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An innovatory interaction region has been recently conceived and realized on the Frascati DA{\Phi}NE lepton collider. The concept of tight focusing and small crossing angle adopted to achieve high luminosity in multibunch collisions has…

Accelerator Physics · Physics 2015-05-30 Catia Milardi , Miro Andrea Preger , Pantaleo Raimondi , Francesco Sgamma

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 design of the region close to the interaction point of the FCC-ee experiments is especially challenging. The beams collide at an angle (+-15 mrad) in the high-field region of the detector solenoid. Moreover, the very low vertical…

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…

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

An interaction region (IR) with head-on collisions is considered as an alternative to the baseline configuration of the International Linear Collider (ILC) which includes two IRs with finite crossing-angles (2 and 20 mrad). Although more…

For removal of disrupted beams at the ILC linear e+e- collider it is desirable to collide beams at some crossing angle. An especially large crossing angle, of about 25 mrad, is necessary for the photon collider, where disrupted beams are…

Accelerator Physics · Physics 2007-05-23 V. I. Telnov

One of the key systems of a Muon Collider (MC) - seen as the most exciting option for the energy frontier machine in the post-LHC era - is its interaction region (IR). Designs of its optics, magnets and machine-detector interface are…

Accelerator Physics · Physics 2012-02-20 N. V. Mokhov , Y. I. Alexahin , V. V. Kashikhin , S. I. Striganov , A. V. Zlobin

Accelerator-based searches for dark matter are aiming for high sensitivity and need an experimental setup with high luminosity. This field of research is often called intensity frontier physics. One of the best motivated portals of…

Accelerator Physics · Physics 2023-01-25 Vasiliy Morozov , Bogdan Wojtsekhowski

Design of a muon collider interaction region (IR) presents a number of challenges arising from low {\beta} * < 1 cm, correspondingly large beta-function values and beam sizes at IR magnets, as well as the necessity to protect…

Accelerator Physics · Physics 2012-02-02 Y. I. Alexahin , E. Gianfelice-Wendt , V. V. Kashikhin , N. V. Mokhov , A. V. Zlobin , V. Y. Alexakhin

Design of a muon collider interaction region (IR) presents a number of challenges arising from low {\beta}* < 1 cm, correspondingly large beta-function values and beam sizes at IR magnets, as well as the necessity to protect superconducting…

Accelerator Physics · Physics 2015-06-04 Y. I. Alexahin , E. Gianfelice-Wendt , V. V. Kashikhin , N. V. Mokhov , A. V. Zlobin , V. Y. Alexakhin

The FCC-ee is a proposed future high-energy, high-intensity and high-precision lepton collider. Here, we present the latest development for the FCC-ee interaction regions, which shall ensure optimum conditions for the particle physics…

The PEP-II luminosity upgrade foreseen for the next years requires an increased number of bunches and lower beta-y* with minor modifications to the present Interaction Region (IR2). When increasing the collision frequency the beams…

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

DAFNE, the Frascati F-factory, has recently completed experimental runs for the three main detectors, KLOE, FINUDA and DEAR achieving 1.6x10E+32 cm-2s-1 peak and 10 pb-1 daily integrated luminosities. Improving these results by a…

Accelerator Physics · Physics 2008-03-11 C. Milardi

In order to achieve luminosities significantly higher than in existing machines, future storage-ring based colliders will need to operate in novel parameter regimes combining ultra-low emittance, large Piwinski angle and high bunch charge;…

Accelerator Physics · Physics 2010-06-08 Mikhail Zobov

TESLA is designed as an electron-positron linear collider (LC) based on super-conducting technology. A second interaction region is forseen to be incorporated in the design allowing its possible operation as a photon collider. In this paper…

High Energy Physics - Experiment · Physics 2011-09-13 Aura Rosca

After the successful completion of the SIDDHARTA experiment run with crab waist collisions, the electron- positron collider DA{\Phi}NE has started routine operations for the KLOE-2 detector. The new interaction region also exploits the crab…

The Supper Proton-Proton Collider is a next-generation hadron collider that is now being designed. A baseline design aims for a peak luminosity of about 1*10^35 cm^-2 s^-1. The focus of this article is the effect of beam-beam interactions…

Accelerator Physics · Physics 2020-06-03 Li-Jiao Wang , Tanaji Sen , Jing-Yu Tang

Linear colliders offer unique opportunities to study gamma-gamma (gg), gamma-electron (ge) interactions. Using the laser backscattering method one can obtain gg, ge colliding beams with an energy and luminosity comparable to that in e+e-…

High Energy Physics - Experiment · Physics 2008-11-26 R. Brinkmann , I. Ginzburg , N. Holtkamp , G. Jikia , O. Napoly , E. Saldin , E. Schneidmiller , V. Serbo , G. Silvestrov , V. Telnov , A. Undrus , M. Yurkov

The PEP-II interaction region is designed to accommodate asymmetric beam energies, head-on collisions, small bunch spacing and provide low beta* for high luminosity. Local correction schemes are implemented to compensate non-linear…

Accelerator Physics · Physics 2007-05-23 Y. Nosochkov , Y. Cai , M. H. R. Donald , J. Irwin , D. M. Ritson , J. Seeman , M. Sullivan
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