Thursday, December 13, 2012

LHC data publications of the last 12 months

Just keeping tally of archived research material at Cern.

ALICE

  • Pseudorapidity density of charged particles p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, http://arxiv.org/abs/1210.3615, Phys. Rev. Lett..
  • Transverse Momentum Distribution and Nuclear Modification Factor of Charged Particles in p-Pb Collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, http://arxiv.org/abs/1210.4520, Phys. Rev. Lett..
  • Coherent J/$\Psi$ photoproduction in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{NN}}$ =2.76 TeV, http://arxiv.org/abs/1209.3715, Phys. Lett. B.
  • Measurement of inelastic, single- and double-diffraction cross sections in proton-proton collisions at the LHC with ALICE, http://arxiv.org/abs/1208.4968, Eur. Phys. J. C.
  • Measurement of electrons from beauty hadron decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.1902.
  • Centrality Dependence of Charged Particle Production at Large Transverse Momentum in Pb--Pb Collisions at $\sqrt{s_{\rm{NN}}} = 2.76$ TeV, http://arxiv.org/abs/1208.2711, Phys. Lett. B.
  • Pion, Kaon, and Proton Production in Central Pb--Pb Collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1208.1974, Phys. Rev. Lett..
  • D$_s^+$ meson production at central rapidity in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.1948.
  • Production of $K*(892)^0$ and $\phi$(1020) in pp collisions at $\sqrt{s}$ =7 TeV, http://arxiv.org/abs/1208.5717, Eur. Phys. J. C, 72: 2183, 2012.
  • Net-Charge Fluctuations in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV, http://arxiv.org/abs/1207.6068.
  • Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}$= 2.76 TeV, http://arxiv.org/abs/1207.0900.
  • K$^{0}_{s}$-K$^{0}_{s}$ correlations in pp collisions at $\sqrt{s}$=7 TeV from the LHC ALICE experiment, http://arxiv.org/abs/1206.2056.
  • Production of muons from heavy flavour decays at forward rapidity in pp and Pb-Pb collisions at $\sqrt {s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.6443, Phys. Rev. Lett..
  • Anisotropic flow of charged hadrons, pions and (anti-)protons measured at high transverse momentum in Pb-Pb collisions at $\sqrt{s_{NN}}$=2.76 TeV, http://arxiv.org/abs/1205.5761.
  • Transverse sphericity of primary charged particles in minimum bias proton-proton collisions at $\sqrt{s}$=0.9, 2.76 and 7 TeV, http://arxiv.org/abs/1205.3963.
  • Measurement of charm production at central rapidity in proton-proton collisions at $\sqrt{s}$ = 2.76 TeV, http://arxiv.org/abs/1205.4007, J. High Energy Phys., 07: 191, 2012.
  • Measurement of prompt and non-prompt J/$\psi$ production cross sections at mid-rapidity in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5880.
  • Measurement of electrons from semileptonic heavy-flavour hadron decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5423.
  • Multi-strange baryon production in pp collisions at $\sqrt{s}$ = 7 TeV with ALICE, http://arxiv.org/abs/1204.0282, Phys. Lett. B, 712: 309-318, 2012.
  • Suppression of high transverse momentum D mesons in central Pb--Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV, http://arxiv.org/abs/1203.2160.
  • Measurement of the Cross Section for Electromagnetic Dissociation with Neutron Emission in Pb-Pb Collisions at √sNN = 2.76 TeV, http://arxiv.org/abs/1203.2436.
  • Inclusive J/$\psi$ production in pp collisions at $\sqrt{s}$ = 2.76 TeV, http://arxiv.org/abs/1203.3641, Phys. Lett. B, 718: 295-306, 2012.
  • J/$\psi$ Production as a Function of Charged Particle Multiplicity in pp Collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.2816, Phys. Lett. B.
  • Heavy flavour decay muon production at forward rapidity in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1201.3791, Phys. Lett. B, 708: 265-275, 2012.
  • J/$\psi$ production at low transverse momentum in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1202.1383, Phys. Rev. Lett..
  • Measurement of Event Background Fluctuations for Charged Particle Jet Reconstruction in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.2423, J. High Energy Phys., 03: 053, 2012.
  • Neutral pion and $\eta$ meson production in proton-proton collisions at $\sqrt{s}$=0.9 TeV and $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1205.5724.

ATLAS

  • Search for a heavy narrow resonance decaying to $e\mu, e\tau$, or $\mu\tau$ with the ATLAS detector in $\sqrt{s}$ = 7 TeV pp collisions at the LHC, http://arxiv.org/abs/1212.1272, Phys. Lett. B.
  • Measurement of Upsilon production in 7 TeV pp collisions at ATLAS, http://arxiv.org/abs/1211.7255, Phys. Rev. D.
  • Measurement of the $t\bar{t}$ production cross section in the tau+jets channel using the ATLAS detector, http://arxiv.org/abs/1211.7205, Eur. Phys. J. C.
  • Search for new phenomena in events with three charged leptons at a center-of-mass energy of 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.6312, Phys. Rev. D.
  • Measurement of ZZ production in pp collisions at $\sqrt{s}$=7 TeV and limits on anomalous ZZZ and ZZ$\gamma$ couplings with the ATLAS detector, http://arxiv.org/abs/1211.6096, J. High Energy Phys..
  • Search for resonances decaying into top-quark pairs using fully hadronic decays in pp collisions with ATLAS at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.2202, J. High Energy Phys..
  • Measurement of isolated-photon pair production in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.1913, J. High Energy Phys..
  • Searches for heavy long-lived sleptons and R-Hadrons with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.1597, Phys. Lett. B.
  • Search for contact interactions and large extra dimensions in dilepton events from pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.1150, Phys. Rev. D.
  • Search for supersymmetry in events with photons, bottom quarks, and missing transverse momentum in proton-proton collisions at a centre-of-mass energy of 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.1167, Phys. Lett. B.
  • Search for Extra Dimensions in diphoton events using proton-proton collisions recorded at $\sqrt{s}$ = 7 TeV with the ATLAS detector at the LHC, http://arxiv.org/abs/1210.8389, Phys. Lett. B.
  • Search for long-lived, heavy particles in final states with a muon and multi-track displaced vertex in proton-proton collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.7451, Phys. Lett. B.
  • A search for high-mass resonances decaying to tau+tau- in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.6604, Phys. Lett. B.
  • Measurement of Z boson Production in Pb+Pb Collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS Detector, http://arxiv.org/abs/1210.6486, Phys. Rev. Lett..
  • Jet energy resolution in proton-proton collisions at $\sqrt{s}$ = 7 TeV recorded in 2010 with the ATLAS detector, http://arxiv.org/abs/1210.6210, Eur. Phys. J. C.
  • Measurement of angular correlations in Drell-Yan lepton pairs to probe $Z/\gamma*$ boson transverse momentum at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.6899, Phys. Lett., B.
  • Search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.6956, J. High Energy Phys..
  • Search for pair production of heavy top-like quarks decaying to a high-$p_T$ W boson and a b quark in the lepton plus jets final state at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.5468, Phys. Lett. B.
  • Search for doubly-charged Higgs bosons in like-sign dilepton final states at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.5070, Eur. Phys. J. C.
  • Search for pair-produced massive coloured scalars in four-jet final states with the ATLAS detector in proton-proton collisions at sqrt(s) = 7 TeV, http://arxiv.org/abs/1210.4826, Eur. Phys. J. C.
  • Search for pair production of massive particles decaying into three quarks with the ATLAS detector in $\sqrt{s}$ = 7 TeV pp collisions at the LHC, http://arxiv.org/abs/1210.4813, J. High Energy Phys..
  • Search for anomalous production of prompt like-sign lepton pairs at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.4538, J. High Energy Phys..
  • Search for dark matter candidates and large extra dimensions in events with a jet and missing transverse momentum with the ATLAS detector, http://arxiv.org/abs/1210.4491, J. High Energy Phys..
  • Search for R-parity-violating supersymmetry in events with four or more leptons in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1210.4457, J. High Energy Phys..
  • Measurement of $W^+W^-$ production in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector and limits on anomalous WWZ and WW$_{\gamma}$ couplings, http://arxiv.org/abs/1210.2979, Phys. Rev. D.
  • Search for direct chargino production in anomaly-mediated supersymmetry breaking models based on a disappearing-track signature in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.2852, J. High Energy Phys..
  • ATLAS search for new phenomena in dijet mass and angular distributions using pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1210.1718, J. High Energy Phys..
  • Search for Supersymmetry in Events with Large Missing Transverse Momentum, Jets, and at Least One Tau Lepton in 7 TeV Proton-Proton Collision Data with the ATLAS Detector, http://arxiv.org/abs/1210.1314, Eur. Phys. J. C, 72: 2215, 2012.
  • Search for resonant top quark plus jet production in $t\bar{t}$+jets events with the ATLAS detector in pp collisions at $\sqrt{s}$=7  TeV, http://arxiv.org/abs/1209.6593, Phys. Rev. D, 86: 091103(R), 2012.
  • Search for dark matter candidates and large extra dimensions in events with a photon and missing transverse momentum in pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1209.4625, Phys. Rev. Lett..
  • ATLAS search for a heavy gauge boson decaying to a charged lepton and a neutrino in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.4446, Eur. Phys. J. C.
  • Search for a heavy top-quark partner in final states with two leptons with the ATLAS detector at the LHC, http://arxiv.org/abs/1209.4186, J. High Energy Phys., 11: 094, 2012.
  • Search for high-mass resonances decaying to dilepton final states in pp collisions at a center-of-mass energy of 7 TeV with the ATLAS detector, http://arxiv.org/abs/1209.2535, J. High Energy Phys..
  • Search for light top squark pair production in final states with leptons and b-jets with the ATLAS detector in $\sqrt{s}$ = 7 TeV proton-proton collisions, http://arxiv.org/abs/1209.2102, Phys. Lett. B.
  • Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector, http://arxiv.org/abs/1209.0753, Phys. Lett. B, 718: 411-430, 2012.
  • Measurements of the pseudorapidity dependence of the total transverse energy in proton-proton collisions at $\sqrt{s}$ = 7 TeV with ATLAS, http://arxiv.org/abs/1208.6256, J. High Energy Phys..
  • Measurement of the flavour composition of dijet events in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.0441, Eur. Phys. J. C.
  • Further search for supersymmetry at $\sqrt{s}$ = 7 TeV in final states with jets, missing transverse momentum and isolated leptons with the ATLAS detector, http://arxiv.org/abs/1208.4688, Phys. Rev. D, 86: 092002, 2012.
  • Search for light scalar top-quark pair production in final states with two leptons with the ATLAS detector in $\sqrt{s}$ = 7 TeV proton-proton collisions, http://arxiv.org/abs/1208.4305, Eur. Phys. J. C, 72: 2237, 2012.
  • Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1208.3144, Phys. Lett. B.
  • Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.2884, Phys. Lett. B.
  • Search for new phenomena in the $WW \to l\nu l' \nu'$ final state in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.2880, Phys. Lett. B.
  • Search for direct top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}$ = 7 TeV pp collisions using 4.7 fb$^{-1}$ of ATLAS data, http://arxiv.org/abs/1208.2590, Phys. Rev. Lett., 109: 211803, 2012.
  • Search for displaced muonic lepton jets from light Higgs boson decay in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.0435, Phys. Lett. B.
  • Measurement of the jet radius and transverse momentum dependence of inclusive jet suppression in lead-lead collisions at $\sqrt{s_{NN}}$ = 2.76 TeV with the ATLAS detector, http://arxiv.org/abs/1208.1967, Phys. Lett. B.
  • Search for a supersymmetric partner to the top quark in final states with jets and missing transverse momentum at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.1447, Phys. Rev. Lett., 109: 211802, 2012.
  • Measurement of W$^{\pm}$Z production in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.1390, Eur. Phys. J. C, 72: 2173, 2012.
  • Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV proton-proton collision data, http://arxiv.org/abs/1208.0949, Phys. Rev. D.
  • Time-dependent angular analysis of the decay $B_s^0 \to J/\psi \phi$ and extraction of $\Delta \Gamma_s$ and the CP-violating weak phase $\phi_s$ by ATLAS, http://arxiv.org/abs/1208.0572, J. High Energy Phys..
  • Underlying event characteristics and their dependence on jet size of charged-particle jet events in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.0563, Phys. Rev. D, 86: 072004, 2012.
  • Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, http://arxiv.org/abs/1207.7214, Phys. Lett. B, 716: 1-29, 2012.
  • Measurement of charged-particle event shape variables in $\sqrt{s}$ = 7 TeV proton-proton interactions with the ATLAS detector, http://arxiv.org/abs/1207.6915, Phys. Rev. D.
  • Search for magnetic monopoles in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1207.6411, Phys. Rev. Lett..
  • Measurements of top quark pair relative differential cross-sections with ATLAS in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.5644, Eur. Phys. J. C.
  • Search for top and bottom squarks from gluino pair production in final states with missing transverse energy and at least three b-jets with the ATLAS detector, http://arxiv.org/abs/1207.4686, Eur. Phys. J. C, 72: 2174, 2012.
  • A search for $t\bar{t}$ resonances in lepton+jets events with highly boosted top quarks collected in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1207.2409, J. High Energy Phys., 09: 041, 2012.
  • Measurement of the $\Lambda_b^0$ lifetime and mass in the ATLAS experiment, http://arxiv.org/abs/1207.2284, Phys. Rev. D.
  • Combined search for the Standard Model Higgs boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1207.0319, Phys. Rev. D, 86: 032003, 2012.
  • Search for the Standard Model Higgs boson produced in association with a vector boson and decaying to a b-quark pair with the ATLAS detector, http://arxiv.org/abs/1207.0210, Phys. Lett. B, 718: 369-390, 2012.
  • Search for the Standard Model Higgs boson in the $H \to \tau^+ \tau^-$ decay mode in $\sqrt{s}$ = 7 TeV pp collisions with ATLAS, http://arxiv.org/abs/1206.5971, J. High Energy Phys., 09: 070, 2012.
  • Search for the Higgs boson in the $H \to WW \to l\nu jj$ decay channel at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1206.6074, Phys. Lett. B, 718: 391-410, 2012.
  • ATLAS measurements of the properties of jets for boosted particle searches, http://arxiv.org/abs/1206.5369, Phys. Rev. D, 86: 072006, 2012.
  • Measurement of the b-hadron production cross section using decays to $D^{*+}\mu^- X$ final states in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1206.3122, Nucl. Phys. B, 864: 341-381, 2012.
  • Search for a Standard Model Higgs boson in the mass range 200-600 GeV in the $H \to ZZ \to l^+l^-q\bar{q}$ decay channel with the ATLAS detector, http://arxiv.org/abs/1206.2443, Phys. Lett. B, 717: 70–88, 2012.
  • Measurement of event shapes at large momentum transfer with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.2135, Eur. Phys. J. C, 72: 2211, 2012.
  • Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV proton-proton collisions, http://arxiv.org/abs/1206.1760, J. High Energy Phys., 07: 167, 2012.
  • Search for the Standard Model Higgs boson in the $H \to WW^{(*)} \to l\nu l\nu$ decay mode with 4.7 fb$^{-1}$ of ATLAS data at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.0756, Phys. Lett. B, 716: 62-81, 2012.
  • A search for flavour changing neutral currents in top-quark decays in pp collision data collected with the ATLAS detector at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.0257, J. High Energy Phys., 09: 139, 2012.
  • Search for a Standard Model Higgs boson in the $H \to ZZ \to l^+l^-\nu\bar{\nu}$ decay channel using 4.7 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV data with the ATLAS detector, http://arxiv.org/abs/1205.6744, Phys. Lett. B, 717: 29-48, 2012.
  • Evidence for the associated production of a W boson and a top quark in ATLAS at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5764, Phys. Lett. B, 716: 142-159, 2012.
  • A search for $t\bar{t}$ resonances with the ATLAS detector in 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt(s)$ = 7 TeV, http://arxiv.org/abs/1205.5371, Eur. Phys. J. C, 72: 2083, 2012.
  • Search for tb resonances in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1205.1016, Phys. Rev. Lett., 109: 081801, 2012.
  • Measurement of the t-channel single top-quark production cross section in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1205.3130, Phys. Lett. B, 717: 330-350, 2012.
  • Measurement of $W\gamma$ and $Z\gamma$ production cross sections in pp collisions at $\sqrt{s}$ = 7 TeV and limits on anomalous triple gauge couplings with the ATLAS detector, http://arxiv.org/abs/1205.2531, Phys. Lett. B, 717: 49-69, 2012.
  • Measurement of the W boson polarization in top quark decays with the ATLAS detector, http://arxiv.org/abs/1205.2484, J. High Energy Phys., 06: 088, 2012.
  • Measurement of the top quark pair cross section with ATLAS in pp collisions at $\sqrt{s}$ = 7 TeV using final states with an electron or a muon and a hadronically decaying $\tau$ lepton, http://arxiv.org/abs/1205.2067, Phys. Lett. B, 717: 89-108, 2012.
  • Search for lepton flavour violation in the $e\mu$ continuum with the ATLAS detector in $\sqrt{s}$ = 7 TeV pp collisions at the LHC, http://arxiv.org/abs/1205.0725, Eur. Phys. J. C, 72: 2040, 2012.
  • Search for scalar top quark pair production in natural gauge mediated supersymmetry models with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.6736, Phys. Lett. B, 715: 44-60, 2012.
  • Measurement of $\tau$ polarization in $W \to \tau\nu$ decays with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.6720, Eur. Phys. J. C, 72: 2062, 2012.
  • Search for supersymmetry in events with three leptons and missing transverse momentum in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1204.5638, Phys. Rev. Lett., 108: 261804, 2012.
  • Searches for TeV-scale Gravity Signatures in Final States with Leptons and Jets with the ATLAS Detector at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.4646, Phys. Lett. B, 716: 122-141, 2012.
  • Search for supersymmetry with jets, missing transverse momentum and at least one hadronically decaying tau lepton in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1204.3852, Phys. Lett. B, 714: 197-214, 2012.
  • Search for charged Higgs bosons decaying via $H^{\pm} \to \tau \nu$ in $t\bar{t}$ events using pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1204.2760, J. High Energy Phys., 06: 039, 2012.
  • Search for resonant WZ production in the $WZ \to l\nu l'l'$ channel in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1204.1648, Phys. Rev. D, 85: 112012, 2012.
  • Search for Pair Production of a New b′ Quark that Decays into a Z Boson and a Bottom Quark with the ATLAS Detector, http://arxiv.org/abs/1204.1265, Phys. Rev. Lett., 109: 071801, 2012.
  • Search for the decay $B_s^0 \to \mu^+ \mu^-$ with the ATLAS detector, http://arxiv.org/abs/1204.0735, Phys. Lett. B, 713: 387, 2012.
  • Search for a fermiophobic Higgs boson in the diphoton decay channel with the ATLAS detector, http://arxiv.org/abs/1205.0701, Eur. Phys. J. C, 72: 2157, 2012.
  • Search for events with large missing transverse momentum, jets, and at least two tau leptons in 7 TeV proton-proton collision data with the ATLAS detector, http://arxiv.org/abs/1203.6580, Phys. Lett. B, 714: 180-196, 2012.
  • Measurement of the WW cross section in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector and limits on anomalous gauge couplings, http://arxiv.org/abs/1203.6232, Phys. Lett. B, 712: 289-308, 2012.
  • Search for supersymmetry in pp collisions at $\sqrt{s}$ = 7 TeV in final states with missing transverse momentum and b-jets with the ATLAS detector, http://arxiv.org/abs/1203.6193, Phys. Rev. D, 85: 112006, 2012.
  • Search for gluinos in events with two same-sign leptons, jets and missing transverse momentum with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1203.5763, Phys. Rev. Lett., 108: 241802, 2012.
  • Measurement of the top quark mass with the template method in the top antitop $\to$ lepton + jets channel using ATLAS data, http://arxiv.org/abs/1203.5755, Eur. Phys. J. C, 72: 2046, 2012.
  • Search for heavy neutrinos and right-handed W bosons in events with two leptons and jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.5420, Eur. Phys. J. C, 72: 2056, 2012.
  • Measurement of $t\overline{t}$ production with a veto on additional central jet activity in pp collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1203.5015, Eur. Phys. J. C, 72: 2043, 2012.
  • Jet mass and substructure of inclusive jets in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS experiment, http://arxiv.org/abs/1203.4606, J. High Energy Phys., 05: 128, 2012.
  • Measurement of the charge asymmetry in top quark pair production in $pp$ collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1203.4211, Eur. Phys. J. C, 72: 2039, 2012.
  • Observation of spin correlation in $t\overline{t}$ events from $pp$ collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1203.4081, Phys. Rev. Lett., 108: 212001, 2012.
  • Determination of the strange quark density of the proton from ATLAS measurements of the $W \to l\nu$ and $Z \to ll$ cross sections, http://arxiv.org/abs/1203.4051, Phys. Rev. Lett., 109: 012001, 2012.
  • Search for second generation scalar leptoquarks in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.3172, Eur. Phys. J. C, 72: 2151, 2012.
  • Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.3161, Phys. Rev. D, 85: 092014, 2012.
  • Forward-backward correlations and charged-particle azimuthal distributions in $pp$ interactions using the ATLAS detector, http://arxiv.org/abs/1203.3100, J. High Energy Phys., 07: 019, 2012.
  • Measurement of the azimuthal anisotropy for charged particle production in $\sqrt{s_{NN}}$ = 2.76 TeV lead-lead collisions with the ATLAS detector, http://arxiv.org/abs/1203.3087, Phys. Rev. C, 86: 014907, 2012.
  • Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS experiment, http://arxiv.org/abs/1203.2165, Eur. Phys. J. C, 72: 2001, 2012.
  • Search for a light Higgs boson decaying to long-lived weakly-interacting particles in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.1303, Phys. Rev. Lett., 108: 251801, 2012.
  • Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC, http://arxiv.org/abs/1203.1302, Eur. Phys. J. C.
  • Search for new particles decaying to ZZ using final states with leptons and jets with the ATLAS detector in $\sqrt{s}$ = 7 Tev proton-proton collisions, http://arxiv.org/abs/1203.0718, Phys. Lett. B, 712: 331-350, 2012.
  • Search for FCNC single top-quark production at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.0529, Phys. Lett. B, 712: 351-369, 2012.
  • Measurement of the azimuthal ordering of charged hadrons with the ATLAS detector, http://arxiv.org/abs/1203.0419, Phys. Rev. D, 86: 052005, 2012.
  • Search for Down-Type Fourth Generation Quarks with the ATLAS Detector in Events with One Lepton and Hadronically Decaying W Bosons, http://arxiv.org/abs/1202.6540, Phys. Rev. Lett., 109: 032001, 2012.
  • Search for same-sign top-quark production and fourth-generation down-type quarks in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1202.5520, J. High Energy Phys., 04: 069, 2012.
  • Measurement of the cross section for top-quark pair production in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector using final states with two high-pt leptons, http://arxiv.org/abs/1202.4892, J. High Energy Phys., 05: 059, 2012.
  • Search for anomaly-mediated supersymmetry breaking with the ATLAS detector based on a disappearing-track signature in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.4847, Eur. Phys. J. C, 72: 1993, 2012.
  • Search for pair-produced heavy quarks decaying to Wq in the two-lepton channel at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1202.3389, Phys. Rev. D, 86: 012007, 2012.
  • Search for Pair Production of a Heavy Up-Type Quark Decaying to a W Boson and a b Quark in the lepton+jets Channel with the ATLAS Detector, http://arxiv.org/abs/1202.3076, Phys. Rev. Lett., 108: 261802, 2012.
  • Search for the Standard Model Higgs boson in the decay channel $H \to ZZ^{(*)} \to 4l$ with 4.8 fb$^{-1}$ of pp collisions at $\sqrt{s}$=7 TeV with ATLAS, http://arxiv.org/abs/1202.1415, Phys. Lett. B, 710: 383-402, 2012.
  • Combined search for the Standard Model Higgs boson using up to 4.9 fb$^{-1}$ of pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector at the LHC, http://arxiv.org/abs/1202.1408, Phys. Lett. B, 710: 49-66, 2012.
  • Search for the Standard Model Higgs boson in the diphoton decay channel with 4.9 fb$^{-1}$ of pp collisions at $\sqrt{s}$=7 TeV with ATLAS, http://arxiv.org/abs/1202.1414, Phys. Rev. Lett., 108: 111803, 2012.
  • Search for decays of stopped, long-lived particles from 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1201.5595, Eur. Phys. J. C, 72: 1965, 2012.
  • Measurement of inclusive two-particle angular correlations in pp collisions with the ATLAS detector at the LHC, http://arxiv.org/abs/1203.3549, J. High Energy Phys., 05: 157, 2012.
  • Search for excited leptons in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1201.3293, Phys. Rev. D, 85: 072003, 2012.
  • Rapidity gap cross sections measured with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1201.2808, Eur. Phys. J. C, 72: 1926, 2012.
  • Measurement of the top quark pair production cross-section with ATLAS in the single lepton channel, http://arxiv.org/abs/1201.1889, Phys. Lett. B, 711: 244-263, 2012.
  • Study of jets produced in association with a W boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1201.1276, Phys. Rev. D, 85: 092002, 2012.
  • Search for anomalous production of prompt like-sign muon pairs and constraints on physics beyond the Standard Model with the ATLAS detector, http://arxiv.org/abs/1201.1091, Phys. Rev. D, 85: 032004, 2012.
  • Jet energy measurement with the ATLAS detector in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1112.6426, Eur. Phys. J. C.
  • Measurement of inclusive jet and dijet production in pp collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1112.6297, Phys. Rev. D, 86: 014022, 2012.
  • Search for heavy vector-like quarks coupling to light quarks in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.5755, Phys. Lett. B, 712: 22-39, 2012.
  • Observation of a new $\chi_b$ state in radiative transitions to $\Upsilon$(1S) and $\Upsilon$(2S) at ATLAS, http://arxiv.org/abs/1112.5154, Phys. Rev. Lett., 108: 152001, 2012.
  • Search for first generation scalar leptoquarks in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.4828, Phys. Lett. B, 711: 442-455 (Erratum), 2012.
  • Search for contact interactions in dilepton events from pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.4462, Phys. Lett. B, 712: 40-58, 2012.
  • Measurement of $D^{*\pm}$ meson production in jets from pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.4432, Phys. Rev. D, 85: 052005, 2012.
  • Search for scalar bottom pair production with the ATLAS detector in pp Collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1112.3832, Phys. Rev. Lett., 108: 181802, 2012.
  • Search for production of resonant states in the photon-jet mass distribution using pp collisions at $\sqrt{s}$ = 7 TeV collected by the ATLAS detector, http://arxiv.org/abs/1112.3580, Phys. Rev. Lett., 108: 211802, 2012.
  • Search for the Higgs boson in the $H \to WW^{(*)} \to l^{+}\nu l^{-}\bar\nu$ decay channel in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.2577, Phys. Rev. Lett., 108: 111802, 2012.
  • Search for Extra Dimensions using diphoton events in 7 TeV proton-proton collisions with the ATLAS detector, http://arxiv.org/abs/1112.2194, Phys. Lett. B, 710: 538-556, 2012.

CMS

  • Search for heavy resonances in the W/Z-tagged dijet mass spectrum in pp collisions at 7 TeV, http://cdsweb.cern.ch/record/1498395.
  • Search for long-lived particles decaying to photons and missing energy in proton-proton collisions at sqrt(s) = 7 TeV, http://cdsweb.cern.ch/record/1498386.
  • Search for exotic resonances decaying into WZ/ZZ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.5779, J. High Energy Phys..
  • Measurement of the ZZ production cross section and search for anomalous couplings in 2l2l' final states in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1211.4890, J. High Energy Phys..
  • Search for new physics in events with photons, jets, and missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.4784, J. High Energy Phys..
  • Identification of b-quark jets with the CMS experiment, http://arxiv.org/abs/1211.4462, J. Instrum..
  • Search for Z' resonances decaying to $t\bar{t}$ in dilepton+jets final states in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.3338, Phys. Rev. D.
  • Search for supersymmetry in final states with a single lepton, b-quark jets, and missing transverse energy in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.3143, Phys. Rev. D.
  • Search in leptonic channels for heavy resonances decaying to long-lived neutral particles, http://arxiv.org/abs/1211.2472, J. High Energy Phys..
  • Measurement of differential top-quark pair production cross sections in pp colisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.2220.
  • Search for supersymmetry in final states with missing transverse energy and 0, 1, 2, or at least 3 b-quark jets in 7 TeV pp collisions using the variable alphaT, http://arxiv.org/abs/1210.8115.
  • Measurement of the sum of WW and WZ production with W+dijet events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.7544, Eur. Phys. J. C.
  • Search for heavy quarks decaying into a top quark and a W or Z boson using lepton + jets events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.7471, J. High Energy Phys..
  • Search for a non-standard-model Higgs boson decaying to a pair of new light bosons in four-muon final states, http://arxiv.org/abs/1210.7619, Phys. Lett. B.
  • Measurement of the inelastic proton-proton cross section at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.6718, Phys. Lett. B.
  • Search for pair production of third-generation leptoquarks and top squarks in pp collisions at sqrt(s) = 7 TeV, http://arxiv.org/abs/1210.5629, Phys. Rev. Lett..
  • Search for third-generation leptoquarks and scalar bottom quarks in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.5627, J. High Energy Phys..
  • Observation of long-range near-side angular correlations in proton-lead collisions at the LHC, http://arxiv.org/abs/1210.5482, Phys. Lett. B.
  • Observation of Z decays to four leptons with the CMS detector at the LHC, http://arxiv.org/abs/1210.3844, J. High Energy Phys..
  • Search for fractionally charged particles in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2311, Phys. Rev. Lett..
  • Search for heavy neutrinos and W$_R$ bosons with right-handed couplings in a left-right symmetric model in pp collisions at 7 TeV, http://arxiv.org/abs/1210.2402, Phys. Rev. Lett..
  • Search for narrow resonances and quantum black holes in inclusive and b-tagged dijet mass spectra from pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2387, J. High Energy Phys..
  • Search for excited leptons in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2422, Phys. Lett. B.
  • Search for supersymmetry in events with photons and low missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2052, Phys. Lett. B.
  • Search for heavy lepton partners of neutrinos in proton-proton collisions in the context of the type III seesaw mechanism, http://arxiv.org/abs/1210.1797, Phys. Lett. B, 718: 348-368, 2012.
  • Measurement of the relative prompt production rate of $\chi_{c2}$ and $\chi_{c1}$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.0875, Eur. Phys. J. C.
  • Search for anomalous production of highly boosted Z bosons decaying to dimuons in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.0867, Phys. Lett. B.
  • Search for electroweak production of charginos and neutralinos using leptonic final states in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.6620, J. High Energy Phys..
  • Measurement of the single-top-quark t-channel cross section in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.4533, J. High Energy Phys..
  • Search for resonant $t\bar{t}$ production in lepton+jets events in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.4397, J. High Energy Phys..
  • Search for the standard model Higgs boson produced in association with W and Z bosons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.3937, J. High Energy Phys., 11: 088, 2012.
  • Search for a narrow spin-2 resonance decaying to a pair of Z vector bosons in the semileptonic final state, http://arxiv.org/abs/1209.3807, Phys. Lett. B.
  • Evidence for associated production of a single top quark and W boson in pp collisions at 7 TeV, http://arxiv.org/abs/1209.3489, Phys. Rev. Lett..
  • Measurement of the Y(1S), Y(2S) and Y(3S) polarizations in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.2922, Phys. Rev. Lett..
  • Measurement of the top-quark mass in $t\bar{t}$ events with dilepton final states in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.2393, Eur. Phys. J. C, 72: 2202, 2012.
  • Measurement of the top-quark mass in $t\bar{t}$ events with lepton+jets final states in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.2319, J. High Energy Phys..
  • Observation of a diffractive contribution to dijet production in proton-proton collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.1805, Phys. Rev. D.
  • Search for exclusive or semi-exclusive $\gamma\gamma$ production and observation of exclusive and semi-exclusive $e^+e^−$ production in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.1666, J. High Energy Phys., 11: 080, 2012.
  • Combined search for the quarks of a sequential fourth generation, http://arxiv.org/abs/1209.1062, Phys. Rev. D.
  • Search for pair produced fourth-generation up-type quarks in pp collisions at $\sqrt{s}$=7 TeV with a lepton in the final state, http://arxiv.org/abs/1209.0471, Phys. Lett. B, 718: 307-328, 2012.
  • Search for supersymmetry in events with b-quark jets and missing transverse energy in pp collisions at 7 TeV, http://arxiv.org/abs/1208.4859, Phys. Rev. D, 86: 072010, 2012.
  • Study of the dijet mass spectrum in pp $\to$ W + jets events at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1208.3477, Phys. Rev. Lett..
  • Search for three-jet resonances in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.2931, Phys. Lett. B, 718: 329-347, 2012.
  • Observation of sequential Upsilon suppression in PbPb collisions, http://arxiv.org/abs/1208.2826, Phys. Rev. Lett..
  • Measurement of the $t\bar{t}$ production cross section in the dilepton channel in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1208.2671, J. High Energy Phys..
  • Measurement of the azimuthal anisotropy of neutral pions in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1208.2470, Phys. Rev. Lett..
  • Search for flavor changing neutral currents in top quark decays in pp collisions at 7 TeV, http://arxiv.org/abs/1208.0957, Phys. Lett. B.
  • Search for a W' boson decaying to a bottom quark and a top quark in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.0956, Phys. Lett. B.
  • Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC, http://arxiv.org/abs/1207.7235, Phys. Lett. B, 716: 30-61, 2012.
  • Search for pair production of first- and second-generation scalar leptoquarks in pp collisions at $\sqrt{s}$= 7 TeV, http://arxiv.org/abs/1207.5406, Phys. Rev. D, 86: 052013, 2012.
  • Search for heavy Majorana neutrinos in $\mu^{\pm}\mu^{\pm}$ + jets and $e^{\pm}e^{\pm}$ + jets events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.6079, Phys. Lett. B, 717: 109-128, 2012.
  • Study of the inclusive production of charged pions, kaons, and protons in pp collisions at $\sqrt{s}$ = 0.9, 2.76, and 7 TeV, http://arxiv.org/abs/1207.4724, Eur. Phys. J. C, 72: 2164, 2012.
  • Forward-backward asymmetry of Drell-Yan lepton pairs in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.3973, Phys. Lett. B.
  • A search for a doubly-charged Higgs boson in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.2666, Eur. Phys. J. C, 72: 2189, 2012.
  • Measurement of the underlying event activity in pp collisions at $\sqrt{s}$ = 0.9 and 7 TeV with the novel jet-area/median approach, http://arxiv.org/abs/1207.2392, J. High Energy Phys., 08: 130, 2012.
  • Search for supersymmetry in hadronic final states using $M_{T2}$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.1798, J. High Energy Phys., 10: 018, 2012.
  • Search for new physics in the multijet and missing transverse momentum final state in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.1898, Phys. Rev. Lett., 109: 171803, 2012.
  • Search for a fermiophobic Higgs boson in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1207.1130, J. High Energy Phys., 09: 111, 2012.
  • Search for new physics with long-lived particles decaying to photons and missing energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.0627, J. High Energy Phys..
  • Inclusive and differential measurements of the $t\bar{t}$ charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.0065, Phys. Lett. B, 717: 129-150, 2012.
  • Search for stopped long-lived particles produced in pp collisions at $\sqrt{s}$ =7 TeV, http://arxiv.org/abs/1207.0106, J. High Energy Phys., 08: 026, 2012.
  • Search for a light pseudoscalar Higgs boson in the dimuon decay channel in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.6326, Phys. Rev. Lett., 109: 121801, 2012.
  • Search for dark matter and large extra dimensions in monojet events in pp collisions at $\sqrt{s}$= 7 TeV, http://arxiv.org/abs/1206.5663, J. High Energy Phys..
  • Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.3949, Phys. Lett. B.
  • Search for charge-asymmetric production of W' bosons in top pair + jet events from pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.3921, Phys. Lett. B, 717: 351–370, 2012.
  • Measurement of the electron charge asymmetry in inclusive W production in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.2598, Phys. Rev. Lett., 109: 111806, 2012.
  • Search for high mass resonances decaying into $\tau$-lepton pairs in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.1725, Phys. Lett. B, 716: 82-102, 2012.
  • Search for narrow resonances in dilepton mass spectra in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.1849, Phys. Lett. B, 714: 158-179, 2012.
  • Search for a W′ or Techni-$\rho$ Decaying into WZ in pp Collisions at $\sqrt{s}$=7  TeV, http://arxiv.org/abs/1206.0433, Phys. Rev. Lett., 109: 141801, 2012.
  • Study of W boson production in PbPb and pp collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.6334, Phys. Lett. B, 715: 66-87, 2012.
  • Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy, http://arxiv.org/abs/1205.6615, Phys. Rev. Lett., 109: 071803, 2012.
  • Measurement of jet fragmentation into charged particles in pp and PbPb collisions at $\sqrt{s_{NN}}$= 2.76 TeV, http://arxiv.org/abs/1205.5872, J. High Energy Phys., 10: 087, 2012.
  • Search for a light charged Higgs boson in top quark decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5736, J. High Energy Phys., 07: 143, 2012.
  • Search for new physics in events with same-sign dileptons and b-tagged jets in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.3933, J. High Energy Phys., 08: 110, 2012.
  • Measurement of the pseudorapidity and centrality dependence of the transverse energy density in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.2488, Phys. Rev. Lett., 109: 152303, 2012.
  • Measurement of the $\Lambda_b$ cross section and the $\overline{\Lambda}_b$ to $\Lambda_b$ ratio with J/$\psi\Lambda$ decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.0594, Phys. Lett. B, 714: 136-157, 2012.
  • Search for heavy long-lived charged particles in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1205.0272, Phys. Lett. B, 713: 408-433, 2012.
  • Studies of jet quenching using isolated-photon+jet correlations in PbPb and pp collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.0206, Phys. Lett. B.
  • Observation of a New $\Xi_{b}$ Baryon, http://arxiv.org/abs/1204.5955, Phys. Rev. Lett., 108: 252002, 2012.
  • Search for anomalous production of multilepton events in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1204.5341, J. High Energy Phys., 06: 169, 2012.
  • Search for leptonic decays of W' bosons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1204.4764, J. High Energy Phys., 08: 023, 2012.
  • Search for physics beyond the standard model in events with a Z boson, jets, and missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.3774, Phys. Lett. B, 716: 260-284, 2012.
  • Shape, transverse size, and charged hadron multiplicity of jets in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.3170, J. High Energy Phys., 06: 160, 2012.
  • Measurement of the mass difference between top and antitop quarks, http://arxiv.org/abs/1204.2807, J. High Energy Phys., 06: 109, 2012.
  • Search for anomalous $t \bar{t}$ production in the highly-boosted all-hadronic final state, http://arxiv.org/abs/1204.2488, J. High Energy Phys..
  • Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1204.1850, Phys. Rev. Lett., 109: 022301, 2012.
  • Measurement of the Z/$\gamma^*$+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1643, J. High Energy Phys., 06: 126, 2012.
  • Measurement of the underlying event in the Drell-Yan process in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1411, Eur. Phys. J. C, 72: 2080, 2012.
  • Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV, http://arxiv.org/abs/1204.1409, Phys. Rev. C.
  • Search for heavy bottom-like quarks in 4.9 inverse femtobarns of pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1088, J. High Energy Phys., 05: 123, 2012.
  • Search for Dark Matter and Large Extra Dimensions in pp Collisions Yielding a Photon and Missing Transverse Energy, http://arxiv.org/abs/1204.0821, Phys. Rev. Lett., 108: 261803, 2012.
  • Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.0696, Eur. Phys. J. C, 72: 2216, 2012.
  • Measurement of the top quark pair production cross section in pp collisions at $\sqrt{s}$ = 7 TeV in dilepton final states containing a $\tau$, http://arxiv.org/abs/1203.6810, Phys. Rev. D, 85: 112007, 2012.
  • Search for heavy, top-like quark pair production in the dilepton final state in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1203.5410, Phys. Lett. B, 716: 103-121, 2012.
  • Search for $B_s^0 \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays, http://arxiv.org/abs/1203.3976, J. High Energy Phys., 04: 033, 2012.
  • Measurement of the cross section for production of b b-bar X, decaying to muons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1203.3458, J. High Energy Phys., 06: 110, 2012.
  • Search for microscopic black holes in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.6396, J. High Energy Phys., 04: 061, 2012.
  • Search for quark compositeness in dijet angular distributions from pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.5535, J. High Energy Phys., 05: 055, 2012.
  • Jet momentum dependence of jet quenching in PbPb collisions at $\sqrt{s_{NN}}$=2.76 TeV, http://arxiv.org/abs/1202.5022, Phys. Lett. B, 712: 176-197, 2012.
  • Inclusive b-jet production in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.4617, J. High Energy Phys., 04: 084, 2012.
  • Search for the standard model Higgs boson decaying to bottom quarks in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.4195, Phys. Lett. B, 710: 284-306, 2012.
  • Search for neutral Higgs bosons decaying to tau pairs in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.4083, Phys. Lett. B, 713: 68-90, 2012.
  • Search for large extra dimensions in dimuon and dielectron events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.3827, Phys. Lett. B, 711: 15-34, 2012.
  • Search for the standard model Higgs boson in the $H \to ZZ \to l^+l^- \tau^+ \tau^-$ decay channel in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.3617, J. High Energy Phys., 03: 081, 2012.
  • Search for the standard model Higgs boson in the $H \to ZZ \to 2l 2\nu$ channel in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.3478, J. High Energy Phys., 03: 040, 2012.
  • Study of high-$p_T$ charged particle suppression in PbPb compared to pp collisions at $\sqrt{s_{NN}}$=2.76 TeV, http://arxiv.org/abs/1202.2554, Eur. Phys. J. C, 72: 1945, 2012.
  • Search for the standard model Higgs boson in the decay channel $H \to ZZ \to 4 l$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1997, Phys. Rev. Lett., 108: 111804, 2012.
  • Search for the standard model Higgs boson decaying into two photons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.1487, Phys. Lett. B, 710: 403-425, 2012.
  • Search for the standard model Higgs boson decaying to $W^+ W^-$ in the fully leptonic final state in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1489, Phys. Lett. B, 710: 91-113, 2012.
  • Search for a Higgs boson in the decay channel $H \to ZZ^{(*)} \to q\bar{q}l^-l^+$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1416, J. High Energy Phys., 04: 036, 2012.
  • Combined results of searches for the standard model Higgs boson in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1488, Phys. Lett. B, 710: 26-48, 2012.
  • Measurement of the inclusive production cross sections for forward jets and for dijet events with one forward and one central jet in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.0704, J. High Energy Phys., 06: 036, 2012.
  • Suppression of non-prompt J$\psi$, prompt J$\psi$, and $\Upsilon$(1S) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.5069, J. High Energy Phys., 05: 063, 2012.
  • Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.3158, Eur. Phys. J. C, 72: 2012, 2012.
  • Measurement of isolated photon production in pp and PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.3093, Phys. Lett. B, 710: 256-277, 2012.
  • Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1112.5100, Phys. Lett. B, 709: 28-49, 2012.

LHCb

  • Measurement of $J/\psi$ production in $pp$ collisions at $\sqrt{s}=2.76$ TeV, http://arxiv.org/abs/1212.1045, J. High Energy Phys..
  • Implications of LHCb measurements and future prospects, http://arxiv.org/abs/1208.3355, Eur. Phys. J. C.
  • First observation of the $B_{s2}^\ast(5840)^0 \to B^{\ast+} K^-$ decay and properties of the orbitally excited $B^0_s$ mesons, http://arxiv.org/abs/1211.5994, Phys. Rev. Lett..
  • Measurement of the time-dependent $CP$ asymmetry in $B^0 \to J/\psi K^0_{\rm S}$ decays, http://arxiv.org/abs/1211.6093, Phys. Lett. B.
  • First evidence of the $B^0_s \to \mu^+\mu^-$ decay, http://arxiv.org/abs/1211.2674, Phys. Rev. Lett..
  • First observation of the decays $\bar{B}^0_{(s)}\to D_s^+K^-\pi^+\pi^-$ and $\bar{B}^0_s\to D_{s1}(2536)^+\pi^-$, http://arxiv.org/abs/1211.1541, Phys. Rev. D.
  • A study of the $Z$ production cross-section in $pp$ collisions at $\sqrt{s}$ = 7 TeV using tau final states, http://arxiv.org/abs/1210.6289, J. High Energy Physics.
  • Measurement of the $B^0$--$\bar B^0$ oscillation frequency $\Delta m_d$ with the decays $B^0 \to D^- \pi^+$ and $B^0 \to J\ \psi K^{*0}$, http://arxiv.org/abs/1210.6750, Phys. Lett. B.
  • Observation of $D^0 - \overline{D}^0$ oscillations, http://arxiv.org/abs/1211.1230, Phys. Rev. Lett..
  • First observation of the decay $B^+ \to \pi^+ \mu^+\mu^-$, http://arxiv.org/abs/1210.2645, J. High Energy Phys..
  • Measurement of the $C\!P$ asymmetry in $B^0 \to K^{*0} \mu^+ \mu^-$ decays, http://arxiv.org/abs/1210.4492, Phys. Rev. Lett..
  • Measurement of the $D^\pm$ production asymmetry in 7 TeV $pp$ collisions, http://arxiv.org/abs/1210.4112, Phys. Lett. B.
  • Evidence for the decay $B^0 \to J/\psi \omega$ and measurement of the relative branching fractions of $B^0_s$ meson decays to $J/\psi \eta$ and $J/\psi \eta'$, http://arxiv.org/abs/1210.2631, Nucl. Phys. B.
  • First evidence for the annihilation decay mode $B^{+} \to D_{s}^{+} \phi$, http://arxiv.org/abs/1210.1089, J. High Energy Phys..
  • Measurements of $B_c^+$ production and mass with the $B_c^+ \to J/\psi \pi^+$ decay, http://arxiv.org/abs/1209.5634, Phys. Rev. Lett., 109: 232001, 2012.
  • A model-independent Dalitz plot analysis of $B^\pm \to D K^\pm$ with $D \to K^0_{\rm S} h^+h^-$ ($h=\pi, K$) decays and constraints on the CKM angle $\gamma$, http://arxiv.org/abs/1209.5869, Phys. Lett. B, 718: 43-55, 2012.
  • Differential branching fraction and angular analysis of the $B^+ \to K^+ \mu^+ \mu^-$ decay, http://arxiv.org/abs/1209.4284, J. High Energy Phys..
  • Search for the rare decay $K_{\rm\scriptscriptstyle S}^0\rightarrow\mu^{+}\mu^{-}$, http://arxiv.org/abs/1209.4029, J. High Energy Phys..
  • Measurement of the fraction of $\Upsilon(1S)$ originating from $\chi_b(1P)$ decays in $pp$ collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.0282, J. High Energy Phys., 11: 031, 2012.
  • Measurement of the ratio of branching fractions $B(B^0 \to K^{\ast 0} \gamma) / B(B^0_s \to \phi \gamma)$ and the direct $C\!P$ asymmetry in $B^0 \to K^{\ast 0} \gamma$, http://arxiv.org/abs/1209.0313, Nucl. Phys. B, 867: 1-18, 2012.
  • Measurement of the $B^0_s \rightarrow J/\psi \bar{K}^{*0}$ branching fraction and angular amplitudes, http://arxiv.org/abs/1208.0738, Phys. Rev. D, 86: 071102, 2012.
  • Observation of $B^0 \to \bar{D}^0 K^+ K^-$ and evidence of $B^0_s \to \bar{D}^0 K^+ K^-$, http://arxiv.org/abs/1207.5991, Phys. Rev. Lett., 109: 131801, 2012.
  • Measurement of the effective $B_s^0 \to K^+ K^-$ lifetime, http://arxiv.org/abs/1207.5993, Phys. Lett. B, 716: 393-400, 2012.
  • Study of $D_{sJ}$ decays to $D^+K^0_{\rm S}$ and $D^0K^+$ final states in $pp$ collisions, http://arxiv.org/abs/1207.6016, J. High Energy Phys., 10: 151, 2012.
  • Measurement of the $\bar{B}^0_s$ effective lifetime in the $J/\psi f_0(980)$ final state, http://arxiv.org/abs/1207.0878, Phys. Rev. Lett., 109: 152002, 2012.
  • Measurement of prompt hadron production ratios in $pp$ collisions at $\sqrt{s} = $ 0.9 and 7 TeV, http://arxiv.org/abs/1206.5160, Eur. Phys. J. C, 72: 2168, 2012.
  • Measurement of $b$-hadron branching fractions for two-body decays into charmless charged hadrons, http://arxiv.org/abs/1206.2794, J. High Energy Phys., 10: 037, 2012.
  • Observation of excited $\Lambda^0_b$ baryons, http://arxiv.org/abs/1205.3452, Phys. Rev. Lett., 109: 172003, 2012.
  • Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1205.0975, J. High Energy Phys., 06: 141, 2012.
  • Measurement of the $B_s^0\to J/\psi K_S^0$ branching fraction, http://arxiv.org/abs/1205.0934, Phys. Lett. B.
  • Measurement of relative branching fractions of B decays to $\psi(2S)$ and $J/\psi$ mesons, http://arxiv.org/abs/1205.0918, Eur. Phys. J. C.
  • Measurement of the $D_s^+ - D_s^-$ production asymmetry in 7 TeV pp collisions, http://arxiv.org/abs/1205.0897, Phys. Lett. B, 713: 186-195, 2012.
  • Measurement of the isospin asymmetry in $B \to K^{(*)}\mu^+ \mu^-$ decays, http://arxiv.org/abs/1205.3422, J. High Energy Phys., 07: 133, 2012.
  • Measurement of the CP-violating phase $\phi_s$ in $\overline{B}^0_s \to J/\psi\pi^+\pi^-$ decays, http://arxiv.org/abs/1204.5675, Phys. Lett. B.
  • Analysis of the resonant components in $\overline{B}^0_s \to J/\psi\pi^+\pi^-$, http://arxiv.org/abs/1204.5643, Phys. Rev. D.
  • Measurement of the branching fractions of the decays $B_s^0 \rightarrow D_s^\mp K^\pm$ and $B_s^0 \rightarrow D_s^- \pi^+$, http://arxiv.org/abs/1204.1237, J. High Energy Phys..
  • Measurement of the ratio of prompt $\chi_{c}$ to $J/\psi$ production in $pp$ collisions at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1204.1462, Phys. Lett. B, 718: 431-440, 2012.
  • First observation of decay $B_c^+\to J/\psi \pi^+\pi^-\pi^+$, http://arxiv.org/abs/1204.0079, Phys. Rev. Lett..
  • Measurement of the polarization amplitudes and triple product asymmetries in the $B_s^0 \to \phi\phi$ decay, http://arxiv.org/abs/1204.2813, Phys. Lett. B, 713: 369-377, 2012.
  • Inclusive $W$ and $Z$ production in the forward region at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1620, J. High Energy Phys..
  • Measurement of $\psi$(2S) meson production in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1204.1258, Eur. Phys. J. C, 72: 2100, 2012.
  • Strong constraints on the rare decays $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$, http://arxiv.org/abs/1203.4493, Phys. Rev. Lett., 108: 231801, 2012.
  • Observation of $C\!P$ violation in $B^\pm \to D K^\pm$ decays, http://arxiv.org/abs/1203.3662, Phys. Lett. B.
  • Measurements of the branching fractions and $C\!P$ asymmetries of $B^{\pm} \to J\!/\!\psi\, \pi^{\pm}$ and $B^{\pm} \to \psi(2S) \pi^{\pm}$ decays, http://arxiv.org/abs/1203.3592, Phys. Rev. D, 85: 091105(R), 2012.
  • Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s} = 7$ TeV, http://arxiv.org/abs/1202.6579, Eur. Phys. J. C, 72: 2025, 2012.
  • Measurement of the ratio of branching fractions ${\cal B}(B^0 \to K^{\ast 0} \gamma)/{\cal B}(B^0_s \to \phi \gamma)$, http://arxiv.org/abs/1202.6267, Phys. Rev. D, 85: 112013, 2012.
  • First evidence of direct $C\!P$ violation in charmless two-body decays of $B^0_s$ mesons, http://arxiv.org/abs/1202.6251, Phys. Rev. Lett., 108: 201601, 2012.
  • Opposite-side flavour tagging of $B$ mesons at the LHCb experiment, http://arxiv.org/abs/1202.4979, Eur. Phys. J. C, 72: 2022, 2012.
  • Measurement of the $B^\pm$ production cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1202.4812, J. High Energy Phys., 04: 093, 2012.
  • Search for the $X(4140)$ state in $B^+\to J/\psi\phi K^+$ decays, http://arxiv.org/abs/1202.5087, Phys. Rev. D, 85: 091103, 2012.
  • Determination of the sign of the decay width difference in the $B^0_s$ system, http://arxiv.org/abs/1202.4717, Phys. Rev. Lett., 108: 241801, 2012.
  • Measurement of the cross-section ratio $\sigma(\chi_{c2})/\sigma(\chi_{c1})$ for prompt $\chi_c$ production at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1202.1080, Phys. Lett. B, 714: 215-223, 2012.
  • Searches for Majorana neutrinos in $B^-$ decays, http://arxiv.org/abs/1201.5600, Phys. Rev. D, 85: 112004, 2012.
  • First observation of the decays $\overline{B}^0 \to D^+ K^- \pi^+ \pi^-$ and $B^- \to D^0 K^- \pi^+ \pi^-$, http://arxiv.org/abs/1201.4402, Phys. Rev. Lett., 108: 161801, 2012.
  • Observation of X(3872) production in $pp$ collisions at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1112.5310, Eur. Phys. J. C, 72: 1972, 2012.
  • Measurement of $b$-hadron masses, http://arxiv.org/abs/1112.4896, Phys. Lett. B, 708: 241-248, 2012.
  • Observation of $\overline{B}^0_s \to J/\psi f'_2(1525)$ in $J/\psi K^+K^-$ final states, http://arxiv.org/abs/1112.4695, Phys. Rev. Lett., 108: 151801, 2012.
  • Measurement of mixing and CP violation parameters in two-body charm decays, http://arxiv.org/abs/1112.4698, J. High Energy Phys., 04: 129, 2012.
  • Measurement of the $B^0_s-\overline{B}^0_s$ oscillation frequency $\Delta m_s$ in $B^0_s \to D^-_s (3)\pi$ decays, http://arxiv.org/abs/1112.4311, Phys. Lett. B, 709: 177-184, 2012.
  • Measurement of charged particle multiplicities in $pp$ collisions at $\sqrt{s}$ = 7 TeV in the forward region, http://arxiv.org/abs/1112.4592, Eur. Phys. J. C, 72: 1947, 2012.
  • Differential branching fraction and angular analysis of the decay $B^{0} \rightarrow K^{*0} \mu^+ \mu^-$, http://arxiv.org/abs/1112.3515, Phys. Rev. Lett., 108: 181806, 2012.
  • Measurement of the CP-violating phase $\phi_s$ in the decay $B^{0}_s \to J/\psi \phi$, http://arxiv.org/abs/1112.3183, Phys. Rev. Lett., 108: 101803, 2012.
  • Measurement of the CP violating phase $\phi_s$ in $\overline{B}^0_s \to J/\psi f_0(980)$, http://arxiv.org/abs/1112.3056, Phys. Lett. B, 707: 497–505, 2012.

LHCf

  • Measurement of forward neutral pion transverse momentum spectra for $\sqrt{s}$ = 7TeV proton-proton collisions at LHC, http://arxiv.org/abs/1205.4578, Phys. Rev. D.
  • Comparison of hadron interaction models with measurement of forward spectra by the LHCf apparatus, http://cdsweb.cern.ch/record/1434705, Nuovo Cimento C, 034: 135-140, 2011.
  • Measurement of zero degree inclusive photon energy spectra for $\sqrt{s}$= 900 GeV proton-proton collisions at LHC, http://arxiv.org/abs/1207.7183, Phys. Lett. B, 715: 298-303, 2012.

TOTEM

Saturday, December 08, 2012

GRAIL's Gravity Tour of the Moon


Embedded video from
NASA Jet Propulsion Laboratory California Institute of Technology
This movie shows the variations in the lunar gravity field as measured by NASA's Gravity Recovery and Interior Laboratory (GRAIL) during the primary mapping mission from March to May 2012.

Friday, December 07, 2012

Spintronics made easy

Spintronics (a neologism for "spin-based electronics"), also known as magnetoelectronics, is an emerging technology which exploits the quantum spin states of electrons as well as making use of their charge state. The electron spin itself is manifested as a two state magnetic energy system. The discovery of giant magnetoresistance in 1988 by Albert Fert et al. and Peter Grünberg et al. independently is considered as the birth of spintronics.


David Awschalom explains how the spin of the electron could be exploited in completely new types of electronic circuits If you are new to spintronics - or if you are wondering what all the excitement is about -- David Awschalom of the University of California, Santa Barbara provides a fantastic introduction to the field and explains how electron spin could be harnessed to create even denser computer memories and even quantum computers. In this video interview Awschalom also outlines the challenges that must be overcome before we see the next generation of spintronics devices and explains how he is addressing some of these in his lab.




TEDxCaltech - David Awschalom - Spintronics: Abandoning Perfection for the Quantum Age"



 See Also:

My Perspective on the Elemental Nature

The Atomic Structure of Molecules by Matt Strassler December 7, 2012....also precursor to this article also by Matt Strassler, The Molecular Structure of Matter, May 28, 2012





Photo by Graham Challifour. Reproduced from Critchlow, 1979, p. 132.



 
With the discovery of sound waves in the CMB, we have entered a new era of precision cosmology in which we can begin to talk with certainty about the origin of structure and the content of matter and energy in the universe-Wayne Hu

I quoted myself below with regard to Matt Strassler's two articles, because it is of interest to me to say how we might make use of the matters around us. As well,  too point out the Layman I am. I appreciate what is being put out there in terms of the science so as to help one progress in their own studies.
Yes most interesting for sure. Orbitals integration....most important.

Just a few points for consideration in terms of the energy valuations in terms of the Matter construct as energy configurations....right from molecules to proton nucleus(powers of ten). Bohr's Model 

As well Seaborg's contributions, as a precursor to elemental table construction. Quite early, Law of Octaves looking at the historical perspective. 

As a Law of Octave(historically), this also makes for some interesting comparisons in my mind to a string theorist's mind, as a particle interpretation energy valuation description, or, would that be an unfair comparison?? Another way perhaps, in which to perceive the "Pythagorean sound" as weight with water suspended in gourds while plucking strings?:)

In this sense I am speaking in terms of the history of the way on which a mind can perceive being open too, as to what  it is we select to form the realities around us. These are constructive ways in which we may apply a schematic drawing and building up of,  to form the structure of the reality as it is measure and perceived by us. In his answer,  Matt openly addresses the "tent model" by one of his commentators. and says,"Your tent fabric analogy is an interesting one."

This is part of who I am as to my inquiring into the diverse nature of our measures,  which  help to develop the perspective around the elements and how we make use of them. Why I may look to astrophysical sources to help me point toward the reductionist versions of the data we are gaining from measures.  Which  helps ascertain the aspects of the reality building we are doing.

Also too, I have revealed my own bias to "the sound"  as a sensory revelation of sorts. How one may say measure is of this reality,  and is spoken too. In this sense while their is a whole pluralistic need for mathematical ascertains to say one is a string theorist, I would say on a most fundamental level without such structure around me, I may be interpreted "as ignorant" while suggesting the garb and cloak I wear is based on this theatrical disguise.

For consideration by Lumo perhaps then?:)

Now, Aidan says that the electron is not spinning because it's pointlike. Even if we adopt the usual definitions that were developed in the classical framework, this statement by Aidan is wrong at both levels. First, it's not true that the electron is strictly point-like. Before the Planck scale, all particles have to have an internal structure because quantum gravity doesn't allow distances shorter than the Planck length to be resolved. The internal architecture of particles therefore can't be "strictly and sharply point-like". In all perturbative string vacua, the electrons are vibrating strings (occupying space comparable to the string length, a few orders of magnitude longer than the Planck length) and indeed, the spin may be understood as coming from some internal degrees of freedom that are localized at an extended object.

In fact, the stringy picture of the spin tells us exactly where the reasoning that pointlike or tiny objects can't carry a nonzero or rather large angular momentum breaks down. The string is locally a very heavy object – the tension or the linear mass density of the fundamental string in string theory is huge – and the motion of this string just a string length away from the center of mass has a big, Planck's-constant-sized impact on the angular momentum. On the other hand, the overall rest mass of the resulting particle may be small or even zero because of various cancellations, including the fact that the sum of integers is equal to
1/12 which is the primary identity guaranteeing that some stringy vibration modes remain exactly massless (and others' masses only arise from some much smaller corrections).The electron is spinning, after all


But yes, I gaze star-ward as well, as to include in my vision of the reality around us  a fundamental make-up requirement, so as to say,  the LHC is a corresponding feature of the reality coordination as a microscopic understanding of a macroscopic world.





The last major changes to the periodic table was done in the middle of the 20th Century. Glenn Seaborg is given the credit for it. Starting with his discovery of plutonium in 1940, he discovered all the transuranic elements from 94 to 102. He reconfigured the periodic table by placing the actinide series below the lanthanide series. In 1951, Seaborg was awarded the Noble prize in chemistry for his work. Element 106 has been named seaborgium (Sg) in his honor.A BRIEF HISTORY OF THE DEVELOPMENT OF PERIODIC TABLE

Standard form of the periodic table. The colors represent different categories of elements




See Also:


Wednesday, December 05, 2012

Astrophysical Signals for Quantum Gravity Signals







Logo for the Fermi Gamma-ray Space Telescope. Credit: NASA/Sonoma State University/Aurore Simonnet

NASA's newest observatory, the Gamma-ray Large Area Space Telescope, or GLAST, has begun its mission of exploring the universe in high-energy gamma rays. The spacecraft and its revolutionary instruments passed their orbital checkout with flying colors.

NASA announced August 26 that GLAST has been renamed the Fermi Gamma-ray Space Telescope. The new name honors Prof. Enrico Fermi (1901-1954), a pioneer in high-energy physics.
See:NASA Renames Observatory for Fermi, Reveals Entire Gamma-Ray Sky




 
See Also:



Olfactory Experience

 

If you sprinkle fine sand uniformly over a drumhead and then make it vibrate, the grains of sand will collect in characteristic spots and figures, called Chladni patterns. These patterns reveal much information about the size and the shape of the drum and the elasticity of its membrane. In particular, the distribution of spots depends not only on the way the drum vibrated initially but also on the global shape of the drum, because the waves will be reflected differently according to whether the edge of the drumhead is a circle, an ellipse, a square, or some other shape.

In cosmology, the early Universe was crossed by real acoustic waves generated soon after Big Bang. Such vibrations left their imprints 300 000 years later as tiny density fluctuations in the primordial plasma. Hot and cold spots in the present-day 2.7 K CMB radiation reveal those density fluctuations. Thus the CMB temperature fluctuations look like Chaldni patterns resulting from a complicated three-dimensional drumhead that



How we make use of our senses? Does one not wonder about the effect of our memory retention how on how well we can call up memories?

The Vibration theory of smell proposes that a molecule's smell character is due to its vibrational frequency in the infrared range. The theory is opposed to the more widely accepted shape theory of olfaction, which proposes that a molecule's smell character is due to its shape.
I expose myself to a bias in my thinking that seems natural to me with regard to the subject of vibratory reductionism. So the idea of Vibration theory of olfaction is interesting in the sense that we may use a ancient part of our physiological makeup to access memories, that are correlated with this sense as a marker.

 The Shape theory of smell states that a molecule's particular smell is due to a 'lock and key' mechanism by which a scent molecule fits into olfactory receptors in the nasal epithelium.

Would we say that this is a more potent way of remembrance that we may have underestimated the nature and the way that memory induction employed not just in terms of this neurological connection of the time there in association, but as a feature of the biological presences that we muster as matter beings.

That the spectrum of sight is much finer then the matter states of consideration in terms of a waffling of a breeze that carries the scent of let's say mom's apple pie? So we see this impression is made not only in the retention of the memory, but is further compacted, with this "emotional significant association."

This "emotional impact"  is significant? Not just in the smell, but of the vibratory experience we correlate with let's say music here, so as to retain and impress upon our youth and vigor,  the choices made then.

So memory is vital in the sense that olfactory experience is important in the retention of these memories. Thus to an understanding and constructive creative schematic of defining our experiences in terms of how well such "other sense are used" to impress upon and recount experience.



Big Ideas presents Seth Lloyd of the Massachusetts Institute for Technology on Quantum Life, how organisms have evolved to make use of quantum effects.


See:

Tuesday, November 27, 2012

Quantum Foam and Discrete Measures


Physicists would dearly love to study this foam but there's a problem. Spacetime only becomes foam-like on the tiniest scale, at so-called Planck lengths of 10^-35 metres or so. See: How to Measure Quantum Foam With a Tabletop Experiment
An ongoing question was raised by Bee of Backreaction and thoughts I have had as to the applicability of it's experimental design.



 It's difficult to see that while seeing the larger view of a Lagrangian of the universe is to see such an experiment located "as part and parcel of the variance in determination of the strength and weaknesses of that Lagrangian."

So you drive the focus down to the microscopic, and then to ask, in what case has the photon's journey been of value in the ascertaining the distance and time, of that photon's journey?

Just trying to orientate perspective in the case of Lagrange, yet we see on the macroscopically that it works.

It is to orientate the thought experiment in the direction of a determination of value when assigned to Lagrangian and its limits at minimal length.

A phenomenological question then about that environment with this application.





On another note then being respective of the drive toward understanding using Higg's,"The solution is to make the equations more complicated and introduce a Higgs field, which, once it is non-zero on average, can give the electron its mass without messing up the workings of the weak nuclear force.1

1.Why the Higgs Field is Necessary

 It is difficult then to ascertain Higgs field at zero, yet I want to count?




See Also

Abell 399 and Abell 401, connected by a bridge of hot gas

This image shows galaxy clusters Abell 399, lower center, and Abell 401 connected by a bridge of hot gas (ESA Planck Collaboration / STScI Digitized Sky Survey)

 Planck’s primary task is to capture the most ancient light of the cosmos. If this faint light interacts with the hot gas permeating different types of space structures including galaxies and galaxy clusters, its energy distribution is modified in a characteristic way, a phenomenon known as the Sunyaev-Zel’dovich (SZ) effect. See: Planck Discovers Huge Gas Filament Connecting Two Galaxy Clusters
 Astronomy & Astrophysics; arXiv: 1208.5911




See Also:


Monday, November 26, 2012

Observational Gravitational-Wave Astronomy.


Figure 1: Gravitational wave strain and strain sensitivity for a 5 year observation with PTAs.
The red dashed line is the approximate strain sensitivity for current PTAs (11), and the green
dashed line shows the previous estimate for the stochastic signal strength that is currently in
standard use for PTA analyses (13, 14). The dark blue solid line corresponds to our mean
estimate for the stochastic signal strength, with the blue shaded region bound by thin solid
blue lines showing our 95% confidence interval for this estimate, based on the observational
uncertainties of our model parameters. The light blue (△ACD) and cyan (△ABE) shaded
regions show the area corresponding to the square root of the 2 integrand, to be integrated over
logarithmic frequency intervals as in Eq. (3), for our expected SNR of 8, and the SNR of 2
expected from previous estimates (13, 14), respectively. See: The Imminent Detection Of Gravitational Waves From Massive Black-Hole Binaries With Pulsar Timing Arrays





As mentioned in article by Technology Review the idea of previous information as to supplying data would have to be identified in future experiments as confirmations. In this instance information gained from Taylor and Hulse  in terms of binary star rotations closeness.