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Measurement of the neutrino velocity with the MINOS detectors and NuMI neutrino beam GdR Saclay – 11/04/08 Magali Besnier hep-ex – 0706.0437v3.

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Presentation on theme: "Measurement of the neutrino velocity with the MINOS detectors and NuMI neutrino beam GdR Saclay – 11/04/08 Magali Besnier hep-ex – 0706.0437v3."— Presentation transcript:

1 Measurement of the neutrino velocity with the MINOS detectors and NuMI neutrino beam GdR Saclay – 11/04/08 Magali Besnier hep-ex – 0706.0437v3

2 Previous measurements Theory : if M < 3 eV/c² *  |v-c| / c < 10 -9 for a 10 GeV *best limit on neutrino mass (cosmological measurement, 2005) But : some theories allow |v-c| / c ~ 10 -4 |β -β μ |< 4×10 -4 (99% confidence level), with |1-β μ |<10 -5 Previous terrestrial measurement with Fermilab neutrino beam :  comparison between detection of µ and µ emitted in the same time (  + /K + decays) Phys. Rev. Lett. 36, 837 - 840 (1976) |β ( ) -β μ |=|β ( ) -1|<4×10 -5 (95% confidence level) E : 30 - 200 GeV. D ~500m 1) First direct velocity measurement (1976) : 2) Second measurement (1979) : Phys. Rev. Lett. 43, 1361 - 1364 (1979)

3 MINOS detectors @Fermilab =3 GeV (LE) D=732 km MINOS measurements of neutrino velocity Difference with previous measurements : Absolute transit time measurement of an ensemble of neutrinos by comparing arrival times between ND and FD FD ND CCevents @ND

4 Event selection ND selections for  CC-like events: | Tarrival-Texpected | < 7µs At least 1 “good ” reconstructed track  select  or  events Track-Vertex inside the fiducial volume  Remove cosmic background E v reco <30 GeV (E v reco =E µ + P had ) Cut on a likelihood-based variable (PID) to separate NC and CC events ( ) FD selections : | T arrival -T expected | < 50µs 1 “good” track reconstructed with direction within 53° of that of the beam Track-Vertex inside the fiducial volume Neutrino-induced rock muons (track entering from the front face of the detector with direction within 26°) and shower events inside detector volume (mostly NC) also accepted 473 induced events, with 258  CC-events ( ) 1.6 10 6 events

5 Timing measurement ND FD timet FD t ND t0t0 t1=t ND - t 0 - d ND t2=t FD - t 0 - d FD t 0 : time of proton extraction magnet signal t ND and t FD : time of the earliest scintillator hit d ND and d FD : known timing delays (readout time, electronic latency, GPS antenna fiber delays) Deviation from the expected TOF  (massless neutrino)   = (t2- t1) –  Uncorrelated jitter of the GPS clocks   (t ND - t FD )=150 ns. MI Identical GPS receiver underground connected to surface with optical fibers Uncertainty :  |d ND – d FD |) = 64 ns @ 68% CL, mostly due to GPS optical fibers NO ! The neutrino beam pulse is not instantaneous … but 9.7 µs long !

6 Timing measurement ND profile interactions measured @ND P 1 6 (t 1 ) P 1 5 (t 1 ) PDF P 1 n (t 1 ) measured @ ND  (t ND - t FD )=150 ns Expected PDF @ FD : P 2 n (t 2 )=  1/(2  ) exp (- (t 2 -t’)/(2  ²)) P 1 n (t’) dt’ Deviation  from the expected time t 2 -   maximisation of L=  ln(P 2 (t 2 i -  -  )) time of FD events relative to prediction after fitting the TOF  P 2 5 (t 2 -  ) P 2 6 (t 2 -  ) FD  = -126 ± 32(stat.) ± 64(sys.) ns @68% C.L. ( Remember :  |d ND – d FD |) = 64 ns ) NuMI beam pulse is 9.7 µs long with 5 or 6 batches

7 Relativistic mass measurement T m (E )=   ( 1-m c²/E ) Time of flight of a relativistic with a mass m Log-likelihood function : m : free parameter E i reco : reconstructed energy R(E i v, E i reco ) : detector response parametrised through MC E i v : fitted true energy constrained by R and E i reco.  : free parameter constrained by earlier systematic measurement by a gaussian with   =64ns. m =17 +33 -56 (stat.+syst.) MeV/c² @99%C.L. With  =-46 ns E i reco < 10 GeV M =50MeV/c² M =17Mev/c² m =14 +42 -98 (stat.+syst.) MeV/c² @99%C.L. With  =-99  140 (stat) ns

8 Velocity measurement Remember :  = -126 ± 32(stat.) ± 64(sys.) ns @68% C.L. |v-c|/c=|-  /(  )|=5.1 ± 2.9 (stat.+syst.) 10 -5 @68%C.L. For between 1-30 GeV Consistent with the speed of light at less than 1.8 . Most sensitive test of neutrino velocity : Arrival time comparison of photons and neutrinos from SN1987a : |v-c|/c< 2 10 -9, but only for E ~10 MeV L.Stodolsky, Phys. Lett. B201, 353 (1988) Neutrino velocity could be strong function of E. MINOS is the only one measurement constraining v in the 1-30 GeV range. But no improvements wrt previous terrestrial measurements.

9 OPERA is a long baseline neutrino experiment at Gran Sasso laboratories, receiving a  beam ( =17 GeV) from CERN, 730 km away.  It will be able to provide another measurement of v in the 1-30 GeV range Future measurements Possible improvements : Actual OPERA GPS system is equivalent to the one of MINOS. New timing system based on GPS/atomic clock will be installed in the next months both at CERN and LNGS, 10-100 times more precise. Combination with other neutrino experiments at LNGS will improve statistics. Talk from D. Autiero will give more informations on this subject in following GdR meetings

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11 Long base=730 km  T= L/c = 2.4 msec L and  T from GPS expected as the best  T < 10 nsec  L < 5 cm ( ? ) Then |  -1|~   ~ 4*10 -6 Remember : FNAL(1976-77) -> 10 -4 CNGS – time of proton bunches OPERA – time of event using RPCs OPERA neutrino velocity measurement Worse case :  GPS > p bunch interspace ( 5ns now)  T ~ p batch length/  12  N (now 2 batchs with 10.5  s length) At present  t ~ 10  s/  12  1000 ~ 100ns   ~ 4*10-5 Is it possible to have 20 p batchs with 1  s length ? Better case :  GPS < p bunch interspace ( 25ns as for LHC)  T ~  GPS ~ 10 ns   ~ 4*10-6 Expected OPERA accuracy


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