scholarly journals Preliminary design report of a relativistic-Klystron two-beam-accelerator based power source for a 1 TeV center-of-mass next linear collider

1995 ◽  
Author(s):  
S. Yu ◽  
N. Goffeney ◽  
E. Henestroza
1995 ◽  
Author(s):  
S. Yu ◽  
F. Deadrick ◽  
N. Goffeney ◽  
E. Henestroza ◽  
T. Houck ◽  
...  

Author(s):  
G.V. Dolbilov ◽  
I.N. Ivanov ◽  
N.I. Azorsky ◽  
V.S. Shvetsov ◽  
V.E. Balakin ◽  
...  

Author(s):  
Dan Yu ◽  
Manqi Ruan ◽  
Vincent Boudry ◽  
Henri Videau ◽  
Jean-Claude Brient ◽  
...  

AbstractThe Circular Electron Positron Collider and the International Linear Collider are two electron-positron Higgs factories. They are designed to operate at a center-of-mass energy of 240 and 250 GeV and accumulate 5.6 and 2 $$ab^{-1}$$ab-1 of integrated luminosity. This paper estimates their performance on the $$H \rightarrow \tau ^{+}\tau ^{-}$$H→τ+τ- benchmark measurement. Using the full simulation analysis, the CEPC is expected to measure the signal strength to a relative accuracy of 0.8%. Extrapolating to the ILC setup, we conclude the ILC can reach a relative accuracy of 1.1% or 1.2%, corresponding to two benchmark beam polarization setups. The physics requirement on the mass resolution of the Higgs boson with hadronic decay final states is also discussed, showing that the CEPC baseline design and reconstruction fulfill the accuracy requirement of the $$H\rightarrow \tau ^{+}\tau ^{-}$$H→τ+τ- signal strength.


2001 ◽  
Vol 16 (supp01c) ◽  
pp. 1190-1192
Author(s):  
◽  
WINFRIED DECKING

The international TESLA collaboration proposes a 500-800 GeV center-of-mass linear collider based on super-conducting 1.3 GHz cavities. This technology promises a luminosity of 3.4×1034 cm-2 s-1. Results from the cavity R&D program at the TESLA test facility and details of the collider design will be presented.


1999 ◽  
Author(s):  
S. M. Lidia ◽  
D. E. Anderson ◽  
S. Eylon ◽  
E. Henestroza ◽  
T. L. Houck ◽  
...  

2001 ◽  
Vol 16 (supp01c) ◽  
pp. 1193-1196
Author(s):  
T. O. Raubenheimer

An electron/positron linear collider with a center-of-mass energy between 0.5 and 1 TeV would be an important complement to the physics program of the LHC in the next decade. The Next Linear Collider (NLC) is being designed by a US collaboration (FNAL, LBNL, LLNL, and SLAC) which is working closely with the Japanese collaboration that is designing the Japanese Linear Collider (JLC). This paper will discuss the technical difficulties encountered as well as the changes that have been made to the NLC design over the last year. These changes include improvements to the X-band rf system as well as modifications to the beam delivery system. The net effect has been to reduce the length of the collider from about 32 km to 25 km and to reduce the number of klystrons and modulators by a factor of two. Together these lead to significant cost savings.


1993 ◽  
Vol 08 (24) ◽  
pp. 2237-2248 ◽  
Author(s):  
◽  
K. ABE ◽  
I. ABT ◽  
P. D. ACTON ◽  
C. E. ADOLPHSEN ◽  
...  

We present the first measurement of the left-right cross-section asymmetry (A LR ) in Z-boson production observed at the SLAC Linear Collider. In 1992 the SLD detector recorded 10 224 Z events produced by the collision of longitudinally polarized electrons with an unpolarized positron beam at a center-of-mass energy of 91.55 GeV. The average electron beam polarization during the run was (22.4 ± 0.6)%. We measure A LR to be 0.100 ± 0.0440 (stat.) ±0.004 (syst.) , which determines the effective weak mixing angle to be [Formula: see text].


2009 ◽  
Vol 24 (28n29) ◽  
pp. 5299-5318 ◽  
Author(s):  
A. GUTIÉRREZ-RODRÍGUEZ ◽  
M. A. HERNÁNDEZ-RUÍZ ◽  
O. A. SAMPAYO

We study pair-production as well as the triple self-couplings of the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) at the future International Linear e+e-Collider (ILC) and Compact Linear Collider (CLIC). The analysis is based on the reactions [Formula: see text] with hi= h, H, A. We evaluate the total cross-section for both [Formula: see text] and calculate the total number of events considering the complete set of Feynman diagrams at tree-level. We vary the triple couplings κλhhh, κλHhh, κλhAA, κλHAA, κλhHHand κλHHHwithin the range κ = -1 and +2. The numerical computation is done for the energies expected at the ILC with a center-of-mass energy 500, 1000, 1600 GeV and a luminosity 1000 fb-1. The channels [Formula: see text] and [Formula: see text] are also discussed to a center-of-mass energy of 3 TeV and luminosities of 1000 fb-1and 5000 fb-1.


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