Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where C.F. Perdrisat is active.

Publication


Featured researches published by C.F. Perdrisat.


Physical Review Letters | 2004

Cross sections and transverse single-spin asymmetries in forward neutral-pion production from proton collisions at sqrt[s]=200 GeV.

L. C. Bland; E. Brash; H. J. Crawford; A.A. Derevschikov; K. A. Drees; J. Engelage; C. Folz; M. K. Jones; E. G. Judd; X. Li; N. Liyanage; Y. I. Makdisi; N.G. Minaev; R.N. Munroe; L. Nogach; A. Ogawa; C.F. Perdrisat; C. Perkins; M. Planinic; V. Punjabi; G. Schnell; Goran Simatović; T. G. Throwe; C. Van Hulse; A.N. Vasiliev

Abstract Measurements of the production of forward jets from transversely polarized proton collisions at s = 500 xa0GeV conducted at the Relativistic Heavy Ion Collider (RHIC) are reported. Our measured jet cross section is consistent with hard scattering expectations. Our measured analyzing power for forward jet production is small and positive, and provides constraints on the Sivers functions that are related to partonic orbital angular momentum through theoretical models.


Physical Review Letters | 2003

Polarization transfer in the 4He(e-->,e'p-->)3H reaction up to Q2=2.6 (GeV/c)2.

S. Strauch; S Dieterich; K. A. Aniol; Annand; O. K. Baker; W. Bertozzi; M. Boswell; E. J. Brash; Z. Chai; J. P. Chen; M. E. Christy; E. Chudakov; Cochran A; De Leo R; R. Ent; M. B. Epstein; J. M. Finn; Kevin Fissum; T. A. Forest; S. Frullani; F. Garibaldi; A. Gasparian; Gayou O; S. Gilad; R. Gilman; C. Glashausser; J. Gomez; Gorbenko; P. Gueye; J. O. Hansen

We have measured the proton recoil polarization in the 4He(e-->,e()p-->)4H reaction at Q(2)=0.5, 1.0, 1.6, and 2.6 (GeV/c)(2). The measured ratio of polarization transfer coefficients differs from a fully relativistic calculation, favoring the inclusion of a medium modification of the proton form factors predicted by a quark-meson coupling model. In addition, the measured induced polarizations agree reasonably well with the fully relativistic calculation indicating that the treatment of final-state interactions is under control.


Physical Review Letters | 2002

Measurement of GEp/GMp in ep → ep to Q2 = 5.6 GeV2

O. Gayou; K.A. Aniol; T. Averett; F. Benmokhtar; W. Bertozzi; L. Bimbot; E. J. Brash; J. R. Calarco; C. Cavata; Z. Chai; C. C. Chang; T. Chang; J. P. Chen; E. Chudakov; R. De Leo; S. Dieterich; R. Endres; M. B. Epstein; S. Escoffier; K. G. Fissum; H. Fonvieille; S. Frullani; J. Gao; F. Garibaldi; S. Gilad; R. Gilman; A. Glamazdin; C. Glashausser; J. Gomez; V. Gorbenko

The ratio of the electric and magnetic form factors of the proton G(Ep)/G(Mp), which is an image of its charge and magnetization distributions, was measured at the Thomas Jefferson National Accelerator Facility (JLab) using the recoil polarization technique. The ratio of the form factors is directly proportional to the ratio of the transverse to longitudinal components of the polarization of the recoil proton in the elastic (e) over right arrowp --> e (p) over right arrow reaction. The new data presented span the range 3.5 < Q(2) < 5.6 GeV2 and are well described by a linear Q(2) fit. Also, the ratio rootQ(2) F-2p/F-1p reaches a constant value above Q(2) = 2 GeV2.The ratio of the electric and magnetic form factors of the proton G(E(p))/G(M(p)), which is an image of its charge and magnetization distributions, was measured at the Thomas Jefferson National Accelerator Facility (JLab) using the recoil polarization technique. The ratio of the form factors is directly proportional to the ratio of the transverse to longitudinal components of the polarization of the recoil proton in the elastic e(-->)p---> e(-->)p reaction. The new data presented span the range 3.5< Q(2)< 5.6 GeV(2) and are well described by a linear Q(2) fit. Also, the ratio sqrt[Q(2)] F(2(p))/F(1(p)) reaches a constant value above Q(2) = 2 GeV(2).


Nuclear Physics | 1973

Two-body pion production d(p, π+)t AT 470 and 590 MeV

W. Dollhopf; C. Lunke; C.F. Perdrisat; W.K. Roberts; P. Kitching; W.C. Olsen; J. R. Priest

Abstract The differential cross section for the reaction d(p, π + )t has been measured for c.m. angles between 37° and 160°, at incident proton energies of 470 and 590 MeV. The results are in qualitative agreement with the predictions of a two-nucleon model of the reaction when the D-state contribution is included, except for the existence of a backward peak at 470 MeV. Other models of the reaction are discussed; none of them gives a rationale for the backward peak at 470 MeV. A similar peak is present in older data at 325 MeV.


Physical Review C | 1998

Induced Proton Polarization for pi0 Electroproduction at Q2 = 0.126 GeV2/c2 Around the Delta(1232) Resonance

G. Warren; R. Alarcon; C. Armstrong; B. Asavapibhop; D. Barkhuff; W. Bertozzi; V. D. Burkert; Jiunn-Wei Chen; J. P. Chen; D. Dale; G. Dodson; S. Dolfini; K. Dow; M. B. Epstein; M. Farkhondeh; J. M. Finn; S. Gilad; R. W. Gothe; X. Jiang; M. K. Jones; K. Joo; A. Karabarbounis; J. J. Kelly; S. Kowalski; C. Kunz; D. Liu; R. W. Lourie; R. Madey; D. J. Margaziotis; P. Markowitz

We present a measurement of the induced proton polarization P{sub n} in {pi}{sup 0} electroproduction on the proton around the {Delta} resonance. The measurement was made at a central invariant mass and a squared four-momentum transfer of W = 1231 MeV and Q{sup 2} = 0.126 GeV{sup 2}/c{sup 2}, respectively. We measured a large induced polarization, P{sub n} = -0.397 {+-} 0.055 {+-} 0.009. The data suggest that the scalar background is larger than expected from a recent effective Hamiltonian model.


Physics Letters B | 1975

The 6Li(α, 2α)2H reaction at 700 MeV and the α-d momentum distribution

W. Dollhopf; C.F. Perdrisat; P. Kitching; W.C. Olsen

Abstract The results of an experimental study of the reaction 6Li(α, 2α)2H at 700 MeV are given. A comparison with the data from seven other reactions pertaining to the α+d cluster structure of 6Li is presented. The amplitude for the virtual transition 6Li→α+d obtained three of these experiments and the present one are comparable. The internal momentum distributions extracted with the plane-wave impulse approximation in four of the experiments are compatible with a pole form, the width parameter being given by the α-separation energy in 6Li. The remarkable consistency among these results is seen as evidence for the validity of the simple models used for both the reaction mechanism (PWIA) and to describe the α d-vertex (pole approximation) in 6Li.


Physical Review Letters | 2005

Quasielastic He-3(e,e(')p)H-2 reaction at Q(2)=1.5 GeV2 for recoil momenta up to 1 GeV/c

M. Rvachev; F Benmokhtar; E. Penel-Nottaris; K. A. Aniol; W. Bertozzi; W. Boeglin; F. Butaru; Calarco; Z. Chai; C.C. Chang; J. P. Chen; E. Chudakov; E. Cisbani; A. Cochran; J. C. Cornejo; S Dieterich; P. Djawotho; W. Duran; M. B. Epstein; J. M. Finn; Kevin Fissum; A. Frahi-Amroun; S. Frullani; C. Furget; F. Garibaldi; O. Gayou; S. Gilad; R. Gilman; C. Glashausser; J. O. Hansen

We have studied the quasielastic He-3(e,e()p)H-2 reaction in perpendicular coplanar kinematics, with the energy and the momentum transferred by the electron fixed at 840 MeV and 1502 MeV/c, respectively. The He-3(e,e()p)H-2 cross section was measured for missing momenta up to 1000 MeV/c, while the A(TL) asymmetry was extracted for missing momenta up to 660 MeV/c. For missing momenta up to 150 MeV/c, the cross section is described by variational calculations using modern He-3 wave functions. For missing momenta from 150 to 750 MeV/c, strong final-state interaction effects are observed. Near 1000 MeV/c, the experimental cross section is more than an order of magnitude larger than predicted by available theories. The A(TL) asymmetry displays characteristic features of broken factorization with a structure that is similar to that generated by available models.


Physical Review Letters | 2005

Q^2 Dependence of the Neutron Spin Structure Function g~2^n at Low Q^2

K. Kramer; D.S. Armstrong; T. Averett; W. Bertozzi; S. Binet; C. Butuceanu; A. Camsonne; G. D. Cates; J. P. Chen; S. Choi; E. Chudakov; F. Cusanno; A Deur; P Djawotho; D. Dutta; J. M. Finn; H. Gao; F. Garibaldi; O. Gayou; R. Gilman; A. Glamazdin; Gorbenko; K. A. Griffioen; J. O. Hansen; D. W. Higinbotham; W. Hinton; T. Horn; C. W. de Jager; X. Jiang; W. Korsch

We present the first measurement of the Q2 dependence of the neutron spin structure function g2(n) at five kinematic points covering 0.57 (GeV/c)2 < or = Q2 < or = 1.34 (GeV/c)2 at x approximately = 0.2. Though the naive quark-parton model predicts g2 = 0, nonzero values occur in more realistic models of the nucleon which include quark-gluon correlations, finite quark masses, or orbital angular momentum. When scattering from a noninteracting quark, g2(n) can be predicted using next-to-leading order fits to world data for g1(n). Deviations from this prediction provide an opportunity to examine QCD dynamics in nucleon structure. Our results show a positive deviation from this prediction at lower Q2, indicating that contributions such as quark-gluon interactions may be important. Precision data obtained for g1(n) are consistent with next-to-leading order fits to world data.


Physics Letters B | 1977

180° production of protons in high-energy p, d, and α reactions in nuclei

H. Brody; S. Frankel; W. Frati; D. Yang; C.F. Perdrisat; J.C. Comiso; K.O.H. Ziock

Abstract Measurement of the differential cross sections for the 180° production of protons from 6 Li, C, and Ta by protons (600 MeV), duetrons (361 MeV), and α-particles (726 MeV) have been carried out. The results are shown to be in accord with “quasi-two body scaling”. The data follow a structure function distribution G(k)≈ e − k k 0 up to internal nucleon momenta, k = 1.3 GeV/ c . The measurements in 6 Li extend the validity of this functional form up to values of k close to the elastic scattering limit.


Physics Letters B | 1980

Differential cross section and analyzing power for backward pions in 2H(p, π+)3H☆

E.G. Auld; R.R. Johnson; G. Jones; E.L. Mathie; P. Walden; D.A. Hutcheon; P. Kitching; W.C. Olsen; C.F. Perdrisat; B. Tatischeff

Abstract Cross sections and analyzing powers are presented for the reaction 2 H ( p , π + ) 3 H at 400, 425, 443 and 470 MeV, and laboratory pion angles of 120°, 130°, 140°, 150° and 160°. The cross sections have flat angular distributions, are in contradiction with an earlier experiment which indicated a backward peak at 470 MeV, but are in quantitative agreement with a calculation based on the two-nucleon model.

Collaboration


Dive into the C.F. Perdrisat's collaboration.

Top Co-Authors

Avatar
Top Co-Authors

Avatar
Top Co-Authors

Avatar
Top Co-Authors

Avatar

E. Chudakov

Thomas Jefferson National Accelerator Facility

View shared research outputs
Top Co-Authors

Avatar

J. P. Chen

Thomas Jefferson National Accelerator Facility

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar
Top Co-Authors

Avatar
Top Co-Authors

Avatar

S. Frankel

University of Pennsylvania

View shared research outputs
Top Co-Authors

Avatar

V. Punjabi

Norfolk State University

View shared research outputs
Researchain Logo
Decentralizing Knowledge