Secondary positrons and electrons measured by PAMELA experiment

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Presentation transcript:

Secondary positrons and electrons measured by PAMELA experiment Vladimir Mikhailov (MEPhI) For PAMELA collaboration ECSR , 4-9 September, 2016, Torino, Italy

PAMELA Collaboration Italy: Russia: Germany: Sweden: Bari Florence Frascati Trieste Naples Rome CNR, Florence Moscow St. Petersburg Russia: Germany: Siegen Sweden: KTH, Stockholm

~40 km ~500 km Atmospheric boundary Primary cosmic ray ~40 km Atmospheric boundary N. Grigorov Possibility of existence of a radiation belt around the earth consisting of electr.ons with energies of 100 MeV and above. Soviet Physics Doklady, Vol. 22, p.305, 1977 Production of charged pions in CR protons interaction with residual atmosphere е Trapping of secondary particles by the Earth magnetic field livetime T(h)~ 1/(h) Intensity Ie(h) ~Icr×(h)×T(h)~ ·/ Ie(h) ~ constant (h) from ~100 to ~1000км Basilova et al. 1978 Kurnosova et al.1979: first measurements Galper et al 1983 : electron excess in SAA

The PAMELA Experiment PAMELA is here Resurs DK satellite built by the Space factory «TsSKB Progress» in Samara (Russia) PAMELA is here Satellite was launched 15.06.2006 on elliptical polar orbit with inclination 700, altitude 350-610km. Circular orbit with altitude ~570km from September 2010 Mass: 6.7 tons Height: 7.4 m Solar array area: 36 m2 Since July 2006 till Junuary 2016: ~3200 days of data taking ~50 TByte of raw data downlinked ~9•109 triggers recorded and analyzed Trigger rate ~25Hz (outside radiation belts) Event size (compressed mode) ~ 5kB 25 Hz x 5 kB/ev  ~ 10 GB/day

Spectra in different parts of magnetosphere Analyzed data July 2006 – November 2009 (~1400 days) Identified ~ 1 106 electrons and ~ 1 105 positrons between 50 MeV and 100 GeV Trapped protons in SAA. Magnetic polar cups ( galactic protons) S3 count rate, au Secondary re-entrant-albedo protons Latutude, deg Longitude, deg Geomagnetic cutoff

Positron to electron ratio for secondary particles AMS-01 experiment (1998) Due to East-West effect ratio e+/e- is about ~5 In near equatorial region Result of AMS-01 confirmed by PAMELA Adriani et al , JGR ,2009

Data analysis Trajectories of positrons and electrons were reconstructed in the Earth's magnetic field IGRF field model was used (http:/nssdcftp.gsfc.nasa.gov) Boundary : Losses in atmosphere Hmin=30 km, Escaping Hmax=20000 km Time of tracing Tmax=35 second (correspond to drift time around the Earth for particles with energy E~100 MeV) The method of tracing was used previously in AMS-01 experiment Z, 1000км Y, 1000км X, 1000км Reconstructed trajectories of electrons and positrons detected by PAMELA during several orbits

Samples of particles trajectories: Simple reentrant albedo: Altitude vs latitude Z, 1000км Х, 1000км У, 1000км Trajectory of re-entrant albedo positrons with rigidity R=1.24 GV Time of flight ~0.1 s

Quasi-trapped particles: X, 1000км Z, 1000км Y, 1000км Positron trajectory with rigidity R~0.5 GV Positron trajectory with rigidity R~1.2 GV, Time of flight >>0.1 s at R<1GV. The time is decreasing with R increasing

Trapped positron Z, 1000км У, 1000км Х, 1000км Altitude vs longitude. Minimal trajectory altitude is in South Atlantic Anomaly region. Positron trajectory with rigidity R~1 GV, pitch-angle about 90 °.

Quasi-trapped particle near geomagnetic cut-off Positron trajectory with rigidity R=2.24 GV, with small pitch-angle

Cosmic ray trajectory near geomagnetic cut-off Chaotic trajectory of non-adiabatic type .

Electron and positron flight time in magnetosphere Cosmic ray (CR) selected by Hmax>20000 km The flight time versus energy from the tracing of leptons. Difference with AMS-01: More wide interval of altitudes (350-600 km), possibility to work in SAA. There is trapped component with very long flight time

Re-entrant albedo: point of origin PAMELA electrons AMS-01 positrons M. Agular, et al. Physics Reports. 2002. V. 366. P. 331

Quasi-trapped albedo: points of detection positrons electrons

Quasi-trapped particles: points of origin PAMELA AMS-01 electrons positrons

Positron to electron ratio vs energy PAMELA AMS-01 Ek (GeV)

Stably trapped particles: points of detection positrons electrons

Space distribution of trapped particles positrons electrons

Space distribution of trapped particles

Geomagnetic coordinates L-B of detected trapped particles

Positron to electron ratio

Sources of trapped electrons and positrons with E>10 MeV Gusev et al, 2001, 2004 :TP source are limited in spatial distribution at around L=1.2± 0.1 with the energy spectrum showing a steep cutoff at energy of about ~ 300 MeV. The calculated e+/e- flux ratios in the belt due to this source are high and attain values of ≥7 in the energy range of 10 to 500 MeV. The simulated results for the CR source, at the center of the positron belt, are about 100 times lower than the positron fluxes of the TP origin at L=1.2. Trapped proton (TR) interactions CR interaction with residual atmosphere

Ratio of positrons to electrons vs L-shell for trapped particles

Ratio of positrons to electrons vs L-shell for trapped particles CR source CR source

ratio e+/e- in LB coordinates for trapped particles Altitude increasing

ratio e+/e- in LB coordinates for trapped particles Altitude increasing 0.18<B<0.2 G , 1.12<L<1.3

Energy distributions of trapped electrons and positrons 0.18<B<0.2 G , 1.12<L<1.3

Conclusion 1. Particle tracing in magnetosphere selects - cosmic ray - re-entrant albedo - quasitrapped - trapped electron and positron 2. Charge composition of stably trapped particles in radiation belt differs from longlived quasitrapped component 3. PAMELA detects more electrons then positrons on boundary of radiation belt at E <0.5 GeV

Thank you!

Spare slides

PAMELA detectors Main requirements  high-sensitivity antiparticle identification and precise momentum measure + - Time-Of-Flight plastic scintillators + PMT: Trigger Albedo rejection; Mass identification up to 1 GeV; - Charge identification from dE/dX. Electromagnetic calorimeter W/Si sampling (16.3 X0, 0.6 λI) Discrimination e+ / p, anti-p / e- (shower topology) Direct E measurement for e- Neutron detector 3He tubes + polyethylene moderator: High-energy e/h discrimination Overview of the apparatus GF: 21.5 cm2 sr Mass: 470 kg Size: 130x70x70 cm3 Power Budget: 360W Spectrometer microstrip silicon tracking system + permanent magnet It provides: - Magnetic rigidity  R = pc/Ze Charge sign Charge value from dE/dx

Electron and positron spectra in SAA

Отношение e+/e- для 0.18<B<0.2 , 1.18<L<1.13