International linear collider reference design report

Aarons, Gerald

doi:10.2172/929487

Cited by 40 publications

(45 citation statements)

References 15 publications

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“…(A.35) and (A.36). Writing dp 2 T = 2p T dp T , we arrive at our final result, 14 dσ dp T = Bp T 8πξs 3 …”

Section: Jhep01(2011)138mentioning

confidence: 93%

“…Indeed, there is a rich program of precision supersymmetry proposed for an experimental program at the ILC [3]. However, until the ILC becomes a reality (current projections suggest that this is unlikely during the present decade), we must rely on the LHC running at high luminosity to provide the necessary data for interpreting the fundamental nature of new physics discoveries.…”

Section: Jhep01(2011)138mentioning

confidence: 99%

“…It was found that for very light dark matter, below 5 GeV, the inferred Tevatron bounds are stronger than those from direct detection. 3 Pair production of dark matter particles in association with one or more jets at Tevatron and LHC, was also considered in ref. [46].…”

Section: Jhep01(2011)138mentioning

confidence: 99%

“…[53].) If the higgsino component were dominant, 3 Although the absence of direct detection signals is always subject to a potentially large systematic of unknown density of dark matter at the site of the experiment. 4 Cosmological and laboratory constraints rule out other possible candidates such as the sneutrino [49], gluino [50,51] or charged slepton [52] in almost all possible parameter regimes.…”

Section: The Nature Of the Lspmentioning

confidence: 99%

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Supersymmetric monojets at the Large Hadron Collider

Allanach

Grab

Haber

2011

J. High Energ. Phys.

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Supersymmetric monojets may be produced at the Large Hadron Collider by the process qg → q χ 0 1 → q χ 0 1 χ 0 1 , leading to a jet recoiling against missing transverse momentum. We discuss the feasibility and utility of the supersymmetric monojet signal. In particular, we examine the possible precision with which one can ascertain the χ 0 1 qq coupling via the rate for monojet events. Such a coupling contains information on the composition of the χ 0 1 and helps bound dark matter direct detection cross-sections and the dark matter relic density of the χ 0 1 . It also provides a check of the supersymmetric relation between gauge couplings and gaugino-quark-squark couplings.

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“…(A.35) and (A.36). Writing dp 2 T = 2p T dp T , we arrive at our final result, 14 dσ dp T = Bp T 8πξs 3 …”

Section: Jhep01(2011)138mentioning

confidence: 93%

Section: Jhep01(2011)138mentioning

confidence: 99%

Section: Jhep01(2011)138mentioning

confidence: 99%

Section: The Nature Of the Lspmentioning

confidence: 99%

See 2 more Smart Citations

Supersymmetric monojets at the Large Hadron Collider

Allanach

Grab

Haber

2011

J. High Energ. Phys.

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“…A large volume of phenomenological studies available in this case are summarized in refs. [81][82][83][84]. This process is sensitive to scalar and tensor resonances, as well as the vector resonances arising in gauge boson scattering.…”

Section: Jhep03(2012)060mentioning

confidence: 99%

Probing strongly interacting W’s at the ILC with polarized beams

Ananthanarayan

Patra

Poulose

2012

J. High Energ. Phys.

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Abstract:We study the possibility of fingerprinting a strongly interacting W boson sector which is consistent with present day LHC searches at the ILC with longitudinal as well as transversely polarized electron and positron beams. We account for the final state interaction using a suitable Omnès formalism in terms of a plausible resonance description, and carry out thorough analyses of cross sections, asymmetries and angular distributions of the W ′ s. We carry out a comparison with other extensions of the Standard Model, where heavy additional Z ′ bosons arise naturally. We also consider the effect of the strong final state interaction on a correlation that depends on (φ − − φ + ), where the φ ∓ are the azimuthal angles of decay leptons, and find that it is a useful discriminant.

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Future Developments of Detectors

Behnke¹,

Buesser²,

Mussgiller³

2020

Particle Physics Reference Library

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Large scale detectors in particle physics take many years to plan and to build. The last generation of large particle physics detectors for the energy frontier, ATLAS and CMS, have been operating for more than 10 years, and upgrades for them are now being done. Studies for the next generation of experimental facilities have been ongoing for a number of years. In this section future directions in integrated detector design are discussed, as they were visible at the time of writing this report. At the moment the biggest approved project in particle physics is the upgrade of the Large Hadron Collider (LHC) towards high luminosity running. This project is scheduled to be completed by 2027, and major upgrades to the two main collider detectors ATLAS and CMS are planned. Beyond the LHC, an electron-positron collider has been discussed for many years, to fully explore the Higgs and the top sector and to complement the discovery reach of a hadron machine at the energy frontier with a high precision program. The requirements as far as detectors are concerned are very different for these two types of projects: for the LHC luminosity upgrade fundamental changes to the underlying philosophy of the existing detectors are not possible, but significant technological development is needed to meet the challenges of extreme radiation environments and high event rates. For a yet not existing electron-positron collider a detector can be designed from ground up, optimised to meet the ambitious physics agenda of such a facility.

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International linear collider reference design report

Cited by 40 publications

References 15 publications

Supersymmetric monojets at the Large Hadron Collider

Supersymmetric monojets at the Large Hadron Collider

Probing strongly interacting W’s at the ILC with polarized beams

Future Developments of Detectors

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