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8 Jan 2013: This can be an important source of (SM and SUSY) Higgs bosons and other exotic new particles at the LHC. ... We have also recently begun looking, in collaboration with Steve Kom (Liverpool) and Kazuki Sakurai (DESY), at methods for extracting the masses

22 Oct 2013: I decided to write a program that would test the user's ability at italian cooking Being new to computing this was great fun and learning how to use the "if"

4 Jan 2013: MuCTPi. New SW. CaloRODs. PhaseIITrig13Oct2011. L1Track. L1. MDT Trigger New for Phase I. ... New for Phase II. L0 L1L1A. MDT. DPS. L0A. LArTBB. FEx.

22 Jul 2013: Use of version 6.520 or higher is strongly recommended. See also the HERWIG wiki for latest news and updates.

22 Oct 2013: user their new favourite number A program to divide a product by a sum, or the reciprocal.

10 Sep 2013: The new diagram. interferes negatively with the above two diagrams fixing the unitarity problem. ... The new boson is associated with a new gauge symmetry similar to that.

10 Sep 2013: If we are then presented with a new Feynman diagram. we don’t want to go through the full calculation again.

4 Jan 2013: Flexibility – moving from ILC to LAr reconstruction, involved almost no code changes (just new algortithms). ... 16. Remnant Consolidation Either use the remnant clusters to build new particles, or merge them into the existing particles.

4 Jan 2013:  Phase-2 will represent 90 % of all ATLAS data  We hope for new physics…  At this stage trigger needs flexibility  Strong desire to trigger on leptons at

10 Sep 2013: term to allow for parity violation. New structure function. For anti-neutrino scattering new structure function enters with opposite sign.

10 Sep 2013: spin-spin interaction. the new term:. The above differential cross-section depends on a single parameter.

10 Sep 2013: used in place of MX. For inelastic scattering introduce four new kinematic variables:. ... variables. are not independent. Can rewrite the new kinematic variables in terms of the squared.

4 Jan 2013:  potentially smaller than number of variables « Came up with a new approach (Cambridge/CalTech) « Use hit patterns directly - no loss of information! ... But early days… « If true, good news for future of field… CP… mass hierarchy….

10 Sep 2013: From each of the above 4 states. get two new isospin states with.

10 Sep 2013: the wave-function has new degrees of freedom! For the Hamiltonian to be Hermitian. ... and is not a constant of motion. (A.1). Introduce a new 4x4 operator:.

10 Sep 2013: phase transformation FORCED to introduce a massless gauge boson,. The Dirac equation has to be modified to include this new field:. ... Two new vertices (no QED analogues). triple-gluon vertex. quartic-gluon vertex. In addition to quark-quark scattering,

10 Sep 2013: measured from. peak cross sections. calculated, e.g. question 26. ONLY 3 GENERATIONS (unless a new 4th generation neutrino has very large mass).

4 Sep 2013: If you want to start a new wash programme, check whether there is any. ... First cancel the dishwashing cycle, then re-set the time delay, lastly select the new dishwashing cycle.

1 Sep 2013: If you want to start a new wash programme, check whether there is any. ... First cancel the dishwashing cycle, then re-set the time delay, lastly select the new dishwashing cycle.

24 Jan 2013: Table compares the new result in the same two bins to the previous results (all numbers are percentages). ... jets. This latter dataset makes up the “loose muon”sample, which is a new addition compared to the previous version of this analysis.

17 Jul 2013: Preprint typeset in JHEP style - PAPER VERSION Cavendish–HEP–10/12. CERN-TH/2010-216. IPPP/10/62. DCPT/10/124. The MC@NLO 4.10 Event Generator. Stefano Frixione†. PH Department, TH Unit, CERN, CH-1211 Geneva 23, Switzerland. ITPP, EPFL,