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Within the general frame of the upgrade of the collider DAFNE to the neutron-antineutron energy threshold (2-2.5 GeV c.m.), modifications and different options for the accelerator design are discussed and a possible lattice for the Main…

Accelerator Physics · Physics 2007-05-23 G. Benedetti

The design of an Interaction Region (IR) suitable to reach low values of the beta functions at the Interaction Point (IP) and a high collision frequency is a rather difficult task in a short ring as DAPHNE, where an upgrade of the peak…

Accelerator Physics · Physics 2007-05-23 M. E. Biagini

The Frascati Phi-factory DAFNE has successfully completed experimental runs for the three main detectors, KLOE, FINUDA and DEAR. The best peak luminosity achieved so far is 1.6x10^32 cm-2s-1, while the best daily integrated luminosity is 10…

Accelerator Physics · Physics 2019-08-14 M. Zobov

Interest in highly-compressed electron beams has been increasing in recent times, driven by the study of non-linear and even non-perturbative aspects of QED [2]. The FACET-II [7] facility at SLAC is currently (at the time of writing) being…

Accelerator Physics · Physics 2018-11-30 Glen White , Vitaly Yakimenko

A ring-based Higgs factory with a center-of-mass energy of 240 GeV residing in the existing LEP tunnel is studied at a level of concrete lattice. We found that low-emittance lattice is essential to mitigate the effect of beamstrahlung on…

Accelerator Physics · Physics 2013-09-11 Yunhai Cai , Alex Chao , Yuri Nosochkov , Uli Wienands , Frank Zimmermann

Muon collider is a promising candidate for the next energy frontier machine. However, in order to obtain peak luminosity in the 1035/cm2/s range the collider lattice design must satisfy a number of stringent requirements, such as low beta…

Accelerator Physics · Physics 2012-02-03 Y. Alexahin , E. Gianfelice-Wendt , A. Netepenko

Numerical simulations of beam-beam effects in the electron-positron Phi-factory DAPhNE taking into account the measured cubic nonlinearities have shown that the nonlinearities have a strong impact on the collider luminosity performance. The…

Accelerator Physics · Physics 2007-05-23 M. Zobov

We consider the possibility of a 120x120 GeV e+e- ring collider in the LHC tunnel. A luminosity of 10^34/cm2/s can be obtained with a luminosity life time of a few minutes. A high operation efficiency would require two machines: a low…

High Energy Physics - Experiment · Physics 2012-02-16 Alain Blondel , Frank Zimmermann

Recently the peak luminosity achieved on the DA{\Phi}NE collider has been improved by almost a factor three by implementing a novel collision scheme based on large Piwinski angle and Crab-Waist. This encouraging result opened new…

A second major upgrade of the LHCb detector is necessary to allow full exploitation of the HL-LHC for flavour physics. The new detector will be installed during long shutdown 4 (LS4), and will operate at instantaneous luminosity up to $1.5…

High Energy Physics - Experiment · Physics 2025-04-01 LHCb collaboration

Linac-ring type colliders will open new windows for both energy frontier and particle factories. Concerning the first direction, these machines seem to be a sole way to TeV scale in lepton-hadron collisison at constituent level. An…

Accelerator Physics · Physics 2007-05-23 A. K. Ciftci , E. Recepoglu , S. Sultansoy , O. Yavas , M. Yilmaz

The Super Tau-Charm Facility (STCF) is a proposed high-luminosity electron-positron collider operating in the beam energy range of 1-3.5 GeV, targeting a peak luminosity larger than $0.5\times10^{35}\ \mathrm{cm^{-2}s^{-1}}$ at 2 GeV. In…

Accelerator Physics · Physics 2026-05-19 Tao Liu , Anton Bogomyagkov , Demin Zhou , Penghui Yang , Sangya Li , Linhao Zhang , Ye Zou , Jingyu Tang , Qing Luo

Gamma sources with high flux and spectral densities are the main requirements for new nuclear physics experiments to be performed in several worldwide laboratories and envisaged in the ELI-NP (Extreme Light Infrastructure-Nuclear Physics)…

Accelerator Physics · Physics 2014-05-06 D. Alesini , I. Chaikovska , A. Variola , S. Guiducci , F. Zomer , C. Milardi , M. Zobov

We discuss a preliminary design for a high luminosity 4 TeV center of mass $\mu^+\,\mu^-$ collider ring.

acc-phys · Physics 2009-09-15 A. Garren , E. Courant , J. Gallardo , R. Palmer , D. Trbojevic , C. Johnstone , K-Y. Ng

We present a study of high-$\beta$* optics configurations at Interaction Point 2 (IP2) of the Large Hadron Collider (LHC), developed to enable forward and diffractive physics measurements with the ALICE experiment during Runs 3 and 4. Using…

High Energy Physics - Experiment · Physics 2025-05-22 Sorina Popescu

Lambda-hypernuclei are produced and studied, with the FINUDA spectrometer, for the first time at an e+e- collider: DAPHNE, the Frascati phi-factory. The slow negative kaons from phi(1020) decay are stopped in thin (0.2 g/cm^2) nuclear…

Nuclear Experiment · Physics 2015-06-26 FINUDA Collaboration

A Super Flavor Factory, an asymmetric energy e+e- collider with a luminosity of order 10^36 cm-2s-1, can provide a sensitive probe of new physics in the flavor sector of the Standard Model. The success of the PEP-II and KEKB asymmetric…

Accelerator Physics · Physics 2008-11-26 J. T. Seeman , Y. Cai , S. Ecklund , A. Novokhatski , A. Seryi , M. Sullivan , U. Wienands , M. Biagini , P. Raimondi

A strong candidate for the Standard Model Scalar boson, H(126), has been discovered by the Large Hadron Collider (LHC) experiments. In order to study this fundamental particle with unprecedented precision, and to perform precision tests of…

The physics objectives of SuperB, an asymmetric electron-positron collider with a luminosity above 10^36/cm^2/s are described, together with the conceptual design of a novel low emittance design that achieves this performance with wallplug…

High Energy Physics - Experiment · Physics 2012-08-27 SuperB Collaboration

At present, the PEP-II bunch length and vertical beta function at the Interaction Point (IP) are about of the same size. To increase luminosity, it is planned to gradually reduce the IP beta function. For the maximum effect, bunch length…

Accelerator Physics · Physics 2008-11-26 Y. Cai , M. H. R. Donald , Y. Nosochkov
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