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SNO+

SNO+ detector. The inner vessel is filled with 780T of liquid scintillator and surrounded by a geodesic sphere of photomultiplier tubes immersed in ultra-pure water. The detector is located 2.1km underground at Canada's SNOLAB, outside of Sudbury, Western Ontario.

Credit: SNOLAB

Jeff Tseng

Professor of Physics

Research theme

  • Particle astrophysics & cosmology
  • Fundamental particles and interactions

Sub department

  • Particle Physics

Research groups

  • Rubin-LSST
  • SNO+
Jeff.Tseng@physics.ox.ac.uk
Telephone: 01865 (2)73398
Denys Wilkinson Building, room 674
Home page
  • About
  • Publications

ATLAS upgrade plans for the SLHC

NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS 177 (2008) 212-216
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BlackMax: A black-hole event generator with rotation, recoil, split branes and brane tension

ArXiv 0711.3012 (2007)

Authors:

De-Chang Dai, Glenn Starkman, Dejan Stojkovic, Cigdem Issever, Eram Rizvi, Jeff Tseng

Abstract:

We present a comprehensive black-hole event generator, BlackMax, which simulates the experimental signatures of microscopic and Planckian black-hole production and evolution at the LHC in the context of brane world models with low-scale quantum gravity. The generator is based on phenomenologically realistic models free of serious problems that plague low-scale gravity, thus offering more realistic predictions for hadron-hadron colliders. The generator includes all of the black-hole graybody factors known to date and incorporates the effects of black-hole rotation, splitting between the fermions, non-zero brane tension and black-hole recoil due to Hawking radiation (although not all simultaneously). The generator can be interfaced with Herwig and Pythia.
Details from ArXiV
More details from the publisher

The ATLAS semiconductor tracker end-cap module

Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 575:3 (2007) 353-389

Authors:

A Abdesselam, PJ Adkin, PP Allport, J Alonso, L Andricek, F Anghinolfi, AA Antonov, RJ Apsimon, T Atkinson, LE Batchelor, RL Bates, G Beck, H Becker, P Bell, W Bell, P Beneš, J Bernabeu, S Bethke, JP Bizzell, J Blocki, Z Broklová, J Brož, J Bohm, P Booker, G Bright, TJ Brodbeck, P Bruckman, CM Buttar, JM Butterworth, F Campabadal, D Campbell, C Carpentieri, JL Carroll, AA Carter, JR Carter, GL Casse, P Čermák, M Chamizo, DG Charlton, A Cheplakov, E Chesi, A Chilingarov, S Chouridou, D Chren, A Christinet, ML Chu, V Cindro, A Ciocio, JV Civera, A Clark, AP Colijn, PA Cooke, MJ Costa, D Costanzo, W Dabrowski, KM Danielsen, VR Davies, I Dawson, P de Jong, P Dervan, F Doherty, Z Doležal, M Donega, M D'Onofrio, O Dorholt, Z Drásal, JD Dowell, IP Duerdoth, R Duxfield, M Dwuznik, JM Easton, S Eckert, L Eklund, C Escobar, V Fadeyev, D Fasching, L Feld, DPS Ferguson, P Ferrari, D Ferrere, C Fleta, R Fortin, JM Foster, C Fowler, H Fox, J Freestone, RS French, J Fuster, S Gadomski, BJ Gallop, C García, JE García-Navarro, S Gibson, MGD Gilchriese, F Gonzalez, S Gonzalez-Sevilla, MJ Goodrick, A Gorisek, E Gornicki, A Greenall

Abstract:

The challenges for the tracking detector systems at the LHC are unprecedented in terms of the number of channels, the required read-out speed and the expected radiation levels. The ATLAS Semiconductor Tracker (SCT) end-caps have a total of about 3 million electronics channels each reading out every 25 ns into its own on-chip 3.3 μ s buffer. The highest anticipated dose after 10 years operation is 1.4 × 1014 cm- 2 in units of 1 MeV neutron equivalent (assuming the damage factors scale with the non-ionising energy loss). The forward tracker has 1976 double-sided modules, mostly of area ∼ 70 cm2, each having 2 × 768 strips read out by six ASICs per side. The requirement to achieve an average perpendicular radiation length of 1.5% X0, while coping with up to 7 W dissipation per module (after irradiation), leads to stringent constraints on the thermal design. The additional requirement of 1500 e- equivalent noise charge (ENC) rising to only 1800 e- ENC after irradiation, provides stringent design constraints on both the high-density Cu/Polyimide flex read-out circuit and the ABCD3TA read-out ASICs. Finally, the accuracy of module assembly must not compromise the 16 μ m (r φ) resolution perpendicular to the strip directions or 580 μ m radial resolution coming from the 40 mrad front-back stereo angle. A total of 2210 modules were built to the tight tolerances and specifications required for the SCT. This was 234 more than the 1976 required and represents a yield of 93%. The component flow was at times tight, but the module production rate of 40-50 per week was maintained despite this. The distributed production was not found to be a major logistical problem and it allowed additional flexibility to take advantage of where the effort was available, including any spare capacity, for building the end-cap modules. The collaboration that produced the ATLAS SCT end-cap modules kept in close contact at all times so that the effects of shortages or stoppages at different sites could be rapidly resolved. © 2007 Elsevier B.V. All rights reserved.
More details from the publisher

Measurement of σΛb0/ σB̄0×B(Λb0→Λc+π-)/B(B̄0→D+π- ) in pp̄ Collisions at s=1.96TeV

Physical Review Letters 98:12 (2007)

Authors:

A Abulencia, J Adelman, T Affolder, T Akimoto, MG Albrow, D Ambrose, S Amerio, D Amidei, A Anastassov, K Anikeev, A Annovi, J Antos, M Aoki, G Apollinari, JF Arguin, T Arisawa, A Artikov, W Ashmanskas, A Attal, F Azfar, P Azzi-Bacchetta, P Azzurri, N Bacchetta, W Badgett, A Barbaro-Galtieri, VE Barnes, BA Barnett, S Baroiant, V Bartsch, G Bauer, F Bedeschi, S Behari, S Belforte, G Bellettini, J Bellinger, A Belloni, D Benjamin, A Beretvas, J Beringer, T Berry, A Bhatti, M Binkley, D Bisello, RE Blair, C Blocker, B Blumenfeld, A Bocci, A Bodek, V Boisvert, G Bolla, A Bolshov, D Bortoletto, J Boudreau, A Boveia, B Brau, L Brigliadori, C Bromberg, E Brubaker, J Budagov, HS Budd, S Budd, S Budroni, K Burkett, G Busetto, P Bussey, KL Byrum, S Cabrera, M Campanelli, M Campbell, F Canelli, A Canepa, S Carillo, D Carlsmith, R Carosi, M Casarsa, A Castro, P Catastini, D Cauz, M Cavalli-Sforza, A Cerri, L Cerrito, SH Chang, YC Chen, M Chertok, G Chiarelli, G Chlachidze, F Chlebana, I Cho, K Cho, D Chokheli, JP Chou, G Choudalakis, SH Chuang, K Chung, WH Chung, YS Chung, M Ciljak, CI Ciobanu, MA Ciocci, A Clark

Abstract:

We present the first observation of the baryon decay Λb0→ Λc+π- followed by Λc+→pK-π+ in 106pb-1 pp̄ collisions at s=1.96TeV in the CDF experiment. In order to reduce systematic error, the measured rate for Λb0 decay is normalized to the kinematically similar meson decay B̄0→D+π- followed by D+→π+K-π+. We report the ratio of production cross sections (σ) times the ratio of branching fractions (B) for the momentum region integrated above pT>6GeV/c and pseudorapidity range |η|<1.3: σ(pp̄→Λb0X)/ σ(pp̄→B̄0X)×B(Λb0→Λc+π-)/ B(B̄0→D+π-)=0.82±0.08(stat)±0.11(syst)±0. 22[B(Λc+→pK-π+)]. © 2007 The American Physical Society.
More details from the publisher

Measurement of sigma(Lambda_b)/sigma(B0) x B(Lambda_b->Lambda_c pi)/B(B0->Dpi) in ppbar Collisions at sqrt(s)=1.96 TeV

Physical Review Letters 98 (2007) 122002 7pp

Authors:

JC Tseng, Y Le, M Martin, P Maksimovic
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