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Related papers: Deuteron photodisintegration with polarized lasers

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Deuteron Compton scattering is calculated to $\mathcal{O}(Q^2)$ in pionless effective field theory using a dibaryon approach. The vector amplitude, which was not included in the previous pionless calculations, contributes to the cross…

Nuclear Theory · Physics 2009-11-10 Jiunn-Wei Chen , Xiangdong Ji , Yingchuan Li

For deuteron photo- and electrodisintegration the selection of complete sets of polarization observables is discussed in detail by applying a recently developed new criterion for the check of completeness of a chosen set of observables. The…

Nuclear Theory · Physics 2009-10-31 Hartmuth Arenhoevel , Winfried Leidemann , Edward L. Tomusiak

We extend the original idea of reduced nuclear amplitudes to capture individual helicity amplitudes and discuss various applications to exclusive processes involving the deuteron. Specifically, we consider deuteron form factors, structure…

Nuclear Theory · Physics 2023-05-03 J. Flores , S. S. Chabysheva , J. R. Hiller

A general formalism for the calculation of the differential cross section and polarization observables, for the process of deuteron electrodisintegration, is developed in the framework of relativistic impulse approximation. A detailed…

High Energy Physics - Phenomenology · Physics 2012-06-06 G. I. Gakh , A. P. Rekalo , Egle Tomasi-Gustafsson

We apply the chiral potential with the momentum space semi-local regularization to the $^2$H and $^3$He photodisintegration processes and to the (anti)neutrino induced deuteron breakup reactions. Specifically, the differential cross…

Nuclear Theory · Physics 2021-02-17 V. Urbanevych , R. Skibiński , H. Witała , J. Golak , K. Topolnicki , A. Grassi , E. Epelbaum , H. Krebs

The beam-spin asymmetry, $\Sigma$, for the reaction $\gamma d\rightarrow pn$ has been measured using the CEBAF Large Acceptance Spectrometer (CLAS) at the Thomas Jefferson National Accelerator Facility (JLab) for six photon-energy bins…

Nuclear Experiment · Physics 2019-08-13 Nicholas Zachariou , Yordanka Ilieva , Nikolay Ya. Ivanov , Misak M Sargsian , Robert Avakian , Gerald Feldman , Pawel Nadel-Turonski , K. P. Adhikari , D. Adikaram , M. D. Anderson , S. Anefalos Pereira , H. Avakian , R. A. Badui , N. A. Baltzell , M. Battaglieri , V. Baturin , I. Bedlinskiy , A. S. Biselli , W. J. Briscoe , W. K. Brooks , V. D. Burkert , T. Cao , D. S. Carman , A. Celentano , S. Chandavar , G. Charles , L. Colaneri , P. L. Cole , N. Compton , M. Contalbrigo , O. Cortes , V. Crede , A. D'Angelo , R. De Vita , E. De Sanctis , A. Deur , C. Djalali , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , G. Fedotov , S. Fegan , A. Filippi , J. A. Fleming , T. A. Forest , A. Fradi , N. Gevorgyan , Y. Ghandilyan , G. P. Gilfoyle , K. L. Giovanetti , F. X. Girod , D. I. Glazier , E. Golovatch , R. W. Gothe , K. A. Griffioen , M. Guidal , K. Hafidi , C. Hanretty , N. Harrison , M. Hattawy , K. Hicks , D. Ho , M. Holtrop , S. M. Hughes , D. G. Ireland , B. S. Ishkhanov , E. L. Isupov , H. Jiang , H. S. Jo , K. Joo , D. Keller , G. Khachatryan , M. Khandaker , A. Kim , W. Kim , F. J. Klein , V. Kubarovsky , P. Lenisa , K. Livingston , H. Y. Lu , I . J . D. MacGregor , N. Markov , P. T. Mattione , B. McKinnon , T. Mineeva , M. Mirazita , V. I. Mokeeev , R. A. Montgomery , H. Moutarde , C. Munoz Camacho , L. A. Net , S. Niccolai , G. Niculescu , I. Niculescu , M. Osipenko , A. I. Ostrovidov , K. Park , E. Pasyuk , W. Phelps , J. J. Phillips , S. Pisano , O. Pogorelko , S. Pozdniakov , J. W. Price , S. Procureur , Y. Prok , D. Protopopescu , A. J. R. Puckett , M. Ripani , A. Rizzo , G. Rosner , P. Rossi , P. Roy , F. Sabatié , C. Salgado , D. Schott , R. A. Schumacher , E. Seder , I. Senderovich , Y. G. Sharabian , Iu. Skorodumina , G. D. Smith , D. I. Sober , D. Sokhan , N. Sparveris , S. Stepanyan , S. Strauch , V. Sytnik , M. Taiuti , Ye Tian , M. Ungaro , H. Voskanyan , E. Voutier , N. K. Walford , D. Watts , X. Wei , M. H. Wood , L. Zana , J. Zhang , Z. W. Zhao , I. Zonta

The two-body photodisintegration of 3He has been investigated using tagged photons with energies from 14 -- 31 MeV at MAX-lab in Lund, Sweden. The two-body breakup channel was unambiguously identified by the (nonsimultaneous) detection of…

Nuclear fusion in ultra-dense deuterium D(-1) induced by 0.2 J pulses with 5 ns pulse length ejects ions with energies in the MeV range. The ns-resolved signal to a collector can be observed directly on an oscilloscope, showing ions…

Instrumentation and Detectors · Physics 2019-04-30 Leif Holmlid

Spin polarization observables of the deuteron photodisintegration at low energies are studied in a pionless effective field theory up to next-to-next-to-leading order (NNLO). The total and differential cross sections, induced neutron…

Nuclear Theory · Physics 2017-07-19 Young-Ho Song , Shung-Ichi Ando , Chang Ho Hyun

A complete set of linearly independent observables in Compton scattering with arbitrarily polarised real photons off an arbitrarily polarised spin-1 target is introduced, for the case that the final-state polarisations are not measured.…

Nuclear Theory · Physics 2018-04-12 Harald W. Griesshammer

It is known that the linearly polarized photons can partly transform to circularly polarized ones via forward Compton scattering in a background such as the external magnetic field or noncommutative space time. Based on this fact we explore…

High Energy Physics - Phenomenology · Physics 2017-03-08 S. Tizchang , S. Batebi , M. Haghighat , R. Mohammadi

We calculate P-odd difference of the total cross-sections of the deuteron disintegration by left and right polarized photons. The relative magnitude of this difference in the threshold region is about 10^{-7}. Its experimental measurement…

Nuclear Theory · Physics 2007-05-23 I. B. Khriplovich , R. V. Korkin

Incoherent pion photoproduction on the deuteron is studied in the first resonance region. The unpolarized cross section, the beam asymmetry, and the vector and tensor target asymmetries are calculated in the framework of a diagrammatic…

Nuclear Theory · Physics 2009-11-11 M. I. Levchuk , A. Yu. Loginov , A. A. Sidorov , V. N. Stibunov , M. Schumacher

Deuteron-proton elastic scattering is considered at the energies from 880 MeV to 2 GeV at the scattering angles $\theta^*\ge 140^\circ$. The multiple-scattering method is used to calculate the reaction amplitude. Four reaction mechanisms…

Nuclear Theory · Physics 2024-07-02 Nadezhda Ladygina

Recent years have seen much activity in searches for dark-sector messenger particles in the 10-100 MeV mass range, especially in view of a potential new light boson conjectured by the ATOMKI collaboration, X17. Under the assumption that the…

High Energy Physics - Phenomenology · Physics 2024-04-26 Cornelis J. G. Mommers , Marc Vanderhaeghen

The first measurements of the differential cross section for the d(gamma,p)n reaction up to 4.0 GeV were performed at Continuous Electron Beam Accelerator Facility (CEBAF) at Jefferson Lab. We report the cross sections at the proton…

Nuclear Experiment · Physics 2012-08-27 012 Collaboration , C. Bochna , B. P. Terburg et al

We report measurements of differential cross sections and decay asymmetries of incoherent $\phi$-meson photoproduction from the deuteron at forward angles using linearly polarized photons at \Eg=1.5-2.4 GeV. The nuclear transparency ratio…

We built a Low Energy Deuteron Polarimeter which measures the spin-polarization of deuteron beams in the energy range of 25 to 80 keV. This polarimeter works by measuring azimuthal asymmetries in the D(\vec d, n)^{3}He reaction and…

Nuclear Experiment · Physics 2015-07-14 Michael Bellos

Three (or four) straightforward experiments would contribute greatly to completing the spectroscopy of baryons and light mesons. In the baryon sector, data are needed on inelastic reactions from a polarised target with pi and kaon beams up…

High Energy Physics - Experiment · Physics 2009-12-17 D. V. Bugg