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A8hd A8ij:eA8uv:eA8:ewT$SAhd T&$Study: SAhd T$-Q2 dependence of GDH sum rule at low Q2 rangeS0APddd8A @WW8Num1A8-hd A8:eA8&(:e3T$Slope of GDH sum rule at Q2 ~ 0S0APddd8A @WW8Num1A8hd A8:e3Tx$&Extrapolation to the real photon pointS?APddd8Ahd A @WW8Num13T$GAssumption that the polarized 3He target is a polarized neutron targetS0APddd8A @WW8Num1A8Ghd A8:e3T6$S+APdddAhd T=$SAhd o+:*SA  PA Pl:%+ SAPA0PN'T$3HeA8:eA  PAPGAP,A PAPAHPHT$SAhd T$SAhd o+:,SA  PA Po+:-SA  PA Po+:.SA  PA Po+:/ SA  PA PTt$SAhd o+:0SA  PA Po+:1SA  PA PTI$SAhd o+:2SA  PA PTI$SAhd o+:3SA  PA PT8$SAhd l:%4S AP\AVPNMTD$)Figure 1: 3He and neutron spin directionA8 :eA  PAPAP@ A PAPAHPHT$SAhd T&$Reasons:SAhd T$/Add an essential data set to the world data setS?APddd8Ahd A @WW8Num13T$)Understand 3He and neutron spin structureS0APddd8A @WW8Num1A8)hd A8 :e3Tb$Study resonancesS?APddd8Ahd A @WW8Num13Tu$Test 3He modelsS0APddd8A @WW8Num1A8hd A8:e3T?$Experimental Equipment ISAPdddT $i T$SAhd Tw$%Jefferson Lab polarized electron beamS?APddd8Ahd A @WW8Num13T]$'- Approximately 80% polarization using S+APdddAhd T]$ strained GaAs cathodeS+APdddAhd w T$1 to 15 mA beamS0APdddA @WW8Num2A8hd A8  Symbol3T$JMonitor beam polarization using the Hall A Mller and Compton polarimetersS?APdddAhd A @WW8Num23w+T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T}$+Hall A High Resolution Spectrometers (HRS) S?APddd8Ahd A @WW8Num13 Tj$Standard spectrometersS?APdddAhd A @WW8Num13  Tb$Septum MagnetsS?APdddAhd A @WW8Num13  T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd Td$Experimental Equipment IIS@APdddA PAd A @T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd Tc$ Septum Magnets S?APddd8Ahd A @WW8Num13 Tv$"Added to the two HRS spectrometersS?APdddAhd A @WW8Num13  T$)Change the minimum angle to 6 from 12.5S0APdddA @WW8Num1A8)hd A8 SymbolA8() Symbol3  T$PWill be used by hypernuclear electroproduction experiment (E94-107) in June 2002S?APdddAhd A @WW8Num13  T $iTr$ 3He TargetSAAP+dddFAhd A @ 374841221A8:e3 Tw$#Glass target cell with two chambersS?APdddAhd A @WW8Num13  Tj$25 Gauss holding fieldS?APdddAhd A @WW8Num13  Tp$Oven to heat pumping chamberS?APdddAhd A @WW8Num13  T{$'30 Watt diode lasers to optically pump S?APdddAhd A @WW8Num13  TF$ Rb vaporSAhd wTA$S6APdddAd A @T'$SAPdddT'$SAPdddT'$SAPdddT'$SAPdddT'$SAPdddT'$SAPdddTB$Progress in the Past Year ISAPdddT$SAhd T$SAhd T$SAhd T$SAhd T$SAhd Ta$Cell ProductionS?APddd8Ahd A @WW8Num13 T$9Assisted in production of 11 successful cell fills at W&MS?APdddAhd A @WW8Num13  T$aIncluding Shapiro, 40 cm cell, used during E97-103, and Tilghman, 25 cm cell, used during E99-117S?APdddAhd A @WW8Num13  T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T$Cell 3He density measurementsS0APddd8A @WW8Num1A8hd A8:e3 T$93He density measurements by method of pressure broadeningS0APdddA @WW8Num1A89hd A8:e3  T~$*Check for possible errors and cell leakageS?APdddAhd A @WW8Num13  T$SAhd T$SAhd TT$SAd A @o+:7 SA  PA PT$t laser beam Photodiode SA @o+:8SA  PA Po+:9SA  PA Po+:;SA  PA PA8thd A8#$@d A8$)d A8,>d A8EWd A8W^d Tb$1 OvenA8-hd A8-1d T$SA @TM$$Figure 2: Density measurement setupSA@d A @T)$SA@d A @T)$SAhd A @T$ (3)SAhd A @Aq0lf:(:SWAPIA%PNO ObjBFFFE791APA PT)$SA@d A @T)$SA@d A @T)$SA@d A @TE$Progress in the Past Year IISAd A @T$SAhd T$SAhd T$SAhd T$SAhd T$SAhd Tm$Wall thickness measurementsS?APddd8Ahd A @WW8Num13 T$DDetect the interference pattern from the reflection off a glass cellS?APdddAhd A @WW8Num13  Ty$%Used in radiative corrections and NMRS?APdddAhd A @WW8Num13  TN$ measurementsS+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T]$S'APdddA @o+:=SA  PA PT$?Photo-Diode S'APdddA @A8 d T$Iris S6APdddAhd A @o+:?SA  PA Po+:ASA  PA Po+:BSA  PA PA8d T$ Target cellS6APdddAd A @o+:>SA  PA Po+:@SA  PA PTE$ S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @Tn$-Figure 3: Wall thickness measurement setup S6APdddA@d A @TA$S6APdddA@d A @TA$S6APdddA@d A @T$ (4)S6APdddAhd A @Aq0lf:(<SWAPA%PNO ObjBFFFE794APA PT$SAhd T6$S+APdddAhd T6$S+AP8ddd8Ahd T6$S+APdddAhd T$SAhd T$SAhd T$SAhd TD$ Progress in the Past Year IIISAPdddT6$S+APdddAhd T6$S+APdddAhd Ty$ '~ 30 total Shifts on E99-117 (A1n) and S0APddd8A @WW8Num13wTd$ .E97-103 (g2n) this past summer to learn about:SAPddhdw T_$ 3He targetS0APdddA @WW8Num1A8:e3 TY$ Hall A spectrometersS0APdddA @WW8Num13 Tc$ Hall A data acquisition systemS0APdddA @WW8Num13 T'$ SAPdddT'$ SAPdddT$ JAssisted in the transfer of 3He equipment back to the 3He test lab at JLabS0APddd8A @WW8Num1A8:eA867:e3T'$ SAPdddT'$ SAPdddTr$ /Working with a MIT and Temple graduate student S0APddd8A @WW8Num13Tm$ 6to set up the 3He system and do various target studiesSAP8ddd8A8:eT'$ SAPdddT'$ SAPdddTz$ 'Responsibilities for the 3He target labS0APddd8A @WW8Num1A8:e3TO$ NMR systemS0APdddA @WW8Num13 T_$ Optics and laser alignmentS0APdddA @WW8Num13 TL$ TargetsS0APdddA @WW8Num13 TW$ Water calibrationsS0APdddA @WW8Num13 Tg$ LabView ProgrammingS0APdddA @WW8Num13 wTl$ 'Density and wall thickness measurementsS0APdddA @WW8Num13 T $ T'$ SAPdddT'$ SAPdddT$SA @T)$SAd A @T:$Future Time TableSAd A @T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd Tp$ October 2001 to July 2002:SAAPdddAhd A @ 3726102213T$/ - Continue to work in the 3He target lab and SAAPdddAhd A @ 372610221A8:e3 !T$, and become a target expert for E97-110SAAPdddAhd A @ 3726102213 !T$/ - Continue to learn and and study the physicsSAAPdddAhd A @ 3726102213 !Tv$ theory of the GDH sum ruleSAAPdddAhd A @ 3726102213 !T$/ - Take shifts on experiments to become betterSAAPdddAhd A @ 3726102213 !T$2 acquainted with the Hall A spectrometers andSAAPdddAhd A @ 3726102213 !Tm$ data analysisS2APdddA @ 372610221A8hd 3 !T6$S+APdddAhd Tt$ Mid-July to early August 2002:SAAPdddAhd A @ 3732252213T$% - Move the 3He system to Hall AS2APdddA @ 373225221A8%hd A8:e3 T$3 - Setup the electronics, optics, and softwareSAAPdddAhd A @ 3732252213 T6$S+APdddAhd Tm$ August to October 2002:SAAPdddAhd A @ 3734572213Tw$# - Take shifts on my experimentSAAPdddAhd A @ 3734572213 T$3 - Monitor the 3He target during the experimentS2APdddA @ 373457221A83hd A8:e3 Tp$ - Initial data analysisSAAPdddAhd A @ 3734572213 TT$SAAPdddAhd A @ 3734572213 Tn$ October 2002 to May 2004SAAPdddAhd A @ 3734572213Tp$ - Finish data analysisSAAPdddAhd A @ 3734572213 Tu$! - Write Ph. D. DissertationSAAPdddAhd A @ 3734572213 Tw$# - Defend Ph. D. Dissertation SAAPdddAhd A @ 3734572213 T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd T6$S+APdddAhd TM$ GDH Sum RuleS6APdddAd A @TA$S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @T$'Original Gerasimov-Drell-Hearn sum ruleSLAPdddAhd A @A @ 3804682213T$2 - Relates an integral over the spin-dependent SLAPdddAhd A @A @ 3804682213 T$5 cross sections for total photoproduction to theSLAPdddAhd A @A @ 3804682213 T$. anomalous magnetic moment of the nucleonSLAPdddAhd A @A @ 3804682213 T$0 - Pertains strictly to real photons at Q2 = 0SLAPdddAhd A @A @ 380468221A8+,:e3 T`$ SLAPdddAhd A @A @ 3804682213 T$ (1)SLAPdddAhd A @A @ 380468221A0 l:(5 SAP!A%PNO ObjBFFFE7A2A  PAPAPA P A P3 TA$S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @TA$S6APdddAhd A @Tw$Generalized GDH sum ruleSLAPdddAhd A @A @ 3804682213T$4 - Includes scattering from virtual photons Q2 > 0SLAPdddAhd A @A @ 380468221A8/1:eA1dA824d3 T$3 - Provides a quantity which can be studied from SXAPdddA dAhd A @A @ 3804682213 T$3 a regime of quark confinement to a regime of SXAPdddA dAhd A @A @ 3804682213 T$ asymptotic freedomSXAPdddA dAhd A @A @ 3804682213 TA$S6APdddAhd A @TA$S6APdddAhd A @T$ (2) S6APdddAhd A @Aq0 lf:(6 SWAPA%PNO ObjBFFFE7A4AP A P JTektronix Phaser 840 PlusTKP840P4 PostScriptD`Tl`Tld,,lpr -P colorcolorTKP840P47 U@9V88/5? и/=U!2PCCšU!2?$B!fBf!fB!fB2!fB!fB!fBd!fB !fB0 !f B !f B !f Bb! 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