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151. Erratum: First Measurement of the Double Spin Asymmetry ine→p→→e′π+nin the Resonance Region [Phys. Rev. Lett. 88, 082001 (2002)]

152. Q2Dependence of Quadrupole Strength in theγ*p→Δ+(1232)→pπ0Transition

153. First Measurement of the Double Spin Asymmetry ine→p→→e′π+nin the Resonance Region

154. Corrected Article: Exclusive electroproduction of φ mesons at 4.2 GeV [Phys. Rev. C63, 065205 (2001)]

155. Photoproduction of theρ0Meson on the Proton at Large Momentum Transfer

156. Relativistic Effects and Two-Body Currents inH2(e→,e′p)nUsing Out-of-Plane Detection

157. Electroproduction of the Λ(1520) hyperon

158. Dynamics of the16O(e,e′p)Reaction at High Missing Energies

159. Exclusive electroproduction ofφmesons at 4.2 GeV

160. Theep→e′pηReaction at and above theS11(1535)Baryon Resonance

161. Photoproduction ofφ(1020)Mesons on the Proton at Large Momentum Transfer

162. Polarization transfer in the16O(e→,e′p→)15Nreaction

163. Dynamical Relativistic Effects in Quasielastic1p-Shell Proton Knockout fromO16

164. Pion absorptionon4He into theppdfinal state

165. π+absorption on N and Ar

166. Total cross sections of the charge exchange reaction(π+,π0) on2H,3He, and4He across theΔ(1232)resonance

167. Measurements of the Deuteron Elastic Structure FunctionA(Q2)for0.7≤Q2≤6.0(GeV/c)2at Jefferson Laboratory

168. Exclusive [formula omitted] meson electroproduction from hydrogen at CLAS

169. Two step processes in pion single charge exchange on2HatTπ+=239MeV

170. Total and partial pion absorption cross sections on4Hein the Δ resonance region

171. Multinucleon pion absorption on4He into thepppnfinal state

172. Pion absorption on3He and4He with emission of three energetic protons

173. New perspectives in multi-nucleon pion absorption on light nuclei

174. Evidence of initial state interactions in multinucleon pion absorption

175. Contribution of initial state interactions to the three-nucleon absorption of pions by 3He

176. A Large Acceptance Detector System (LADS) for studies of pion absorption

177. Large-Solid-Angle Study of Pion Absorption onHe3

178. Two-nucleon pion absorption in 4He at 1 GeV/c

179. LADS — large acceptance detector system for pion-nucleus reactions

180. Measurement of the transverse–longitudinal cross sections in the [formula omitted] reaction in the Δ region

181. Dental attitudes of primigravid women.

183. Measurement of the x- and Q2-dependence of the asymmetry A1 on the nucleon

184. Measurement of the transverse–longitudinal cross sections in the p(e→,e′p)π0 reaction in the Δ region

185. Moments of the spin structure functions g1p and g1d for 0.05<Q2<3.0 GeV2

186. Initial State Interaction in the (π+,3 p ) Reaction on N, Ar and Xe

187. First measurement of the double spin asymmetry in e→ p→ → e′ π+ n in the resonance region

188. Q2Evolution of the Neutron Spin Structure Moments using a3He Target

189. η photoproduction on the proton for photon energies from 0.75 to 1.95 GeV

190. First measurement of transferred polarization in the exclusive e→p → e′ K+Λ→reaction

191. Measurement of ep → e′ pπ+π-and Baryon resonance analysis

192. Measurement of the generalized polarizabilities of the proton in virtual Compton scattering at Q**2 = 0.92-GeV**2 and 1.76-GeV**2. 2. Dispersion relation analysis

193. Photon electroproduction from hydrogen at backward angles and momentum transfer squared of $Q^2 = 1.0$GeV$^2$

194. Kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments

195. Observation of nuclear scaling in the A(e,e′) reaction at X B>1

196. Q2 dependence of quadrupole strength in the γ*p → Δ+(1232) → pπ0 transition

197. Measurement of the generalized polarizabilities of the proton in virtual Compton scattering at Q**2 = 0.92-GeV**2 and 1.76-GeV**2. 1. Low-energy expansion analysis

198. Measurement of the proton spin structure function g1(x, Q2) for Q2 from 0.15 to 1.6 GeV2 with CLAS

199. Q2dependence of quadrupole strength in the γ*p → Δ+(1232) → pπ0transition

200. Two-Nucleon Momentum Distributions Measured in 3 He(e, e′pp)n

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