Observation of B→D(*) π

We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯â†’D^(*)π^(+)π^(-)ℓ^(-)ν¯, where D^(*) represents a D or D^(*) meson and ℓ^(-) is an electron or a muon. These measurements are based on 471×10^(6) BB ¯ pairs recorded with the BABAR detector at the SLAC asymmetric B factory PEP-II. We determine the branching fraction ratios R_{π^{+}π^{-}}^{(*)}=B(B[over ¯]→D^{(*)}π^{+}π^{-}ℓ^{-}ν[over ¯])/B(B[over ¯]→D^{(*)}ℓ^{-}ν[over ¯]) using events in which the second B meson is fully reconstructed. We find R_{π^{+}π^{-}}=0.067±0.010±0.008 and R_{π^{+}π^{-}}^{*}=0.019±0.005±0.004, where the first uncertainty is statistical and the second is systematic. Based on these results and assuming isospin invariance, we estimate that B[over ¯]→D^{(*)}ππℓ^{-}ν[over ¯] decays, where π denotes either a π^{±} and π^{0} meson, account for up to half the difference between the measured inclusive semileptonic branching fraction to charm hadrons and the corresponding sum of previously measured exclusive branching fractions.

Search for Long-Lived Particles in e+ e- Collisions.

We present a search for a neutral, long-lived particle L that is produced in e+ e- collisions and decays at a significant distance from the e+ e- interaction point into various flavor combinations of two oppositely charged tracks. The analysis uses an e+ e- data sample with a luminosity of 489.1 fb(-1) collected by the BABAR detector at the ϒ(4S), ϒ(3S), and ϒ(2S) resonances and just below the ϒ(4S). Fitting the two-track mass distribution in search of a signal peak, we do not observe a significant signal, and set 90% confidence level upper limits on the product of the L production cross section, branching fraction, and reconstruction efficiency for six possible two-body L decay modes as a function of the L mass. The efficiency is given for each final state as a function of the mass, lifetime, and transverse momentum of the candidate, allowing application of the upper limits to any production model. In addition, upper limits are provided on the branching fraction B(B→XsL), where Xs is a strange hadronic system.

Study of CP asymmetry in B

We present a measurement of the asymmetry A_{CP} between same-sign inclusive dilepton samples ℓ^{+}ℓ^{+} and ℓ^{-}ℓ^{-} (ℓ=e, µ) from semileptonic B decays in ϒ(4S)→BB[over ¯] events, using the complete data set recorded by the BABAR experiment near the ϒ(4S) resonance, corresponding to 471×10^{6} BB[over ¯] pairs. The asymmetry A_{CP} allows comparison between the mixing probabilities P(B[over ¯]^{0}→B^{0}) and P(B^{0}→B[over ¯]^{0}), and therefore probes CP and T violation. The result, A_{CP}=[-3.9±3.5(stat)±1.9(syst)]×10^{-3}, is consistent with the standard model expectation.

Search for a dark photon in e(+)e(-) collisions at BABAR.

Dark sectors charged under a new Abelian interaction have recently received much attention in the context of dark matter models. These models introduce a light new mediator, the so-called dark photon (A^{'}), connecting the dark sector to the standard model. We present a search for a dark photon in the reaction e^{+}e^{-}→γA^{'}, A^{'}→e^{+}e^{-}, µ^{+}µ^{-} using 514 fb^{-1} of data collected with the BABAR detector. We observe no statistically significant deviations from the standard model predictions, and we set 90% confidence level upper limits on the mixing strength between the photon and dark photon at the level of 10^{-4}-10^{-3} for dark photon masses in the range 0.02-10.2 GeV. We further constrain the range of the parameter space favored by interpretations of the discrepancy between the calculated and measured anomalous magnetic moment of the muon.

Measurement of the D*(2010)+ meson width and the D*(2010)+ - D0 mass difference.

We measure the mass difference Δm0 between the D*(2010)+ and the D0 and the natural linewidth Γ of the transition D*(2010)+ → D0π+. The data were recorded with the BABAR detector at center-of-mass energies at and near the Υ(4S) resonance, and correspond to an integrated luminosity of approximately 477 fb(-1). The D0 is reconstructed in the decay modes D0 → K- π+ and D0 → K- π+ π- π+. For the decay mode D0 → K- π+ we obtain Γ = (83.4±1.7±1.5) keV and Δm0 = (145425.6±0.6±1.7) keV, [corrected] where the quoted errors are statistical and systematic, respectively. For the D0 → K- π+ π- π+ mode we obtain Γ = (83.2±1.5±2.6) keV and Δm0 = (145426.6±0.5±1.9) keV. [corrected] The combined measurements yield Γ = (83.3±1.2±1.4) keV and Δm0 = (145425.9±0.4±1.7) keV; the width is a factor of approximately 12 times more precise than the previous value, while the mass difference is a factor of approximately 6 times more precise.

Search for CP violation in B0-B0 mixing using partial reconstruction of B0→D*- Xℓ+ νℓ and a kaon tag.

We present results of a search for CP violation in B0- B0 mixing with the BABAR detector. We select a sample of B0→D*- Xℓ+ ν decays with a partial reconstruction method and use kaon tagging to assess the flavor of the other B meson in the event. We determine the CP violating asymmetry ACP≡[N(B0B0)-N(B0B0)]/[N(B0B0)+N(B0B0)]=(0.06±0.17(-0.32)(+0.38))%, corresponding to ΔCP=1-|q/p|=(0.29±0.84(-1.61)(+1.88))×10(-3).

Precision measurement of the B → Xs γ photon energy spectrum, branching fraction, and direct CP asymmetry A(CP)((B → X(s+d)γ).

The photon spectrum in the inclusive electromagnetic radiative decays of the B meson, B → X(s)γ plus B → X(d)γ, is studied using a data sample of (382.8 ± 4.2) × 10(6)Υ(4S) → BB decays collected by the BABAR experiment at SLAC. The spectrum is used to extract the branching fraction B(B → X(s)γ) = (3.21 ± 0.33) × 10(-4) for E(γ) >1.8 GeV and the direct CP asymmetry A(CP) (B → X(s+d)γ) = 0.057 ± 0.063. The effects of detector resolution and Doppler smearing are unfolded to measure the photon energy spectrum in the B meson rest frame.

Observation of time-reversal violation in the B0 meson system.

Although CP violation in the B meson system has been well established by the B factories, there has been no direct observation of time-reversal violation. The decays of entangled neutral B mesons into definite flavor states (B(0) or B(0)), and J/ψK(L)(0) or ccK(S)(0) final states (referred to as B(+) or B(-)), allow comparisons between the probabilities of four pairs of T-conjugated transitions, for example, B(0) → B(-) and B(-) → B(0), as a function of the time difference between the two B decays. Using 468 × 10(6) BB pairs produced in Υ(4S) decays collected by the BABAR detector at SLAC, we measure T-violating parameters in the time evolution of neutral B mesons, yielding ΔS(T)(+) = -1.37 ± 0.14(stat) ± 0.06(syst) and ΔS(T)(-) = 1.17 ± 0.18(stat) ± 0.11(syst). These nonzero results represent the first direct observation of T violation through the exchange of initial and final states in transitions that can only be connected by a T-symmetry transformation.

Evidence for an excess of B→D*τ(-)ν(τ) decays.

Based on the full BABAR data sample, we report improved measurements of the ratios R(D(*))=B(B[over ¯]→D(*)τ(-)ν[over ¯](τ))/B(B[over ¯]→D(*)ℓ(ℓ)(-)ν[over ¯](ℓ)), where ℓ is either e or µ. These ratios are sensitive to new physics contributions in the form of a charged Higgs boson. We measure R(D)=0.440±0.058±0.042 and R(D(*))=0.332±0.024±0.018, which exceed the standard model expectations by 2.0σ and 2.7σ, respectively. Taken together, our results disagree with these expectations at the 3.4σ level. This excess cannot be explained by a charged Higgs boson in the type II two-Higgs-doublet model.

Search for low-mass dark-sector Higgs bosons.

Recent astrophysical and terrestrial experiments have motivated the proposal of a dark sector with GeV-scale gauge boson force carriers and new Higgs bosons. We present a search for a dark Higgs boson using 516 fb(-1) of data collected with the BABAR detector. We do not observe a significant signal and we set 90% confidence level upper limits on the product of the standard model-dark-sector mixing angle and the dark-sector coupling constant.

Search for hadronic decays of a light Higgs boson in the radiative decay Υ→γA0.

We search for hadronic decays of a light Higgs boson (A(0)) produced in radiative decays of an Υ(2S) or Υ(3S) meson, Υ→γA(0). The data have been recorded by the BABAR experiment at the Υ(3S) and Υ(2S) center-of-mass energies and include (121.3±1.2)×10(6) Υ(3S) and (98.3±0.9)×10(6) Υ(2S) mesons. No significant signal is observed. We set 90% confidence level upper limits on the product branching fractions B(Υ(nS)→γA(0))B(A(0)→hadrons) (n=2 or 3) that range from 1×10(-6) for an A(0) mass of 0.3 GeV/c(2) to 8×10(-5) at 7 GeV/c(2).

Diagnosis of Os odontoideum using kinematic magnetic resonance imaging. A case report.

STUDY DESIGN: A case of os odontoideum diagnosed using kinematic magnetic resonance imaging is presented. OBJECTIVES: To evaluate the kinematic magnetic resonance imaging findings of os odontoideum and the possible use these findings might have to guide treatment. BACKGROUND: Kinematic magnetic resonance imaging is a new imaging modality that is able to produce realtime images of a structure through a range of motion. This makes it well suited for investigating dynamic processes such as cervical instability. METHODS: A single subject with known os odontoideum was examined using a Sigma SPR Kinematic Magnetic Resonance Imager (General Electric, Florence, SC). RESULTS: Kinematic magnetic resonance imaging demonstrated cervical spinal cord impingement and cervical instability throughout flexion and extension, but not during lateral bending or rotation. CONCLUSIONS: Kinematic magnetic resonance imaging can evaluate the cervical spine in an axially loaded position throughout its range of motion. This modality may be a useful method for diagnosing and classifying abnormalities of the spine.

Retroperitoneal pseudomeningocele complicated by meningitis following a lumbar burst fracture. A case report.

STUDY DESIGN: This case report demonstrates an unusual complication after anterior decompression and fusion of a lumbar burst fracture. OBJECTIVES: The treatment of this patient involved placement of a computed tomography-guided percutaneous drain and intravenous antibiotics to treat an infected retroperitoneal pseudomeningocele. SUMMARY OF BACKGROUND DATA: A case of an anterior retroperitoneal pseudomeningocele complicated by meningitis is presented. This pseudomeningocele occurred in a patient after an L3 burst fracture associated with a dural laceration. METHODS: The patient was admitted to the authors' trauma unit after a motor vehicle accident with an acute L3 fracture associated with incomplete paraplegia. He underwent an urgent anterior corpectomy, strut grafting, and instrumentation. At surgery, he was noted to have a large anterior dural laceration. After surgery, a large retroperitoneal pseudomeningocele developed that became infected with Staphylococcus epidermidis. RESULTS: After placement of a computed tomography-guided percutaneous drain and intravenous antibiotics, the pseudomeningocele resolved. His anterior fusion healed uneventfully and his neurologic deficit improved dramatically. CONCLUSIONS: A case of an anterior retroperitoneal pseudomeningocele complicated by meningitis is presented. This pseudomeningocele occurred in a patient after an L3 burst fracture associated with a dural laceration. The patient was treated successfully with computed tomography-guided percutaneous drain placement and intravenous antibiotics. He made an excellent functional recovery after a severe neurologic injury.

Biomechanical evaluation of cervical spine stabilization methods using a porcine model.

STUDY DESIGN: The biomechanical stability of three different methods of cervical spine stabilization was evaluated in a porcine model. Specimens were tested in flexion, extension, and axial rotation. OBJECTIVES: Our goal was to determine if posterior lateral mass plating after anterior reconstruction provided more stability compared with unicortical or bicortical anterior plate fixation after a simulated corpectomy. SUMMARY OF BACKGROUND DATA: Previous implant biomechanical evaluations use ligamentous and intervertebral disc disruption models under constrained and nonrepetitive loading. This study examines implant performance using a corpectomy model loaded for multiple cycles, allowing for unconstrained motion. METHODS: Twenty-one porcine cervical spines were destabilized with a one-level cervical corpectomy and reconstructed with an anterior methacrylate graft. Each construct was stabilized with either an AO Morscher plate system with unicortical, self-locking screws; a Caspar plate with biocortical screws; or two posterior lateral mass plates. Testing with cyclic loads was performed on an MTS machine in flexion, extension, and axial rotation. RESULTS: There was no statistical difference between the two anterior forms of fixation in flexion, extension, or axial rotation. Posterior lateral mass plating was significantly more stable than either anterior construct. Screw loosening was seen more frequently with bicortical Caspar plating. CONCLUSIONS: After a single-level cervical corpectomy and idealized grafting, all three surgical constructs provided stability equal to or greater than the intact condition in flexion, extension, and axial rotation. In unstable cervical spine injury patterns involving anterior disruption, this study supports the use of anterior grafting combined with posterior lateral mass plating to achieve maximum stability.

The role of arthroscopy in the management of synovial chondromatosis of the shoulder. A case report.

A case of synovial chondromatosis of the shoulder is reported in a 28-year-old man with long-standing shoulder pain after a remote episode of trauma. Although plain roentgenograms were normal, arthrograms revealed the characteristic findings of synovial chondromatosis. Treatment consisted of arthroscopic removal of multiple cartilaginous loose bodies and partial synovectomy. Synovial chondromatosis of the shoulder treated with arthroscopic debridement and synovectomy rather than traditional open arthrotomy seems not to have been reported previously.

The plantar ecchymosis sign in fractures of the calcaneus.

The appearance of a central plantar ecchymosis is not an uncommon occurrence 24-48 hours after a compression fracture of the calcaneus. In order to understand the development of this characteristic ecchymosis, the authors studied the anatomy of the fascial compartments in five adult cadaveric feet. The anatomic basis for the plantar ecchymosis sign is demonstrated through dissection of the three osteofascial compartments within the sole of the foot. Dye injected into the central compartment overlying the calcaneal tuberosity reproduces the observed clinical sign. The specificity of this sign for compression fractures of the calcaneus makes it a useful clinical observation in cases where the diagnosis of fracture is uncertain.