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Magnetic field for “PANDA*” *Proton Asymmetry in Neutron DecAy

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Presentation on theme: "Magnetic field for “PANDA*” *Proton Asymmetry in Neutron DecAy"— Presentation transcript:

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2 Magnetic field for “PANDA*” *Proton Asymmetry in Neutron DecAy
For the SNS-FnPB Magnet meeting Prepared by Tim Chupp

3 The proton Asymmetry e e p p N+ n N- n N+ - N- N+ + N-
Asymmetry: __________ = C Pn A F (1-f) + Afalse background spin flip efficacy analyzing power neutron polarization gA gV C = k(A+B) = 4k ________ |l| 1+3| l |2 l = ____ k= Standard Model _____________ = S(Ee) [1 + a ______ + b ___ + ___.(A____ + B____ + D _______ )] dW pe.pn me J pe pn pexpn dEedWedWn EeEn Ee J Ee En EeEn JTW-57

4 C and l C = k(A+B) = 4k ________ PDG 2005 ___ ___
sl l sx x PDG 2005 ___ ___ l ±0.0029 a ± A ± B ± C ±0.011* D ±0.0006 f ±0.0029 * Abele, 2005 _____________ = S(Ee) [1 + a ______ + b ___ + ___.(A____ + B____ + D _______ )] dW pe.pn me J pe pn pexpn dEedWedWn EeEn Ee J Ee En EeEn JTW-57

5 Neutron spins tranported
Rudimentary Layout By For adiabatic neutron spin transport Bx M1 M2 Neutron spins tranported Through detector polarizer Spin Flipper analyzer X N0(v) y neutrons P(v) TP(v) A(v) TA(v) R z Detector L Detector 1 Detector 2 Neutron beam Into page +30 kV V0 ~ ~ ~ ~ Allows proton spectroscopy Detailed design work needed. Uniform field B

6 General Design Issues Goal: sx/x ~ 10-3 or better Neutron spin transported adiabatically from polarizer to analyzer (through detector) Uniform B in decay region: mitigates proton reflections from magnetic traps Proton orbit: d= 8 mm/B(T): 1-2T Needed (2 T for emiT proton segment Electrostatic proton energy resolution desired: requirements on B in proton drift region TBA Vacuum requirements: TBA

7 Neutron Polarization and Polarimetry
polarizer Spin Flipper analyzer X N0(v) neutrons P(v) TP(v) A(v) TA(v) R Detector G±=S±D RExp= S( ) + D( ) =N0T1T2TP [G0+DPR] M1= N0e1+B1 M2= N0T1T2TPTAe3 [ 1+PAR ] +B2 P/A Pn (5Å) Tn P2T features PSM 99.x% % fixed; limited l bite 3He (60%) 80% % flip P3; P3 varies Flipper: Ru= 1 (unflipped); Rf=F≈-1 (flipped) ( for AFP) (M2u - M2f) (M2u + M2f) _________ ~ PA(1-F) (1-f2) BR (1% need to know to 0.1%)

8 Detector ~ ~ ~ ~ Detailed design work needed. Uniform field B
Neutron beam Into page +30 kV V0 ~ ~ ~ ~ Allows proton spectroscopy Detailed design work needed. Uniform field B Ideal: A1=A2=1, e1=e2=1, f1=f2=0 • with adiabatic spin transport J||B • with adiabatic proton orbits, A=1 (scattering: resid. gas, baffles, etc.) Proton detection: e.g. emiT2

9 Statistics rn ~ 103/cm3 We expect about 0.5 decays per pulse: about 2.5 million events per day. 0.1% precision requires < a few days NOT STATISTICS LIMITED Focus on systematics…

10 Systematics N+ - N- __________ = C Pn A F (1-f) + Afalse N+ + N-
background spin flip efficacy analyzing power neutron polarization Need to know: neutron polarization analyzing power spin flip efficiency backgrounds spin independent spin dependent (false asymmetry) e.g. False asymmetry from electrons emited from n-decay (BR) - study of proton energy dependence Noise, gain shifts, etc. - flip 3He C is INDEPENDENT of Pn, xy, L, tof, 3He, B, BR, … statistical power


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