107656092
Results of the studies on energy deposition in IR6 superconducting magnets from continuous beam loss on the TCDQ system
SummaryA single sided mobile graphite diluter block TCDQ, in combination with a two-sidedsecondary collimator TCS and an iron shield TCDQM, will be installed in front of thesuperconducting quadrupole Q4 magnets in IR6, in order to protect it and other downstreamLHC machine elements from destruction in the event of a beam dump that is not synchronisedwith the abort gap. The TCDQ will be positioned close to the beam, and will intercept theparticles from the secondary halo during low beam lifetime. Previous studies [1-4] haveshown that the energy deposited in the Q4 magnet coils can be close to or above the quenchlimit. In this note the results of the latest FLUKA energy deposition simulations for Beam 2are described, including an upgrade possibility for the TCDQ system with an additionalshielding device. The results are discussed in the context of the expected performance levelsfor the different phases of LHC operation. 1. Introduction The LHC beam dumping system includes a single sided mobile diluter block TCDQ [5],consisting of two blocks namely TCDQA and TCDQB, in combination with a secondarycollimator TCS and an iron shield TCDQM [6], installed in front of the superconductingquadrupole Q4 magnet in IR6, in order to protect it and other LHC machine elements fromdestruction in the event of a beam dump that is not synchronised with the abort gap [7]. TheTCDQ element should protect the LHC from damage from swept bunches under all conditions,in particular the arc aperture at 450 GeV, the low-beta triplet aperture and the tungsten tertiarycollimators at 7 TeV. The TCDQ must also prevent quenches of Q4, arising from spuriousparticles in the abort gap during a normal beam dump, and from particles lost from the beamhalo during regular operation.The two-jawed TCS collimator is located immediately after the TCDQ to precisely definethe horizontal beam position and to achieve higher precision collimation of secondary haloparticles from both sides. The TCS will receive a potentially high load from the secondary haloin the event of low beam lifetime. The nominal settings of the TCDQ and TCS are assumed tobe 8 and 7 s
2362172
LHC collimation system hardware commissioning
The stored energy and intensity of the LHC beam exceed the damage level of the machine and the quench level of the magnets by far. Therefore a robust and reliable collimation system is required which prevents the quenching of the magnets during regular operation and protects the accelerator components from damage in the event of beam loss. To assure that the installed collimators will protect the machine and permit the required performance of the collider, an appropriate hardware commissioning has to be implemented. In this contribution we describe the procedures for the hardware commissioning of the LHC collimation system. These procedures will establish the required precision and reliability of collimator movements and settings before the start of beam operation.
2759886
Construction and Performance of a Micro-Pattern Stereo Detector with Two Gas Electron Multipliers
Abstract The construction of a micro-pattern gas detector of dimensions 40×10 cm 2 is described. Two gas electron multiplier foils (GEM) provide the internal amplification stages. A two-layer readout structure was used, manufactured using the same technology as the GEM foils. The strips of each layer cross at an effective crossing angle of 6.7° and have a 406 μm pitch. The performance of the detector has been evaluated in a muon beam at CERN using a silicon telescope as reference system. The position resolutions of two orthogonal coordinates are measured to be 50 μm and 1 mm , respectively. The muon detection efficiency for two-dimensional space points reaches 96%.
55572949
CRITICAL HALO LOSS LOCATIONS IN THE LHC
Results of simulations with all movable elements of the LHC collimation system [1] are discussed for various operation modes. Compared to previous results, the placing of additional collimators reduced the beam losses by a factor 10 in the ideal machine case, i.e. nominal collimators settings for both 450 GeV and 7 TeV beam energies. First results for Beam 2 are also reviewed. The sensitivity of the system to free orbit oscillations is addressed. These results show that it is sufficient to use a limited number of beam loss monitors (BLMs) for the setup and optimization of the LHC Collimation System.
27473327
Transverse impendance of LHC collimators
The transverse impedance in the LHC is expected to be dominated by the numerous collimators, most of which are made of Fibre-Reinforced-Carbon to withstand the impacts of high intensity proton beams in case of failures, and which will be moved very close to the beam, with full gaps of few millimetres, in order to protect surrounding super-conducting equipments. We present an estimate of the transverse resistive-wall impedance of the LHC collimators, the total impedance in the LHC at injection and top energy, the induced coupled-bunch growth rates and tune shifts, and finally the result of the comparison of the theoretical predictions with measurements performed in 2004 and 2006 on a prototype collimator installed in the SPS.
2156470
Performance reach of the "phase 1" LHC collimation system
State-of-the-art tracking tools have been developed for detailed LHC collimation and beam loss studies. This includes full chromatic treatment of both beam lines and error models. This paper reviews the main results on the performance reach of the multi-stage LHC collimation system that is being installed in the LHC. Limitations on the allowed proton loss rates and the stored intensity can be derived from the comparison of local losses with estimated quench limits for the superconducting magnets. The origins of the cleaning-related performance limitations are presented and possible improvements are discussed.
122052216
Charm production by partons in neutrino scattering
Abstract We present quantitative quark-parton model calculations of charm production contributions in neutrino scattering, to compare with the experimental indications of possible charm production, namely dimuon events and ḡnN y -distributions. Within the uncertainties in the present data and in the quark density distributions, charm production in the Glashow-Iliopoulos-Maiani scheme appears to offer a viable explanation of both effects.
119576402
Neutrino mass and mixing implied by underground deficit of low energy muon-neutrino events
Abstract Recent observations of a deficit of cosmic ray muon-neutrino interactions in underground detectors suggest that the muon neutrinos may have oscillated to another state. We examine possible neutrino mass and mixing patterns, and their implications for vacuum and matter effects on solar neutrinos, on neutrinos passing through the earth, and on terrastrial neutrino beams. By invoking the see-saw mechanism of neutrino mass generation, we draw inferences on closure of the universe with neutrino masses, on the number of generations, on t-quark and fourth generation masses, and on the Peccei-Quinn symmetry breaking scale. Testable predictions are suggested.
119113030
Searching for the Layered Structure of Space at the LHC
Alignment of the main energy fluxes along a straight line in a target plane has been observed in families of cosmic ray particles detected in the Pamir mountains. The fraction of events with alignment is statistically significant for families with superhigh energies and large numbers of hadrons. This can be interpreted as evidence for coplanar hard scattering of secondary hadrons produced in the early stages of the atmospheric cascade development. This phenomenon can be described within the recently proposed 'crystal world,' with latticized and anisotropic spatial dimensions. Planar events are expected to dominate particle collisions at a hard-scattering energy exceeding the scale {Lambda}{sub 3} at which space transitions from 3D{r_equilibrium}2D. We study specific collider signatures that will test this hypothesis. We show that the energy spectrum of Drell-Yan (DY) scattering is significantly modified in this framework. At the LHC, two jet and three jet events are necessarily planar, but four jet events can test the hypothesis. Accordingly, we study in a model-independent way the 5{sigma} discovery reach of the ATLAS and CMS experiments for identifying four jets coplanarities. For the extreme scenario in which all pp {yields} 4 jet scattering processes become coplanar above {Lambda}{sub 3}, we show that withmore » an integrated luminosity of 10(100) fb{sup -1} the LHC experiments have the potential to discover correlations between jets if {Lambda}{sub 3} {approx}< 1.25(1.6) TeV.« less
14054232
An evaluation of the exposure in nadir observation of the JEM-EUSO mission
We evaluate the exposure during nadir observations with JEM-EUSO, the Extreme Universe Space Observatory, on-board the Japanese Experiment Module of the International Space Station. Designed as a mission to explore the extreme energy Universe from space, JEM-EUSO will monitor the Earth's nighttime atmosphere to record the ultraviolet light from tracks generated by extensive air showers initiated by ultra-high energy cosmic rays. In the present work, we discuss the particularities of space-based observation and we compute the annual exposure in nadir observation. The results are based on studies of the expected trigger aperture and observational duty cycle, as well as, on the investigations of the effects of clouds and different types of background light. We show that the annual exposure is about one order of magnitude higher than those of the presently operating ground-based observatories.
119117884
Proceedings of the 2nd Workshop on Flavor Symmetries and Consequences in Accelerators and Cosmology (FLASY12)
Although existing theoretical models generally prefer extremely heavy right-handed neutrinos to generate light neutrino masses via the seesaw mechanism, there are several observed phenomena that point to the existence of both keVand eV-scale sterile neutrinos. We present two A4 flavor symmetry models that can accommodate light sterile neutrinos and remain compatible with neutrino data. Higher order seesaw terms and higher-dimensional operators are studied, and the phenomenological implications of light sterile neutrinos on neutrinoless double beta decay are discussed. 1.