1. Physics at the VLENF (very low energy neutrino factory) IDS-NF plenary meeting October 19-21, 2011 Arlington, VA, USA Walter Winter Universität Würzburg TexPoint fonts used in EMF: AAAAA A A A

2. DISCLAIMER: Talk similar to VLENF meeting (Fermilab), Sept. 1, 2011 Most of the following is based on the high energy Neutrino Factory with high luminosity However: many of the basic conclusions/optimization should be 1:1 transferable … [… and perhaps VLENF and LL-LENF (low luminosity) will merge into same concept at some point in the future]

3. 3 Contents  Neutrino factory flux  Treatment of near detectors  Treatment of sterile neutrinos  Systematics/energy resolution issues  Conclusions (for sterile neutrino searches in long+short baseline combined scenarios, see my other talk later today)

4. 4 Neutrino factory flux  Sometimes useful to integrate over energy: [neglect beam actual beam “divergence“ for the moment, since machine- dependent; focus on muon decay kinematics]

5. 5 Geometry of the beam  Beam diameter ~ 2 x L x   We use two beam angles:  Beam opening angle:  Beam divergence: contains 90% of total flux (arXiv:0903.3039) Beam divergence Beam opening angle 4 m at d=20 m Diameter ~0.4 m at d=20 m

6. 6  Example: high energy version  d = distance from end of straight  s = length of straight  L = baseline (from decay point to detector) Geometry of decay ring (arXiv:0903.3039) L  decay

7. 7 Approximations  Far distance approximation: Flux in whole detector looks like on-axis flux  Point source approximation: Extension of source can be neglected d ~ L >> s (arXiv:0903.3039)

8. 8 Extreme cases  Far detector limit: Far distance approximation for any point of the decay straight, i.e., the detector diameter D < 2 x L x , where  is the beam opening angle  Near detector limit: The detector catches almost the whole flux for any point of the decay straight, i.e., the detector diameter D > 2 x L x , where  is the beam divergence (arXiv:0903.3039)

9. 9 Extreme cases: Spectra  Some examples (HENF): ~ND limit~FD limit (arXiv:0903.3039)

10. 10 Some technicalities  How to treat arbitrary detectors in GLoBES? (which uses the point source and far distance approximations) 1)Take into account extension of detector 2)Take into account extension of straight (for details: arXiv:0903.3039) GLoBES built-in with

11. 11 Examples for near detectors Near detector limit Far detector limit SciBar-sizeSilicon- vertex size? OPERA- size Hypothetical Nearest point Farthest point Averaged  =1: FD limit Dashed: ND limit (Tang, Winter, arXiv:0903.3039)  Leads to excess of low-E events  near detector has to be large enough to have sufficient rates in high energy bins!  VLENF example: 200t TASD @ 20m, 2-3 m radius: ~ qualitatively similar to ND 3  VLENF example: 800t @ >> 600m, 6-7 m radius: ~ qualitatively similar to ND 4

12. 12 Sterile neutrinos: thoughts  First approximation (use L eff !):  Examples (VLENF): E ~ 2-3 GeV s=75 m, d=20 m: L eff =84 m   m 2 ~ 30 eV 2 s=75 m, d=1000 m: L eff = 1037 m   m 2 ~ 2 eV 2  The problem: are there effects from averaging over the straight?  Oscillations depend on x=L/E, where dx/x ~ |dL/L| + |dE/E| ~ f*s/L eff + 0.05 (TASD) (f= O(1) factor taking into account the decay position distribution)  s/L eff ~ f*77% in near detector (d=20 m) s/L eff ~ f*7% in far detector (d=1000 m)  At least in near detector, constrained by extension of straight, not energy resolution of detector!

13. 13 Treatment of steriles  Requires generalization of ND scheme:  So far only tested for  ~ 1 (far detector limit); however, not in principle impossible if  integrated in osc. engine (GLoBES) (Giunti, Laveder, Winter, arXiv:0907.5487) Effect of beam geometry Effect of osc. prob. Assumption: muon decays per dL ~ const

14. 14 Example: e disappearance  e disppearance:  Averaging over straight important (dashed versus solid curves)  VLENF: Expect significant averaging effects if d <~ s, i.e., in near detector  Impact on near-far extrapolation? (arXiv:0907.5487) 90% CL, 2 d.o.f., No systematics, E  =25 GeV, s=600m VLENF FD- equivalent

15. 15 Two-detector combination?  Depending on  m 2, far and near detectors change their roles: (arXiv:0907.5487)

16. 16 Disappearance systematics  Systematics similar to reactor experiments: Use two detectors to cancel X-Sec errors (arXiv:0907.5487) 10% shape error arXiv:0907.3145

17. 17 On the VLENF optimization (general conclusions)  E  can be rescaled if the baselines are adjusted accordingly (e.g. if required by X-sec measurements) from physics point of view  Advantage: Higher E   longer d  less rel. effect of averaging of the straight; X-sec measurements  In principle: d >~ 1000m necessary if 5% energy resolution needs to be useful in FD  However: not so clear to me where such a high energy resolution is important … [maybe not at first osc. maximum – remains to be tested]

18. 18 On the VLENF optimization (technical conclusions)  Numerical studies challenging, since optimization depends on detector geometry and straight averaging (needs some coding), but recipe clear  But: sensitivity to sterile neutrinos will mostly depend on far detector, which can be typically approximated by far detector limit  One has to ensure that the near detector has a sufficient event rate at high energies (geometry becomes important); it may limit the energy resolution of the system because of the decay straight averaging  Some systematics difference between appearance and disappearance searches!

19. 19 Outlook: other physics  Example: discovery reach for CPT violation Dashed-solid contours: effect of straight averaging (arXiv:0907.5487)