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Subthreshold rho-0 Photoproduction on 2H, 3He and 12C  [PDF]
G. J. Lolos
Physics , 2001,
Abstract: The rho-0 has been photoproduced using tagged photon energies in the 700-1120 MeV region on 2H, 3He and 12C by utilizing the Fermi momentum of the bound nucleons to produce the rho-0. These energies lie mostly below the production threshold on the free proton. Large mass modifications are indicated from the analysis, together with large polarizations of the produced rho-0 mesons with helicity zero, unlike the case of coherent rho-0 production on nuclei.
Subthreshold $K^+$ Production on Nuclei by $π^+$ Mesons  [PDF]
S. V. Efremov,E. Ya. Paryev
Physics , 1995,
Abstract: The inclusive $K^+$ mesons production in $\pi^+$--nucleus reactions in the subthreshold energy regime is analyzed with respect to the one--step ($\pi^+n\to K^+\Lambda$) and the two--step ($\pi^+n\to \eta p_1,~ \eta p_2\to K^+\Lambda$) incoherent production processes on the basis of an appropriate folding model, which allows one to take into account the various forms of an internal nucleon momentum distribution as well as on-- and off--shell propagation of the struck target nucleon. Contrary to proton--nucleus reactions primary reaction channel is found to be significant practically at all considered energies. Detailed predictions for the $K^+$ total and invariant differential cross sections from \piC-- and \piPb--collisions at subthreshold energies are provided.
Signatures of primordial helicity in the CMBR  [PDF]
Levon Pogosian,Tanmay Vachaspati,Serge Winitzki
Physics , 2002, DOI: 10.1016/j.newar.2003.07.017
Abstract: We have studied ways in which helical primordial magnetic fields could be constrained by measurements of the cosmic microwave background radiation (CMBR). If there were helical flows in the primordial plasma at the time of recombination, they would produce parity violating temperature-polarization correlations ($C_l^{TB}$ and $C_l^{EB}$). However, the magnitude of helical flows induced by helical magnetic fields is unobservably small. We discuss an alternate scheme for extracting the helicity of a stochastically homogeneous and isotropic primordial magnetic field using Faraday rotation measure maps of the CMBR and the power spectrum of B-type polarization ($C_l^{BB}$).
Subthreshold rho^0 photoproduction on 3He  [PDF]
TAGX Collaboration,M. A. Kagarlis,Z. Papandreou,G. M. Huber,G. J. Lolos,A. Shinozaki,E. J. Brash,F. Farzanpay,M. Iurescu,A. Weinerman,G. Garino,K. Maruyama,O. Konno,K. Maeda,T. Terasawa,H. Yamazaki,T. Emura,H. Hirosawa,K. Niwa,H. Yamashita,S. Endo,K. Miyamoto,Y. Sumi,A. Leone,R. Perrino,T. Maki,A. Sasaki,J. C. Kim
Physics , 1998, DOI: 10.1103/PhysRevC.60.025203
Abstract: A large reduction of the rho^0 mass in the nuclear medium is reported, inferred from dipion photoproduction spectra in the 1 GeV region, for the reaction 3He(gamma,pi+ pi-)X with a 10% duty factor tagged-photon beam and the TAGX multi-particle spectrometer. The energy range covered (800 < E(gamma) < 1120 MeV) lies mostly below the free rho^0 production threshold, a region which is believed sensitive to modifications of light vector-meson properties at nuclear-matter densities. The rho^0 masses extracted from the MC fitting of the data, m*(rho^0) = 642 +/- 40, 669 +/- 32, and 682 +/- 56 MeV/c^2 for E(gamma) in the 800-880, 880-960, and 960-1040 MeV regions respectively, are independently corroborated by a measured, assumption-free, kinematical observable. This mass shift, far exceeding current mean-field driven theoretical predictions, may be suggestive of rho^0 decay within the range of the nucleonic field.
Subthreshold rho contribution in J/psi decay to omega pion pion and Kaon anti-Kaon pion  [PDF]
F. Q. Wu,B. S. Zou
Physics , 2006, DOI: 10.1103/PhysRevD.73.114008
Abstract: We carry out a theoretical and Monte Carlo study on the $J/\psi$ decays into $\omega\pi\pi$ and $K\bar{K}\pi$ through intermediate subthreshold $\rho$ meson by using SU(3)-symmetric Lagrangian approach. It is found that the subthreshold $\rho$ contribution is not negligible and may have significant influence on partial wave analysis of resonances in these channels, especially near the $\omega \pi$ and $K \bar{K}$ thresholds.
Signatures of kinetic and magnetic helicity in the CMBR  [PDF]
Levon Pogosian,Tanmay Vachaspati,Serge Winitzki
Physics , 2001, DOI: 10.1103/PhysRevD.65.083502
Abstract: P and CP violation in cosmology can be manifested as large-scale helical velocity flows in the ambient plasma and as primordial helical magnetic fields. We show that kinetic helicity at last scattering leads to temperature-polarization correlations ($C_l^{TB}$ and $C_l^{EB}$) in the cosmic microwave background radiation (CMBR) and calculate the magnitude of the effect. Helical primordial magnetic fields, expected from cosmic events such as electroweak baryogenesis, can lead to helical velocity flows and hence to non-vanishing correlations of the temperature and B-type polarization. However we show that the magnitude of the induced helical flow is unobservably small because the helical component of a magnetic field is almost force-free. We discuss an alternate scheme for extracting the helicity of a stochastically homogeneous and isotropic primordial magnetic field using observations of the CMBR. The scheme involves constructing Faraday rotation measure maps of the CMBR and thus determining the sum of the helical and non-helical components of the primordial magnetic field. The power spectrum of B-type polarization fluctuations, on the other hand, are sensitive only to the non-helical component of the primordial magnetic field. The primordial magnetic helicity can then be derived by combining these two sets of observations.
Measurements of the Branching Fractions and Helicity Amplitudes in B --> D* rho Decays  [PDF]
CLEO Collaboration,S. E. Csorna
Physics , 2003, DOI: 10.1103/PhysRevD.67.112002
Abstract: Using 9.1 fb-1 of e+ e- data collected at the Upsilon(4S) with the CLEO detector using the Cornell Electron Storage Ring, measurements are reported for both the branching fractions and the helicity amplitudes for the decays B- -> D*0 rho- and B0bar -> D*+ rho-. The fraction of longitudinal polarization in B0bar -> D*+ rho- is found to be consistent with that in B0bar -> D*+ l- nubar at q^2 = M^2_rho, indicating that the factorization approximation works well. The longitudinal polarization in the B- mode is similar. The measurements also show evidence of non-trivial final-state interaction phases for the helicity amplitudes.
Rho-0 Meson Helicity Amplitude Ratios at HERMES  [PDF]
Morgan Murray
Physics , 2012,
Abstract: The study of {\rho}0 meson helicity amplitude ratios at HERMES shows that the amplitude hierarchy expected from pQCD is confirmed. The contribution of Unnatural Parity Exchange in the production of {\rho}0 mesons is significant at HERMES kinematics and there is a large phase-difference in the leading F11 and F01 amplitudes. The kinematic dependences of the amplitude ratios only sometimes follow theory-based expectations.
Ratios of Helicity Amplitudes for Exclusive rho-0 Electroproduction  [PDF]
The HERMES Collaboration,A. Airapetian,N. Akopov,Z. Akopov,E. C. Aschenauer,W. Augustyniak,R. Avakian,A. Avetissian,E. Avetisyan,S. Belostotski,N. Bianchi,H. P. Blok,A. Borissov,J. Bowles,V. Bryzgalov,J. Burns,M. Capiluppi,G. P. Capitani,E. Cisbani,G. Ciullo,M. Contalbrigo,P. F. Dalpiaz,W. Deconinck,R. De Leo,L. De Nardo,E. De Sanctis,M. Diefenthaler,P. Di Nezza,M. Dueren,M. Ehrenfried,G. Elbakian,F. Ellinghaus,R. Fabbri,A. Fantoni,L. Felawka,S. Frullani,D. Gabbert,G. Gapienko,V. Gapienko,F. Garibaldi,G. Gavrilov,V. Gharibyan,F. Giordano,S. Gliske,M. Golembiovskaya,C. Hadjidakis,M. Hartig,D. Hasch,G. Hill,A. Hillenbrand,M. Hoek,Y. Holler,I. Hristova,Y. Imazu,A. Ivanilov,H. E. Jackson,H. S. Jo,S. Joosten,R. Kaiser,G. Karyan,T. Keri,E. Kinney,A. Kisselev,N. Kobayashi,V. Korotkov,V. Kozlov,P. Kravchenko,V. G. Krivokhijine,L. Lagamba,R. Lamb,L. Lapikas,I. Lehmann,P. Lenisa,L. A. Linden-Levy,A. Lopez Ruiz,W. Lorenzon,X. -G. Lu,X. -R. Lu,B. -Q. Ma,D. Mahon,N. C. R. Makins,S. I. Manaenkov,L. Manfre,Y. Mao,B. Marianski,A. Martinez de la Ossa,H. Marukyan,C. A. Miller,Y. Miyachi,A. Movsisyan,V. Muccifora,M. Murray,A. Mussgiller,E. Nappi,Y. Naryshkin,A. Nass,M. Negodaev,W. -D. Nowak,L. L. Pappalardo,R. Perez-Benito,N. Pickert,P. E. Reimer,A. R. Reolon,C. Riedl,K. Rith,G. Rosner,A. Rostomyan,J. Rubin,D. Ryckbosch,Y. Salomatin,F. Sanftl,A. Schaefer,G. Schnell,K. P. Schueler,B. Seitz,T. -A. Shibata,V. Shutov,M. Stancari,M. Statera,E. Steffens,J. J. M. Steijger,F. Stinzing,S. Taroian
Physics , 2010, DOI: 10.1140/epjc/s10052-011-1609-2
Abstract: Exclusive rho^0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 GeV^2 < Q^2 < 7.0 GeV^2, 3.0 GeV < W < 6.3 GeV, and -t' < 0.4 GeV^2. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T_{11} (\gamma^*_T --> \rho_T), T_{01} (\gamma^*_T --> \rho_L), T_{10} (\gamma^*_L --> \rho_T), and T_{1-1} (\gamma^*_{-T} -->\rho_T) to T_{00} (\gamma^*_L --> \rho_L) are extracted from the data. For the unnatural-parity-exchange amplitude U_{11}, the ratio |U_{11}/T_{00}| is obtained. The Q^2 and t' dependences of these ratios are presented and compared with perturbative QCD predictions.
Rho-meson mass in light nuclei  [PDF]
K. Saito,K. Tsushima,A. W. Thomas
Physics , 1997, DOI: 10.1103/PhysRevC.56.566
Abstract: The quark-meson coupling (QMC) model is applied to a study of the mass of the $\rho$-meson in helium and carbon nuclei. The average mass of a $\rho$-meson formed in $^{3,4}$He and $^{12}$C is expected to be around 730, 690 and 720 MeV, respectively.
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