bocci; A Bondar; N Bondar; W Bonivento; S Borghi; A Borgia; M Borsato; T J V Bowcock; E Bowen; C Bozzi; T Brambach; J van den Brand; J Bressieux; D Brett; M Britsch; T Britton; J Brodzicka; N H Brook; H Brown; A Bursche; G Busetto; J Buytaert; S Cadeddu; R Calabrese; M Calvi; M Calvo Gomez; P Campana; D Campora Perez; A Carbone; G Carboni; R Cardinale; A Cardini; L Carson; K Carvalho Akiba; G Casse; L Cassina; L Castillo Garcia; M Cattaneo; Ch Cauet; R Cenci; M Charles; Ph Charpentier; S Chen; S-F Cheung; N Chiapolini; M Chrzaszcz; K Ciba; X Cid Vidal; G Ciezarek; P E L Clarke; M Clemencic; H V Cliff; J Closier; V Coco; J Cogan; E Cogneras; P Collins; A Comerma-Montells; A Contu; A Cook; M Coombes; S Coquereau; G Corti; M Corvo; I Counts; B Couturier; G A Cowan; D C Craik; M Cruz Torres; S Cunliffe; R Currie; C D'Ambrosio; J Dalseno; P David; P N Y David; A Davis; K De Bruyn; S De Capua; M De Cian; J M De Miranda; L De Paula; W De Silva; P De Simone; D Decamp; M Deckenhoff; L Del Buono; N Déléage; D Derkach; O Deschamps; F Dettori; A Di Canto; H Dijkstra; S Donleavy; F Dordei; M Dorigo; A Dosil Suárez; D Dossett; A Dovbnya; K Dreimanis; G Dujany; F Dupertuis; P Durante; R Dzhelyadin; A Dziurda; A Dzyuba; S Easo; U Egede; V Egorychev; S Eidelman; S Eisenhardt; U Eitschberger; R Ekelhof; L Eklund; I El Rifai; Ch Elsasser; S Ely; S Esen; H-M Evans; T Evans; A Falabella; C Färber; C Farinelli; N Farley; S Farry; Rf Fay; D Ferguson; V Fernandez Albor; F Ferreira Rodrigues; M Ferro-Luzzi; S Filippov; M Fiore; M Fiorini; M Firlej; C Fitzpatrick; T Fiutowski; M Fontana; F Fontanelli; R Forty; O Francisco; M Frank; C Frei; M Frosini; J Fu; E Furfaro; A Gallas Torreira; D Galli; S Gallorini; S Gambetta; M Gandelman; P Gandini; Y Gao; J García Pardiñas; J Garofoli; J Garra Tico; L Garrido; C Gaspar; R Gauld; L Gavardi; G Gavrilov; E Gersabeck; M Gersabeck; T Gershon; Ph Ghez; A Gianelle; S Giani'; V Gibson; L Giubega; V V Gligorov; C Göbel; D Golubkov; A Golutvin; A Gomes; H Gordon; C Gotti; M Grabalosa Gándara; R Graciani Diaz; L A Granado Cardoso; E Graugés; G Graziani; A Grecu; E Greening; S Gregson; P Griffith; L Grillo; O Grünberg; B Gui; E Gushchin; Yu Guz; T Gys; C Hadjivasiliou; G Haefeli; C Haen; S C Haines; S Hall; B Hamilton; T Hampson; X Han; S Hansmann-Menzemer; N Harnew; S T Harnew; J Harrison; J He; T Head; V Heijne; K Hennessy; P Henrard; L Henry; J A Hernando Morata; E van Herwijnen; M Heß; A Hicheur; D Hill; M Hoballah; C Hombach; W Hulsbergen; P Hunt; N Hussain; D Hutchcroft; D Hynds; M Idzik; P Ilten; R Jacobsson; A Jaeger; J Jalocha; E Jans; P Jaton; A Jawahery; F Jing; M John; D Johnson; C R Jones; C Joram; B Jost; N Jurik; M Kaballo; S Kandybei; W Kanso; M Karacson; T M Karbach; S Karodia; M Kelsey; I R Kenyon; T Ketel; B Khanji; C Khurewathanakul; S Klaver; K Klimaszewski; O Kochebina; M Kolpin; I Komarov; R F Koopman; P Koppenburg; M Korolev; A Kozlinskiy; L Kravchuk; K Kreplin; M Kreps; G Krocker; P Krokovny; F Kruse; W Kucewicz; M Kucharczyk; V Kudryavtsev; K Kurek; T Kvaratskheliya; V N La Thi; D Lacarrere; G Lafferty; A Lai; D Lambert; R W Lambert; G Lanfranchi; C Langenbruch; B Langhans; T Latham; C Lazzeroni; R Le Gac; J van Leerdam; J-P Lees; R Lefèvre; A Leflat; J Lefrançois; S Leo; O Leroy; T Lesiak; B Leverington; Y Li; M Liles; R Lindner; C Linn; F Lionetto; B Liu; G Liu; S Lohn; I Longstaff; J H Lopes; N Lopez-March; P Lowdon; H Lu; D Lucchesi; H Luo; A Lupato; E Luppi; O Lupton; F Machefert; I V Machikhiliyan; F Maciuc; O Maev; S Malde; G Manca; G Mancinelli; J Maratas; J F Marchand; U Marconi; C Marin Benito; P Marino; R Märki; J Marks; G Martellotti; A Martens; A Martín Sánchez; M Martinelli; D Martinez Santos; F Martinez Vidal; D Martins Tostes; A Massafferri; R Matev; Z Mathe; C Matteuzzi; A Mazurov; M McCann; J McCarthy; A McNab; R McNulty; B McSkelly; B Meadows; F Meier; M Meissner; M Merk; D A Milanes; M-N Minard; N Moggi; J Molina Rodriguez; S Monteil; M Morandin; P Morawski; A Mordà; M J Morello; J Moron; A-B Morris; R Mountain; F Muheim; K Müller; M Mussini; B Muster; P Naik; T Nakada; R Nandakumar; I Nasteva; M Needham; N Neri; S Neubert; N Neufeld; M Neuner; A D Nguyen; T D Nguyen; C Nguyen-Mau; M Nicol; V Niess; R Niet; N Nikitin; T Nikodem; A Novoselov; D P O'Hanlon; A Oblakowska-Mucha; V Obraztsov; S Oggero; S Ogilvy; O Okhrimenko; R Oldeman; G Onderwater; M Orlandea; J M Otalora Goicochea; P Owen; A Oyanguren; B K Pal; A Palano; F Palombo; M Palutan; J Panman; A Papanestis; M Pappagallo; C Parkes; C J Parkinson; G Passaleva; G D Patel; M Patel; C Patrignani; A Pazos Alvarez; A Pearce; A Pellegrino; M Pepe Altarelli; S Perazzini; E Perez Trigo; P Perret; M Perrin-Terrin; L Pescatore; E Pesen; K Petridis; A Petrolini; E Picatoste Olloqui; B Pietrzyk; T Pilař; D Pinci; A Pistone; S Playfer; M Plo Casasus; F Polci; A Poluektov; E Polycarpo; A Popov; D Popov; B Popovici; C Potterat; E Price; J Prisciandaro; A Pritchard; C Prouve; V Pugatch; A Puig Navarro; G Punzi; W Qian; B Rachwal; J H Rademacker; B Rakotomiaramanana; M Rama; M S Rangel; I Raniuk; N Rauschmayr; G Raven; S Reichert; M M Reid; A C Dos Reis; S Ricciardi; S Richards; M Rihl; K Rinnert; V Rives Molina; D A Roa Romero; P Robbe; A B Rodrigues; E Rodrigues; P Rodriguez Perez; S Roiser; V Romanovsky; A Romero Vidal; M Rotondo; J Rouvinet; T Ruf; F Ruffini; H Ruiz; P Ruiz Valls; J J Saborido Silva; N Sagidova; P Sail; B Saitta; V Salustino Guimaraes; C Sanchez Mayordomo; B Sanmartin Sedes; R Santacesaria; C Santamarina Rios; E Santovetti; A Sarti; C Satriano; A Satta; D M Saunders; M Savrie; D Savrina; M Schiller; H Schindler; M Schlupp; M Schmelling; B Schmidt; O Schneider; A Schopper; M-H Schune; R Schwemmer; B Sciascia; A Sciubba; M Seco; A Semennikov; I Sepp; N Serra; J Serrano; L Sestini; P Seyfert; M Shapkin; I Shapoval; Y Shcheglov; T Shears; L Shekhtman; V Shevchenko; A Shires; R Silva Coutinho; G Simi; M Sirendi; N Skidmore; T Skwarnicki; N A Smith; E Smith; E Smith; J Smith; M Smith; H Snoek; M D Sokoloff; F J P Soler; F Soomro; D Souza; B Souza De Paula; B Spaan; A Sparkes; P Spradlin; S Sridharan; F Stagni; M Stahl; S Stahl; O Steinkamp; O Stenyakin; S Stevenson; S Stoica; S Stone; B Storaci; S Stracka; M Straticiuc; U Straumann; R Stroili; V K Subbiah; L Sun; W Sutcliffe; K Swientek; S Swientek; V Syropoulos; M Szczekowski; P Szczypka; D Szilard; T Szumlak; S T'Jampens; M Teklishyn; G Tellarini; F Teubert; C Thomas; E Thomas; J van Tilburg; V Tisserand; M Tobin; S Tolk; L Tomassetti; D Tonelli; S Topp-Joergensen; N Torr; E Tournefier; S Tourneur; M T Tran; M Tresch; A Tsaregorodtsev; P Tsopelas; N Tuning; M Ubeda Garcia; A Ukleja; A Ustyuzhanin; U Uwer; V Vagnoni; G Valenti; A Vallier; R Vazquez Gomez; P Vazquez Regueiro; C Vázquez Sierra; S Vecchi; J J Velthuis; M Veltri; G Veneziano; M Vesterinen; B Viaud; D Vieira; M Vieites Diaz; X Vilasis-Cardona; A Vollhardt; D Volyanskyy; D Voong; A Vorobyev; V Vorobyev; C Voß; H Voss; J A de Vries; R Waldi; C Wallace; R Wallace; J Walsh; S Wandernoth; J Wang; D R Ward; N K Watson; D Websdale; M Whitehead; J Wicht; D Wiedner; G Wilkinson; M P Williams; M Williams; F F Wilson; J Wimberley; J Wishahi; W Wislicki; M Witek; G Wormser; S A Wotton; S Wright; S Wu; K Wyllie; Y Xie; Z Xing; Z Xu; Z Yang; X Yuan; O Yushchenko; M Zangoli; M Zavertyaev; L Zhang; W C Zhang; Y Zhang; A Zhelezov; A Zhokhov; L Zhong; A Zvyagin
Journal:  Phys Rev Lett       Date:  2014-10-06       Impact factor: 9.161

4.  Observation of the rare B(s)(0) →µ+µ− decay from the combined analysis of CMS and LHCb data.

Authors: 
Journal:  Nature       Date:  2015-06-04       Impact factor: 49.962

5.  Precision measurement of CP violation in B(S)(0)→J/ΨK+K- decays.

Authors:  R Aaij; B Adeva; M Adinolfi; A Affolder; Z Ajaltouni; S Akar; J Albrecht; F Alessio; M Alexander; S Ali; G Alkhazov; P Alvarez Cartelle; A A Alves; S Amato; S Amerio; Y Amhis; L An; L Anderlini; J Anderson; R Andreassen; M Andreotti; J E Andrews; R B Appleby; O Aquines Gutierrez; F Archilli; A Artamonov; M Artuso; E Aslanides; G Auriemma; M Baalouch; S Bachmann; J J Back; A Badalov; C Baesso; W Baldini; R J Barlow; C Barschel; S Barsuk; W Barter; V Batozskaya; V Battista; A Bay; L Beaucourt; J Beddow; F Bedeschi; I Bediaga; S Belogurov; K Belous; I Belyaev; E Ben-Haim; G Bencivenni; S Benson; J Benton; A Berezhnoy; R Bernet; A Bertolin; M-O Bettler; M van Beuzekom; A Bien; S Bifani; T Bird; A Bizzeti; P M Bjørnstad; T Blake; F Blanc; J Blouw; S Blusk; V Bocci; A Bondar; N Bondar; W Bonivento; S Borghi; A Borgia; M Borsato; T J V Bowcock; E Bowen; C Bozzi; D Brett; M Britsch; T Britton; J Brodzicka; N H Brook; A Bursche; J Buytaert; S Cadeddu; R Calabrese; M Calvi; M Calvo Gomez; P Campana; D Campora Perez; A Carbone; G Carboni; R Cardinale; A Cardini; L Carson; K Carvalho Akiba; R C M Casanova Mohr; G Casse; L Cassina; L Castillo Garcia; M Cattaneo; Ch Cauet; R Cenci; M Charles; Ph Charpentier; M Chefdeville; S Chen; S-F Cheung; N Chiapolini; M Chrzaszcz; X Cid Vidal; G Ciezarek; P E L Clarke; M Clemencic; H V Cliff; J Closier; V Coco; J Cogan; E Cogneras; V Cogoni; L Cojocariu; G Collazuol; P Collins; A Comerma-Montells; A Contu; A Cook; M Coombes; S Coquereau; G Corti; M Corvo; I Counts; B Couturier; G A Cowan; D C Craik; A C Crocombe; M Cruz Torres; S Cunliffe; R Currie; C D'Ambrosio; J Dalseno; P David; P N Y David; A Davis; K De Bruyn; S De Capua; M De Cian; J M De Miranda; L De Paula; W De Silva; P De Simone; C-T Dean; D Decamp; M Deckenhoff; L Del Buono; N Déléage; D Derkach; O Deschamps; F Dettori; A Di Canto; A Di Domenico; H Dijkstra; S Donleavy; F Dordei; M Dorigo; A Dosil Suárez; D Dossett; A Dovbnya; K Dreimanis; G Dujany; F Dupertuis; P Durante; R Dzhelyadin; A Dziurda; A Dzyuba; S Easo; U Egede; V Egorychev; S Eidelman; S Eisenhardt; U Eitschberger; R Ekelhof; L Eklund; I El Rifai; Ch Elsasser; S Ely; S Esen; H-M Evans; T Evans; A Falabella; C Färber; C Farinelli; N Farley; S Farry; R Fay; D Ferguson; V Fernandez Albor; F Ferreira Rodrigues; M Ferro-Luzzi; S Filippov; M Fiore; M Fiorini; M Firlej; C Fitzpatrick; T Fiutowski; P Fol; M Fontana; F Fontanelli; R Forty; O Francisco; M Frank; C Frei; M Frosini; J Fu; E Furfaro; A Gallas Torreira; D Galli; S Gallorini; S Gambetta; M Gandelman; P Gandini; Y Gao; J García Pardiñas; J Garofoli; J Garra Tico; L Garrido; D Gascon; C Gaspar; U Gastaldi; R Gauld; L Gavardi; G Gazzoni; A Geraci; E Gersabeck; M Gersabeck; T Gershon; Ph Ghez; A Gianelle; S Gianì; V Gibson; L Giubega; V V Gligorov; C Göbel; D Golubkov; A Golutvin; A Gomes; C Gotti; M Grabalosa Gándara; R Graciani Diaz; L A Granado Cardoso; E Graugés; E Graverini; G Graziani; A Grecu; E Greening; S Gregson; P Griffith; L Grillo; O Grünberg; B Gui; E Gushchin; Yu Guz; T Gys; C Hadjivasiliou; G Haefeli; C Haen; S C Haines; S Hall; B Hamilton; T Hampson; X Han; S Hansmann-Menzemer; N Harnew; S T Harnew; J Harrison; J He; T Head; V Heijne; K Hennessy; P Henrard; L Henry; J A Hernando Morata; E van Herwijnen; M Heß; A Hicheur; D Hill; M Hoballah; C Hombach; W Hulsbergen; N Hussain; D Hutchcroft; D Hynds; M Idzik; P Ilten; R Jacobsson; A Jaeger; J Jalocha; E Jans; P Jaton; A Jawahery; F Jing; M John; D Johnson; C R Jones; C Joram; B Jost; N Jurik; S Kandybei; W Kanso; M Karacson; T M Karbach; S Karodia; M Kelsey; I R Kenyon; T Ketel; B Khanji; C Khurewathanakul; S Klaver; K Klimaszewski; O Kochebina; M Kolpin; I Komarov; R F Koopman; P Koppenburg; M Korolev; L Kravchuk; K Kreplin; M Kreps; G Krocker; P Krokovny; F Kruse; W Kucewicz; M Kucharczyk; V Kudryavtsev; K Kurek; T Kvaratskheliya; V N La Thi; D Lacarrere; G Lafferty; A Lai; D Lambert; R W Lambert; G Lanfranchi; C Langenbruch; B Langhans; T Latham; C Lazzeroni; R Le Gac; J van Leerdam; J-P Lees; R Lefèvre; A Leflat; J Lefrançois; O Leroy; T Lesiak; B Leverington; Y Li; T Likhomanenko; M Liles; R Lindner; C Linn; F Lionetto; B Liu; S Lohn; I Longstaff; J H Lopes; P Lowdon; D Lucchesi; H Luo; A Lupato; E Luppi; O Lupton; F Machefert; I V Machikhiliyan; F Maciuc; O Maev; S Malde; A Malinin; G Manca; G Mancinelli; A Mapelli; J Maratas; J F Marchand; U Marconi; C Marin Benito; P Marino; R Märki; J Marks; G Martellotti; M Martinelli; D Martinez Santos; F Martinez Vidal; D Martins Tostes; A Massafferri; R Matev; Z Mathe; C Matteuzzi; A Mazurov; M McCann; J McCarthy; A McNab; R McNulty; B McSkelly; B Meadows; F Meier; M Meissner; M Merk; D A Milanes; M-N Minard; N Moggi; J Molina Rodriguez; S Monteil; M Morandin; P Morawski; A Mordà; M J Morello; J Moron; A-B Morris; R Mountain; F Muheim; K Müller; M Mussini; B Muster; P Naik; T Nakada; R Nandakumar; I Nasteva; M Needham; N Neri; S Neubert; N Neufeld; M Neuner; A D Nguyen; T D Nguyen; C Nguyen-Mau; M Nicol; V Niess; R Niet; N Nikitin; T Nikodem; A Novoselov; D P O'Hanlon; A Oblakowska-Mucha; V Obraztsov; S Ogilvy; O Okhrimenko; R Oldeman; C J G Onderwater; M Orlandea; J M Otalora Goicochea; A Otto; P Owen; A Oyanguren; B K Pal; A Palano; F Palombo; M Palutan; J Panman; A Papanestis; M Pappagallo; L L Pappalardo; C Parkes; C J Parkinson; G Passaleva; G D Patel; M Patel; C Patrignani; A Pearce; A Pellegrino; G Penso; M Pepe Altarelli; S Perazzini; P Perret; L Pescatore; E Pesen; K Petridis; A Petrolini; E Picatoste Olloqui; B Pietrzyk; T Pilař; D Pinci; A Pistone; S Playfer; M Plo Casasus; F Polci; A Poluektov; I Polyakov; E Polycarpo; A Popov; D Popov; B Popovici; C Potterat; E Price; J D Price; J Prisciandaro; A Pritchard; C Prouve; V Pugatch; A Puig Navarro; G Punzi; W Qian; B Rachwal; J H Rademacker; B Rakotomiaramanana; M Rama; M S Rangel; I Raniuk; N Rauschmayr; G Raven; F Redi; S Reichert; M M Reid; A C dos Reis; S Ricciardi; S Richards; M Rihl; K Rinnert; V Rives Molina; P Robbe; A B Rodrigues; E Rodrigues; P Rodriguez Perez; S Roiser; V Romanovsky; A Romero Vidal; M Rotondo; J Rouvinet; T Ruf; H Ruiz; P Ruiz Valls; J J Saborido Silva; N Sagidova; P Sail; B Saitta; V Salustino Guimaraes; C Sanchez Mayordomo; B Sanmartin Sedes; R Santacesaria; C Santamarina Rios; E Santovetti; A Sarti; C Satriano; A Satta; D M Saunders; D Savrina; M Schiller; H Schindler; M Schlupp; M Schmelling; B Schmidt; O Schneider; A Schopper; M-H Schune; R Schwemmer; B Sciascia; A Sciubba; A Semennikov; I Sepp; N Serra; J Serrano; L Sestini; P Seyfert; M Shapkin; I Shapoval; Y Shcheglov; T Shears; L Shekhtman; V Shevchenko; A Shires; R Silva Coutinho; G Simi; M Sirendi; N Skidmore; I Skillicorn; T Skwarnicki; N A Smith; E Smith; E Smith; J Smith; M Smith; H Snoek; M D Sokoloff; F J P Soler; F Soomro; D Souza; B Souza De Paula; B Spaan; P Spradlin; S Sridharan; F Stagni; M Stahl; S Stahl; O Steinkamp; O Stenyakin; F Sterpka; S Stevenson; S Stoica; S Stone; B Storaci; S Stracka; M Straticiuc; U Straumann; R Stroili; L Sun; W Sutcliffe; K Swientek; S Swientek; V Syropoulos; M Szczekowski; P Szczypka; T Szumlak; S T'Jampens; M Teklishyn; G Tellarini; F Teubert; C Thomas; E Thomas; J van Tilburg; V Tisserand; M Tobin; J Todd; S Tolk; L Tomassetti; D Tonelli; S Topp-Joergensen; N Torr; E Tournefier; S Tourneur; M T Tran; M Tresch; A Trisovic; A Tsaregorodtsev; P Tsopelas; N Tuning; M Ubeda Garcia; A Ukleja; A Ustyuzhanin; U Uwer; C Vacca; V Vagnoni; G Valenti; A Vallier; R Vazquez Gomez; P Vazquez Regueiro; C Vázquez Sierra; S Vecchi; J J Velthuis; M Veltri; G Veneziano; M Vesterinen; J V V B Viana Barbosa; B Viaud; D Vieira; M Vieites Diaz; X Vilasis-Cardona; A Vollhardt; D Volyanskyy; D Voong; A Vorobyev; V Vorobyev; C Voß; J A de Vries; R Waldi; C Wallace; R Wallace; J Walsh; S Wandernoth; J Wang; D R Ward; N K Watson; D Websdale; M Whitehead; D Wiedner; G Wilkinson; M Wilkinson; M P Williams; M Williams; H W Wilschut; F F Wilson; J Wimberley; J Wishahi; W Wislicki; M Witek; G Wormser; S A Wotton; S Wright; K Wyllie; Y Xie; Z Xing; Z Xu; Z Yang; X Yuan; O Yushchenko; M Zangoli; M Zavertyaev; L Zhang; W C Zhang; Y Zhang; A Zhelezov; A Zhokhov; L Zhong
Journal:  Phys Rev Lett       Date:  2015-01-30       Impact factor: 9.161

6.  Study of CP asymmetry in B^{0}-B[over ¯]^{0} mixing with inclusive dilepton events.

Authors:  J P Lees; V Poireau; V Tisserand; E Grauges; A Palano; G Eigen; B Stugu; D N Brown; L T Kerth; Yu G Kolomensky; M J Lee; G Lynch; H Koch; T Schroeder; C Hearty; T S Mattison; J A McKenna; R Y So; A Khan; V E Blinov; A R Buzykaev; V P Druzhinin; V B Golubev; E A Kravchenko; A P Onuchin; S I Serednyakov; Yu I Skovpen; E P Solodov; K Yu Todyshev; A J Lankford; M Mandelkern; B Dey; J W Gary; O Long; C Campagnari; M Franco Sevilla; T M Hong; D Kovalskyi; J D Richman; C A West; A M Eisner; W S Lockman; W Panduro Vazquez; B A Schumm; A Seiden; D S Chao; C H Cheng; B Echenard; K T Flood; D G Hitlin; T S Miyashita; P Ongmongkolkul; F C Porter; M Röhrken; R Andreassen; Z Huard; B T Meadows; B G Pushpawela; M D Sokoloff; L Sun; P C Bloom; W T Ford; A Gaz; J G Smith; S R Wagner; R Ayad; W H Toki; B Spaan; D Bernard; M Verderi; S Playfer; D Bettoni; C Bozzi; R Calabrese; G Cibinetto; E Fioravanti; I Garzia; E Luppi; L Piemontese; V Santoro; A Calcaterra; R de Sangro; G Finocchiaro; S Martellotti; P Patteri; I M Peruzzi; M Piccolo; M Rama; A Zallo; R Contri; M Lo Vetere; M R Monge; S Passaggio; C Patrignani; E Robutti; B Bhuyan; V Prasad; A Adametz; U Uwer; H M Lacker; P D Dauncey; U Mallik; C Chen; J Cochran; S Prell; H Ahmed; A V Gritsan; N Arnaud; M Davier; D Derkach; G Grosdidier; F Le Diberder; A M Lutz; B Malaescu; P Roudeau; A Stocchi; G Wormser; D J Lange; D M Wright; J P Coleman; J R Fry; E Gabathuler; D E Hutchcroft; D J Payne; C Touramanis; A J Bevan; F Di Lodovico; R Sacco; G Cowan; J Bougher; D N Brown; C L Davis; A G Denig; M Fritsch; W Gradl; K Griessinger; A Hafner; K R Schubert; R J Barlow; G D Lafferty; R Cenci; B Hamilton; A Jawahery; D A Roberts; R Cowan; G Sciolla; R Cheaib; P M Patel; S H Robertson; N Neri; F Palombo; L Cremaldi; R Godang; P Sonnek; D J Summers; M Simard; P Taras; G De Nardo; G Onorato; C Sciacca; M Martinelli; G Raven; C P Jessop; J M LoSecco; K Honscheid; R Kass; E Feltresi; M Margoni; M Morandin; M Posocco; M Rotondo; G Simi; F Simonetto; R Stroili; S Akar; E Ben-Haim; M Bomben; G R Bonneaud; H Briand; G Calderini; J Chauveau; Ph Leruste; G Marchiori; J Ocariz; M Biasini; E Manoni; S Pacetti; A Rossi; C Angelini; G Batignani; S Bettarini; M Carpinelli; G Casarosa; A Cervelli; M Chrzaszcz; F Forti; M A Giorgi; A Lusiani; B Oberhof; E Paoloni; A Perez; G Rizzo; J J Walsh; D Lopes Pegna; J Olsen; A J S Smith; R Faccini; F Ferrarotto; F Ferroni; M Gaspero; L Li Gioi; A Pilloni; G Piredda; C Bünger; S Dittrich; O Grünberg; M Hess; T Leddig; C Voß; R Waldi; T Adye; E O Olaiya; F F Wilson; S Emery; G Vasseur; F Anulli; D Aston; D J Bard; C Cartaro; M R Convery; J Dorfan; G P Dubois-Felsmann; W Dunwoodie; M Ebert; R C Field; B G Fulsom; M T Graham; C Hast; W R Innes; P Kim; D W G S Leith; P Lewis; D Lindemann; S Luitz; V Luth; H L Lynch; D B MacFarlane; D R Muller; H Neal; M Perl; T Pulliam; B N Ratcliff; A Roodman; A A Salnikov; R H Schindler; A Snyder; D Su; M K Sullivan; J Va'vra; W J Wisniewski; H W Wulsin; M V Purohit; R M White; J R Wilson; A Randle-Conde; S J Sekula; M Bellis; P R Burchat; E M T Puccio; M S Alam; J A Ernst; R Gorodeisky; N Guttman; D R Peimer; A Soffer; S M Spanier; J L Ritchie; A M Ruland; R F Schwitters; B C Wray; J M Izen; X C Lou; F Bianchi; F De Mori; A Filippi; D Gamba; L Lanceri; L Vitale; F Martinez-Vidal; A Oyanguren; P Villanueva-Perez; J Albert; Sw Banerjee; A Beaulieu; F U Bernlochner; H H F Choi; G J King; R Kowalewski; M J Lewczuk; T Lueck; I M Nugent; J M Roney; R J Sobie; N Tasneem; T J Gershon; P F Harrison; T E Latham; H R Band; S Dasu; Y Pan; R Prepost; S L Wu
Journal:  Phys Rev Lett       Date:  2015-02-25       Impact factor: 9.161

7.  Measurement of the Bs(0)→μ+ μ- branching fraction and search for B(0)→μ+ μ- with the CMS experiment.

Authors:  S Chatrchyan; V Khachatryan; A M Sirunyan; A Tumasyan; W Adam; T Bergauer; M Dragicevic; J Erö; C Fabjan; M Friedl; R Frühwirth; V M Ghete; N Hörmann; J Hrubec; M Jeitler; W Kiesenhofer; V Knünz; M Krammer; I Krätschmer; D Liko; I Mikulec; D Rabady; B Rahbaran; C Rohringer; H Rohringer; R Schöfbeck; J Strauss; A Taurok; W Treberer-Treberspurg; W Waltenberger; C-E Wulz; V Mossolov; N Shumeiko; J Suarez Gonzalez; S Alderweireldt; M Bansal; S Bansal; T Cornelis; E A De Wolf; X Janssen; A Knutsson; S Luyckx; L Mucibello; S Ochesanu; B Roland; R Rougny; Z Staykova; H Van Haevermaet; P Van Mechelen; N Van Remortel; A Van Spilbeeck; F Blekman; S Blyweert; J D'Hondt; A Kalogeropoulos; J Keaveney; S Lowette; M Maes; A Olbrechts; S Tavernier; W Van Doninck; P Van Mulders; G P Van Onsem; I Villella; C Caillol; B Clerbaux; G De Lentdecker; L Favart; A P R Gay; T Hreus; A Léonard; P E Marage; A Mohammadi; L Perniè; T Reis; T Seva; L Thomas; C Vander Velde; P Vanlaer; J Wang; V Adler; K Beernaert; L Benucci; A Cimmino; S Costantini; S Dildick; G Garcia; B Klein; J Lellouch; A Marinov; J Mccartin; A A Ocampo Rios; D Ryckbosch; M Sigamani; N Strobbe; F Thyssen; M Tytgat; S Walsh; E Yazgan; N Zaganidis; S Basegmez; C Beluffi; G Bruno; R Castello; A Caudron; L Ceard; G G Da Silveira; C Delaere; T du Pree; D Favart; L Forthomme; A Giammanco; J Hollar; P Jez; V Lemaitre; J Liao; O Militaru; C Nuttens; D Pagano; A Pin; K Piotrzkowski; A Popov; M Selvaggi; M Vidal Marono; J M Vizan Garcia; N Beliy; T Caebergs; E Daubie; G H Hammad; G A Alves; M Correa Martins Junior; T Martins; M E Pol; M H G Souza; W L Aldá Júnior; W Carvalho; J Chinellato; A Custódio; E M Da Costa; D De Jesus Damiao; C De Oliveira Martins; S Fonseca De Souza; H Malbouisson; M Malek; D Matos Figueiredo; L Mundim; H Nogima; W L Prado Da Silva; A Santoro; A Sznajder; E J Tonelli Manganote; A Vilela Pereira; C A Bernardes; F A Dias; T R Fernandez Perez Tomei; E M Gregores; C Lagana; P G Mercadante; S F Novaes; Sandra S Padula; V Genchev; P Iaydjiev; S Piperov; M Rodozov; G Sultanov; M Vutova; A Dimitrov; R Hadjiiska; V Kozhuharov; L Litov; B Pavlov; P Petkov; J G Bian; G M Chen; H S Chen; C H Jiang; D Liang; S Liang; X Meng; J Tao; X Wang; Z Wang; C Asawatangtrakuldee; Y Ban; Y Guo; W Li; S Liu; Y Mao; S J Qian; H Teng; D Wang; L Zhang; W Zou; C Avila; C A Carrillo Montoya; L F Chaparro Sierra; J P Gomez; B Gomez Moreno; J C Sanabria; N Godinovic; D Lelas; R Plestina; D Polic; I Puljak; Z Antunovic; M Kovac; V Brigljevic; K Kadija; J Luetic; D Mekterovic; S Morovic; L Tikvica; A Attikis; G Mavromanolakis; J Mousa; C Nicolaou; F Ptochos; P A Razis; M Finger; M Finger; Y Assran; S Elgammal; A Ellithi Kamel; A M Kuotb Awad; M A Mahmoud; A Radi; M Kadastik; M Müntel; M Murumaa; M Raidal; L Rebane; A Tiko; P Eerola; G Fedi; M Voutilainen; J Härkönen; V Karimäki; R Kinnunen; M J Kortelainen; T Lampén; K Lassila-Perini; S Lehti; T Lindén; P Luukka; T Mäenpää; T Peltola; E Tuominen; J Tuominiemi; E Tuovinen; L Wendland; T Tuuva; M Besancon; F Couderc; M Dejardin; D Denegri; B Fabbro; J L Faure; F Ferri; S Ganjour; A Givernaud; P Gras; G Hamel de Monchenault; P Jarry; E Locci; J Malcles; L Millischer; A Nayak; J Rander; A Rosowsky; M Titov; S Baffioni; F Beaudette; L Benhabib; M Bluj; P Busson; C Charlot; N Daci; T Dahms; M Dalchenko; L Dobrzynski; A Florent; R Granier de Cassagnac; M Haguenauer; P Miné; C Mironov; I N Naranjo; M Nguyen; C Ochando; P Paganini; D Sabes; R Salerno; Y Sirois; C Veelken; A Zabi; J-L Agram; J Andrea; D Bloch; J-M Brom; E C Chabert; C Collard; E Conte; F Drouhin; J-C Fontaine; D Gelé; U Goerlach; C Goetzmann; P Juillot; A-C Le Bihan; P Van Hove; S Gadrat; S Beauceron; N Beaupere; G Boudoul; S Brochet; J Chasserat; R Chierici; D Contardo; P Depasse; H El Mamouni; J Fan; J Fay; S Gascon; M Gouzevitch; B Ille; T Kurca; M Lethuillier; L Mirabito; S Perries; L Sgandurra; V Sordini; M Vander Donckt; P Verdier; S Viret; H Xiao; Z Tsamalaidze; C Autermann; S Beranek; M Bontenackels; B Calpas; M Edelhoff; L Feld; N Heracleous; O Hindrichs; K Klein; A Ostapchuk; A Perieanu; F Raupach; J Sammet; S Schael; D Sprenger; H Weber; B Wittmer; V Zhukov; M Ata; J Caudron; E Dietz-Laursonn; D Duchardt; M Erdmann; R Fischer; A Güth; T Hebbeker; C Heidemann; K Hoepfner; D Klingebiel; S Knutzen; P Kreuzer; M Merschmeyer; A Meyer; M Olschewski; K Padeken; P Papacz; H Pieta; H Reithler; S A Schmitz; L Sonnenschein; J Steggemann; D Teyssier; S Thüer; M Weber; V Cherepanov; Y Erdogan; G Flügge; H Geenen; M Geisler; W Haj Ahmad; F Hoehle; B Kargoll; T Kress; Y Kuessel; J Lingemann; A Nowack; I M Nugent; L Perchalla; O Pooth; A Stahl; I Asin; N Bartosik; J Behr; W Behrenhoff; U Behrens; A J Bell; M Bergholz; A Bethani; K Borras; A Burgmeier; A Cakir; L Calligaris; A Campbell; S Choudhury; F Costanza; C Diez Pardos; S Dooling; T Dorland; G Eckerlin; D Eckstein; G Flucke; A Geiser; I Glushkov; A Grebenyuk; P Gunnellini; S Habib; J Hauk; G Hellwig; D Horton; H Jung; M Kasemann; P Katsas; C Kleinwort; H Kluge; M Krämer; D Krücker; E Kuznetsova; W Lange; J Leonard; K Lipka; W Lohmann; B Lutz; R Mankel; I Marfin; I-A Melzer-Pellmann; A B Meyer; J Mnich; A Mussgiller; S Naumann-Emme; O Novgorodova; F Nowak; J Olzem; H Perrey; A Petrukhin; D Pitzl; R Placakyte; A Raspereza; P M Ribeiro Cipriano; C Riedl; E Ron; M Ö Sahin; J Salfeld-Nebgen; R Schmidt; T Schoerner-Sadenius; N Sen; M Stein; R Walsh; C Wissing; M Aldaya Martin; V Blobel; H Enderle; J Erfle; E Garutti; U Gebbert; M Görner; M Gosselink; J Haller; K Heine; R S Höing; G Kaussen; H Kirschenmann; R Klanner; R Kogler; J Lange; I Marchesini; T Peiffer; N Pietsch; D Rathjens; C Sander; H Schettler; P Schleper; E Schlieckau; A Schmidt; M Schröder; T Schum; M Seidel; J Sibille; V Sola; H Stadie; G Steinbrück; J Thomsen; D Troendle; E Usai; L Vanelderen; C Barth; C Baus; J Berger; C Böser; E Butz; T Chwalek; W De Boer; A Descroix; A Dierlamm; M Feindt; M Guthoff; F Hartmann; T Hauth; H Held; K H Hoffmann; U Husemann; I Katkov; J R Komaragiri; A Kornmayer; P Lobelle Pardo; D Martschei; M U Mozer; Th Müller; M Niegel; A Nürnberg; O Oberst; J Ott; G Quast; K Rabbertz; F Ratnikov; S Röcker; F-P Schilling; G Schott; H J Simonis; F M Stober; R Ulrich; J Wagner-Kuhr; S Wayand; T Weiler; M Zeise; G Anagnostou; G Daskalakis; T Geralis; S Kesisoglou; A Kyriakis; D Loukas; A Markou; C Markou; E Ntomari; I Topsis-giotis; L Gouskos; A Panagiotou; N Saoulidou; E Stiliaris; X Aslanoglou; I Evangelou; G Flouris; C Foudas; P Kokkas; N Manthos; I Papadopoulos; E Paradas; G Bencze; C Hajdu; P Hidas; D Horvath; F Sikler; V Veszpremi; G Vesztergombi; A J Zsigmond; N Beni; S Czellar; J Molnar; J Palinkas; Z Szillasi; J Karancsi; P Raics; Z L Trocsanyi; B Ujvari; N Sahoo; S K Swain; S B Beri; V Bhatnagar; N Dhingra; R Gupta; M Kaur; M Z Mehta; M Mittal; N Nishu; A Sharma; J B Singh; Ashok Kumar; Arun Kumar; S Ahuja; A Bhardwaj; B C Choudhary; A Kumar; S Malhotra; M Naimuddin; K Ranjan; P Saxena; V Sharma; R K Shivpuri; S Banerjee; S Bhattacharya; K Chatterjee; S Dutta; B Gomber; Sa Jain; Sh Jain; R Khurana; A Modak; S Mukherjee; D Roy; S Sarkar; M Sharan; A P Singh; A Abdulsalam; D Dutta; S Kailas; V Kumar; A K Mohanty; L M Pant; P Shukla; A Topkar; T Aziz; R M Chatterjee; S Ganguly; S Ghosh; M Guchait; A Gurtu; G Kole; S Kumar; M Maity; G Majumder; K Mazumdar; G B Mohanty; B Parida; K Sudhakar; N Wickramage; S Banerjee; S Dugad; H Arfaei; H Bakhshiansohi; S M Etesami; A Fahim; A Jafari; M Khakzad; M Mohammadi Najafabadi; S Paktinat Mehdiabadi; B Safarzadeh; M Zeinali; M Grunewald; M Abbrescia; L Barbone; C Calabria; S S Chhibra; A Colaleo; D Creanza; N De Filippis; M De Palma; L Fiore; G Iaselli; G Maggi; M Maggi; B Marangelli; S My; S Nuzzo; N Pacifico; A Pompili; G Pugliese; G Selvaggi; L Silvestris; G Singh; R Venditti; P Verwilligen; G Zito; G Abbiendi; A C Benvenuti; D Bonacorsi; S Braibant-Giacomelli; L Brigliadori; R Campanini; P Capiluppi; A Castro; F R Cavallo; G Codispoti; M Cuffiani; G M Dallavalle; F Fabbri; A Fanfani; D Fasanella; P Giacomelli; C Grandi; L Guiducci; S Marcellini; G Masetti; M Meneghelli; A Montanari; F L Navarria; F Odorici; A Perrotta; F Primavera; A M Rossi; T Rovelli; G P Siroli; N Tosi; R Travaglini; S Albergo; G Cappello; M Chiorboli; S Costa; F Giordano; R Potenza; A Tricomi; C Tuve; G Barbagli; V Ciulli; C Civinini; R D'Alessandro; E Focardi; S Frosali; E Gallo; S Gonzi; V Gori; P Lenzi; M Meschini; S Paoletti; G Sguazzoni; A Tropiano; L Benussi; S Bianco; F Fabbri; D Piccolo; P Fabbricatore; R Ferretti; F Ferro; M Lo Vetere; R Musenich; E Robutti; S Tosi; A Benaglia; M E Dinardo; S Fiorendi; S Gennai; A Ghezzi; P Govoni; M T Lucchini; S Malvezzi; R A Manzoni; A Martelli; D Menasce; L Moroni; M Paganoni; D Pedrini; S Ragazzi; N Redaelli; T Tabarelli de Fatis; S Buontempo; N Cavallo; A De Cosa; F Fabozzi; A O M Iorio; L Lista; S Meola; M Merola; P Paolucci; P Azzi; N Bacchetta; M Biasotto; D Bisello; A Branca; R Carlin; P Checchia; T Dorigo; U Dosselli; M Galanti; F Gasparini; U Gasparini; P Giubilato; A Gozzelino; K Kanishchev; S Lacaprara; I Lazzizzera; M Margoni; A T Meneguzzo; M Nespolo; J Pazzini; N Pozzobon; P Ronchese; F Simonetto; E Torassa; M Tosi; S Vanini; P Zotto; A Zucchetta; G Zumerle; M Gabusi; S P Ratti; C Riccardi; P Vitulo; M Biasini; G M Bilei; L Fanò; P Lariccia; G Mantovani; M Menichelli; A Nappi; F Romeo; A Saha; A Santocchia; A Spiezia; K Androsov; P Azzurri; G Bagliesi; T Boccali; G Broccolo; R Castaldi; M A Ciocci; R T D'Agnolo; R Dell'Orso; F Fiori; L Foà; A Giassi; M T Grippo; A Kraan; F Ligabue; T Lomtadze; L Martini; A Messineo; C S Moon; F Palla; A Rizzi; A Savoy-Navarro; A T Serban; P Spagnolo; P Squillacioti; R Tenchini; G Tonelli; A Venturi; P G Verdini; C Vernieri; L Barone; F Cavallari; D Del Re; M Diemoz; M Grassi; E Longo; F Margaroli; P Meridiani; F Micheli; S Nourbakhsh; G Organtini; R Paramatti; S Rahatlou; C Rovelli; L Soffi; N Amapane; R Arcidiacono; S Argiro; M Arneodo; R Bellan; C Biino; N Cartiglia; S Casasso; 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P Lamichhane; A Sakharov; D A Belknap; L Borrello; D Carlsmith; M Cepeda; S Dasu; S Duric; E Friis; M Grothe; R Hall-Wilton; M Herndon; A Hervé; P Klabbers; J Klukas; A Lanaro; R Loveless; A Mohapatra; I Ojalvo; T Perry; G A Pierro; G Polese; I Ross; T Sarangi; A Savin; W H Smith; J Swanson
Journal:  Phys Rev Lett       Date:  2013-09-05       Impact factor: 9.161

8.  Measurement of the Bs(0)→μ+ μ- branching fraction and search for B(0)→μ+ μ- decays at the LHCb experiment.

Authors:  R Aaij; B Adeva; M Adinolfi; C Adrover; A Affolder; Z Ajaltouni; J Albrecht; F Alessio; M Alexander; S Ali; G Alkhazov; P Alvarez Cartelle; A A Alves; S Amato; S Amerio; Y Amhis; L Anderlini; J Anderson; R Andreassen; J E Andrews; R B Appleby; O Aquines Gutierrez; F Archilli; A Artamonov; M Artuso; E Aslanides; G Auriemma; M Baalouch; S Bachmann; J J Back; A Badalov; C Baesso; V Balagura; W Baldini; R J Barlow; C Barschel; S Barsuk; W Barter; Th Bauer; A Bay; J Beddow; F Bedeschi; I Bediaga; S Belogurov; K Belous; I Belyaev; E Ben-Haim; G Bencivenni; S Benson; J Benton; A Berezhnoy; R Bernet; M-O Bettler; M van Beuzekom; A Bien; S Bifani; T Bird; A Bizzeti; P M Bjørnstad; T Blake; F Blanc; S Blusk; V Bocci; A Bondar; N Bondar; W Bonivento; S Borghi; A Borgia; T J V Bowcock; E Bowen; C Bozzi; T Brambach; J van den Brand; J Bressieux; D Brett; M Britsch; T Britton; N H Brook; H Brown; I Burducea; A Bursche; G Busetto; J Buytaert; S Cadeddu; O Callot; M Calvi; M Calvo Gomez; A Camboni; P Campana; D Campora Perez; A Carbone; G Carboni; R Cardinale; A Cardini; H Carranza-Mejia; L Carson; K Carvalho Akiba; G Casse; L Castillo Garcia; M Cattaneo; Ch Cauet; R Cenci; M Charles; Ph Charpentier; P Chen; N Chiapolini; M Chrzaszcz; K Ciba; X Cid Vidal; G Ciezarek; P E L Clarke; M Clemencic; H V Cliff; J Closier; C Coca; V Coco; J Cogan; E Cogneras; P Collins; A Comerma-Montells; A Contu; A Cook; M Coombes; S Coquereau; G Corti; B Couturier; G A Cowan; E Cowie; D C Craik; S Cunliffe; R Currie; C D'Ambrosio; P David; P N Y David; A Davis; I De Bonis; K De Bruyn; S De Capua; M De Cian; J M De Miranda; L De Paula; W De Silva; P De Simone; D Decamp; M Deckenhoff; L Del Buono; N Déléage; D Derkach; O Deschamps; F Dettori; A Di Canto; H Dijkstra; M Dogaru; S Donleavy; F Dordei; A Dosil Suárez; D Dossett; A Dovbnya; F Dupertuis; P Durante; R Dzhelyadin; A Dziurda; A Dzyuba; S Easo; U Egede; V Egorychev; S Eidelman; D van Eijk; S Eisenhardt; U Eitschberger; R Ekelhof; L Eklund; I El Rifai; Ch Elsasser; A Falabella; C Färber; C Farinelli; S Farry; D Ferguson; V Fernandez Albor; F Ferreira Rodrigues; M Ferro-Luzzi; S Filippov; M Fiore; C Fitzpatrick; M Fontana; F Fontanelli; R Forty; O Francisco; M Frank; C Frei; M Frosini; E Furfaro; A Gallas Torreira; D Galli; M Gandelman; P Gandini; Y Gao; J Garofoli; P Garosi; J Garra Tico; L Garrido; C Gaspar; R Gauld; E Gersabeck; M Gersabeck; T Gershon; Ph Ghez; V Gibson; L Giubega; V V Gligorov; C Göbel; D Golubkov; A Golutvin; A Gomes; P Gorbounov; H Gordon; C Gotti; M Grabalosa Gándara; R Graciani Diaz; L A Granado Cardoso; E Graugés; G Graziani; A Grecu; E Greening; S Gregson; P Griffith; O Grünberg; B Gui; E Gushchin; Yu Guz; T Gys; C Hadjivasiliou; G Haefeli; C Haen; S C Haines; S Hall; B Hamilton; T Hampson; S Hansmann-Menzemer; N Harnew; S T Harnew; J Harrison; T Hartmann; J He; T Head; V Heijne; K Hennessy; P Henrard; J A Hernando Morata; E van Herwijnen; M Hess; A Hicheur; E Hicks; D Hill; M Hoballah; M Holtrop; C Hombach; W Hulsbergen; P Hunt; T Huse; N Hussain; D Hutchcroft; D Hynds; V Iakovenko; M Idzik; P Ilten; R Jacobsson; A Jaeger; E Jans; P Jaton; A Jawahery; F Jing; M John; D Johnson; C R Jones; C Joram; B Jost; M Kaballo; S Kandybei; W Kanso; M Karacson; T M Karbach; I R Kenyon; T Ketel; B Khanji; O Kochebina; I Komarov; R F Koopman; P Koppenburg; M Korolev; A Kozlinskiy; L Kravchuk; K Kreplin; M Kreps; G Krocker; P Krokovny; F Kruse; M Kucharczyk; V Kudryavtsev; K Kurek; T Kvaratskheliya; V N La Thi; D Lacarrere; G Lafferty; A Lai; D Lambert; R W Lambert; E Lanciotti; G Lanfranchi; C Langenbruch; T Latham; C Lazzeroni; R Le Gac; J van Leerdam; J-P Lees; R Lefèvre; A Leflat; J Lefrançois; S Leo; O Leroy; T Lesiak; B Leverington; Y Li; L Li Gioi; M Liles; R Lindner; C Linn; B Liu; G Liu; S Lohn; I Longstaff; J H Lopes; N Lopez-March; H Lu; D Lucchesi; J Luisier; H Luo; F Machefert; I V Machikhiliyan; F Maciuc; O Maev; S Malde; G Manca; G Mancinelli; J Maratas; U Marconi; P Marino; R Märki; J Marks; G Martellotti; A Martens; A Martín Sánchez; M Martinelli; D Martinez Santos; D Martins Tostes; A Martynov; A Massafferri; R Matev; Z Mathe; C Matteuzzi; E Maurice; A Mazurov; J McCarthy; A McNab; R McNulty; B McSkelly; B Meadows; F Meier; M Meissner; M Merk; D A Milanes; M-N Minard; J Molina Rodriguez; S Monteil; D Moran; P Morawski; A Mordà; M J Morello; R Mountain; I Mous; F Muheim; K Müller; R Muresan; B Muryn; B Muster; P Naik; T Nakada; R Nandakumar; I Nasteva; M Needham; S Neubert; N Neufeld; A D Nguyen; T D Nguyen; C Nguyen-Mau; M Nicol; V Niess; R Niet; N Nikitin; T Nikodem; A Nomerotski; A Novoselov; A Oblakowska-Mucha; V Obraztsov; S Oggero; S Ogilvy; O Okhrimenko; R Oldeman; M Orlandea; J M Otalora Goicochea; P Owen; A Oyanguren; B K Pal; A Palano; T Palczewski; M Palutan; J Panman; A Papanestis; M Pappagallo; C Parkes; C J Parkinson; G Passaleva; G D Patel; M Patel; G N Patrick; C Patrignani; C Pavel-Nicorescu; A Pazos Alvarez; A Pellegrino; G Penso; M Pepe Altarelli; S Perazzini; E Perez Trigo; A Pérez-Calero Yzquierdo; P Perret; M Perrin-Terrin; L Pescatore; E Pesen; K Petridis; A Petrolini; A Phan; E Picatoste Olloqui; B Pietrzyk; T Pilař; D Pinci; S Playfer; M Plo Casasus; F Polci; G Polok; A Poluektov; E Polycarpo; A Popov; D Popov; B Popovici; C Potterat; A Powell; J Prisciandaro; A Pritchard; C Prouve; V Pugatch; A Puig Navarro; G Punzi; W Qian; J H Rademacker; B Rakotomiaramanana; M S Rangel; I Raniuk; N Rauschmayr; G Raven; S Redford; S Reichert; M M Reid; A C dos Reis; S Ricciardi; A Richards; K Rinnert; V Rives Molina; D A Roa Romero; P Robbe; D A Roberts; E Rodrigues; P Rodriguez Perez; S Roiser; V Romanovsky; A Romero Vidal; J Rouvinet; T Ruf; F Ruffini; H Ruiz; P Ruiz Valls; G Sabatino; J J Saborido Silva; N Sagidova; P Sail; B Saitta; V Salustino Guimaraes; B Sanmartin Sedes; R Santacesaria; C Santamarina Rios; E Santovetti; M Sapunov; A Sarti; C Satriano; A Satta; M Savrie; D Savrina; M Schiller; H Schindler; M Schlupp; M Schmelling; B Schmidt; O Schneider; A Schopper; M-H Schune; R Schwemmer; B Sciascia; A Sciubba; M Seco; A Semennikov; K Senderowska; I Sepp; N Serra; J Serrano; P Seyfert; M Shapkin; I Shapoval; P Shatalov; Y Shcheglov; T Shears; L Shekhtman; O Shevchenko; V Shevchenko; A Shires; R Silva Coutinho; M Sirendi; N Skidmore; T Skwarnicki; N A Smith; E Smith; J Smith; M Smith; M D Sokoloff; F J P Soler; F Soomro; D Souza; B Souza De Paula; B Spaan; A Sparkes; P Spradlin; F Stagni; S Stahl; O Steinkamp; S Stevenson; S Stoica; S Stone; B Storaci; M Straticiuc; U Straumann; V K Subbiah; L Sun; S Swientek; V Syropoulos; M Szczekowski; P Szczypka; T Szumlak; S T'Jampens; M Teklishyn; E Teodorescu; F Teubert; C Thomas; E Thomas; J van Tilburg; V Tisserand; M Tobin; S Tolk; D Tonelli; S Topp-Joergensen; N Torr; E Tournefier; S Tourneur; M T Tran; M Tresch; A Tsaregorodtsev; P Tsopelas; N Tuning; M Ubeda Garcia; A Ukleja; A Ustyuzhanin; U Uwer; V Vagnoni; G Valenti; A Vallier; M Van Dijk; R Vazquez Gomez; P Vazquez Regueiro; C Vázquez Sierra; S Vecchi; J J Velthuis; M Veltri; G Veneziano; M Vesterinen; B Viaud; D Vieira; X Vilasis-Cardona; A Vollhardt; D Volyanskyy; D Voong; A Vorobyev; V Vorobyev; C Voß; H Voss; R Waldi; C Wallace; R Wallace; S Wandernoth; J Wang; D R Ward; N K Watson; A D Webber; D Websdale; M Whitehead; J Wicht; J Wiechczynski; D Wiedner; L Wiggers; G Wilkinson; M P Williams; M Williams; F F Wilson; J Wimberley; J Wishahi; W Wislicki; M Witek; G Wormser; S A Wotton; S Wright; S Wu; K Wyllie; Y Xie; Z Xing; Z Yang; X Yuan; O Yushchenko; M Zangoli; M Zavertyaev; F Zhang; L Zhang; W C Zhang; Y Zhang; A Zhelezov; A Zhokhov; L Zhong; A Zvyagin
Journal:  Phys Rev Lett       Date:  2013-09-05       Impact factor: 9.161

9.  B(s,d)→ℓ(+)ℓ(-) in the standard model with reduced theoretical uncertainty.

Authors:  Christoph Bobeth; Martin Gorbahn; Thomas Hermann; Mikołaj Misiak; Emmanuel Stamou; Matthias Steinhauser
Journal:  Phys Rev Lett       Date:  2014-03-11       Impact factor: 9.161

10.  Measurement of the semileptonic CP asymmetry in B0-B[over ¯]0 mixing.

Authors:  R Aaij; B Adeva; M Adinolfi; A Affolder; Z Ajaltouni; S Akar; J Albrecht; F Alessio; M Alexander; S Ali; G Alkhazov; P Alvarez Cartelle; A A Alves; S Amato; S Amerio; Y Amhis; L An; L Anderlini; J Anderson; R Andreassen; M Andreotti; J E Andrews; R B Appleby; O Aquines Gutierrez; F Archilli; A Artamonov; M Artuso; E Aslanides; G Auriemma; M Baalouch; S Bachmann; J J Back; A Badalov; C Baesso; W Baldini; R J Barlow; C Barschel; S Barsuk; W Barter; V Batozskaya; V Battista; A Bay; L Beaucourt; J Beddow; F Bedeschi; I Bediaga; S Belogurov; K Belous; I Belyaev; E Ben-Haim; G Bencivenni; S Benson; J Benton; A Berezhnoy; R Bernet; M-O Bettler; M van Beuzekom; A Bien; S Bifani; T Bird; A Bizzeti; P M Bjørnstad; T Blake; F Blanc; J Blouw; S Blusk; V Bocci; A Bondar; N Bondar; W Bonivento; S Borghi; A Borgia; M Borsato; T J V Bowcock; E Bowen; C Bozzi; T Brambach; D Brett; M Britsch; T Britton; J Brodzicka; N H Brook; H Brown; A Bursche; J Buytaert; S Cadeddu; R Calabrese; M Calvi; M Calvo Gomez; P Campana; D Campora Perez; A Carbone; G Carboni; R Cardinale; A Cardini; L Carson; K Carvalho Akiba; G Casse; L Cassina; L Castillo Garcia; M Cattaneo; Ch Cauet; R Cenci; M Charles; Ph Charpentier; M Chefdeville; S Chen; S-F Cheung; N Chiapolini; M Chrzaszcz; X Cid Vidal; G Ciezarek; P E L Clarke; M Clemencic; H V Cliff; J Closier; V Coco; J Cogan; E Cogneras; V Cogoni; L Cojocariu; G Collazuol; P Collins; A Comerma-Montells; A Contu; A Cook; M Coombes; S Coquereau; G Corti; M Corvo; I Counts; B Couturier; G A Cowan; D C Craik; M Cruz Torres; S Cunliffe; R Currie; C D'Ambrosio; J Dalseno; P David; P N Y David; A Davis; K De Bruyn; S De Capua; M De Cian; J M De Miranda; L De Paula; W De Silva; P De Simone; C-T Dean; D Decamp; M Deckenhoff; L Del Buono; N Déléage; D Derkach; O Deschamps; F Dettori; A Di Canto; H Dijkstra; S Donleavy; F Dordei; M Dorigo; A Dosil Suárez; D Dossett; A Dovbnya; K Dreimanis; G Dujany; F Dupertuis; P Durante; R Dzhelyadin; A Dziurda; A Dzyuba; S Easo; U Egede; V Egorychev; S Eidelman; S Eisenhardt; U Eitschberger; R Ekelhof; L Eklund; I El Rifai; Ch Elsasser; S Ely; S Esen; H-M Evans; T Evans; A Falabella; C Färber; C Farinelli; N Farley; S Farry; R F Fay; D Ferguson; V Fernandez Albor; F Ferreira Rodrigues; M Ferro-Luzzi; S Filippov; M Fiore; M Fiorini; M Firlej; C Fitzpatrick; T Fiutowski; P Fol; M Fontana; F Fontanelli; R Forty; O Francisco; M Frank; C Frei; M Frosini; J Fu; E Furfaro; A Gallas Torreira; D Galli; S Gallorini; S Gambetta; M Gandelman; P Gandini; Y Gao; J García Pardiñas; J Garofoli; J Garra Tico; L Garrido; D Gascon; C Gaspar; R Gauld; L Gavardi; A Geraci; E Gersabeck; M Gersabeck; T Gershon; Ph Ghez; A Gianelle; S Gianì; V Gibson; L Giubega; V V Gligorov; C Göbel; D Golubkov; A Golutvin; A Gomes; C Gotti; M Grabalosa Gándara; R Graciani Diaz; L A Granado Cardoso; E Graugés; E Graverini; G Graziani; A Grecu; E Greening; S Gregson; P Griffith; L Grillo; O Grünberg; B Gui; E Gushchin; Yu Guz; T Gys; C Hadjivasiliou; G Haefeli; C Haen; S C Haines; S Hall; B Hamilton; T Hampson; X Han; S Hansmann-Menzemer; N Harnew; S T Harnew; J Harrison; J He; T Head; V Heijne; K Hennessy; P Henrard; L Henry; J A Hernando Morata; E van Herwijnen; M Heß; A Hicheur; D Hill; M Hoballah; C Hombach; W Hulsbergen; P Hunt; N Hussain; D Hutchcroft; D Hynds; M Idzik; P Ilten; R Jacobsson; A Jaeger; J Jalocha; E Jans; P Jaton; A Jawahery; F Jing; M John; D Johnson; C R Jones; C Joram; B Jost; N Jurik; S Kandybei; W Kanso; M Karacson; T M Karbach; S Karodia; M Kelsey; I R Kenyon; T Ketel; B Khanji; C Khurewathanakul; S Klaver; K Klimaszewski; O Kochebina; M Kolpin; I Komarov; R F Koopman; P Koppenburg; M Korolev; A Kozlinskiy; L Kravchuk; K Kreplin; M Kreps; G Krocker; P Krokovny; F Kruse; W Kucewicz; M Kucharczyk; V Kudryavtsev; K Kurek; T Kvaratskheliya; V N La Thi; D Lacarrere; G Lafferty; A Lai; D Lambert; R W Lambert; G Lanfranchi; C Langenbruch; B Langhans; T Latham; C Lazzeroni; R Le Gac; J van Leerdam; J-P Lees; R Lefèvre; A Leflat; J Lefrançois; S Leo; O Leroy; T Lesiak; B Leverington; Y Li; T Likhomanenko; M Liles; R Lindner; C Linn; F Lionetto; B Liu; S Lohn; I Longstaff; J H Lopes; N Lopez-March; P Lowdon; D Lucchesi; H Luo; A Lupato; E Luppi; O Lupton; F Machefert; I V Machikhiliyan; F Maciuc; O Maev; S Malde; A Malinin; G Manca; G Mancinelli; A Mapelli; J Maratas; J F Marchand; U Marconi; C Marin Benito; P Marino; R Märki; J Marks; G Martellotti; A Martín Sánchez; M Martinelli; D Martinez Santos; F Martinez Vidal; D Martins Tostes; A Massafferri; R Matev; Z Mathe; C Matteuzzi; B Maurin; A Mazurov; M McCann; J McCarthy; A McNab; R McNulty; B McSkelly; B Meadows; F Meier; M Meissner; M Merk; D A Milanes; M-N Minard; N Moggi; J Molina Rodriguez; S Monteil; M Morandin; P Morawski; A Mordà; M J Morello; J Moron; A-B Morris; R Mountain; F Muheim; K Müller; M Mussini; B Muster; P Naik; T Nakada; R Nandakumar; I Nasteva; M Needham; N Neri; S Neubert; N Neufeld; M Neuner; A D Nguyen; T D Nguyen; C Nguyen-Mau; M Nicol; V Niess; R Niet; N Nikitin; T Nikodem; A Novoselov; D P O'Hanlon; A Oblakowska-Mucha; V Obraztsov; S Oggero; S Ogilvy; O Okhrimenko; R Oldeman; C J G Onderwater; M Orlandea; J M Otalora Goicochea; A Otto; P Owen; A Oyanguren; B K Pal; A Palano; F Palombo; M Palutan; J Panman; A Papanestis; M Pappagallo; L L Pappalardo; C Parkes; C J Parkinson; G Passaleva; G D Patel; M Patel; C Patrignani; A Pearce; A Pellegrino; M Pepe Altarelli; S Perazzini; P Perret; M Perrin-Terrin; L Pescatore; E Pesen; K Petridis; A Petrolini; E Picatoste Olloqui; B Pietrzyk; T Pilař; D Pinci; A Pistone; S Playfer; M Plo Casasus; F Polci; A Poluektov; E Polycarpo; A Popov; D Popov; B Popovici; C Potterat; E Price; J D Price; J Prisciandaro; A Pritchard; C Prouve; V Pugatch; A Puig Navarro; G Punzi; W Qian; B Rachwal; J H Rademacker; B Rakotomiaramanana; M Rama; M S Rangel; I Raniuk; N Rauschmayr; G Raven; F Redi; S Reichert; M M Reid; A C dos Reis; S Ricciardi; S Richards; M Rihl; K Rinnert; V Rives Molina; P Robbe; A B Rodrigues; E Rodrigues; P Rodriguez Perez; S Roiser; V Romanovsky; A Romero Vidal; M Rotondo; J Rouvinet; T Ruf; H Ruiz; P Ruiz Valls; J J Saborido Silva; N Sagidova; P Sail; B Saitta; V Salustino Guimaraes; C Sanchez Mayordomo; B Sanmartin Sedes; R Santacesaria; C Santamarina Rios; E Santovetti; A Sarti; C Satriano; A Satta; D M Saunders; D Savrina; M Schiller; H Schindler; M Schlupp; M Schmelling; B Schmidt; O Schneider; A Schopper; M Schubiger; M-H Schune; R Schwemmer; B Sciascia; A Sciubba; A Semennikov; I Sepp; N Serra; J Serrano; L Sestini; P Seyfert; M Shapkin; I Shapoval; Y Shcheglov; T Shears; L Shekhtman; V Shevchenko; A Shires; R Silva Coutinho; G Simi; M Sirendi; N Skidmore; I Skillicorn; T Skwarnicki; N A Smith; E Smith; E Smith; J Smith; M Smith; H Snoek; M D Sokoloff; F J P Soler; F Soomro; D Souza; B Souza De Paula; B Spaan; P Spradlin; S Sridharan; F Stagni; M Stahl; S Stahl; O Steinkamp; O Stenyakin; S Stevenson; S Stoica; S Stone; B Storaci; S Stracka; M Straticiuc; U Straumann; R Stroili; V K Subbiah; L Sun; W Sutcliffe; K Swientek; S Swientek; V Syropoulos; M Szczekowski; P Szczypka; T Szumlak; S T'Jampens; M Teklishyn; G Tellarini; F Teubert; C Thomas; E Thomas; J van Tilburg; V Tisserand; M Tobin; J Todd; S Tolk; L Tomassetti; D Tonelli; S Topp-Joergensen; N Torr; E Tournefier; S Tourneur; M T Tran; M Tresch; A Trisovic; A Tsaregorodtsev; P Tsopelas; N Tuning; M Ubeda Garcia; A Ukleja; A Ustyuzhanin; U Uwer; C Vacca; V Vagnoni; G Valenti; A Vallier; R Vazquez Gomez; P Vazquez Regueiro; C Vázquez Sierra; S Vecchi; J J Velthuis; M Veltri; G Veneziano; M Vesterinen; B Viaud; D Vieira; M Vieites Diaz; X Vilasis-Cardona; A Vollhardt; D Volyanskyy; D Voong; A Vorobyev; V Vorobyev; C Voß; J A de Vries; R Waldi; C Wallace; R Wallace; J Walsh; S Wandernoth; J Wang; D R Ward; N K Watson; D Websdale; M Whitehead; J Wicht; D Wiedner; G Wilkinson; M Wilkinson; M P Williams; M Williams; H W Wilschut; F F Wilson; J Wimberley; J Wishahi; W Wislicki; M Witek; G Wormser; S A Wotton; S Wright; K Wyllie; Y Xie; Z Xing; Z Xu; Z Yang; X Yuan; O Yushchenko; M Zangoli; M Zavertyaev; L Zhang; W C Zhang; Y Zhang; A Zhelezov; A Zhokhov; L Zhong
Journal:  Phys Rev Lett       Date:  2015-01-28       Impact factor: 9.161
  10 in total

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