78 results on '"Cooper, J."'
Search Results
2. Search for new particles decaying to tt in pp collisions at square root s=1.8 TeV
- Author
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Affolder, T., Akimoto, H., Akopian, A., Albrow, M.G., Amaral, P., Amendolia, S.R., Amidei, D., Anikeev, K., Antos, J., Apollinari, G., Arisawa, T., Asakawa, T., Ashmanskas, W., Atac, M., Azfar, E., Azzi-Bacchetta, P., Bacchetta, N., Bailey, M.W., Bailey, S., de Barbaro, P., Barbaro-Galtieri, A., Barnes, V.E., Barnett, B.A., Barone, M., Bauer, G., Bedeschi, F., Belforte, S., Bellettimi, G., Bellinger, J., Benjamin, D., Bensinger, J., Beretvas, A., Berge, J.P., Berryhill, J., Bevensee, B., Bhatti, A., Binkley, M., Bisello, D., Blair, R.E., Blocker, C., Bloom, K., Blumenfeld, B., Blusk, S.R., Bocci, A., Bodek, A., Bokhari, W., Bolla, G., Bonushkin, Y., Bortoletto, D., Boudreau, J., Brandl, A., van den Brink, S., Bromberg, C., Brozovic, M., Bruner, N., Buckley-Geer, E., Budagov, J., Budd, H.S., Burkett, K., Busetto, G., Byon-Wagner, A., Byrum, K.L., Campbell, M., Carithers, W., Carlson, J., Carlsmith, D., Cassada, J., Castro, A., Cauz, D., Cerri, A., Chan, A.W., Chang, P.S., Chang, P.T., Chapman, J.N., Chen, C., Chen, Y.C., Cheng, M.T., Chertok, M., Chiarelli, G., Chirikov-Zorin, I., Chlachidze, G., Chlebana, F., Christofek, L., Chu, M.L., Cihangir, S., Ciobanu, C.I., Clark, A.G., Connolly, A., Conway, J., Cooper, J., Cordelli, M., Cranshaw, J., Cronin-Hennessy, D., Cropp, R., Culbertson, R., Dagenhart, D., DeJongh, F., Dell'Agnello, S., Dell'Orso, M, Demina, R., Demortier, L., Dennino, M., Derwent, P.F., Devlin, T., Ditmann, J.R., Donati, S., Done, J., Dorigo, T., Eddy, N., Einsweiler, K., Elias, J.E., Engels, E., Erdmann, W., Errede, D., Errede, S., Fan, Q., Feild, R.G., Ferretti, C., Field, R.D., Fiori, I., Flaugher, B., Foster, G.W., Franklin, M., Freeman, J., Friedman, J., Fukui, Y., Galeotti, S., Gallinaro, M., Gao, T., Garcia-Sciveres, M., Garfinkel, A.F., Gatti, P., Gay, C., Geer, S., Gerdes, D.W., Giannetti, P., Giromini, P., Glagolev, V., Gold, M., Goldstein, J., Gordon, A., Goshaw, A.T., Gotra, Y., Goulianos, K., Green, C., Groer, L., Grosso-Pilcher, C., Guenther, M., Guillian, G., Guimaraes da Costa, J., Guo, R.S., Haber, C., Hafen, E., Hahn, S.R., Hall, C., Handa, T., Handler, R., Hao, W., Happacher, F., Hara, K., Hardman, A.D., Harrison, R.M., Hartmann, F., Hatakeyama, K., Hauser, J., Heinrich, J., Heiss, A., Herndon, M., Hinrichsen, B., Hoffman, K.D., Holck, C., Hollebeek, R., Holloway, L., Hughes, R., Huston, J., Huth, J., Ikeda, H., Incandela, J., Introzzi, G., Iwai, J., Iwata, Y., James, E., Jensen, H., Jones, M., Joshi, U., Kambara, H., Kamon, T., Kaneko, T., Karr, K., Kasha, H., Kato, Y., Keaffaber, T.A., Kelley, K., Kelly, M., Kennedy, R.D., Kephart, R., Khazins, D., Kikuchi, T., Kirk, M., Kim, B.J., Kim, D.H., Kim, H.S., Kim, M.J., Kim, S.H., Kim, Y.K., Kirsch, L., Klimenko, S., Koehn, P., Kongeter, A., Kondo, K., Konigsberg, J., Kordas, K., Korn, A., Korytov, A., Kovacs, E., Kroll, J., Kruse, M., Kuhlmann, S.E., Kurino, K., Kuwabara, T., Laasanen, A.T., Lai, N., Lami, S., Lammel, S., Lamoureux, J.I., Lancaster, M., Latino, G., LeCompte, T., Lee, A.M., Lee, K., Leone, S., Lewis, J.D., Lindgren, M., Liss, T.M., Liu, J.B., Liu, Y.C., Lockyer, N., Loken, J., Loreti, M., Lucchesi, D., Lukens, P., Lusin, S., Lyons, L., Lys, J., Madrak, R., Maeshima, K., Maksimovic, P., Malferrari, L., Mangano, M., Mariotti, M., Martignon, G., Martin, A., Matthews, J.A.J., Mayer, J., and Mazzanti, P.
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High Energy Physics::Experiment ,QC - Abstract
We use 106 pb/sup -1/ of data collected with the Collider Detector at Fermilab to search for narrow-width, vector particles decaying to a top and an antitop quark. Model independent upper limits on the cross section for narrow, vector resonances decaying to tt are presented. At the 95% confidence level, we exclude the existence of a leptophobic Z' boson in a model of top-color-assisted technicolor with mass M/sub Z'/ lt 480 GeV/c/sup 2/ for natural width Gamma =0.012M/sub Z'/, and M/sub Z'/ lt 780 GeV/c/sup 2/ for Gamma =0.04M/sub Z'/.
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- 2000
3. Pseudogap in YBa2Cu3O6+Δ is not bounded by a line of phase transitions: Thermodynamic evidence.
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Cooper, J. R., Loram, J. W., Kokanović, I., Storey, J. G., and Tallon, J. L.
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PHASE transitions , *THERMODYNAMICS , *RESONANT ultrasound spectroscopy , *HEAT capacity , *SUPERCONDUCTORS - Abstract
We discuss a recent resonant ultrasound spectroscopy (RUS) study of YBa2Cu3O6+Δ, which infers a line of phase transitions bounding the pseudogap phase and argue that this scenario is not supported by thermodynamic evidence. We show that the anomalies in RUS, heat capacity, and thermal expansion at the superconducting transition temperatures agree well, but there are large discrepancies between RUS and thermodynamic measurements at T× where the pseudogap phase transitions are purported to occur. Moreover, the frequency and temperature dependence of the RUS data for the crystal with Δ = 0.98, interpreted in terms of critical slowing down near an electronic phase transition, is five orders of magnitude smaller than what is expected. For this crystal the RUS data near T× are more consistent with nonequilibrium effects, such as oxygen relaxation. [ABSTRACT FROM AUTHOR]
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- 2014
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4. Laser stabilization using saturated absorption in a cavity-QED system.
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Tieri, D. A., Cooper, J., Christensen, Bjarke T. R., Thomsen, J. W., and Holland, M. J.
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QUANTUM electrodynamics , *ABSORPTION , *KELVIN temperature scale , *DOPPLER effect , *OPTICAL properties - Abstract
We consider the phase stability of a local oscillator (or laser) locked to a cavity-QED system composed of atoms with an ultranarrow optical transition. The atoms are cooled to milli-Kelvin temperatures and then released into the optical cavity. Although the atomic motion introduces Doppler broadening, the standing-wave nature of the cavity causes saturated absorption features to appear, which are much narrower than the Doppler width. These features can be used to achieve an extremely high degree of phase stabilization, competitive with the current state of the art. Furthermore, the inhomogeneity introduced by finite atomic velocities can cause optical bistability to disappear, resulting in no regions of dynamic instability and thus enabling a new regime accessible to experiments where optimum stabilization may be achieved. [ABSTRACT FROM AUTHOR]
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- 2015
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5. Spin injection and transport in a solution-processed organic semiconductor at room temperature.
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Mooser, S., Cooper, J. F. K., Banger, K. K., Wunderlich, J., and Sirringhaus, H.
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ELECTRON transport , *SPINTRONICS , *SOLUTION (Chemistry) , *ORGANIC semiconductors , *TEMPERATURE effect , *PENTACENE , *SPIN valves , *CHLOROFORM - Abstract
Spin injection and transport in solution-processed 6,13-bis(triisopropylsilylethynyl)-pentacene (TIPS-pentacene) are investigated using vertical CoPt/TIPS-pentacene/AlOx/Co spin valve architectures. The morphology and the molecular orientation of TIPS-pentacene spin-coated from a chloroform solution as grown in the spin valve devices are characterized by means of atomic force microscopy and x-ray diffraction, where the π-π stacking is found to be in planes oriented parallel to the substrate plane on CoPt (not L10-ordered). The magnetization hysteresis loops recorded with a superconducting quanmm interference device show an individual switching of the magnetization of the two ferromagnetic layers. The antiparallel state of the relative orientation of CoPt and Co is achieved due to their different coercive fields. A spin valve effect is observed at room temperature. The scaling of the magnetoresistance (MR) with the bulk mobility of TIPS-pentacene as a function of temperature together with the dependence of the MR on the interlayer thickness clearly indicates spin injection and transport in TIPS-pentacene. From organic semiconductor-spacer thickness-dependent MR measurements, we estimate a spin relaxation length of TIPS-pentacene of λs = (24 ± 6) nm and a spin relaxation time of approximately τs = 3.5 μs at r = 300 K, taking the measured bulk mobility of holes into account. [ABSTRACT FROM AUTHOR]
- Published
- 2012
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6. Robust Quantum Enhanced Phase Estimation in a Multimode Interferometer.
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Cooper, J. J., Hallwood, D. W., Dunningham, J. A., and Brand, J.
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QUANTUM theory , *INTERFEROMETERS , *ATOMS , *ROTATIONAL motion , *FERMIONS , *INTERACTING boson models , *ESTIMATION theory - Abstract
By exploiting the correlation properties of ultracold atoms in a multimode interferometer, we show how quantum enhanced measurement precision can be achieved with strong robustness to particle loss. While the potential for enhanced measurement precision is limited for even moderate loss in two-mode schemes, multimode schemes can be more robust. A ring interferometer for sensing rotational motion with noninteracting fermionic atoms can realize an uncertainty scaling of 1 /(N√&eegr;) for N particles with a fraction &eegr; remaining after loss, which undercuts the shot-noise limit of two-mode interferometers. A second scheme with strongly interacting bosons achieves a comparable measurement precision and improved readout. [ABSTRACT FROM AUTHOR]
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- 2012
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7. Valency and spin states of substituent cations in Bi2.15Sr1.85CaCu2O8+δ.
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Benseman, T. M., Cooper, J. R., Zentile, C. L., Lemberger, L., and Balakrishnan, G.
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TEMPERATURE , *SUPERCONDUCTORS , *MAGNETICS , *IONIZATION (Atomic physics) , *ANISOTROPY , *CRYSTALS , *TRANSITION temperature - Abstract
We studied the valency and spin behavior of M = Mn, Fe, Co, Li, and Al in the high-temperature superconducting compound Bi2.15 Sr1.85Ca(Cu1-zMz)2O8+δ (Bi-2212) for small values of z. Mn, Fe, aud Co retain their magnetic moments, and our thermopower and magnetic susceptibility data imply ionization states Mn3+, Fe-2+, and Co2+, while Li and Al are accommodated in the charge reservoir layers. Single-crystal studies show that the susceptibility of Co2+ ions in Bi-2212 is strongly anisotropic, with a weak anisotropy detected for Mn3+ and none for Fe2+. Fits to a pseudogap formula for a pure Bi-2212 crystal suggest that the spin susceptibility of the host compound is more anisotropic than previously realized. Data in the superconducting state allow us to compare the pair-breaking properties of the different impurities. Several aspects of the data, including the stronger suppression of the superconducting transition temperature Tc by Co compared with Fe for underdoped and optimally doped samples, show that the d-level structure of the magnetic ions and multiorbital effects are important. We also find that the temperatures of the magnetization crossing points are equal to the low-field Tc values to within 1% or 2%. This agrees with a 2D thermodynamic fluctuation argument given by Junod et al. [ABSTRACT FROM AUTHOR]
- Published
- 2011
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8. Measuring a completely unknown phase with sub-shot-noise precision in the presence of loss.
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Gkortsilas, N., Cooper, J. J., and Dunningham, J. A.
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PHYSICAL measurements , *ELECTRONIC noise , *PHASE equilibrium , *QUANTUM entanglement , *BAYESIAN analysis , *QUANTUM theory - Abstract
We present a practical scheme for measuring completely unknown phases with a precision beyond the shot-noise limit even in the presence of loss. Our scheme consists of sending a sequence of unentangled particles and NOON states through an interferometer and analyzing the measurement outcomes using a Bayesian analysis. We compare our results with two recent schemes [L. Pezzé and A. Smerzi, Europhys. Lett. 78, 30004 (2007); B. L. Higgins et al., Nature (London) 450, 393 (2007)] that are closely related but operate in the lossless regime. We show that our technique outperforms the previous schemes when even a modest amount of loss is present and so may prove to be a valuable technique for making precision measurements beyond the classical limit in a range of practical scenarios. [ABSTRACT FROM AUTHOR]
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- 2012
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9. Unexpected structural and magnetic depth dependence of YIG thin films.
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Cooper, J. F. K., Kinane, C. J., Langridge, S., Ali, M., Hickey, B. J., Niizeki, T., Uchida, K., Saitoh, E., Ambaye, H., and Glavic, A.
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THIN films , *YTTRIUM aluminum garnet , *MAGNETIC fields - Abstract
We report measurements on yttrium iron garnet (YIG) thin films grown on both gadolinium gallium garnet (GGG) and yttrium aluminum garnet (YAG) substrates, with and without thin Pt top layers. We provide three principal results: the observation of an interfacial region at the Pt/YIG interface, we place a limit on the induced magnetism of the Pt layer, and confirm the existence of an interfacial layer at the GGG/YIG interface. Polarized neutron reflectometry (PNR) was used to give depth dependence of both the structure and magnetism of these structures. We find that a thin film of YIG on GGG is best described by three distinct layers: an interfacial layer near the GGG, around 5 nm thick and nonmagnetic, a magnetic "bulk" phase, and a nonmagnetic and compositionally distinct thin layer near the surface. We theorize that the bottom layer, which is independent of the film thickness, is caused by Gd diffusion. The top layer is likely to be extremely important in inverse spin Hall effect measurements, and is most likely Y2O3 or very similar. Magnetic sensitivity in the PNR to any induced moment in the Pt is increased by the existence of the Y2O3 layer; any moment is found to be less than 0.02μB/atom. [ABSTRACT FROM AUTHOR]
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- 2017
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10. Magnetic susceptibility of YBa2Cu3O6+x crystals: Unusual Curie behavior and small contributions from charge density waves.
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Kokanović, I. and Cooper, J. R.
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YTTRIUM compounds , *MAGNETIC susceptibility , *CHARGE density waves - Abstract
We report measurements of the magnetic susceptibility of twinned single crystals of YBa2Cu3O6+x from just above their superconducting transition temperatures to 300 K with magnetic fields of up to 5 T applied parallel and perpendicular to the CuO2 planes at seven values of x. Appropriate analysis allows the relatively small, but still important, Curie terms to be separated from other contributions to the susceptibility. Our data support a picture in which the Curie terms arise from oxygen disorder in the Cu-O chains. This agrees with published work on polycrystalline samples where the sample cooling rate was varied, but here we show that the Curie plots flatten out above 200 K. We identify small effects of charge density wave (CDW) instabilities in the temperature (T) derivative of the in-plane susceptibility dχab(T)/dT and discuss their x dependence. For x=0.67 we make a detailed comparison with published high energy x-ray diffraction data using a minimal model involving Fermi arcs, thereby obtaining values for the CDW energy gap and the Helmholtz free energy in a coherence volume. At 80 and 100 K the latter is comparable with, or smaller than, kBT, respectively, highlighting the probable importance of thermal fluctuations. We note that the effect of the Lorentz force on charge carriers in the Fermi arcs could provide a simple mechanism for enhancing the CDWs in high magnetic fields, as suggested by recent experiments. [ABSTRACT FROM AUTHOR]
- Published
- 2016
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11. Publisher's Note: Laser stabilization using saturated absorption in a cavity-QED system [Phys. Rev. A 92, 013817 (2015)].
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Tieri, D. A., Cooper, J., Christensen, Bjarke T. R., Thomsen, J. W., and Holland, M. J.
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QUANTUM electrodynamics , *LASERS , *ABSORPTION - Abstract
A correction to the article "Laser stabilization using saturated absorption in a cavity-QED system" is presented.
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- 2015
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12. Electronic specific heat of Ba1-xKxFe2As2 from 2 to 380 K.
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Storey, J. G., Loram, J. W., Cooper, J. R., Bukowski, Z., and Karpinski, J.
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SPECIFIC heat , *MAGNETIC fields , *RENORMALIZATION (Physics) , *SUPERCONDUCTING transitions , *FLUCTUATIONS (Physics) , *MEAN field theory , *FERMI surfaces - Abstract
Using a high-resolution differential technique we have determined the electronic specific heat coefficient γ(T)=Cel/T of Ba1-xKxFe2As2 with x=0 to 1.0, at temperatures (T) from 2 K to 380 K and in magnetic fields H=0 to 13 T. In the normal state γn(x,T) increases strongly with x at low temperature, compatible with a mass renormalization ~12 at x=1, and decreases weakly with x at high temperature. A superconducting transition is seen in all samples from x=0.2 to 1, with transition temperatures and condensation energies peaking sharply at x=0.4. Superconducting coherence lengths ξab~20 Å and ξc~3 Å are estimated from an analysis of Gaussian fluctuations. For many dopings we see features in the H and T dependencies of γs(T,H) in the superconducting state that suggest superconducting gaps in three distinct bands. A broad "knee" and a sharp mean-field-like peak are typical of two coupled gaps. However, several samples show a shoulder above the sharp peak with an abrupt onset at Tc,s and a T dependence γs(T)∝√1-T/Tc,s. We provide strong evidence that the shoulder is not due to doping inhomogeneity and suggest it is a distinct gap with an unconventional T dependence Δs(T)∝(1-T/Tc,s)0.75 near Tc,s. We estimate band fractions and T=0 gaps from three-band α-model fits to our data and compare the x dependencies of the band fractions with spectroscopic studies of the Fermi surface. [ABSTRACT FROM AUTHOR]
- Published
- 2013
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13. Magnetization of underdoped YBa2Cu3Oy above the irreversibility field.
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Jing Fei Yu, Ramshaw, B. J., Kokanović, I., Modic, K. A., Harrison, N., Day, James, Ruixing Liang, Hardy, W. N., Bonn, D. A., McCollam, A., Julian, S. R., and Cooper, J. R.
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MAGNETIZATION , *YTTRIUM barium copper oxide , *DIAMAGNETISM , *TORQUE , *SUPERCONDUCTIVITY , *CHARGE density waves - Abstract
Torque magnetization measurements on YBa2Cu3Oy (YBCO) at doping y=6.67 (p=0.12), in dc fields (B) up to 33 T and temperatures down to 4.5 K, show that weak diamagnetism persists above the extrapolated irreversibility field Hirr(T=0)≈24 T. The differential susceptibility dM/dB, however, is more rapidly suppressed for B≳16 T than expected from the properties of the low field superconducting state, and saturates at a low value for fields B≳24 T. In addition, torque measurements on a p=0.11 YBCO crystal in pulsed field up to 65 T and temperatures down to 8 K show similar behavior, with no additional features at higher fields. We offer two candidate scenarios to explain these observations: (a) superconductivity survives but is heavily suppressed at high field by competition with charge-density-wave (CDW) order; (b) static superconductivity disappears near 24 T and is followed by a region of fluctuating superconductivity, which causes dM/dB to saturate at high field. The diamagnetic signal observed above 50 T for the p=0.11 crystal at 40 K and below may be caused by changes in the normal state susceptibility rather than bulk or fluctuating superconductivity. There will be orbital (Landau) diamagnetism from electron pockets and possibly a reduction in spin susceptibility caused by the stronger three-dimensional ordered CDW. [ABSTRACT FROM AUTHOR]
- Published
- 2015
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14. Controlled suppression of superconductivity by the generation of polarized Cooper pairs in spin-valve structures.
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Flokstra, M. G., Cunningham, T. C., Kim, J., Satchell, N., Burnell, G., Curran, P. J., Bending, S. J., Kinane, C. J., Cooper, J. F. K., Langridge, S., Isidori, A., Pugach, N., Eschrig, M., and Lee, S. L.
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COOPER pair , *SPIN valves , *SUPERCONDUCTIVITY , *OSCILLATIONS , *TRANSITION temperature - Abstract
Transport measurements are presented on thin-film superconducting spin-valve systems, where the controlled noncollinear arrangement of twoferromagnetic Co layers can be used to influence the superconducting state of Nb. We observe a very clear oscillation of the superconducting transition temperature with the relative orientation of the twoferromagnetic layers. Our measurements allow us to distinguish between the competing influences of domain averaging, stray dipolar fields, and the formation of superconducting spin triplets. Domain averaging is shown to lead to a weak enhancement of transition temperature for the antiparallel configuration of exchange fields, while much larger changes are observed for other configurations, which can be attributed to drainage currents due to spin triplet formation. [ABSTRACT FROM AUTHOR]
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- 2015
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15. Comparative study of intersubband absorption in AlGaN/GaN and AHnN/GaN superlattices: Impact of material inhomogeneities.
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Edmunds, C., Tang, L., Cervantes, M., Shirazi-HD, M., Shao, J., Grier, A., Valavanis, A., Cooper, J. D., Li, D., Gardner, G., Zakharov, D. N., Ikonić, Z., Indjin, D., Harrison, P., Manfra, M. J., and Malis, O.
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SPECTRUM analysis , *SUPERLATTICES , *COMPARATIVE studies , *INHOMOGENEOUS materials , *NEAR infrared radiation , *ABSORPTION spectra , *TRANSMISSION electron microscopy - Abstract
We report a systematic and quantitative study of near-infrared intersubband absorption in strained AlGaN/GaN and lattice-matched AHnN/GaN superlattices grown by plasma-assisted molecular-beam epitaxy as a function of Si-doping profile with and without S doping. For AlGaN/GaN, we obtained good theoretical agreement with experimental measurements of transition energy, integrated absorbance and linewidth by considering many-body effects, interface roughness, and calculations of the transition lifetime that include dephasing. For the AHnN/GaN system, experimental measurements of the integrated absorbance due to the superlattice transitions produced values more than one order of magnitude lower than AlGaN/GaN heterostructures at similar doping levels. Furthermore, observed transition energies were roughly 150 meV higher than expected. The weak absorption and high transition energies measured in these structures is attributed to columnar alloy inhomogeneity in the AlInN barriers observed in high-angle annular dark-field scanning transmission electron microscopy. We simulated the effect of these inhomogeneities using three-dimensional band-structure calculations. The inhomogeneities were modeled as AlInN nanorods with radially varying In composition embedded in the barrier material of the superlattice. We show that inclusion of the nanorods leads to the depletion of the quantum wells (QWs) due to localization of charge carriers in high-in-containing regions. The higher energy of the intersubband transitions was attributed to the relatively uniform regions of the QWs surrounded by high Al (95%) composition barriers. The calculated transition energy assuming Al0.95ln0.05 N barriers was in good agreement with experimental results. [ABSTRACT FROM AUTHOR]
- Published
- 2013
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16. Diamagnetism of YBa2Cu3O6+x crystals above Tc: Evidence for Gaussian fluctuations.
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Kokanović, I., Hills, D. J., Sutherland, M. L., Liang, R., and Cooper, J. R.
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YTTRIUM barium copper oxide , *COPPER oxide superconductors , *SINGLE crystals , *DIAMAGNETISM , *INELASTIC scattering , *MAGNETIC transition temperature , *TORQUE - Abstract
The magnetization of three high-quality single crystals of YBa2Cu3O6+x, from slightly overdoped to heavily underdoped, has been measured using torque magnetometry. Striking effects in the angular dependence of the torque for the two underdoped crystals, a few degrees above the superconducting transition temperature (Tc), are described well by the theory of Gaussian superconducting fluctuations using a single adjustable parameter. The data at higher temperatures (T) are consistent with a strong cutoff in the fluctuations for T ≳ 1.1 Tc. Numerical estimates suggest that inelastic scattering could be responsible for this cutoff. [ABSTRACT FROM AUTHOR]
- Published
- 2013
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17. Evidence for Dirac nodes from quantum oscillations in SrFe2As2.
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Sutherland, Mike, Hills, D. J., Tan, B. S., Altarawneh, M. M., Harrison, N., Gillett, J., O'Farrell, E. C. T., Benseman, T. M., Kokanovic, I., Syers, P., Cooper, J. R., and Sebastian, Suchitra E.
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MAGNETIC fields , *SINGLE crystals , *SUPERCONDUCTING magnets , *CYCLOTRONS , *DIRAC function - Abstract
We present a detailed study of quantum oscillations in the antiferromagnetically ordered pnictide compound SrFe2As2 as the angle between the applied magnetic field and crystalline axes is varied. Our measurements were performed on high-quality single crystals in a superconducting magnet, and in pulsed magnetic fields up to 60 T allowing us to observe orbits from several small Fermi-surface pockets. We extract the cyclotron effective mass m* and frequency F for these orbits and track their values as the field is rotated away from the c axis. While a constant ratio of m*/F is expected for a parabolic band, we observe deviations from this behavior. We conclude that this observation points to orbits derived from a band with Dirac dispersion near the Fermi level. [ABSTRACT FROM AUTHOR]
- Published
- 2011
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18. Thickness-dependent magnetic properties of oxygen-deficient EuO.
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Barbagallo, M., Stollenwerk, T., Kroha, J., Steinke, N.-J., Hine, N. D. M., Cooper, J. F. K., Barnes, C. H. W., Ionescu, A., Monteiro, P. M. D. S., Kim, J.-Y., Ziebeck, K. R. A., Kinane, C. J., Dalgliesh, R. M., Charlton, T. R., and Langridge, S.
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THICKNESS measurement , *MAGNETIC properties of thin films , *REFLECTOMETER , *POLARIZATION (Nuclear physics) , *CURIE temperature , *SURFACE defects - Abstract
We have studied how the magnetic properties of oxygen-deficient EuO sputtered thin films vary as a function of thickness. The magnetic moment, measured by polarized neutron reflectometry, and the Curie temperature are found to decrease with reducing thickness. Our results indicate that these surface-induced effects are caused by the reduced number of nearest neighbors, band bending, and the partial depopulation of the 4f states of Eu. [ABSTRACT FROM AUTHOR]
- Published
- 2011
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19. Search for exotic spin-dependent couplings of the neutron with matter using spin-echo based neutron interferometry.
- Author
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Parnell, S. R., van Well, A. A., Plomp, J., Dalgliesh, R. M., Steinke, N.-J., Cooper, J. F. K., Geerits, N., Steffen, K. E., Snow, W. M., and de Haan, V. O.
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NEUTRONS , *INTERFEROMETRY , *NEUTRON spectrometers , *MATTER , *BOSONS - Abstract
Various theories beyond the Standard Model predict new particles with masses in the sub-eV range with very weak couplings to ordinary matter which can possess spin-dependent couplings to electrons and nucleons. We report null results of a search for possible exotic spin-dependent couplings of the neutron which could be induced by the exchange of light weakly coupled bosons or spin-gravity coupling conducted using a spin-echo neutron spectrometer. We constrain the products g²A and g A g V of the axial vector coupling of the neutron to the matter of the Earth through the exchange of a weakly coupled vector boson for force ranges between the metre scale and the radius of the Earth. We also constrain the constants in some theories of exotic spin-gravity couplings. [ABSTRACT FROM AUTHOR]
- Published
- 2020
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20. Supercooling of Atoms in an Optical Resonator.
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Minghui Xu, Jäger, Simon B., Schütz, S., Cooper, J., Morigi, Giovanna, and Holland, M. J.
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OPTICAL resonators , *ATOMS , *SUPERCOOLING - Abstract
We investigate laser cooling of an ensemble of atoms in an optical cavity. We demonstrate that when atomic dipoles are synchronized in the regime of steady-state superradiance, the motion of the atoms may be subject to a giant frictional force leading to potentially very low temperatures. The ultimate temperature limits are determined by a modified atomic linewidth, which can be orders of magnitude smaller than the cavity linewidth. The cooling rate is enhanced by the superradiant emission into the cavity mode allowing reasonable cooling rates even for dipolar transitions with ultranarrow linewidth. [ABSTRACT FROM AUTHOR]
- Published
- 2016
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21. First measurement of neutrino oscillation parameters using neutrinos and antineutrinos by NOvA.
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Acero MA, Adamson P, Aliaga L, Alion T, Allakhverdian V, Altakarli S, Anfimov N, Antoshkin A, Aurisano A, Back A, Backhouse C, Baird M, Balashov N, Baldi P, Bambah BA, Bashar S, Bays K, Bending S, Bernstein R, Bhatnagar V, Bhuyan B, Bian J, Blackburn T, Blair J, Booth AC, Bour P, Bromberg C, Buchanan N, Butkevich A, Calvez S, Campbell M, Carroll TJ, Catano-Mur E, Cedeno A, Childress S, Choudhary BC, Chowdhury B, Coan TE, Colo M, Cooper J, Corwin L, Cremonesi L, Davies GS, Derwent PF, Ding P, Djurcic Z, Doyle D, Dukes EC, Duyang H, Edayath S, Ehrlich R, Elkins M, Feldman GJ, Filip P, Flanagan W, Frank MJ, Gallagher HR, Gandrajula R, Gao F, Germani S, Giri A, Gomes RA, Goodman MC, Grichine V, Groh M, Group R, Guo B, Habig A, Hakl F, Hartnell J, Hatcher R, Hatzikoutelis A, Heller K, Hewes J, Himmel A, Holin A, Howard B, Huang J, Hylen J, Jediny F, Johnson C, Judah M, Kakorin I, Kalra D, Kaplan DM, Keloth R, Klimov O, Koerner LW, Kolupaeva L, Kotelnikov S, Kourbanis I, Kreymer A, Kulenberg C, Kumar A, Kuruppu CD, Kus V, Lackey T, Lang K, Lin S, Lokajicek M, Lozier J, Luchuk S, Maan K, Magill S, Mann WA, Marshak ML, Martinez-Casales M, Matveev V, Méndez DP, Messier MD, Meyer H, Miao T, Miller WH, Mishra SR, Mislivec A, Mohanta R, Moren A, Mualem L, Muether M, Mufson S, Mulder K, Murphy R, Musser J, Naples D, Nayak N, Nelson JK, Nichol R, Nikseresht G, Niner E, Norman A, Nosek T, Olshevskiy A, Olson T, Paley J, Patterson RB, Pawloski G, Pershey D, Petrova O, Petti R, Phan DD, Plunkett RK, Potukuchi B, Principato C, Psihas F, Radovic A, Raj V, Rameika RA, Rebel B, Rojas P, Ryabov V, Samoylov O, Sanchez MC, Sánchez Falero S, Seong IS, Shanahan P, Sheshukov A, Singh P, Singh V, Smith E, Smolik J, Snopok P, Solomey N, Song E, Sousa A, Soustruznik K, Strait M, Suter L, Sutton A, Talaga RL, Tapia Oregui B, Tas P, Thayyullathil RB, Thomas J, Tiras E, Torbunov D, Tripathi J, Tsaris A, Torun Y, Urheim J, Vahle P, Vasel J, Vinton L, Vokac P, Vrba T, Wallbank M, Wang B, Warburton TK, Wetstein M, While M, Whittington D, Wojcicki SG, Wolcott J, Yadav N, Yallappa Dombara A, Yonehara K, Yu S, Zadorozhnyy S, Zalesak J, Zamorano B, and Zwaska R
- Abstract
The NOvA experiment has seen a 4.4σ signal of ν[over ¯]_{e} appearance in a 2 GeV ν[over ¯]_{μ} beam at a distance of 810 km. Using 12.33×10^{20} protons on target delivered to the Fermilab NuMI neutrino beamline, the experiment recorded 27 ν[over ¯]_{μ}→ν[over ¯]_{e} candidates with a background of 10.3 and 102 ν[over ¯]_{μ}→ν[over ¯]_{μ} candidates. This new antineutrino data are combined with neutrino data to measure the parameters |Δm_{32}^{2}|=2.48_{-0.06}^{+0.11}×10^{-3} eV^{2}/c^{4} and sin^{2}θ_{23} in the ranges from (0.53-0.60) and (0.45-0.48) in the normal neutrino mass hierarchy. The data exclude most values near δ_{CP}=π/2 for the inverted mass hierarchy by more than 3σ and favor the normal neutrino mass hierarchy by 1.9σ and θ_{23} values in the upper octant by 1.6σ.
- Published
- 2019
- Full Text
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22. Dynamical Phase Transitions to Optomechanical Superradiance.
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Jäger SB, Cooper J, Holland MJ, and Morigi G
- Abstract
We theoretically analyze superradiant emission of light from an ultracold gas of bosonic atoms confined in a bad cavity. A metastable dipolar transition of the atoms couples to the cavity field and is incoherently pumped, and the mechanical effects of cavity-atom interactions tend to order the atoms in the periodic cavity potential. By means of a mean-field model we determine the conditions on the cavity parameters and pump rate that lead to the buildup of a stable macroscopic dipole emitting coherent light. We show that this occurs when the superradiant decay rate and the pump rate exceed threshold values of the order of the photon recoil energy. Above these thresholds superradiant emission is accompanied by the formation of stable matter-wave gratings that diffract the emitted photons. Outside of this regime, instead, the optomechanical coupling can give rise to dephasing or chaos, for which the emitted light is respectively incoherent or chaotic. These behaviors exhibit the features of a dynamical phase transitions and emerge from the interplay between global optomechanical interactions, quantum fluctuations, and noise.
- Published
- 2019
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23. Constraints on Oscillation Parameters from ν_{e} Appearance and ν_{μ} Disappearance in NOvA.
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Adamson P, Aliaga L, Ambrose D, Anfimov N, Antoshkin A, Arrieta-Diaz E, Augsten K, Aurisano A, Backhouse C, Baird M, Bambah BA, Bays K, Behera B, Bending S, Bernstein R, Bhatnagar V, Bhuyan B, Bian J, Blackburn T, Bolshakova A, Bromberg C, Brown J, Brunetti G, Buchanan N, Butkevich A, Bychkov V, Campbell M, Catano-Mur E, Childress S, Choudhary BC, Chowdhury B, Coan TE, Coelho JAB, Colo M, Cooper J, Corwin L, Cremonesi L, Cronin-Hennessy D, Davies GS, Davies JP, Derwent PF, Dharmapalan R, Ding P, Djurcic Z, Dukes EC, Duyang H, Edayath S, Ehrlich R, Feldman GJ, Frank MJ, Gabrielyan M, Gallagher HR, Germani S, Ghosh T, Giri A, Gomes RA, Goodman MC, Grichine V, Group R, Grover D, Guo B, Habig A, Hartnell J, Hatcher R, Hatzikoutelis A, Heller K, Himmel A, Holin A, Hylen J, Jediny F, Judah M, Kafka GK, Kalra D, Kasahara SMS, Kasetti S, Keloth R, Kolupaeva L, Kotelnikov S, Kourbanis I, Kreymer A, Kumar A, Kurbanov S, Lang K, Lee WM, Lin S, Liu J, Lokajicek M, Lozier J, Luchuk S, Maan K, Magill S, Mann WA, Marshak ML, Matera K, Matveev V, Méndez DP, Messier MD, Meyer H, Miao T, Miller WH, Mishra SR, Mohanta R, Moren A, Mualem L, Muether M, Mufson S, Murphy R, Musser J, Nelson JK, Nichol R, Niner E, Norman A, Nosek T, Oksuzian Y, Olshevskiy A, Olson T, Paley J, Pandey P, Patterson RB, Pawloski G, Pershey D, Petrova O, Petti R, Phan-Budd S, Plunkett RK, Poling R, Potukuchi B, Principato C, Psihas F, Radovic A, Rameika RA, Rebel B, Reed B, Rocco D, Rojas P, Ryabov V, Sachdev K, Sail P, Samoylov O, Sanchez MC, Schroeter R, Sepulveda-Quiroz J, Shanahan P, Sheshukov A, Singh J, Singh J, Singh P, Singh V, Smolik J, Solomey N, Song E, Sousa A, Soustruznik K, Strait M, Suter L, Talaga RL, Tamsett MC, Tas P, Thayyullathil RB, Thomas J, Tian X, Tognini SC, Tripathi J, Tsaris A, Urheim J, Vahle P, Vasel J, Vinton L, Vold A, Vrba T, Wang B, Wetstein M, Whittington D, Wojcicki SG, Wolcott J, Yadav N, Yang S, Zalesak J, Zamorano B, and Zwaska R
- Abstract
Results are reported from an improved measurement of ν_{μ}→ν_{e} transitions by the NOvA experiment. Using an exposure equivalent to 6.05×10^{20} protons on target, 33 ν_{e} candidates are observed with a background of 8.2±0.8 (syst.). Combined with the latest NOvA ν_{μ} disappearance data and external constraints from reactor experiments on sin^{2}2θ_{13}, the hypothesis of inverted mass hierarchy with θ_{23} in the lower octant is disfavored at greater than 93% C.L. for all values of δ_{CP}.
- Published
- 2017
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24. Measurement of the Neutrino Mixing Angle θ_{23} in NOvA.
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Adamson P, Aliaga L, Ambrose D, Anfimov N, Antoshkin A, Arrieta-Diaz E, Augsten K, Aurisano A, Backhouse C, Baird M, Bambah BA, Bays K, Behera B, Bending S, Bernstein R, Bhatnagar V, Bhuyan B, Bian J, Blackburn T, Bolshakova A, Bromberg C, Brown J, Brunetti G, Buchanan N, Butkevich A, Bychkov V, Campbell M, Catano-Mur E, Childress S, Choudhary BC, Chowdhury B, Coan TE, Coelho JAB, Colo M, Cooper J, Corwin L, Cremonesi L, Cronin-Hennessy D, Davies GS, Davies JP, Derwent PF, Desai S, Dharmapalan R, Ding P, Djurcic Z, Dukes EC, Duyang H, Edayath S, Ehrlich R, Feldman GJ, Frank MJ, Gabrielyan M, Gallagher HR, Germani S, Ghosh T, Giri A, Gomes RA, Goodman MC, Grichine V, Group R, Grover D, Guo B, Habig A, Hartnell J, Hatcher R, Hatzikoutelis A, Heller K, Himmel A, Holin A, Hylen J, Jediny F, Judah M, Kafka GK, Kalra D, Kasahara SMS, Kasetti S, Keloth R, Kolupaeva L, Kotelnikov S, Kourbanis I, Kreymer A, Kumar A, Kurbanov S, Lang K, Lee WM, Lin S, Liu J, Lokajicek M, Lozier J, Luchuk S, Maan K, Magill S, Mann WA, Marshak ML, Matera K, Matveev V, Méndez DP, Messier MD, Meyer H, Miao T, Miller WH, Mishra SR, Mohanta R, Moren A, Mualem L, Muether M, Mufson S, Murphy R, Musser J, Nelson JK, Nichol R, Niner E, Norman A, Nosek T, Oksuzian Y, Olshevskiy A, Olson T, Paley J, Pandey P, Patterson RB, Pawloski G, Pershey D, Petrova O, Petti R, Phan-Budd S, Plunkett RK, Poling R, Potukuchi B, Principato C, Psihas F, Radovic A, Rameika RA, Rebel B, Reed B, Rocco D, Rojas P, Ryabov V, Sachdev K, Sail P, Samoylov O, Sanchez MC, Schroeter R, Sepulveda-Quiroz J, Shanahan P, Sheshukov A, Singh J, Singh J, Singh P, Singh V, Smolik J, Solomey N, Song E, Sousa A, Soustruznik K, Strait M, Suter L, Talaga RL, Tamsett MC, Tas P, Thayyullathil RB, Thomas J, Tian X, Tognini SC, Tripathi J, Tsaris A, Urheim J, Vahle P, Vasel J, Vinton L, Vold A, Vrba T, Wang B, Wetstein M, Whittington D, Wojcicki SG, Wolcott J, Yadav N, Yang S, Zalesak J, Zamorano B, and Zwaska R
- Abstract
This Letter reports new results on muon neutrino disappearance from NOvA, using a 14 kton detector equivalent exposure of 6.05×10^{20} protons on target from the NuMI beam at the Fermi National Accelerator Laboratory. The measurement probes the muon-tau symmetry hypothesis that requires maximal θ_{23} mixing (θ_{23}=π/4). Assuming the normal mass hierarchy, we find Δm_{32}^{2}=(2.67±0.11)×10^{-3} eV^{2} and sin^{2}θ_{23} at the two statistically degenerate values 0.404_{-0.022}^{+0.030} and 0.624_{-0.030}^{+0.022}, both at the 68% confidence level. Our data disfavor the maximal mixing scenario with 2.6σ significance.
- Published
- 2017
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25. Supercooling of Atoms in an Optical Resonator.
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Xu M, Jäger SB, Schütz S, Cooper J, Morigi G, and Holland MJ
- Abstract
We investigate laser cooling of an ensemble of atoms in an optical cavity. We demonstrate that when atomic dipoles are synchronized in the regime of steady-state superradiance, the motion of the atoms may be subject to a giant frictional force leading to potentially very low temperatures. The ultimate temperature limits are determined by a modified atomic linewidth, which can be orders of magnitude smaller than the cavity linewidth. The cooling rate is enhanced by the superradiant emission into the cavity mode allowing reasonable cooling rates even for dipolar transitions with ultranarrow linewidth.
- Published
- 2016
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26. First Measurement of Electron Neutrino Appearance in NOvA.
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Adamson P, Ader C, Andrews M, Anfimov N, Anghel I, Arms K, Arrieta-Diaz E, Aurisano A, Ayres DS, Backhouse C, Baird M, Bambah BA, Bays K, Bernstein R, Betancourt M, Bhatnagar V, Bhuyan B, Bian J, Biery K, Blackburn T, Bocean V, Bogert D, Bolshakova A, Bowden M, Bower C, Broemmelsiek D, Bromberg C, Brunetti G, Bu X, Butkevich A, Capista D, Catano-Mur E, Chase TR, Childress S, Choudhary BC, Chowdhury B, Coan TE, Coelho JA, Colo M, Cooper J, Corwin L, Cronin-Hennessy D, Cunningham A, Davies GS, Davies JP, Del Tutto M, Derwent PF, Deepthi KN, Demuth D, Desai S, Deuerling G, Devan A, Dey J, Dharmapalan R, Ding P, Dixon S, Djurcic Z, Dukes EC, Duyang H, Ehrlich R, Feldman GJ, Felt N, Fenyves EJ, Flumerfelt E, Foulkes S, Frank MJ, Freeman W, Gabrielyan M, Gallagher HR, Gebhard M, Ghosh T, Gilbert W, Giri A, Goadhouse S, Gomes RA, Goodenough L, Goodman MC, Grichine V, Grossman N, Group R, Grudzinski J, Guarino V, Guo B, Habig A, Handler T, Hartnell J, Hatcher R, Hatzikoutelis A, Heller K, Howcroft C, Huang J, Huang X, Hylen J, Ishitsuka M, Jediny F, Jensen C, Jensen D, Johnson C, Jostlein H, Kafka GK, Kamyshkov Y, Kasahara SM, Kasetti S, Kephart K, Koizumi G, Kotelnikov S, Kourbanis I, Krahn Z, Kravtsov V, Kreymer A, Kulenberg Ch, Kumar A, Kutnink T, Kwarciancy R, Kwong J, Lang K, Lee A, Lee WM, Lee K, Lein S, Liu J, Lokajicek M, Lozier J, Lu Q, Lucas P, Luchuk S, Lukens P, Lukhanin G, Magill S, Maan K, Mann WA, Marshak ML, Martens M, Martincik J, Mason P, Matera K, Mathis M, Matveev V, Mayer N, McCluskey E, Mehdiyev R, Merritt H, Messier MD, Meyer H, Miao T, Michael D, Mikheyev SP, Miller WH, Mishra SR, Mohanta R, Moren A, Mualem L, Muether M, Mufson S, Musser J, Newman HB, Nelson JK, Niner E, Norman A, Nowak J, Oksuzian Y, Olshevskiy A, Oliver J, Olson T, Paley J, Pandey P, Para A, Patterson RB, Pawloski G, Pearson N, Perevalov D, Pershey D, Peterson E, Petti R, Phan-Budd S, Piccoli L, Pla-Dalmau A, Plunkett RK, Poling R, Potukuchi B, Psihas F, Pushka D, Qiu X, Raddatz N, Radovic A, Rameika RA, Ray R, Rebel B, Rechenmacher R, Reed B, Reilly R, Rocco D, Rodkin D, Ruddick K, Rusack R, Ryabov V, Sachdev K, Sahijpal S, Sahoo H, Samoylov O, Sanchez MC, Saoulidou N, Schlabach P, Schneps J, Schroeter R, Sepulveda-Quiroz J, Shanahan P, Sherwood B, Sheshukov A, Singh J, Singh V, Smith A, Smith D, Smolik J, Solomey N, Sotnikov A, Sousa A, Soustruznik K, Stenkin Y, Strait M, Suter L, Talaga RL, Tamsett MC, Tariq S, Tas P, Tesarek RJ, Thayyullathil RB, Thomsen K, Tian X, Tognini SC, Toner R, Trevor J, Tzanakos G, Urheim J, Vahle P, Valerio L, Vinton L, Vrba T, Waldron AV, Wang B, Wang Z, Weber A, Wehmann A, Whittington D, Wilcer N, Wildberger R, Wildman D, Williams K, Wojcicki SG, Wood K, Xiao M, Xin T, Yadav N, Yang S, Zadorozhnyy S, Zalesak J, Zamorano B, Zhao A, Zirnstein J, and Zwaska R
- Abstract
We report results from the first search for ν_{μ}→ν_{e} transitions by the NOvA experiment. In an exposure equivalent to 2.74×10^{20} protons on target in the upgraded NuMI beam at Fermilab, we observe 6 events in the Far Detector, compared to a background expectation of 0.99±0.11(syst) events based on the Near Detector measurement. A secondary analysis observes 11 events with a background of 1.07±0.14(syst). The 3.3σ excess of events observed in the primary analysis disfavors 0.1π<δ_{CP}<0.5π in the inverted mass hierarchy at the 90% C.L.
- Published
- 2016
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27. Observation of motion-dependent nonlinear dispersion with narrow-linewidth atoms in an optical cavity.
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Westergaard PG, Christensen BT, Tieri D, Matin R, Cooper J, Holland M, Ye J, and Thomsen JW
- Abstract
As an alternative to state-of-the-art laser frequency stabilization using ultrastable cavities, it has been proposed to exploit the nonlinear effects from coupling of atoms with a narrow transition to an optical cavity. Here, we have constructed such a system and observed nonlinear phase shifts of a narrow optical line by a strong coupling of a sample of strontium-88 atoms to an optical cavity. The sample temperature of a few mK provides a domain where the Doppler energy scale is several orders of magnitude larger than the narrow linewidth of the optical transition. This makes the system sensitive to velocity dependent multiphoton scattering events (Dopplerons) that affect the cavity field transmission and phase. By varying the number of atoms and the intracavity power, we systematically study this nonlinear phase signature which displays roughly the same features as for much lower temperature samples. This demonstration in a relatively simple system opens new possibilities for alternative routes to laser stabilization at the sub-100 mHz level and superradiant laser sources involving narrow-line atoms. The understanding of relevant motional effects obtained here has direct implications for other atomic clocks when used in relation to ultranarrow clock transitions.
- Published
- 2015
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28. Atomtronic circuits of diodes and transistors.
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Pepino RA, Cooper J, Anderson DZ, and Holland MJ
- Abstract
We illustrate that open quantum systems composed of neutral, ultracold atoms in one-dimensional optical lattices can exhibit behavior analogous to semiconductor electronic circuits. A correspondence is demonstrated for bosonic atoms, and the experimental requirements to realize these devices are established. The analysis follows from a derivation of a quantum master equation for this general class of open quantum systems.
- Published
- 2009
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29. Nernst effect measurements of epitaxial Y0.95Ca0.05Ba2(Cu1-xZnx)3Oy and Y0.9Ca0.1Ba2Cu3Oy superconducting films.
- Author
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Kokanović I, Cooper JR, and Matusiak M
- Abstract
We report Nernst effect data for crystalline films of Y0.95Ca0.05Ba2(Cu1-xZnx)3Oy (with x=0, 0.02, and 0.04) and Y0.9Ca0.1Ba2Cu3Oy grown by pulsed laser deposition. We show that our own results and published data for LSCO are consistent with the theory of Gaussian superconducting fluctuations. We also show that Zn doping increases the Nernst coefficient simply because it reduces the in-plane conductivity.
- Published
- 2009
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30. Comparison of Faxén's correction for a microsphere translating or rotating near a surface.
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Leach J, Mushfique H, Keen S, Di Leonardo R, Ruocco G, Cooper JM, and Padgett MJ
- Abstract
Boundary walls in microfluidic devices have a strong influence on the fluid flow and drag forces on moving objects. The Stokes drag force acting on a sphere translating in the fluid is increased by the presence of a neighboring wall by a factor given by Faxén's correction. A similar increase in the rotational drag is expected when spinning close to a wall. We use optical tweezers to confirm the translational drag correction and report the hitherto unmeasured rotational equivalent. We find that the corrections for the rotational motion is only required for particle-wall separations an order of magnitude shorter than that for the translational cases. These results are particularly significant in the use of optical tweezers for measuring viscosity on a picolitre scale.
- Published
- 2009
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31. Quantum oscillations in the underdoped cuprate YBa2Cu4O8.
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Yelland EA, Singleton J, Mielke CH, Harrison N, Balakirev FF, Dabrowski B, and Cooper JR
- Abstract
We report the observation of quantum oscillations in the underdoped cuprate superconductor YBa2Cu4O8 using a tunnel-diode oscillator technique in pulsed magnetic fields up to 85 T. There is a clear signal, periodic in inverse field, with frequency 660+/-15 T and possible evidence for the presence of two components of slightly different frequency. The quasiparticle mass is m(*)=3.0+/-0.3m(e). In conjunction with the results of Doiron-Leyraud et al. for YBa2Cu3O6.5, the present measurements suggest that Fermi surface pockets are a general feature of underdoped copper oxide planes and provide information about the doping dependence of the Fermi surface.
- Published
- 2008
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32. Multipoint holographic optical velocimetry in microfluidic systems.
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Di Leonardo R, Leach J, Mushfique H, Cooper JM, Ruocco G, and Padgett MJ
- Abstract
We show how holographic optical trapping can be used for the multipoint measurement of fluid flow in microscopic geometries. An array of microprobes can be simultaneously trapped and used to map out the fluid flow in a microfluidic device. The optical traps are alternately turned on and off such that the probe particles are displaced by the flow of the surrounding fluid and then retrapped. The particles' displacements are monitored by digital video microscopy and directly converted into velocity field values. This technique enables the measurement of a two-dimensional flow field at points arbitrarily distributed in a three-dimensional volume. The validity of the technique is demonstrated for the case of the flow around a spinning sphere and the flow at the outlet of a microchannel.
- Published
- 2006
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33. Isotope effect in the superfluid density of high-temperature superconducting cuprates: stripes, pseudogap, and impurities.
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Tallon JL, Islam RS, Storey J, Williams GV, and Cooper JR
- Abstract
Underdoped cuprates exhibit a normal-state pseudogap, and their spins and doped carriers tend to spatially separate into 1D or 2D stripes. Some view these as central to superconductivity and others as peripheral and merely competing. Using La(2-x)Sr(x)Cu(1-y)Zn(y)O4 we show that an oxygen isotope effect in Tc and in the superfluid density can be used to distinguish between the roles of stripes and pseudogap and also to detect the presence of impurity scattering. We conclude that stripes and pseudogap are distinct, and both compete and coexist with superconductivity.
- Published
- 2005
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34. Determination of the Fermi surface of MgB2 by the de Haas-van Alphen effect.
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Carrington A, Meeson PJ, Cooper JR, Balicas L, Hussey NE, Yelland EA, Lee S, Yamamoto A, Tajima S, Kazakov SM, and Karpinski J
- Abstract
We report measurements of the de Haas-van Alphen (dHvA) effect for single crystals of MgB2, in magnetic fields up to 32 T. In contrast to our earlier work, dHvA orbits from all four sheets of the Fermi surface were detected. Our results are in good overall agreement with calculations of the electronic structure and the electron-phonon mass enhancements of the various orbits, but there are some small quantitative discrepancies. In particular, systematic differences in the relative volumes of the Fermi-surface sheets and the magnitudes of the electron-phonon coupling constants could be large enough to affect detailed calculations of T(c) and other superconducting properties.
- Published
- 2003
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35. B(E2) values in 150Nd and the critical point symmetry X(5).
- Author
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Krücken R, Albanna B, Bialik C, Casten RF, Cooper JR, Dewald A, Zamfir NV, Barton CJ, Beausang CW, Caprio MA, Hecht AA, Klug T, Novak JR, Pietralla N, and Von Brentano P
- Abstract
Lifetimes of states in 150Nd were measured using the recoil distance method following Coulomb excitation of 150Nd by a 132 MeV 32S beam. The experiment was performed at the Yale Tandem accelerator, employing the SPEEDY gamma-ray detector array and the New Yale Plunger Device. Reduced transition probabilities in 150Nd are compared to the predictions of the critical point symmetry X(5) of the phase/shape transition that occurs for the N = 90 rare earth isotones. Very good agreement was observed between the parameter-free (apart from scale) X(5) predictions and the low-spin level scheme of 150Nd, revealing this as the best case thus far for the realization of the X(5) symmetry.
- Published
- 2002
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36. de Haas-van Alphen effect in single crystal MgB2.
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Yelland EA, Cooper JR, Carrington A, Hussey NE, Meeson PJ, Lee S, Yamamoto A, and Tajima S
- Abstract
We report observations of quantum oscillations in single crystals of the high temperature superconductor MgB2. Three de Haas-van Alphen frequencies are clearly resolved. Comparison with band structure calculations strongly suggests that two of these come from a single warped Fermi surface tube along the c direction, and that the third arises from cylindrical sections of an in-plane honeycomb network. The measured values of the effective mass range from (0.44-0.68)m(e). By comparing these to calculated band masses, we find that the electron-phonon coupling strength lambda is a factor of approximately 3 larger for the c-axis tube orbits than for the in-plane network orbit, in accord with recent microscopic calculations.
- Published
- 2002
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37. Crossing of shears bands in (197)Pb: B(M1) values and semiclassical description.
- Author
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Cooper JR, Krücken R, Beausang CW, Novak JR, Dewald A, Klug T, Kemper G, von Brentano P, Carpenter MP, Janssens RV, Lister CJ, and Wiedenhöver I
- Abstract
Subpicosecond lifetimes of states in shears band 1 in (197)Pb were measured by means of the recoil distance method employing Gammasphere and the New Yale Plunger Device. The extracted reduced matrix elements, B(M1), show a clear sensitivity to the crossing of different shears configurations reflecting the closing and reopening of the shears blades. The energies and B(M1) values in the band crossing region are successfully described in the framework of the semiclassical model of the shears bands. The relevance of core rotation contributions are shown. The results point to the existence of shears states with an angular momentum coupling angle larger than 90 degrees.
- Published
- 2001
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38. Evolution of fractal patterns during a classical-quantum transition.
- Author
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Micolich AP, Taylor RP, Davies AG, Bird JP, Newbury R, Fromhold TM, Ehlert A, Linke H, Macks LD, Tribe WR, Linfield EH, Ritchie DA, Cooper J, Aoyagi Y, and Wilkinson PB
- Abstract
We investigate how fractals evolve into nonfractal behavior as the generation process is gradually suppressed. Fractals observed in the conductance of semiconductor billiards are of particular interest because the generation process is semiclassical and can be suppressed by transitions towards either fully classical or fully quantum-mechanical conduction. Investigating a range of billiards, we identify a "universal" behavior in the changeover from fractal to nonfractal conductance, which is described by a smooth evolution rather than deterioration in the fractal scaling properties.
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- 2001
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39. Measurement of J/psi and psi(2S) polarization in pp collisions at sqrt[s] = 1.8 TeV.
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Affolder T, Akimoto H, Akopian A, Albrow MG, Amaral P, Amendolia SR, Amidei D, Anikeev K, Antos J, Apollinari G, Arisawa T, Asakawa T, Ashmanskas W, Atac M, Azfar F, Azzi-Bacchetta P, Bacchetta N, Bailey MW, Bailey S, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Barone M, Bauer G, Bedeschi F, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Berryhill J, Bevensee B, Bhatti A, Binkley M, Bisello D, Blair RE, Blocker C, Bloom K, Blumenfeld B, Blusk SR, Bocci A, Bodek A, Bokhari W, Bolla G, Bonushkin Y, Bortoletto D, Boudreau J, Brandl A, van den Brink S, Bromberg C, Brozovic M, Bruner N, Buckley-Geer E, Budagov J, Budd HS, Burkett K, Busetto G, Byon-Wagner A, Byrum KL, Calafiura P, Campbell M, Carithers W, Carlson J, Carlsmith D, Cassada J, Castro A, Cauz D, Cerri A, Chan AW, Chang PS, Chang PT, Chapman J, Chen C, Chen YC, Cheng MT, Chertok M, Chiarelli G, Chirikov-Zorin I, Chlachidze G, Chlebana F, Christofek L, Chu ML, Ciobanu CI, Clark AG, Connolly A, Conway J, Cooper J, Cordelli M, Cranshaw J, Cronin-Hennessy D, Cropp R, Culbertson R, Dagenhart D, DeJongh F, Dell'Agnello S, Dell'Orso M, Demina R, Demortier L, Deninno M, Derwent PF, Devlin T, Dittmann JR, Donati S, Done J, Dorigo T, Eddy N, Einsweiler K, Elias JE, Engels E Jr, Erdmann W, Errede D, Errede S, Fan Q, Feild RG, Ferretti C, Field RD, Fiori I, Flaugher B, Foster GW, Franklin M, Freeman J, Friedman J, Fukui Y, Furic I, Galeotti S, Gallinaro M, Gao T, Garcia-Sciveres M, Garfinkel AF, Gatti P, Gay C, Geer S, Gerdes DW, Giannetti P, Giromini P, Glagolev V, Gold M, Goldstein J, Gordon A, Goshaw AT, Gotra Y, Goulianos K, Green C, Groer L, Grosso-Pilcher C, Guenther M, Guillian G, Guimaraes da Costa J, Guo RS, Haas RM, Haber C, Hafen E, Hahn SR, Hall C, Handa T, Handler R, Hao W, Happacher F, Hara K, Hardman AD, Harris RM, Hartmann F, Hatakeyama K, Hauser J, Heinrich J, Heiss A, Herndon M, Hinrichsen B, Hoffman KD, Holck C, Hollebeek R, Holloway L, Hughes R, Huston J, Huth J, Ikeda H, Incandela J, Introzzi G, Iwai J, Iwata Y, James E, Jensen H, Jones M, Joshi U, Kambara H, Kamon T, Kaneko T, Karr K, Kasha H, Kato Y, Keaffaber TA, Kelley K, Kelly M, Kennedy RD, Kephart R, Khazins D, Kikuchi T, Kilminster B, Kirby M, Kirk M, Kim BJ, Kim DH, Kim HS, Kim MJ, Kim SH, Kim YK, Kirsch L, Klimenko S, Koehn P, Köngeter A, Kondo K, Konigsberg J, Kordas K, Korn A, Korytov A, Kovacs E, Kroll J, Kruse M, Kuhlmann SE, Kurino K, Kuwabara T, Laasanen AT, Lai N, Lami S, Lammel S, Lamoureux JI, Lancaster M, Latino G, LeCompte T, Lee AM 4th, Lee K, Leone S, Lewis JD, Lindgren M, Liss TM, Liu JB, Liu YC, Lockyer N, Loken J, Loreti M, Lucchesi D, Lukens P, Lusin S, Lyons L, LysV J, Madrak R, Maeshima K, Maksimovic P, Malferrari L, Mangano M, Mariotti M, Martignon G, Martin A, Matthews JA, Mayer J, Mazzanti P, McFarland KS, McIntyre P, McKigney E, Menguzzato M, Menzione A, Mesropian C, Miao T, Miller R, Miller JS, Minato H, Miscetti S, Mishina M, Mitselmakher G, Moggi N, Moore E, Moore R, Morita Y, Mulhearn M, Mukherjee A, Muller T, Munar A, Murat P, Murgia S, Musy M, Nachtman J, Nahn S, Nakada H, Nakaya T, Nakano I, Nelson C, Neuberger D, Newman-Holmes C, Ngan CY, Nicolaidi P, Niu H, Nodulman L, Nomerotski A, Oh SH, Ohmoto T, Ohsugi T, Oishi R, Okusawa T, Olsen J, Orejudos W, Pagliarone C, Palmonari F, Paoletti R, Papadimitriou V, Pappas SP, Partos D, Patrick J, Pauletta G, Paulini M, Paus C, Pescara L, Phillips TJ, Piacentino G, Pitts KT, Plunkett R, Pompos A, Pondrom L, Pope G, Popovic M, Prokoshin F, Proudfoot J, Ptohos F, Pukhov O, Punzi G, Ragan K, Rakitine A, Reher D, Reichold A, Riegler W, Ribon A, Rimondi F, Ristori L, Robertson WJ, Robinson A, Rodrigo T, Rolli S, Rosenson L, Roser R, Rossin R, Safonov A, Sakumoto WK, Saltzberg D, Sansoni A, Santi L, Sato H, Savard P, Schlabach P, Schmidt EE, Schmidt MP, Schmitt M, Scodellaro L, Scott A, Scribano A, Segler S, Seidel S, Seiya Y, Semenov A, Semeria F, Shah T, Shapiro MD, Shepard PF, Shibayama T, Shimojima M, Shochet M, Siegrist J, Signorelli G, Sill A, Sinervo P, Singh P, Slaughter AJ, Sliwa K, Smith C, Snider FD, Solodsky A, Spalding J, Speer T, Sphicas P, Spinella F, Spiropulu M, Spiegel L, Steele J, Stefanini A, Strologas J, Strumia F, Stuart D, Sumorok K, Suzuki T, Takano T, Takashima R, Takikawa K, Tamburello P, Tanaka M, Tannenbaum B, Taylor W, Tecchio M, Teng PK, Terashi K, Tether S, Theriot D, Thurman-Keup R, Tipton P, Tkaczyk S, Tollefson K, Tollestrup A, Toyoda H, Trischuk W, de Troconiz JF, Tseng J, Turini N, Ukegawa F, Vaiciulis T, Valls J, Vejcik S 3rd, Velev G, Vidal R, Vilar R, Volobouev I, Vucinic D, Wagner RG, Wagner RL, Wahl J, Wallace NB, Walsh AM, Wang C, Wang CH, Wang MJ, Watanabe T, Waters D, Watts T, Webb R, Wenzel H, Wester WC 3rd, Wicklund AB, Wicklund E, Williams HH, Wilson P, Winer BL, Winn D, Wolbers S, Wolinski D, Wolinski J, Wolinski S, Worm S, Wu X, Wyss J, Yagil A, Yao W, Yeh GP, Yeh P, Yoh J, Yosef C, Yoshida T, Yu I, Yu S, Yu Z, Zanetti A, Zetti F, and Zucchelli S
- Abstract
We have measured the polarization of J/psi and psi(2S) mesons produced in pp collisions at sqrt[s] = 1.8 TeV, using data collected at the Collider Detector at Fermilab during 1992-1995. The polarization of promptly produced J/psi [psi(2S)] mesons is isolated from those produced in B-hadron decay, and measured over the kinematic range 4 [5.5]
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- 2000
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40. Search for a W' boson via the decay mode W'-->munumu in 1.8 TeV pp collisions.
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Abe F, Akimoto H, Akopian A, Albrow MG, Amendolia SR, Amidei D, Antos J, Aota S, Apollinari G, Arisawa T, Asakawa T, Ashmanskas W, Atac M, Azzi-Bacchetta P, Bacchetta N, Bagdasarov S, Bailey MW, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Barone M, Bauer G, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Berryhill J, Bertolucci S, Bettelli S, Bevensee B, Bhatti A, Biery K, Bigongiari C, Binkley M, Bisello D, Blair RE, Blocker C, Bloom K, Blusk S, Bodek A, Bokhari W, Bolla G, Bonushkin Y, Bortoletto D, Boudreau J, Brandl A, Breccia L, Bromberg C, Bruner N, Brunetti R, Buckley-Geer E, Budd HS, Burkett K, Busetto G, Byon-Wagner A, Byrum KL, Campbell M, Caner A, Carithers W, Carlsmith D, Cassada J, Castro A, Cauz D, Cerri A, Chang PS, Chang PT, Chao HY, Chapman J, Cheng MT, Chertok M, Chiarelli G, Chiou CN, Chlebana F, Christofek L, Chu ML, Cihangir S, Clark AG, Cobal M, Cocca E, Contreras M, Conway J, Cooper J, Cordelli M, Costanzo D, Couyoumtzelis C, Cronin-Hennessy D, Cropp R, Culbertson R, Dagenhart D, Daniels T, DeJongh F, Dell'Agnello S, Dell'Orso M, Demina R, Demortier L, Dennino M, Derwent PF, Devlin T, Dittmann JR, Donati S, Done J, Dorigo T, Eddy N, Einsweiler K, Elias JE, Ely R, Engels E Jr, Erdmann W, Errede D, Errede S, Fan Q, Feild RG, Feng Z, Ferretti C, Fiori I, Flaugher B, Foster GW, Franklin M, Freeman J, Friedman J, Frisch H, Fukui Y, Gadomski S, Galeotti S, Gallinaro M, Ganel O, Garcia-Sciveres M, Garfinkel AF, Gay C, Geer S, Gerdes DW, Giannetti P, Giokaris N, Giromini P, Giusti G, Gold M, Gordon A, Goshaw AT, Gotra Y, Goulianos K, Grassmann H, Green C, Groer L, Grosso-Pilcher C, Guillian G, Guimaraes da Costa J, Guo RS, Haber C, Hafen E, Hahn SR, Hamilton R, Handa T, Handler R, Hao W, Happacher F, Hara K, Hardman AD, Harris RM, Hartmann F, Hauser J, Hayashi E, Heinrich J, Heiss A, Hinrichsen B, Hoffman KD, Holck C, Hollebeek R, Holloway L, Huang Z, Huffman BT, Hughes R, Huston J, Huth J, Ikeda H, Incagli M, Incandela J, Introzzi G, Iwai J, Iwata Y, James E, Jensen H, Joshi U, Kajfasz E, Kambara H, Kamon T, Kaneko T, Karr K, Kasha H, Kato Y, Keaffaber TA, Kelley K, Kelly M, Kennedy RD, Kephart R, Kestenbaum D, Khazins D, Kikuchi T, Kirk M, Kim BJ, Kim HS, Kim SH, Kim YK, Kirsch L, Klimenko S, Knoblauch D, Koehn P, Köngeter A, Kondo K, Konigsberg J, Kordas K, Korytov A, Kovacs E, Kowald W, Kroll J, Kruse M, Kuhlmann SE, Kuns E, Kurino K, Kuwabara T, Laasanen AT, Lami S, Lammel S, Lamoureux JI, Lancaster M, Lanzoni M, Latino G, LeCompte T, Lee AM 4th, Leone S, Lewis JD, Lindgren M, Liss TM, Liu JB, Liu YC, Lockyer N, Long O, Loreti M, Lucchesi D, Lukens P, Lusin S, Lys J, Maeshima K, Maksimovic P, Mangano M, Mariotti M, Marriner JP, Martignon G, Martin A, Matthews JA, Mazzanti P, McFarland K, McIntyre P, Melese P, Menguzzato M, Menzione A, Meschi E, Metzler S, Miao C, Miao T, Michail G, Miller R, Minato H, Miscetti S, Mishina M, Miyashita S, Moggi N, Moore E, Morita Y, Mukherjee A, Muller T, Munar A, Murat P, Murgia S, Musy M, Nakada H, Nakaya T, Nakano I, Nelson C, Neuberger D, Newman-Holmes C, Ngan CY, Niu H, Nodulman L, Nomerotski A, Oh SH, Ohmoto T, Ohsugi T, Oishi R, Okabe M, Okusawa T, Olsen J, Pagliarone C, Paoletti R, Papadimitriou V, Pappas SP, Parashar N, Parri A, Partos D, Patrick J, Pauletta G, Paulini M, Perazzo A, Pescara L, Peters MD, Phillips TJ, Piacentino G, Pillai M, Pitts KT, Plunkett R, Pompos A, Pondrom L, Proudfoot J, Ptohos F, Punzi G, Ragan K, Reher D, Ribon A, Rimondi F, Ristori L, Robertson WJ, Robinson A, Rodrigo T, Rolli S, Rosenson L, Roser R, Saab T, Sakumoto WK, Saltzberg D, Sansoni A, Santi L, Sato H, Savard P, Schlabach P, Schmidt EE, Schmidt MP, Scott A, Scribano A, Segler S, Seidel S, Seiya Y, Semeria F, Shah T, Shapiro MD, Shaw NM, Shepard PF, Shibayama T, Shimojima M, Shochet M, Siegrist J, Sill A, Sinervo P, Singh P, Sliwa K, Smith C, Snider FD, Spalding J, Speer T, Sphicas P, Spinella F, Spiropulu M, Spiegel L, Stanco L, Steele J, Stefanini A, Ströhmer R, Strologas J, Strumia F, Stuart D, Sumorok K, Suzuki J, Suzuki T, Takahashi T, Takano T, Takashima R, Takikawa K, Tanaka M, Tannenbaum B, Tartarelli F, Taylor W, Tecchio M, Teng PK, Teramoto Y, Terashi K, Tether S, Theriot D, Thomas TL, Thurman-Keup R, Timko M, Tipton P, Titov A, Tkaczyk S, Toback D, Tollefson K, Tollestrup A, Toyoda H, Trischuk W, de Troconiz JF, Truitt S, Tseng J, Turini N, Uchida T, Ukegawa F, Valls J, van Den Brink SC, Vejcik S 3rd, Velev G, Vidal R, Vilar R, Vologouev I, Vucinic D, Wagner RG, Wagner RL, Wahl J, Wallace NB, Walsh AM, Wang C, Wang CH, Wang MJ, Warburton A, Watanabe T, Watts T, Webb R, Wei C, Wenzel H, Wester WC 3rd, Wicklund AB, Wicklund E, Wilkinson R, Williams HH, Wilson P, Winer BL, Winn D, Wolinski D, Wolinski J, Worm S, Wu X, Wyss J, Yagil S, Yao W, Yasuoka K, Yeh GP, Yeh P, Yoh J, Yosef C, Yoshida T, Yu I, Zanetti A, Zetti F, and Zucchelli S
- Abstract
We report the results of a search for a W' boson produced in pp collisions at a center-of-mass energy of 1.8 TeV using a 107 pb-1 data sample recorded by the Collider Detector at Fermilab. We consider the decay channel W'-->&munumu and search for anomalous production of high transverse mass munumu lepton pairs. We observe no excess of events above background and set limits on the rate of W' boson production and decay relative to standard model W boson production and decay using a fit of the transverse mass distribution observed. If we assume standard model strength couplings of the W' boson to quark and lepton pairs, we exclude a W' boson with invariant mass less than 660 GeV/c2 at 95% confidence level.
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- 2000
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41. Search for scalar top and scalar bottom quarks in pp collisions at square root s=1.8 TeV.
- Author
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Affolder T, Akimoto H, Akopian A, Albrow MG, Amaral P, Amendolia SR, Amidei D, Anikeev K, Antos J, Apollinari G, Arisawa T, Asakawa T, Ashmanskas W, Atac M, Azfar F, Azzi-Bacchetta P, Bacchetta N, Bailey MW, Bailey S, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Barone M, Bauer G, Bedeschi F, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Berryhill J, Bertolucci S, Bevensee B, Bhatti A, Bigongiari C, Binkley M, Bisello D, Blair RE, Blocker C, Bloom K, Blumenfeld B, Blusk BS, Bocci A, Bodek A, Bokhari W, Bolla G, Bonushkin Y, Bortoletto D, Boudreau J, Brandl A, van den Brink S, Bromberg C, Brozovic M, Bruner N, Buckley-Geer E, Budagov J, Budd HS, Burkett K, Busetto G, Byon-Wagner A, Byrum KL, Campbell M, Caner A, Carithers W, Carlson J, Carlsmith D, Cassada J, Castro A, Cauz D, Cerri A, Chan AW, Chang PS, Chang PT, Chapman J, Chen C, Chen YC, Cheng MT, Chertok M, Chiarelli G, Chirikov-Zorin I, Chlachidze G, Chlebana F, Christofek L, Chu ML, Cihangir S, Ciobanu CI, Clark AG, Cobal M, Cocca E, Connolly A, Conway J, Cooper J, Cordelli M, Costanzo D, Cranshaw J, Cronin-Hennessy D, Cropp R, Culbertson R, Dagenhart D, DeJongh F, Dell'Agnello S, Dell'Orso M, Demina R, Demortier L, Deninno M, Derwent PF, Devlin T, Dittmann JR, Donati S, Done J, Dorigo T 3rd, Eddy N, Einsweiler K, Elias JE, Engels E Jr, Erdmann W, Errede D, Errede S, Fan Q, Feild RG, Ferretti C, Fiori I, Flaugher B, Foster GW, Franklin M, Freeman J, Friedman J, Fukui Y, Galeotti S, Gallinaro M, Gao T, Garcia-Sciveres M, Garfinkel AF, Gatti P, Gay C, Geer S, Gerdes DW, Giannetti P, Giromini P, Glagolev V, Gold M, Goldstein J, Gordon A, Goshaw AT, Gorta Y, Goulianos K, Grassmann H, Green C, Groer L, Grosso-Pilcher C, Guenther M, Guillian G, Guimaraes da Costa J, Guo RS, Haber C, Hafen E, Hahn SR, Hall C, Handa T, Handler R, Hao W, Happacher F, Hara K, Hardman AD, Harris RM, Hartmann F, Hatakeyama K, Hauser J, Heinrich J, Heiss A, Hinrichsen B, Hoffman KD, Holck C, Hollebeek R, Holloway L, Hughes R, Huston J, Huth J, Ikeda H, Incagli M, Incandela J, Introzzi G, Iwai J, Iwata Y, James E, Jensen H, Jones M, Joshi U, Kambara H, Kamon T, Kaneko T, Karr K, Kasha H, Kato Y, Keaffaber TA, Kelley K, Kelly M, Kennedy RD, Kephart R, Khazins D, Kikuchi T, Kirk M, Kim BJ, Kim HS, Kim MJ, Kim SH, Kim YK, Kirsch L, Klimenko S, Knoblauch D, Koehn P, Köngeter A, Kondo K, Konigsberg J, Kordas K, Korn A, Korytov A, Kovacs E, Kroll J, Kruse M, Kuhlmann SE, Kurino K, Kuwabara T, Laasanen AT, Lai N, Lami S, Lammel S, Lamoureux JI, Lancaster M, Latino G, LeCompte T, Lee AM 4th, Leone S, Lewis JD, Lindgren M, Liss TM, Liu JB, Liu YC, Lockyer N, Loken J, Loreti M, Lucchesi D, Lukens P, Lusin S, Lyons L, Lys J, Madrak R, Maeshima K, Maksimovic P, Malferrari L, Mangano M, Mariotti M, Martignon G, Martin A, Matthews JA, Mazzanti P, McFarland KS, McIntyre P, McKigney E, Menguzzato M, Mezione A, Meschi E, Mesropian C, Miao C, Miao T, Miller R, Miller JS, Minato H, Miscetti S, Mishina M, Moggi N, Moore E, Moore R, Morita Y, Mukherjee A, Muller T, Munar A, Murat P, Murgia S, Musy M, Nachtman J, Nahn S, Nakada H, Nakaya T, Nakano I, Nelson C, Neuberger D, Newman-Holmes C, Ngan CY, Nicolaidi P, Niu H, Nodulman L, Nomerotski A, Oh SH, Ohmoto T, Ohsugi T, Oishi R, Okusawa T, Olsen J, Pagliarone C, Palmonari F, Paoletti R, Papadimitriou V, Pappas SP, Parri A, Partos D, Patrick J, Pauletta G, Paulini M, Paus C, Perazzo A, Pescara L, Phillips TJ, Piacentino G, Pitts KT, Plunkett R, Pompos A, Pondrom L, Pope G, Popovic M, Prokoshin F, Proudfoot J, Ptohos F, Punzi G, Ragan K, Rakitine A, Reher D, Reichold A, Riegler W, Ribon A, Rimondi F, Ristori L, Robertson WJ, Robinson A, Rodrigo T, Rolli S, Rosenson L, Roser R, Rossin R, Sakumoto WK, Saltzberg D, Sansoni A, Santi L, Sato H, Savard P, Schlabach P, Schmidt EE, Schmidt MP, Schmitt M, Scodellaro L, Scott A, Scribano A, Segler S, Seidel S, Seiya Y, Semenov A, Semeria F, Shah T, Shapiro MD, Shepard PF, Shibayama T, Shimojima M, Shochet M, Siegrist J, Signorelli G, Sill A, Sinervo P, Singh P, Slaughter AJ, Sliwa K, Smith C, Snider FD, Solodsky A, Spalding J, Speer T, Sphicas P, Spinella F, Spiropulu M, Spiegel L, Stanco L, Steele J, Stefanini A, Strologas J, Strumia F, Stuart D, Sumorok K, Suzuki T, Takashima R, Takikawa K, Tanaka M, Takano T, Tannenbaum B, Taylor W, Tecchio M, Teng PK, Terashi K, Tether S, Theriot D, Thurman-Keup R, Tipton P, Tkaczyk S, Tollefson K, Tollestrup A, Toyoda H, Trischuk W, de Troconiz JF, Truitt S, Tseng J, Turini N, Ukegawa F, Valls J, Vejcik S 3rd, Velev G, Vidal R, Vilar R, Vologouev I, Vucinic D, Wagner RG, Wagner RL, Wahl J, Wallace NB, Walsh AM, Wang C, Wang CH, Wang MJ, Watanabe T, Waters D, Watts T, Webb R, Wenzel H, Wester WC 3rd, Wicklund AB, Wicklund E, Williams HH, Wilson P, Winer BL, Winn D, Wolbers S, Wolinski D, Wolinski J, Worm S, Wu X, Wyss J, Yagil A, Yao W, Yeh GP, Yeh P, Yoh J, Yosef C, Yoshida T, Yu I, Yu S, Zanetti A, Zetti F, and Zucchelli S
- Abstract
We have searched for direct pair production of scalar top and scalar bottom quarks in 88 pb-1 of pp collisions at sqrt[s]=1.8 TeV with the CDF detector. We looked for events with a pair of heavy flavor jets and missing energy, consistent with scalar top (bottom) quark decays to a charm (bottom) quark and a neutralino. The numbers of events that pass our selections show no significant deviation from standard model expectations. We compare our results to the next-to-leading order scalar quark production cross sections to exclude regions in scalar quark-neutralino mass parameter space.
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- 2000
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42. Measurement of b-Quark Fragmentation Fractions in pp[over ¯] Collisions at sqrt[s]=1.8 TeV.
- Author
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Affolder T, Akimoto H, Akopian A, Albrow MG, Amaral P, Amendolia SR, Amidei D, Antos J, Apollinari G, Arisawa T, Asakawa T, Ashmanskas W, Atac M, Azzi-Bacchetta P, Bacchetta N, Bailey MW, Bailey S, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Barone M, Bauer G, Bedeschi F, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Berryhill J, Bertolucci S, Bevensee B, Bhatti A, Bigongiari C, Binkley M, Bisello D, Blair RE, Blocker C, Bloom K, Blumenfeld B, Blusk BS, Bocci A, Bodek A, Bokhari W, Bolla G, Bonushkin Y, Bortoletto D, Boudreau J, Brandl A, van den Brink S, Bromberg C, Bruner N, Buckley-Geer E, Budagov J, Budd HS, Burkett K, Busetto G, Byon-Wagner A, Byrum KL, Campbell M, Caner A, Carithers W, Carlson J, Carlsmith D, Cassada J, Castro A, Cauz D, Cerri A, Chang PS, Chang PT, Chapman J, Chen C, Chen YC, Cheng MT, Chertok M, Chiarelli G, Chirikov-Zorin I, Chlachidze G, Chlebana F, Christofek L, Chu ML, Cihangir S, Ciobanu CI, Clark AG, Cobal M, Cocca E, Connolly A, Conway J, Cooper J, Cordelli M, Guimaraes da Costa J, Costanzo D, Cranshaw J, Cronin-Hennessy D, Cropp R, Culbertson R, Dagenhart D, Dejongh F, Dell'agnello S, Dell'orso M, Demina R, Demortier L, Deninno M, Derwent PF, Devlin T, Dittmann JR, Donati S, Done J, Dorigo T, Eddy N, Einsweiler K, Elias JE, Engels E Jr, Erdmann W, Errede D, Errede S, Fan Q, Feild RG, Ferretti C, Fiori I, Flaugher B, Foster GW, Franklin M, Freeman J, Friedman J, Fukui Y, Gadomski S, Galeotti S, Gallinaro M, Gao T, Garcia-Sciveres M, Garfinkel AF, Gatti P, Gay C, Geer S, Gerdes DW, Giannetti P, Giromini P, Glagolev V, Gold M, Goldstein J, Gordon A, Goshaw AT, Gotra Y, Goulianos K, Grassmann H, Green C, Groer L, Grosso-Pilcher C, Guenther M, Guillian G, Guo RS, Haber C, Hafen E, Hahn SR, Hall C, Handa T, Handler R, Hao W, Happacher F, Hara K, Hardman AD, Harris RM, Hartmann F, Hatakeyama K, Hauser J, Heinrich J, Heiss A, Hinrichsen B, Hoffman KD, Holck C, Hollebeek R, Holloway L, Hughes R, Huston J, Huth J, Ikeda H, Incagli M, Incandela J, Introzzi G, Iwai J, Iwata Y, James E, Jensen H, Jones M, Joshi U, Kambara H, Kamon T, Kaneko T, Karr K, Kasha H, Kato Y, Keaffaber TA, Kelley K, Kelly M, Kennedy RD, Kephart R, Khazins D, Kikuchi T, Kirk M, Kim BJ, Kim HS, Kim SH, Kim YK, Kirsch L, Klimenko S, Knoblauch D, Koehn P, Köngeter A, Kondo K, Konigsberg J, Kordas K, Korytov A, Kovacs E, Kroll J, Kruse M, Kuhlmann SE, Kurino K, Kuwabara T, Laasanen AT, Lai N, Lami S, Lammel S, Lamoureux JI, Lancaster M, Latino G, Lecompte T, Lee AM 4th, Leone S, Lewis JD, Lindgren M, Liss TM, Liu JB, Liu YC, Lockyer N, Loreti M, Lucchesi D, Lukens P, Lusin S, Lys J, Madrak R, Maeshima K, Maksimovic P, Malferrari L, Mangano M, Mariotti M, Martignon G, Martin A, Matthews JA, Mazzanti P, McFarland KS, McIntyre P, McKigney E, Menguzzato M, Menzione A, Meschi E, Mesropian C, Miao C, Miao T, Miller R, Miller JS, Minato H, Miscetti S, Mishina M, Moggi N, Moore E, Moore R, Morita Y, Mukherjee A, Muller T, Munar A, Murat P, Murgia S, Musy M, Nachtman J, Nahn S, Nakada H, Nakaya T, Nakano I, Nelson C, Neuberger D, Newman-Holmes C, Ngan CY, Nicolaidi P, Niu H, Nodulman L, Nomerotski A, Oh SH, Ohmoto T, Ohsugi T, Oishi R, Okusawa T, Olsen J, Pagliarone C, Palmonari F, Paoletti R, Papadimitriou V, Pappas SP, Parri A, Partos D, Patrick J, Pauletta G, Paulini M, Perazzo A, Pescara L, Phillips TJ, Piacentino G, Pitts KT, Plunkett R, Pompos A, Pondrom L, Pope G, Prokoshin F, Proudfoot J, Ptohos F, Punzi G, Ragan K, Reher D, Riegler W, Ribon A, Rimondi F, Ristori L, Robertson WJ, Robinson A, Rodrigo T, Rolli S, Rosenson L, Roser R, Rossin R, Sakumoto WK, Saltzberg D, Sansoni A, Santi L, Sato H, Savard P, Schlabach P, Schmidt EE, Schmidt MP, Schmitt M, Scodellaro L, Scott A, Scribano A, Segler S, Seidel S, Seiya Y, Semenov A, Semeria F, Shah T, Shapiro MD, Shepard PF, Shibayama T, Shimojima M, Shochet M, Siegrist J, Signorelli G, Sill A, Sinervo P, Singh P, Slaughter AJ, Sliwa K, Smith C, Snider FD, Solodsky A, Spalding J, Speer T, Sphicas P, Spinella F, Spiropulu M, Spiegel L, Stanco L, Steele J, Stefanini A, Strologas J, Strumia F, Stuart D, Sumorok K, Suzuki T, Takashima R, Takikawa K, Tanaka M, Takano T, Tannenbaum B, Taylor W, Tecchio M, Teng PK, Terashi K, Tether S, Theriot D, Thurman-Keup R, Tipton P, Tkaczyk S, Tollefson K, Tollestrup A, Toyoda H, Trischuk W, de Troconiz JF, Truitt S, Tseng J, Turini N, Ukegawa F, Valls J, Vejcik S 3rd, Velev G, Vidal R, Vilar R, Vologouev I, Vucinic D, Wagner RG, Wagner RL, Wahl J, Wallace NB, Walsh AM, Wang C, Wang CH, Wang MJ, Watanabe T, Watts T, Webb R, Wenzel H, Wester WC 3rd, Wicklund AB, Wicklund E, Williams HH, Wilson P, Winer BL, Winn D, Wolbers S, Wolinski D, Wolinski J, Worm S, Wu X, Wyss J, Yagil A, Yao W, Yeh GP, Yeh P, Yoh J, Yosef C, Yoshida T, Yu I, Yu S, Zanetti A, Zetti F, and Zucchelli S
- Abstract
We have studied the production of B hadrons in 1.8-TeV pp[over ¯] collisions. We present measurements of the fragmentation fractions, f_{u}, f_{d}, f_{s}, and f_{baryon}, of produced b quarks that yield B^{+}, B^{0}, B_{s}^{0}, and Λ[over ¯]_{b}^{0} hadrons. Reconstruction of five electron-charm final states yields f_{s}/( f_{u}+f_{d})=0.213±0.068 and f_{baryon}/( f_{u}+f_{d})=0.118±0.042, assuming f_{u}=f_{d}. If all B hadrons produced in pp[over ¯] collisions cascade to one of these four hadrons, we determine f_{u}=f_{d}=0.375±0.023, f_{s}=0.160±0.044, and f_{baryon}=0.090±0.029. If we do not assume f_{u}=f_{d}, we find f_{d}/f_{u}=0.84±0.16.
- Published
- 2000
- Full Text
- View/download PDF
43. Measurement of the average lifetime of B hadrons produced in pp-bar collisions at sqrt s =1.8 TeV.
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Abe F, Albrow M, Amidei D, Anway-Wiese C, Apollinari G, Areti H, Auchincloss P, Azfar F, Azzi P, Bacchetta N, Badgett W, Bailey MW, Bao J, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Bauer G, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Benlloch J, Beretvas A, Berge JP, Bhatti A, Biery K, Binkley M, Bird F, Bisello D, Blair RE, Blocker C, Bodek A, Bolognesi V V, Boswell C, Boulos T, Brandenburg G, Buckley-Geer E, Budd HS, Burkett K, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carithers W, Carlsmith D, Castro A, Cen Y, Cervelli F, Chapman J, Chiarelli G, Chikamatsu T, Cihangir S, Clark AG, Cobal M, Contreras M, Cooper J, Cordelli M, and Coupal DP
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- 1993
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44. Observation of the decay Bs0-->J/ psi phi in p-barp collisions at sqrt s =1.8 TeV.
- Author
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Abe F, Albrow M, Amidei D, Anway-Wiese C, Apollinari G, Areti H, Auchincloss P, Azfar F, Azzi P, Bacchetta N, Badgett W, Bailey MW, Bao J, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Bauer G, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Benlloch J, Beretvas A, Bhatti A, Biery K, Binkley M, Bird F, Bisello D, Blair RE, Blocker C, Bodek A, Bolognesi V V, Boswell C, Boulos T, Brandenburg G, Buckley-Geer E, Budd HS, Burkett K, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carithers W, Carlsmith D, Castro A, Cen Y, Cervelli F, Chapman J, Chiarelli G, Chikamatsu T, Cihangir S, Clark AG, Cobal M, Contreras M, Cooper J, Cordelli M, Coupal DP, and Crane D
- Published
- 1993
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45. Electric field effects on barium autoionizing spectra.
- Author
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Armstrong DJ, Greene CH, Wood RP, and Cooper J
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- 1993
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46. Measurement of jet shapes in p-barp collisions at sqrt s =1.8 TeV.
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Abe F, Amidei D, Anway-Weiss C, Apollinari G, Atac M, Auchincloss P, Baden AR, Bacchetta N, Badgett W, Bailey MW, Bamberger A, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Bauer G, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Benlloch J, Bensinger J, Beretvas A, Berge JP, Bertolucci S, Bhadra S, Binkley M, Bisello D, Blair R, Blocker C, Bodek A, Bolognesi V V, Booth AW, Boswell C, Brandenburg G, Brown D, Buckley-Geer E, Budd HS, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carey R, Carithers W, Carlsmith D, Carroll JT, Cashmore R, Castro A, Cervelli F, Chadwick K, Chapman J, Chiarelli G, Chinowsky W, Cihangir S, Clark AG, Cobal M, Connor D, Contreras M, and Cooper J
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- 1993
- Full Text
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47. Limit on the rare decay W+/---> gamma pi +/- in pp-bar collisions at sqrt s =1.8 TeV.
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Abe F, Amidei D, Anway-Weiss C, Apollinari G, Atac M, Auchincloss P, Baden AR, Bacchetta N, Badgett W, Bailey MW, Bamberger A, de Barbaro P, Barbaro-Galtieri A, Barnes VE, Barnett BA, Bauer G, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Benlloch J, Bensinger J, Beretvas A, Berge JP, Bertolucci S, Bhadra S, Binkley M, Bisello D, Blair R, Blocker C, Bodek A, Bolognesi V V, Booth AW, Boswell C, Brandenburg G, Brown D, Buckley-Geer E, Budd HS, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carey R, Carithers W, Carlsmith D, Carroll JT, Cashmore R, Castro A, Cervelli F, Chadwick K, Chapman J, Chiarelli G, Chinowsky W, Cihangir S, Clark AG, Cobal M, Connor D, Contreras M, and Cooper J
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- 1992
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48. Measurement of the production and muonic decay rate of W and Z bosons in pp-bar collisions at sqrt s =1.8 TeV.
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Abe F, Amidei D, Apollinari G, Atac M, Auchincloss P, Baden AR, Bacchetta N, Bailey MW, Bamberger A, de Barbaro P, Barnett BA, Barbaro-Galtieri A, Barnes VE, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Bertolucci S, Bhadra S, Binkley M, Bisello D, Blair R, Blocker C, Bodek A, Bolognesi V V, Booth AW, Boswell C, Brandenburg G, Brown D, Buckley-Geer E, Budd HS, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carey R, Carithers W, Carlsmith D, Carroll JT, Cashmore R, Castro A, Cervelli F, Chadwick K, Chiarelli G, Chinowsky W, Cihangir S, Clark AG, Cobal M, Connor D, Contreras M, Cooper J, Cordelli M, Crane D, Curatolo M, Day C, and DeJongh F
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- 1992
- Full Text
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49. Measurement of the ratio B(W--> tau nu )/B(W-->e nu ) in pp-bar collisions at sqrt s =1.8 TeV.
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Abe F, Amidei D, Apollinari G, Atac M, Auchincloss P, Baden AR, Bacchetta N, Bailey MW, Bamberger A, de Barbaro P, Barnett BA, Barbaro-Galtieri A, Barnes VE, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Bertolucci S, Bhadra S, Binkley M, Blair R, Blocker C, Bloom K, Bolognesi V V, Booth AW, Boswell C, Brandenburg G, Brown D, Buckley-Geer E, Budd HS, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carey R, Carithers W, Carlsmith D, Carroll JT, Cashmore R, Castro A, Cervelli F, Chadwick K, Chiarelli G, Chinowsky W, Cihangir S, Clark AG, Connor D, Contreras M, Cooper J, Cordelli M, Crane D, Curatolo M, Day C, DeJongh F, Dell'Agnello S, and Dell'Orso M
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- 1992
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50. Measurement of the B-meson and b-quark cross sections at sqrt s =1.8 TeV using the exclusive decay B+/--->J/ psi K+/-
- Author
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Abe F, Amidei D, Apollinari G, Atac M, Auchincloss P, Baden AR, Bacchetta N, Bailey MW, Bamberger A, de Barbaro P, Barnett BA, Barbaro-Galtieri A, Barnes VE, Baumann T, Bedeschi F, Behrends S, Belforte S, Bellettini G, Bellinger J, Benjamin D, Bensinger J, Beretvas A, Berge JP, Bertolucci S, Bhadra S, Binkley M, Bisello D, Blair R, Blocker C, Bodek A, Bolognesi V V, Booth AW, Boswell C, Brandenburg G, Brown D, Buckley-Geer E, Budd HS, Busetto G, Byon-Wagner A, Byrum KL, Campagnari C, Campbell M, Caner A, Carey R, Carithers W, Carlsmith D, Carroll JT, Cashmore R, Castro A, Cervelli F, Chadwick K, Chiarelli G, Chinowsky W, Cihangir S, Clark AG, Cobal M, Connor D, Contreras M, Cooper J, Cordelli M, Crane D, Curatolo M, Day C, and DeJongh F
- Published
- 1992
- Full Text
- View/download PDF
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