A high-luminosity factory linear collider using positron recirculation and recovery

Author(s):  
D. Cline ◽  
C. Pellegrini
2000 ◽  
Vol 15 (16) ◽  
pp. 2455-2460
Author(s):  
PAUL H. FRAMPTON

Theoretical background for bileptonic gauge bosons is reviewed — both the SU(15) GUT model and the 3-3-1 model. Mass limits on bileptons are discussed coming from e+e- scattering, polarized muon decay and muonium–antimuonium conversion. Discovery in e-e- at a linear collider at low energy (100 GeV) and high luminosity (1033/cm2/s) is emphasized.


2021 ◽  
Vol 16 (12) ◽  
pp. P12025
Author(s):  
V.I. Telnov

Abstract Superconducting technology makes it possible to build a high energy e+e- linear collider with energy recovery (ERLC) and reusable beams. To avoid parasitic collisions inside the linacs, a twin (dual) LC is proposed. In this article, I consider the principle scheme of the collider and estimate the achievable luminosity, which is limited by collision effects and available power. Such a collider can operate in a duty cycle (DC) and in a continuous (CW) modes, if sufficient power. With current SC Nb technology (T = 1.8 K, f RF = 1.3 GHz, used for ILC) and with power P = 100 MW, a luminosity L ∼ 0.33 × 1036 cm-2 s-1 is possible at the Higgs factory with 2E 0 = 250 GeV. Using superconductors operating at 4.5 K with high Q 0 values, such as Nb3Sn, and f RF = 0.65 GHz, the luminosity can reach L ∼ 1.4 × 1036 cm-2 s-1 at 2EE0 = 250 GeV (with P = 100 MW) and L ∼ 0.8 × 1036 cm-2 s-1 at 2E 0 = 500 GeV (with P = 150 MW), which is almost two orders of magnitude greater than at the ILC, where the beams are used only once. This technology requires additional efforts to obtain the required parameters and reliably operation. Such a collider would be the best machine for precision Higgs studies, including the measurement of Higgs self-coupling.


Author(s):  
Erik Adli

A linear electron-positron collider operating at TeV-scale energies will provide high precision measurements and allow, for example, precision studies of the Higgs boson as well as searches for physics beyond the standard model. A future linear collider should produce collisions at high energy, with high luminosity and with a good wall plug to beam power transfer efficiency. The luminosity per power consumed is a key metric that can be used to compare linear collider concepts. The plasma wakefield accelerator has demonstrated high-gradient, high-efficiency acceleration of an electron beam and is therefore a promising technology for a future linear collider. We will go through the opportunities of using plasma wakefield acceleration technology for a collider, as well as a few of the collider-specific challenges that must be addressed in order for a high-energy, high luminosity-per-power plasma wakefield collider to become a reality. This article is part of the Theo Murphy meeting issue ‘Directions in particle beam-driven plasma wakefield acceleration’.


2000 ◽  
Vol 15 (16) ◽  
pp. 2387-2396
Author(s):  
WOLFGANG KILIAN

If no Higgs boson exists, scattering amplitudes of massive vector bosons become strong at TeV energies. Below the threshold where new resonances appear, they are described by an effective chiral Lagrangian, which introduces a small number of new universal parameters at each order of a low-energy expansion. These parameters can be measured in (quasi-)elastic scattering processes of massive vector bosons in e-e± collisions. Analyzing processes such as e-e-→νeνeW-W-, a sensitivity of the order 10-2 can be reached at a high-luminosity 1 TeV linear collider.


2000 ◽  
Vol 15 (16) ◽  
pp. 2543-2554 ◽  
Author(s):  
J. E. SPENCER

Effects that limit the luminosities of a general purpose linear collider (GLC) capable of [Formula: see text] and [Formula: see text] channels are discussed together with mitigations. Previous results are extended to understand the differences between channels to maximize the generalized luminosity. A standard NLC configuration at [Formula: see text] is used for comparison. Without charge compensation or bunch shaping, such flat beam configurations (aspect ratios R*≫1) imply major disadvantages for e-e- due to the strong disruption (D) and small, longitudinal f-numbers [Formula: see text] that are imposed. Previous round and flat beam configurations are studied as functions of D (or fb#), fl# and the constraints ΔB, Nγ and ϒ. Round beams with decreased disruptions and larger fl-stops are preferred with tensor beams, charge compensation or other bunch manipulation schemes. A low energy, high luminosity prototype is again proposed based on the possible physics.


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