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XIII Advanced Research Workshop on
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� [539.12.01 + 539.12 ... 14
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Analytic perturbation theory and pr
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Measurements of GEp/GMp to high Q 2
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WELCOME ADDRESS Alexei Sissakian Di
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he joined the group of prof. Przemy
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proton. Dividing these 90 ◦ cm p-
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p-p scattering angle fixed at exact
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tuning for each ring. The Workshop
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was only about 10 5 per second, but
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[10] E.F. Parker et al., Phys. Rev.
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MICROSCOPIC STERN-GERLACH EFFECT AN
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DeGrand-Miettinen model predicted P
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TOWARDS STUDY OF LIGHT SCALAR MESON
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104xdBR(φ--> π η 0 -1 γ )/dm, G
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RECURSIVE FRAGMENTATION MODEL WITH
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Figure 2: String decaying into pseu
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pT -distributions in the quark frag
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4 Inclusion of spin-1 mesons For a
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CONSTITUENT QUARK REST ENERGY AND W
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〈r 2 ch 〉≈1fm2 . Now with Eqs
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TOWARDS A MODEL INDEPENDENT DETERMI
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Common for the difference cross sec
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TRANSVERSITY GPDs FROM γN → πρ
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The scattering amplitude of the pro
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INFRARED PROPERTIES OF THE SPIN STR
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5 Acknowledgement B.I. Ermolaev is
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We shall call this model the “sec
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y f ν V = f l V = f u V = f d gz V
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2. We remind, that the celebrated G
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of the resonance A, θV � 39 o .
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• Right-handed EW currents. The c
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pesum- (p Entries 0 + pe)-(p-pe) Me
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CROSS SECTIONS AND SPIN ASYMMETRIES
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R(ρ) 5 4 3 2 1 0 2 3 4 5 6 7 8 9 1
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TWO-PHOTON EXCHANGE IN ELASTIC ELEC
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and depend on three parameters : fN
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O(αs) SPIN EFFECTS IN e + e −
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3 Polarization results for mq → 0
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Since one has (↑↓) pc Born =(
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Figure 1: A typical lowest order Fe
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sin φ S (π + ) A UT 1.0 0.8 0.6 0
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form the agreement with these data
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in settling this dynamical issue. G
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SPIN CORRELATIONS OF THE ELECTRON A
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the two-photon system equaling 1).
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ANOTHER NEW TRACE FORMULA FOR THE C
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Compare the gain of time and effort
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where the triplet and octet axial c
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[2] Y. Prok et al. [CLAS Collaborat
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Melosh rotations which boost the re
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ky �GeV� 0.4 0.2 0.0 �0.2 �
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[2] B. Pasquini, and S. Boffi, Phys
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The appearance of both |+〉 and |
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2.2 Intrinsic Transverse Motion Qua
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are still complex: for a given corr
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- Page 119 and 120: [16] P.G. Ratcliffe and O.V. Teryae
- Page 121 and 122: Figure 1: a)[left] μpG p E /Gp M (
- Page 123 and 124: 4 Conclusion We introduced a simple
- Page 125 and 126: √ δΔq8 x for Δq8 and γΔGx fo
- Page 127 and 128: understanding of polarized light qu
- Page 129 and 130: They are inverse powers of Q 2 kine
- Page 131 and 132: accounts approximately for the TM a
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- Page 135 and 136: When the momentum increases (p >p0)
- Page 137 and 138: EVOLUTION EQUATIONS FOR TRUNCATED M
- Page 139 and 140: 4 Perspectives Evolution equations
- Page 141 and 142: NEW DEVELOPMENTS IN THE QUANTUM STA
- Page 143 and 144: statistical approach compared to th
- Page 145 and 146: POLARIZED HADRON STRUCTURE IN THE V
- Page 147 and 148: g 3 A =Δuv(Q 2 ) − Δdv(Q 2 ), g
- Page 149 and 150: AXIAL ANOMALIES, NUCLEON SPIN STRUC
- Page 151 and 152: 3. Vector current of strange quarks
- Page 153 and 154: ORBITAL MOMENTUM EFFECTS DUE TO A L
- Page 155 and 156: The elastic scattering S-matrix in
- Page 157 and 158: IDENTIFICATION OF EXTRA NEUTRAL GAU
- Page 159 and 160: for final l + l − events (l = μ,
- Page 161 and 162: QUARK INTRINSIC MOTION AND THE LINK
- Page 163 and 164: where wP = − m 2M 2 −p1 cos ω
- Page 165 and 166: where g q 2x − ξ 1(x, pT )= πM2
- Page 167: EXPERIMENTAL RESULTS
- Page 171 and 172: internal target is shown in fig. 2.
- Page 173 and 174: MEASUREMENT OF TENSOR POLARIZATION
- Page 175 and 176: over the distance of ∼ 28 m betwe
- Page 177 and 178: PROSPECTS OF MEASURING ZZ AND WZ PO
- Page 179 and 180: ρ00 correspond to transverse left-
- Page 181 and 182: LATEST RESULTS ON DEEPLY VIRTUAL CO
- Page 183 and 184: 3 Exclusive DVCS Events The HERMES
- Page 185 and 186: cos 0φ LU,I A sin φ ALU,I sin 2φ
- Page 187 and 188: POLARIZATION TRANSFER MECHANISM AS
- Page 189 and 190: Suggestion of the experiments for m
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- Page 195 and 196: xΔ N (1) fu (x) 0.05 0.04 0.03 0.0
- Page 197 and 198: Facility Type s (GeV 2 ) Timeline R
- Page 199 and 200: POLARIZATION OF VALENCE, NON-STRANG
- Page 201 and 202: helicity distributions Δq in the f
- Page 203 and 204: Figure 4: Left: Polarized valence q
- Page 205 and 206: shown in Fig. 6. The parametrizatio
- Page 207 and 208: NEW MONTE-CARLO GENERATOR OF POLARI
- Page 209 and 210: MN 0.06 0.04 0.02 0 -0.02 -0.04 -0.
- Page 211 and 212: HIGH ENERGY SPIN PHYSICS WITH THE P
- Page 213 and 214: magnetic calorimeter (EMCal). Indiv
- Page 215 and 216: Figure 3: Left : ALL for π0 at √
- Page 217 and 218: Figure 5: ALL for h + versus pT mea
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MEASUREMENTS OF THE Ayy, Axx, Axz A
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Typical momentum spectrum for the 1
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OVERVIEW OF RECENT HERMES RESULTS V
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A 2 0.3 0.25 0.2 0.15 0.1 0.05 0 -0
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tries in the two Q 2 regions are fu
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Strange quark distributions. The st
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NLO QCD PREDICTIONS FOR GLUON POLAR
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that NLO QCD corrections can be fac
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NLO Phase Space is simulated correc
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STUDY OF LIGHT NUCLEI SPIN STRUCTUR
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polarization observables are not so
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EXCLUSIVE ELECTROPRODUCTION OF ρ 0
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subtracted using simulated events g
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Re(T 01 /T 00 ) 0.4 0.2 0 HERMES pr
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Table 1: Leading-twist transverse m
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3.3 Single spin asymmetry with a tr
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5 Conclusions Transverse Momentum D
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The asymmetry Ameas N (φ) was calc
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agreement with the previous PROZA d
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Acknowledgement The work was suppor
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from the underlying theory. Higher-
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particularly sensitive to the least
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) 2 (GeV 2 Q DVCS measurements in H
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Figure 2: Compilation of the world
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¯Λ polarization was consistent wi
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Table 1: Status of the DY experimen
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tracking material. With a pitch of
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has ∼20 times larger acceptance t
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References [1] R.D. Klem et al., Ph
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The second condition is the status
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A N , % 0 -25 -50 -75 0 0.5 1 2 -t,
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Table 1: The estimated yields NEV o
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References [1] A. Gaidot et al., Ph
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The data from the former two experi
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charged particles to traverse on th
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[4] M. Dugger, et al. (The CLAS Col
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the polarimetry at the energies bet
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(a) (b) Figure 5: (a) the correlati
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1.1 Nucleon Helicity Structure at l
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15 ND3 for polarized deuterons and
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The 4th order Heavy Baryon Chiral P
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MEASUREMENTS OF GEp/GMp TO HIGH Q 2
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2 Recoil Polarization Method With a
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(a) (b) Figure 3: (a) Selection of
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5 Results of GEp-2γ Experiment So
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the light-front nucleonic wave func
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Figure 10: The test of the modified
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[3] V. Punjabi et al. Phys. Rev. C
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LONGITUDINAL SPIN TRANSFER TO Λ AN
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MB sample were reconstructed in the
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LL D LL D 0.4 0.2 0 -0.2 0.2 0 -0.2
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LONGITUDINAL SPIN TRANSFER OF THE
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LL D 1 0.5 0 -0.5 -1 -1.5 NOMAD HER
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THE GPD PROGRAM AT COMPASS A. Sanda
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COMPASS offers the advantage to pro
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The transverse target pin asymmetri
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are about -0.02, in agreement with
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AZIMUTHAL ASYMMETRIES IN PRODUCTION
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So, the aim of this study is to see
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Dependence of the AA fit parameters
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• the amplitudes asin φ (x, z, p
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quark in an unpolarized hadron. The
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dN/dφ h 8000 6000 4000 2000 0 Azim
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scattering plane [12]. The hadron y
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Coll p A 0.1 0 -0.1 positive hadron
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DELTA-SIGMA EXPERIMENT - THE RESULT
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charge-exchange quasi-elastic diffe
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COMPASS RESULTS ON GLUON POLARISATI
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and ΔG G (xav corr A2h LL (xBj)+A
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The remarkable agreement of the MC
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7 Results The preliminary measureme
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STATUS OF THE PAX EXPERIMENT Erhard
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Figure 2: Using events from elastic
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Figure 6: Target section required f
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ASYMMETRY MEASUREMENTS IN THE ELAST
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P 1 0.8 0.6 0.4 0.2 -0 -0.2 -0.4 -0
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CHARGE ASYMMETRY AND SYMMETRY PROPE
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These model independent statements
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The measured value of the asymmetry
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a term which depends on the maximum
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FIRST MEASUREMENT OF THE INTERFEREN
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pair yields [9]. The di-hadron frag
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projection on the thrust axis. All
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sign change of the IFF can therefor
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References Table 3: Integrated asym
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TECHNICS and NEW DEVELOPMENTS
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2 H-Jet Polarimeter The polarized h
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(and polarization) along axis X:
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AN vs. p for leading neutron T N A
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DEVELOPMENT OF HIGH ENERGY DEUTERON
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ADC, channels 800 600 400 200 100 2
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SPIN-ISOTOPIC ANALYSIS AT SUPERLOW
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3. Squeezing of quadrupole spectra.
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TRANSPARENT SPIN RESONANCE CROSSING
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2 The spin motion description under
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4 Examples of transparent crossing
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DEUTERON BEAM POLARIMETRY AT THE IN
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error bars include both statistical
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SPIN-MANIPULATING POLARIZED DEUTERO
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Several techniques [9] are used to
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A STUDY OF POLARIZED METASTABLE HEL
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The Schroedinger equation is writte
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PROTON POLARIMETER AT 200 MEV ENERG
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P (θ) σ (θ) =sinθ cos θ 2� b
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SPIN-ORBIT POTENTIALS IN NEUTRON-RI
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Figure 2: The differential cross se
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SPIN CONTROL BY RF FIELDS AT ACCELE
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precession in a ”field” h = ɛ
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Till now, RF spin flip has been stu
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RELATED PROBLEMS
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a potential V (r) interpolating bet
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forms on the edge of bubble a close
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where P = 1 D × B is the Poynting
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The action with the approximate sol
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in the four-dimensional and general
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It is clear that the self-adjoint o
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or Equation (1) may then be written
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References [1] S. Weinberg, Gravita
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a describes acceleration of the obs
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the results obtained in the present
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the polarized valence quark and sea
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with a special emphasis on the extr
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longitudinal spin transfer in Λ an
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List of participants of DSPIN-09 Na