Contribution List

15 out of 15 displayed
Export to PDF
  1. Prof. Federico Palmonari (INFN & University, Bologna)
    test
    In the three charged fermion families of the Standard Model, the mass ratios between $2^{nd}$ and $1^{st}$, $3^{rd}$ and $2^{nd}$ generations can be approximated by power laws of the integer numbers 3, 4 and 7 with integer exponents which are function of their generation index i=1, 2, 3. Each recursive formula is extended to i=0 and this mass value is used as a free parameter to fit the...
    Go to contribution page
  2. Giorgio Chiarelli (PI)
    I believe that the scenario for "What Next" in the SM group (and not only) should include the possibility to push for HE-LHC as an alternative to other paths.
    Go to contribution page
  3. Giancarlo Panizzo (U)
    We propose a new type of Z polarization asymmetry in bottom-Z production at LHC that should be realistically measurable and would provide the determination of the so-called Ab parameter, whose available measured value still appears to be in disagreement with the Standard Model prediction. This polarization can be measured independently of a possible existence of Supersymmetry. If Supersymmetry...
    Go to contribution page
  4. Barbara Mele (ROMA1)
    test
    We discuss a few major physics topics where an energy-frontier e+e− collider can contribute beyond the expected reach of the LHC. We focus on precision measurements in the Higgs-boson and top-quark sectors at the International Linear Collider (ILC), an e+e− accelerator featuring a c.o.m. energy ranging from 250 GeV up to 500 GeV, and possibly 1 TeV, at different stages, with luminosities of a...
    Go to contribution page
  5. Dr Graziano Venanzoni (LNF)
    For the precision test of the Standard Model at future e+e- colliders (like TLEP or ILC), as well as for the reduction of the theoretical error of the Muon (g-2), an improvement on the knowledge of the low energy non perturbative effects is mandatory. These effects to alpha_em(M_Z0) and to (g-2)_mu can be obtained by precise measurements of the hadronic cross sections at low e+e- machine...
    Go to contribution page
  6. Collaboration CMS (CERN)
    Estimates of the ultimate precision of measurements of the top-quark mass achievable with 300–3000 fb−1 of proton-proton collisions at a center-of-mass energy of 14 TeV are presented. Possible improvements in the understanding of systematic uncertain- ties are discussed for various top-quark mass measurement techniques. Building on new insights from recent studies at the LHC, the...
    Go to contribution page
  7. Fabio Cossutti (TS on behalf of the CMS Collaboration)
    The physics reach of the CMS detector achievable with 300(0)/fb of proton-proton collisions recorded at sqrt(s) = 14TeV is presented. Ultimate precision on measurements of Higgs boson properties, top quark physics, and electroweak processes are discussed, as well as the discovery potential for new particles beyond the standard model. In addition, the potential for future heavy ion physics is...
    Go to contribution page
  8. Collaboration ATLAS (_)
    Studies are presented on the prospects for measuring Higgs boson production cross sec- tions times branching ratios, and determining couplings to individual fermions and bosons in 14 TeV proton-proton collisions at the LHC with 300 fb−1 and at the HL-LHC with 3000 fb−1. Several studies already presented at the 2012 European Strategy meeting are updated. In addition first analyses are presented...
    Go to contribution page
  9. Collaboration CMS (CERN)
    Searches for t → Zq in top-quark pair events with a topology compatible with the decay chain tt → Zq + Wb → llq + l′ νb (l = e, μ) are presented. Projections on ex- clusion limits with luminosities of 300 fb−1 and 3000 fb−1 of proton-proton collisions at a center-of-mass energy of 14 TeV are considered.
    Go to contribution page
  10. Collaboration ATLAS (_)
    In this note, the prospects for experimental studies of the general HVV tensor coupling using the H → ZZ∗ → 4l decay are presented. The sensitivity of the ATLAS experi- ment to non-Standard Model contributions to the HZZ vertex is estimated for 300 fb−1 and 3000 fb−1 of LHC data at √s = 14 TeV. The exclusion limits on the non-Standard Model CP-even coupling g2 and CP-odd coupling g4, given the...
    Go to contribution page
  11. Paolo Nason (MIB)
    test
    Breve nota sulle future analisi a LHC
    Go to contribution page
  12. Dr paolo walter cattaneo (INFN Pavia)
    An important test of the special relativity theory consists in verifying two key predictions: the relative widths of unstable particles are independent from their Lorentz boost and their laboratory lifetimes is proportional to the boost parameter $\gamma$. These predictions can be subject to experimental tests measuring lifetimes and branching rations of unstable particle in flight at...
    Go to contribution page
  13. Stefania De Curtis (FI)
    test
    The top quark plays a central role in many New Physics (NP) models, and in understanding the details of EWSB. In the short and mid-term future, top quark studies will be mainly driven by the LHC experiments. Exploration of top quarks will, however, be an integral part of particle physics studies at any future facility. An e+e− collider will have a rich top-quark physics program mainly in two...
    Go to contribution page
  14. Fabio Cossutti (TS on behalf of the CMS Collaboration)
    Studies of the pp -> WZjj vector boson scattering process in 14 TeV pp collisions using upgraded CMS detector configurations are presented. These studies include assessments of the discovery potential for observing longitudinal vector boson scattering for luminosities up to 300/fb and for observing anomalous quartic gauge couplings with luminosities of 300/fb and 3000/fb.
    Go to contribution page
  15. Dr Guido Maria Urciuoli (INFN Sezione di Roma)
    test
    Una classe di esperimenti che hanno la potenzialità di effettuare verifiche molte precise del Modello Standard. Si tratta degli esperimenti che misurano la Asimmetria Violante la Parità (APV) nella diffusione di elettroni su nuclei e nucleoni. L’elettrone interagisce con la materia tramite interazione elettrodebole. La parte elettromagnetica di questa interazione è, come ben noto,...
    Go to contribution page