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Related papers: Ultra-High precision Compton polarimetry at 2 GeV

200 papers

In order to fully exploit the physics potential of the ILC, it will be necessary to measure (and control) beam parameters to a permille level precision. In case of the beam polarisation, this can only be achieved with dedicated high energy…

Instrumentation and Detectors · Physics 2009-02-19 Christoph Bartels , Christian Helebrant , Daniela Käfer , Jenny List

An experiment for the advanced undergraduate laboratory allowing students to directly observe the effect of photon polarisation on Compton scattering is described. An initially unpolarised beam of photons is polarised via Compton scattering…

Physics Education · Physics 2018-02-12 P. Knights , F. Ryburn , G. Tungate , K. Nikolopoulos

One of the most surprising discoveries made at Jefferson Lab has been the discrepancy in the determinations of the proton's form factor ratio $\mu_p G_E^p/G_M^p$ between unpolarized cross section measurements and the polarization transfer…

A beam-normal single-spin asymmetry generated in the scattering of transversely polarized electrons from unpolarized nucleons is an observable related to the imaginary part of the two-photon exchange process. We report a 2% precision…

We propose a feasible scenario to directly polarize a relativistic electron beam and obtain overall polarization in various directions through a filter mechanism for single-shot collision between an ultrarelativistic unpolarized electron…

Accelerator Physics · Physics 2023-04-04 Yuhui Tang , Qianyi Ma , Jinqing Yu , Yinren Shou , Xuezhi Wu , Xueqing Yan

We have measured the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from the proton. The result is A = -15.05 +- 0.98(stat) +- 0.56(syst) ppm at the kinematic point theta_lab = 12.3 degrees and Q^2 =…

Nuclear Experiment · Physics 2010-05-27 HAPPEX collaboration , K. A. Aniol

Double-polarization observables in the reaction $\vec{e}p \rightarrow e'\vec{p'}\gamma{}$ have been measured at $Q^2=0.33 (GeV/c)^2$. The experiment was performed at the spectrometer setup of the A1 Collaboration using the 855 MeV polarized…

J-PET is a detector optimized for registration of photons from the electron-positron annihilation via plastic scintillators where photons interact predominantly via Compton scattering. Registration of both primary and scattered photons…

The physics case and an experimental overview of the MOLLER (Measurement Of a Lepton Lepton Electroweak Reaction) experiment at the 12 GeV upgraded Jefferson Lab are presented. A highlight of the Fundamental Symmetries subfield of the 2007…

Nuclear Experiment · Physics 2014-12-04 MOLLER Collaboration , J. Benesch , P. Brindza , R. D. Carlini , J-P. Chen , E. Chudakov , S. Covrig , M. M. Dalton , A. Deur , D. Gaskell , A. Gavalya , J. Gomez , D. W. Higinbotham , C. Keppel , D. Meekins , R. Michaels , B. Moffit , Y. Roblin , R. Suleiman , R. Wines , B. Wojtsekhowski , G. Cates , D. Crabb , D. Day , K. Gnanvo , D. Keller , N. Liyanage , V. V. Nelyubin , H. Nguyen , B. Norum , K. Paschke , V. Sulkosky , J. Zhang , X. Zheng , J. Birchall , P. Blunden , M. T. W. Gericke , W. R. Falk , L. Lee , J. Mammei , S. A. Page , W. T. H. van Oers , K. Dehmelt , A. Deshpande , N. Feege , T. K. Hemmick , K. S. Kumar , T. Kutz , R. Miskimen , M. J. Ramsey-Musolf , S. Riordan , N. Hirlinger Saylor , J. Bessuille , E. Ihloff , J. Kelsey , S. Kowalski , R. Silwal , G. De Cataldo , R. De Leo , D. Di Bari , L. Lagamba , E. NappiV. Bellini , F. Mammoliti , F. Noto , M. L. Sperduto , C. M. Sutera , P. Cole , T. A. Forest , M. Khandekar , D. McNulty , K. Aulenbacher , S. Baunack , F. Maas , V. Tioukine , R. Gilman , K. Myers , R. Ransome , A. Tadepalli , R. Beniniwattha , R. Holmes , P. Souder , D. S. Armstrong , T. D. Averett , W. Deconinck , W. Duvall , A. Lee , M. L. Pitt , J. A. Dunne , D. Dutta , L. El Fassi , F. De Persio , F. Meddi , G. M. Urciuoli , E. Cisbani , C. Fanelli , F. Garibaldi , K. Johnston , N. Simicevic , S. Wells , P. M. King , J. Roche , J. Arrington , P. E. Reimer , G. Franklin , B. Quinn , A. Ahmidouch , S. Danagoulian , O. Glamazdin , R. Pomatsalyuk , R. Mammei , J. W. Martin , T. Holmstrom , J. Erler , Yu. G. Kolomensky , J. Napolitano , K. A. Aniol , W. D. Ramsay , E. Korkmaz , D. T. Spayde , F. Benmokhtar , A. Del Dotto , R. Perrino , S. Barkanova , A. Aleksejevs , J. Singh

The International Linear Collider (ILC) will collide polarised electrons and positrons at beam energies of 45.6 GeV to 250 GeV and optionally up to 500 GeV. To fully exploit the physics potential of this machine, not only the luminosity and…

Instrumentation and Detectors · Physics 2008-10-13 C. Helebrant , D. Käfer , J. List

We report linear polarization measurements of x rays emitted due to dielectronic recombination into highly charged krypton ions. The ions in the He-like through O-like charge states were populated in an electron beam ion trap with the…

The beam energy measurement system for the VEPP-2000 electron-positron collider is described. The method of Compton backscattering of $CO$ laser photons on the electron beam is used. The relative systematic uncertainty of the beam energy…

We describe a feasible implementation of a novel X-ray detector for highly energetic x-ray photons with a large solid angle coverage, optimal for the detection of Compton x-ray scattered photons. The device consists of a 20~cm-thick…

Instrumentation and Detectors · Physics 2022-01-27 Ángela Saá Hernández , Diego González-Díaz , Pablo Villanueva , Carlos Azevedo , Marcos Seoane

The Compton scattering cross section on the proton has been measured at laboratory angles of 90$^\circ$ and 135$^\circ$ using tagged photons in the energy range 70--100 MeV and simultaneously using untagged photons in the range…

Nuclear Experiment · Physics 2008-11-26 B. E. MacGibbon , G. Garino , M. A. Lucas , A. M. Nathan , G. Feldman , B. Dolbilkin

Research in non-perturbative QED in strong-field backgrounds has gained interest in recent years, due to advances in high-intensity laser technologies that make extreme fields accessible in the laboratory. One key signature of strong-field…

This paper reports the measurement of polarized and unpolarized cross sections for the ep -> e'p' reaction, which is comprised of Deeply Virtual Compton Scattering (DVCS) and Bethe-Heitler (BH) processes, at an electron beam energy of 5.88…

High Energy Physics - Experiment · Physics 2018-10-17 N. Hirlinger Saylor , B. Guegan , V. D. Burkert , L. Elouadrhiri , M. Garcon , F. X. Girod , M. Guidal , H. S. Jo , V. Kubarovsky , S. Niccolai , P. Stoler

Compton scattering of a laser beam with a relativistic electron beam has been used to generate intense, highly polarized and nearly monoenergetic x-ray or gamma-ray beams at many facilities. The ability to predict the spatial, spectral and…

Accelerator Physics · Physics 2011-05-09 Changchun Sun , Ying K. Wu

In view of the realistic possibility for operating high-energy polarized proton beams in future collider machines, it is highly desirable to propose for such beams, an absolute calibration allowing to measure accurately their degree of…

High Energy Physics - Phenomenology · Physics 2009-09-25 C. Bourrely , J. Soffer

The spin polarizabilities of the nucleon describe how the spin of the nucleon responds to an incident polarized photon. The most model-independent way to measure the nucleon spin polarizabilities is through polarized Compton scattering.…

Polarization characteristics of the gamma beam obtained by the Compton back scattering of laser photons on high energy electrons are evaluated by Monte-Carlo simulations. It is assumed that outgoing photons are tagged; the energy dispersion…

Instrumentation and Detectors · Physics 2007-05-23 A. S. Omelaenko , Yu. P. Peresunko , Yu. M. Ranyuk , I. M. Shapoval , V. G. Nedorezov