English
Related papers

Related papers: Introduction and recent developments in gamma-gamm…

200 papers

The progressive development of high power lasers over the last several decades, enables the study of $\gamma$-photon generation when an intense laser beam interacts with matter, mainly via inverse Compton scattering at the high intensity…

As part of the Snowmass'21 community planning excercise, the Advanced Accelerator Concepts (AAC) community proposed future linear colliders with center-of-mass energies up to 15 TeV and luminosities up to 50$\times10^{34}$ cm$^{-2}$s$^{-1}$…

We investigate the effects of unparticles on Compton scattering, e gamma -> e gamma based on a future e^+e^- linear collider such as the CLIC. For different polarization configurations, we calculate the lower limits of the unparticle energy…

High Energy Physics - Phenomenology · Physics 2008-11-26 O. Cakir , K. O. Ozansoy

I discuss a proposal for a high intensity $e^+e^-$ linear collider operated at low center of mass energies $\sqrt{s}<5$ GeV with high intensity beams. Such a facility would provide high statistics samples of (charmed) vector mesons and…

High Energy Physics - Experiment · Physics 2007-05-23 A. Schoning

For the first time, the production of a massive dark photon (DP) in the $\gamma e^-$ scattering at the future lepton colliders ILC, CLIC, and CEPC is examined. The invisible decay mode of the DP is addressed. We have studied both the…

High Energy Physics - Phenomenology · Physics 2022-07-13 S. C. İnan , A. V. Kisselev

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

In a strongly-interacting electroweak sector with an isosinglet vector state, such as the techni-omega, $\omega_T$, the direct $\omega_T Z \gamma $ coupling implies that an $\omega_T$ can be produced by $Z \gamma$ fusion in $e\gamma$…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stephen Godfrey , Tao Han , Pat Kalyniak

In a strongly-interacting electroweak sector with an isosinglet vector state, such as the techni-omega, $\omega_T$, the direct $ \omega_T Z \gamma $ coupling implies that an $\omega_T$ can be produced by $Z \gamma$ fusion in $e \gamma$…

High Energy Physics - Phenomenology · Physics 2007-05-23 Stephen Godfrey , Tao Han , Pat Kalyniak

High intensity back-scattered laser beams will allow the efficient conversion of a substantial fraction of the incident lepton energy into high energy photons, thus significantly extending the physics capabilities of an electron-electron or…

High Energy Physics - Phenomenology · Physics 2009-09-11 S. J. Brodsky

We study signatures of heavy Majorana neutrinos at e- gamma colliders. Since these particles violate lepton number, they can give rise to the reactions e- gamma -> W- W- e+ and e- gamma -> W+ mu- mu- nu. The Standard Model background…

High Energy Physics - Phenomenology · Physics 2010-04-05 Simon Bray , Jae Sik Lee , Apostolos Pilaftsis

The process gamma gamma -> l+ l- is highly suppressed when the total angular momentum of the two colliding photons is zero so that it cannot be used for luminosity determination. This configuration, however is needed for Higgs production at…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. Makarenko , K. Moenig , T. Shishkina

Drees and Godbole have proposed that, at the interaction point of an e+e- linear collider, one expects a high rate of hadron production by gamma-gamma collisions, providing an additional background to studies in e+e- annihilation. Using a…

High Energy Physics - Phenomenology · Physics 2009-10-22 Pisin Chen , Timothy L. Barklow , Michael E. Peskin

Laser-plasma technology promises a drastic reduction of the size of high energy electron accelerators. It could make free electron lasers available to a broad scientific community, and push further the limits of electron accelerators for…

We review the most important topics and objectives of the physics program of the gamma-gamma, gamma-electron collider (photon collider) option for an e+e- linear collider.

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Boos , A. De Roeck , I. F. Ginzburg , K. Hagiwara , R. D. Heuer , G. Jikia , J. Kwiecinski , D. J. Miller , T. Takahashi , V. Telnov , T. Rizzo , I. Watanabe , P. M. Zerwas

A novel method of electron beam cooling is considered which can be used for linear colliders. The electron beam is cooled during collision with focused powerful laser pulse. With reasonable laser parameters (laser flash energy about 10 J)…

High Energy Physics - Experiment · Physics 2013-10-25 Valery Telnov

We study the production of jet events containing large rapidity gaps in particle colliders due to the resolved photon mechanism. In particular, we analize these events at DESY HERA and future $e^+e^-$ linear colliders, including the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hung Jung Lu

Compton scattering of photons off high-energy electrons is a fundamental quantum mechanical process widely utilized to produce a $\gamma$-ray beam for scientific research. Instead of injecting laser light into a storage ring as a…

Data from the Large Electron Positron collider (LEP) at CERN on hadron production in gamma-gamma interactions exceed the predictions of the standard model by an order of magnitude at the highest observed transverse momenta in three…

High Energy Physics - Phenomenology · Physics 2009-08-20 Philip Yock

The collisions of high energy photons produced at an electron-positron collider provide a comprehensive laboratory for testing QCD, electroweak interactions, and extensions of the Standard Model. The luminosity and energy of the colliding…

High Energy Physics - Phenomenology · Physics 2009-09-25 Stanley J. Brodsky , SLAC , Peter M. Zerwas , DESY

We discuss diphoton semi(exclusive) production in ultraperipheral lead-lead collisions at energy of $\sqrt{s_{NN}}$ = 5.5 TeV (LHC) and in proton-proton collisions at $\sqrt{s_{pp}}$ = 7 TeV (LHC) and $\sqrt{s_{pp}}$ = 100 TeV (FCC). The…

High Energy Physics - Phenomenology · Physics 2017-11-16 Antoni Szczurek , Mariola Klusek-Gawenda
‹ Prev 1 3 4 5 6 7 10 Next ›