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Related papers: Precision Polarimetry at the ILC: Concepts, Simula…

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Compton telescope is a promising technology to achieve very high sensitivity in the soft gamma-ray band (0.1-10 MeV) by utilizing Compton kinematics. Compton kinematics also enables polarization measurement which will open new windows to…

The International Large Detector, ILD, is a detector concept for an experiment at a future high energy lepton collider. The detector has been optimised for precision physics in a range of energies from 90~GeV to about 1~TeV. ILD features a…

High Energy Physics - Experiment · Physics 2025-06-09 H. Abramowicz , D. Ahmadi , J. Alcaraz , O. Alonso , L. Andricek , J. Anguiano , O. Arquero , F. Arteche , D. Attie , O. Bach , M. Basso , J. Baudot , A. Bean , T. Behnke , A. Bellerive , Y. Benhammou , M. Berggren , G. Bertolone , M. Besancon , A. Besson , O. Bezshyyko , G. Blazey , B. Bliewert , J. Bonis , R. Bosley , V. Boudry , C. Bourgeois , I. Bozovic Jelisavcic , D. Breton , J. -C. Brient , B. Brudnowski , V. Buescher , K. Buesser , P. Buhmann , M. Böhler , S. Callier , E. Calvo Alamillo , M. Cepeda , S. Chen , G. Claus , P. Colas , C. Colledani , C. Combaret , R. Cornat , F. Corriveau , J. Cvach , C. De La Taille , K. Desch , H. Diao , A. Dieguez , R. Diener , A. Dorokhov , A. Drutskoy , B. Dudar , A. Dyshkant , I. Echeverria , U. Einhaus , Z. El Bitar , A. Escalante del Valle , M. Fernandez , M. Firlej , T. Fiutowski , I. Fleck , N. Fourches , M. C. Fouz , K. Francis , C. Fu , K. Fujii , T. Fusayasu , J. Fuster , K. Gadow , F. Gaede , J. Galindo , A. Gallas , S. Ganjour , E. Garutti , I. Giomataris , M. Goffe , A. Gonnin , F. González , O. Gonzalez Lopez , I. Gregor , G. Grenier , P. Göttlicher , F. Hartjes , J. Heilman , C. Hensel , S. Hidalgo , A. Himmi , Y. Horii , R. Hosokawa , C. Huo-Guo , M. Idzik , M. Iglesias , F. Ikeda , A. Irles , A. Ishikawa , M. Iwasaki , K. Jaaskelainen , R. Jaramillo , D. Jeans , J. Jeglot , L. Jönsson , G. Kacarevic , M. Kachel , J. Kalinowski , J. Kaminski , Y. Kamiya , T. Kamiyama , Y. Kato , K. Kawagoe , S. A. Khan , J. Klamka , P. Kluit , M. Kobayashi , K. Kong , A. Korol , P. Koppenburg , K. Krüger , M. Kuriki , J. Kvasnicka , D. Lacour , I. Laktineh , A. Laudrain , F. LeDiberder , A. Levy , I. Levy , W. Li , B. List , J. List , J. Liu , A. Lopez Virto , M. Lopez , Y. Lu , B. Lundberg , J. Maalmi , B. Madison , T. Madlener , A. Martens , S. Martens , I. Masamune , L. Masetti , H. Mathez , A. Matsushita , K. McDonald , K. Mekala , G. Milutinovic Dumbelovic , W. Minori , L. Mirabito , W. Mitaroff , V. Mitsou , U. Mjörnmark , T. Mogi , G. Moortgat-Pick , F. Morel , T. Mori , S. Morimasa , J. Moron , D. Moya , T. Murata , E. Musumeci , J. Márquez Hernández , J. Nakajima , E. Nakano , J. Nanni , S. Narita , J. Nilsson , J. Ninkovic , D. Ntounis , T. Nunez , H. Ogawa , K. Oikawa , Y. Okugawa , T. Omori , H. Ono , W. Ootani , C. Orero , A. Oskarsson , L. Osterman , Q. Ouyang , T. Pasquier , G. Pellegrini , H. Pham , J. Piedrafita , I. Polak , A. Pradas , V. Prahl , T. Price , J. Puerta Pelayo , R. Pöschl , H. Qi , Y. Radkhorrami , G. Raven , L. Reichenbach , M. Reinecke , E. Reynolds , F. Richard , R. Richter , S. Ritter , C. Rogan , J. Rolph , A. Rosmanitz , C. Royon , M. Ruan , S. Rudrabhatla , A. Ruiz-Jimeno , A. Sajbel , R. Sakakibara , I. Salehinia , T. Sanuki , H. Sato , C. Schmitt , T. Schoerner-Sadenius , M. Schumacher , V. Schwan , O. Schäfer , F. Sefkow , T. Seino , S. Senyukov , R. Settles , Z. Shen , A. Shoji , F. Simon , I. Smiljanic , M. Specht , T. Suehara , R. Sugawara , A. Sugiyama , Z. Sun , P. Svihra , K. Swientek , T. Takahashi , T. Takatsu , T. Takeshita , S. Tapprogge , P. Terlecki , A. Thiebault , J. Tian , J. Timmermans , M. Titov , L. Tomasek , J. Torndal , B. Tuchming , M. Tytgat , W. Vaginay , I. Valin , C. Vallee , R. van Kooten , H. van der Graaf , C. Vernieri , I. Vidakovic , H. Videau , I. Vila , A. Vilà , M. Vos , N. Vukasinovic , J. Wang , R. Wanke , K. Watanabe , T. Watanabe , N. Watson , J. Wellhausen , U. Werthenbach , G. Wilson , M. Wing , A. Winter , M. Winter , H. Yamamoto , K. Yamamoto , R. Yonamine , T. Yonemoto , J. Zalesak , A. F. Zarnecki , C. Zeitnitz , K. Zembaczynski , D. Zerwas , Y. Zhang , F. Zomer , V. Zutshi

Astrophysical polarization measurements in the soft gamma-ray band are becoming more feasible as detectors with high position and energy resolution are deployed. Previous work has shown that the minimum detectable polarization (MDP) of an…

A new Compton longitudinal polarimeter currently under construction for HERA is presented. The key component of the polarimeter is a Fabry-Perot cavity located around the electron beam pipe. With such an optical cavity, a continuous laser…

High Energy Physics - Experiment · Physics 2007-05-23 Zhiqing Zhang

The full exploitation of the physics potential of a future Linear Collider requires the development of polarised positron beams. A very promising scheme for the technical realisation is the use of helical undulators, generating circular…

High Energy Physics - Phenomenology · Physics 2011-09-13 Gudrid Moortgat-Pick

The value of accurately knowing the absolute calibration of the polarizing elements in the Near Infrared Camera and Multi-Object Spectrometer (NICMOS) becomes especially important when conducting studies which require measuring degrees of…

Astrophysics · Physics 2009-11-11 D. Batcheldor , A. Robinson , D. Axon , D. C. Hines , W. Sparks , C. Tadhunter

A calibration scheme is presented for improved polarization state measurement of terahertz pulses. In this scheme the polarization response of a two-contact terahertz photoconductive detector is accurately measured, and is used to correct…

Optics · Physics 2012-01-25 M. Neshat , N. P. Armitage

Many theoretical efforts were made to understand the core and conal emission identified from observations by Rankin (1983) and Lyne and Manchester (1988). One of them, named as inverse Compton scattering (ICS) model (Qiao & Lin 1998), has…

Astrophysics · Physics 2007-05-23 G. J. Qiao , R. X. Xu , J. F. Liu , B. Zhang J. L. Han

We describe upgrades to a numerical code which computes synchrotron and inverse-Compton emission from relativistic plasma including full polarization. The introduced upgrades concern scattering kernel which is now capable of scattering the…

High Energy Astrophysical Phenomena · Physics 2022-11-16 M. Moscibrodzka

Short-pulse intense lasers have the potential to model extreme astrophysical environments in laboratories. Although there are diagnostics for energetic electrons and ions resulting from laser-plasma interactions, the diagnostics to measure…

The proposed electron-proton collider LHeC is a unique facility where electroweak interactions can be studied with a very high precision in a largely unexplored kinematic regime of spacelike momentum transfer. We have simulated inclusive…

High Energy Physics - Phenomenology · Physics 2020-07-24 Daniel Britzger , Max Klein , Hubert Spiesberger

Interest in highly-compressed electron beams has been increasing in recent times, driven by the study of non-linear and even non-perturbative aspects of QED [2]. The FACET-II [7] facility at SLAC is currently (at the time of writing) being…

Accelerator Physics · Physics 2018-11-30 Glen White , Vitaly Yakimenko

The International Linear Collider has a rich physics programme, whatever lies beyond the standard model. Accurate measurement of the top quark mass is needed to constrain the model or its extensions. If there is a light Higgs boson the LHC…

High Energy Physics - Phenomenology · Physics 2009-11-10 David J. Miller

Laser-electron beam collisions that aim to generate electron-positron pairs require laser intensities $I \gtrsim 10^{21} ~\textrm{W/cm}^2$, which can be obtained by focusing a 1-PW optical laser to a spot smaller than 10 $~\mu$m. Spatial…

Plasma Physics · Physics 2021-11-17 Óscar Amaro , Marija Vranic

At the international linear collider, measurement of the beam profile at the interaction point is a key issue to achieve high luminosity. We report a simulation study on a new beam profile monitor, called the pair monitor, which uses the…

Instrumentation and Detectors · Physics 2015-05-13 Kazutoshi Ito , Akiya Miyamoto , Tadashi Nagamine , Toshiaki Tauchi , Hitoshi Yamamoto , Yosuke Takubo , Yutaro Sato

The POLISH2 optical polarimeter has been in operation at the Lick Observatory 3-m Shane telescope since 2011, and it was commissioned at the Gemini North 8-m in 2016. This instrument primarily targets exoplanets, asteroids, and the Crab…

The past ten years of physics with e+e- colliding experiments at LEP and SLAC have shown the success of these experiments on not only impressively proving the theoretical predictions of the Standard Model (SM), but also to help provide…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Christova , M. Jack , S. Riemann , T. Riemann

The Polarized Atomic Hydrogen Gas Jet Target polarimeter is employed by the Relativistic Heavy Ion Collider (RHIC) to measure the absolute polarization of each colliding proton beam. Polarimeter detectors and data acquisition were upgraded…

High Energy Physics - Experiment · Physics 2019-10-18 A. A. Poblaguev , A. Zelenski , E. Aschenauer , G. Atoian , K. O. Eyser , H. Huang , Y. Makdisi , W. B. Schmidke , I. Alekseev , D. Svirida , N. H. Buttimore

We propose and numerically simulate an optoelectronic compact circular polarimeter. It allows to electrically measure the degree of circular polarization and light intensity at room temperature for a wide range of incidence angles in a…

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