Qu`attendre des premières données du LHC
... – PT = 150 MeV - tracks reach last SCT layer – PT = 50 MeV - tracks reach all Pixel layers ...
... – PT = 150 MeV - tracks reach last SCT layer – PT = 50 MeV - tracks reach all Pixel layers ...
Proton decay studies in Liquid Argon TPC
... • Three U(1)SU(2)SU(3) interactions into a single one • There are different candidates of the unification group such as SU(6) ... SU(N+1) or SO(10) ... SO(2N+4) • The most attractive groups are SO(10) and E6 ...
... • Three U(1)SU(2)SU(3) interactions into a single one • There are different candidates of the unification group such as SU(6) ... SU(N+1) or SO(10) ... SO(2N+4) • The most attractive groups are SO(10) and E6 ...
PPT about Particle Physics
... First scanning tunneling microscope: G. Binnig et H. Rohrer in 1981 (IBM, Zürich), Nobel prize ...
... First scanning tunneling microscope: G. Binnig et H. Rohrer in 1981 (IBM, Zürich), Nobel prize ...
the compass rich-1 read-out system
... photoelectrons, is displayed. The average number of photoelectrons was 12.4 per ring, as shown in the figure. In the top-right panel the Cherenkov angle for 7 GeV/c pions, as measured for each event averaging over all the clusters, is reported. An angular resolution of about 3.7 mr was observed in g ...
... photoelectrons, is displayed. The average number of photoelectrons was 12.4 per ring, as shown in the figure. In the top-right panel the Cherenkov angle for 7 GeV/c pions, as measured for each event averaging over all the clusters, is reported. An angular resolution of about 3.7 mr was observed in g ...
Particle Accelerators - Stony Brook University
... Machines like LHC and ILC are pushing the limits of technology and cost. Making magnets with > 10 Tesla fields is not presently possible. So circular machines must grow as energy grows. Synchrotron energy grows rapidly as energy increases – ultimately a limit for proton accelerators as well as e ...
... Machines like LHC and ILC are pushing the limits of technology and cost. Making magnets with > 10 Tesla fields is not presently possible. So circular machines must grow as energy grows. Synchrotron energy grows rapidly as energy increases – ultimately a limit for proton accelerators as well as e ...
first determination of the proton`s weak charge
... measurements, the Qweak data allow significant constraints to be extracted for the weak charges of the constituent up and down quarks. These in turn allow us to also evaluate the weak charge of the neutron as , also Q Wn = 0.975 ± 0.010 in agreement with the Standard Model prediction. OUTLOOK The Qw ...
... measurements, the Qweak data allow significant constraints to be extracted for the weak charges of the constituent up and down quarks. These in turn allow us to also evaluate the weak charge of the neutron as , also Q Wn = 0.975 ± 0.010 in agreement with the Standard Model prediction. OUTLOOK The Qw ...
Physics@OLY Review Sheet for Magnetism Name P_____ 3/25/13
... radius to high speeds. The charged particles are subjected to both an electric field and a magnetic field. One of these fields increases the speed of the particles, and the other field holds them in a circular path. Which field performs which function? 7. A magnetic field can deflect a beam of elect ...
... radius to high speeds. The charged particles are subjected to both an electric field and a magnetic field. One of these fields increases the speed of the particles, and the other field holds them in a circular path. Which field performs which function? 7. A magnetic field can deflect a beam of elect ...
Antiproton Decelerator
_Hall.jpg?width=300)
The Antiproton Decelerator (AD) is a storage ring at the CERN laboratory in Geneva. It was built as a successor to the Low Energy Antiproton Ring (LEAR) and started operation in the year 2000. The decelerated antiprotons are ejected to one of several connected experiments.