Geomagnetic cutoff calculations for the interpretation of low-rigidity cosmic-ray antiparticle measurements

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Geomagnetic cutoff calculations for the interpretation of low-rigidity cosmic-ray antiparticle measurements ICRC Busan, July 2017 Philip von Doetinchem philipvd@hawaii.edu Department of Physics & Astronomy University of Hawai'i at Manoa http://www.phys.hawaii.edu/~philipvd

Low-energy d and dark matter GAPS and AMS sensitivities are based on simulations Antideuterons are the most important unexplored indirect detection technique! Uncertainties: dark matter annihilation or decay dark matter clumping antideuteron production Galactic propagation solar modulation factor 100 geomagnetic deflection atmospheric interactions interactions in detector P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.2p

Outline of geomagnetic calculations Geomagnetic simulations with PLANETOCOSMICS (L. Desorgher) based on Geant4: http://cosray.unibe.ch/~laurent/planetocosmics/ Geomagnetic cutoff calculations with backtracing added latest IGRF-12 coefficients added Tsyganenko 2004 [N. Tsyganenko, J. Geophys. Res. 110, A03208 (2005)] dynamical data-based model of the inner magnetosphere, representing its structure and temporal variation during geomagnetic storms data base of all parameters as a function of time available http://geo.phys.spbu.ru/~tsyganenko/modeling.html Backtracing method: [Cooke et al., Il Nuovo Cimento 14C, 213, 1991] trajectories of cosmic rays with different rigidities, arriving at the same observing position and from the same direction of incidence are computed backward in time all cutoff values shown are effective cutoff rigidities R c Sampling of geomagnetic cutoff behavior for time of AMS-02 operation study of protons and antiprotons as function of time, location, direction compare to (U)LDB trajectories University of Hawaii HPC cluster: ~more than 100years of CPU time P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.3p

Magnetic field 5/19/2011 Absolute horizontal magnetic field with respect to Earth surface P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.4p

Magnetic field 6/22/2012 Absolute horizontal magnetic field with respect to Earth surface P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.5p

Magnetic field 7/27/2013 Absolute horizontal magnetic field with respect to Earth surface P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.6p

Backtracing 5/19/11 starting location reverse computation of antiproton trajectories starting at the same location with different rigidities P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.7p

Backtracing 3/7/12 starting location reverse computation of antiproton trajectories starting at the same location with different rigidities change in magnetic environment changes the trajectories drastically changes geomagnetic cutoff values P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.8p

Averaged cutoffs 5/19/11 geomagnetic cutoff for antiprotons averaged over an isotropic incoming particle distribution for cos(zenith) between 0.6-1 (typical opening angles) P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.9p

Cutoff as function of direction 5/19/11 cutoff values as a function of direction for 50 S, 0 W depend not only on zenith, but also on azimuth need to evaluate both P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.10p

Geomagnetic efficiency for antiprotons GAPS AMS-02 TOF geomagnetic cutoff efficiency: ratio of measurement time of particles of cosmic origin within acceptance and total measurement time efficiency averaged over flight trajectory AMS-02 is installed on the ISS (latitude ±52 ) understanding of geomagnetic environment crucial for low rigidities ISS averaged over calculations from 5/19/11-10/6/15 with 100 day steps (U)LDB averaged over 5/12/11, 13/1/8, 2/12/14, 12/10/14 GAPS is planned to fly from Antarctica (~-80 ) geomagnetic corrections are minimal P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.11p

Antiproton-proton comparison ratio of antiproton and proton efficiencies for the same trajectories and times below ~3GV all three trajectories show a dependence on the charge LDB flights from Antarctica: antiprotons are less suppressed compared to protons better suited for antiproton measurements ISS averaged over calculations from 5/19/11-10/6/15 with 100 day steps (U)LDB averaged over 5/12/11, 13/1/8, 2/12/14, 12/10/14 P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.12p

Time dependence for antiprotons ISS trajectory low-rigidity range exposes strong cutoff efficiency variations as a function of time without an apparent trend correlation of mean value of the horizontal magnetic field with geomagnetic efficiencies at different rigidity steps stronger field results in a larger geomagnetic efficiency for all rigidity steps from straight line fits at mean BH =9.5nT (over the whole period): (4.8±0.3)% at 1GV P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.13p (21.7±0.7)% at 3GV

ISS trajectory Solar X-ray flare event quiet 3/8/12-0:00UT extreme UV flash of X5-class solar flare March 7, 2012 significant increase of geomagnetic cutoff efficiency geomagnetic efficiency is again correlated with BH windows in the geomagnetic field open and close quickly P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.14p

ISS trajectory Solar X-ray flare event quiet 3/9/12-0:00UT extreme UV flash of X5-class solar flare March 7, 2012 significant increase of geomagnetic cutoff efficiency geomagnetic efficiency is again correlated with BH windows in the geomagnetic field open and close quickly P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.15p

ISS trajectory Solar X-ray flare event rise 3/9/12-1:30UT extreme UV flash of X5-class solar flare March 7, 2012 significant increase of geomagnetic cutoff efficiency geomagnetic efficiency is again correlated with BH windows in the geomagnetic field open and close quickly P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.16p

ISS trajectory Solar X-ray flare event peak 3/9/12-7:30UT extreme UV flash of X5-class solar flare March 7, 2012 significant increase of geomagnetic cutoff efficiency geomagnetic efficiency is again correlated with BH windows in the geomagnetic field open and close quickly P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.17p

ISS trajectory Solar X-ray flare event decline 3/9/12-15:00UT extreme UV flash of X5-class solar flare March 7, 2012 significant increase of geomagnetic cutoff efficiency geomagnetic efficiency is again correlated with BH windows in the geomagnetic field open and close quickly P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.18p

ISS trajectory Solar X-ray flare event quiet 3/10/12-6:00UT extreme UV flash of X5-class solar flare March 7, 2012 significant increase of geomagnetic cutoff efficiency geomagnetic efficiency is again correlated with BH windows in the geomagnetic field open and close quickly geomagnetic efficiency increase due to enlarged allowed windows P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.19p

Postdoc opening in Hawaii for GAPS North Shore View from the office P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.20p

Conclusions extensive geomagnetic cutoff calculations were carried out with PLANETOCOSMICS with the Tsyganenko 2004 model during which AMS-02 was operational cutoff has to be treated as function of position and direction of the incoming particle most suitable location for low-rigidity antiparticle measurements is an Antarctic flight large variability of geomagnetic efficiency at low rigidities, depends linearly on the mean of the absolute horizontal magnetic field component variability can happen on timescales as short as a few hours for extreme solar events P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.21p

Regions of increased cutoffs increased geomagnetic cutoff regions for antiprotons for the lower part of the Southern Hemisphere regions with increased cutoffs change location, size, and maximum value over time similar behavior was also found for protons, but location of regions with increased cutoffs differ between antiprotons and protons needs more studies P. von Doetinchem Cutoff for low-rigidity antiparticles Jul 17 p.22p