Neutron lifetime experiment HOPE

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Neutron lifetime experiment HOPE Peter Geltenbort, Sergey Ivanov, Fabien Lafont, Thorsten Lauer, Kent Leung, Florian Martin, Felix Rosenau, Martin Simson Oliver Zimmer Institut Laue Langevin Grenoble Beta-decay weak interaction studies in the era of the LHC, Brussels, 3 September 2014

CKM unitarity test - goals for neutron decay? V ud 2 4908.7 (1.)s 9 n 2 1 3 Marciano & Sirlin PRL 96 (2006) 032002 uncertainty due to radiative corrections: n 2 4 Vud 3.810 RC accuracy goal: 0.34 s 0.0003 PDG: 880 ± 1.1 s (S=1.8) - 1.2701 ± 0.0025 (S=1.9) Perkeo II: Mund et al. PRL 110 (2013) - 1.2748 ± 0.0013 UCNA: Liu et al. PRL 105 (2010) 181803-1.2759 ± 0.0043 Perkeo III: Maerkisch et al. - 1.2??? ± 0.00067

Experimental situation In-beam experiments 886.3 ± 1.2 stat ± 3.2 syst s Nico et al. Phys. Rev. C 71 (2005) 055502 Material bottle experiments 888.4 ± 3.3 s (t 12 s) Nesvizhevsky et al. JETP 75 (1992) 405 885.4 ± 0.9 stat ± 0.4 syst s (t 100 s) Arzumanov et al. Phys. Lett. B 483 (2000) 15 878.5 ± 0.8 s (t 5 s) Serebrov et al. Phys. Lett. B 605 (2005) 72 880.7 ± 1.8 s (t 110 s) Pichlmaier et al. Phys. Lett. B 693 (2010) 221 881.6 ± 0.8 stat ± 1.9 syst s Arzumanov et al. JETP Lett. 95 (2012) 224 Magnetic bottle experiments permanent magnet 20-pole bottle t N( t) N( t0) exp n Ezhov et al., still unpublished He-II filled 4-pole trap: 833 +74 63 s Dzhosyuk et al. J. Res. NIST 110 (2005) 339 Projects: PENeLOPE, UCN, HOPE... all aiming at n << 1 s

UCN (electron detection) PENeLOPE (proton detection) TU Munich perm. mag. trap ( fill and empty ) Walstrom et al., LANL Nucl. Instr. Meth. A 599 (2009) 82 PNPI / LPC / ILL V. Ezhov et al. J. Res. NIST 110 (2005) 345 R. Picker et al., J. Res. NIST 110 (2005) 357

Benefit/challenge comparison of two magnetic trapping strategies t N( t) N( t0) exp n fill and empty detection of UCN need to determine N(t 0 ) fast coil ramping required high SNR Low sensitivity to timedependent backgrounds Monitoring of depolarisation and leakage of marginally trapped neutrons counting the deads detection of decay or proton get decay curve in one shot needs only slow coil ramping SNR for -detection stability issue for p-detection susceptible to timedependent backgrounds and variations of neutron density distributions

HOPE Halbach OctuPole neutron lifetime Experiment PhD works Felix Rosenau, Fabien Lafont, Kent Leung magneto-gravitational trap V eff 2 l trap depth 47 nev high-density UCN source counting the dead & survivors

HOPE Halbach OctuPole neutron lifetime Experiment magneto-gravitational trap V eff 2 l trap depth 47 nev high-density UCN source counting the dead & survivors

Halbach octupole B(r) = B R (r/r) 3 32 magnet slices NdFeB magnets: B R = 1.35 T 94 mm

12 octupoles + hands & forces = magnetic trap

UCN trapping tests at PF2 storage 800 s (teflon plug at trap bottom and a few mt bias field) PhD thesis Kent Leung

Shutter coil for vertical confinement for fill and empty method (5 T upper coil for later, optional proton focusing onto an aspect-type SDD) lower superconducting coil: 1.7 T @ 300 A 5 s ramping time (29 V)

Bias coil to guide decay products to detector for counting the deads p/e - detector PhD thesis Fabien Lafont (electron detector) p and gyrate about vertical bias field Simulation: 60 % probability to reach detector

Simple geometry with free access from top and bottom Preparation of spectrum Diffusive piston for trajectory mixing Cut into spectrum with absorber get rid of marginally trapped neutrons absorber 42 nev diffusive piston Kent Leung

Experiments? Start with well established fill and empty method Full-bore access from top and bottom: insertion of diffusive paddle and absorber monitoring of depolarisation detection of marginally trapped neutrons Couple experiment to superfluid-helium UCN source SUN-2 at ILL (pessimistic estimate: 3000 UCN/fill) n ~ 0.5 s in 50 days (statistical) To be started in mid 2014

Various minor problems : 15 months delay of cryostat delivery too much heat generated in current leads (solved by redesign in our group) superconducting switches transit at 220 A 5 times less UCN in trap at 200 A several l/h liquid helium consumption at 300 A

First runs at PF2 just started Study magnetic UCN storage benchmark for other UCN sources Switch problem to be solved later Felix Rosenau

Project SuperSUN (3 m magnetic 12-pole UCN reflector) Zimmer & Golub, arxiv:1303.1944 In-situ UCN polarizer Enhancement of UCN spectrum possible Weak dependence of UCN on wall quality (values in source for E < 296 nev): = W/V numbers for monochromatic beam H172b (5 times more in direct beam)