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Eun-Suk Seo [email protected] Inst. for Phys. Sci. & Tech. and Department of Physics University of Maryland Cosmic SIG
13

Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

Jul 17, 2020

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Page 1: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

Eun-Suk [email protected]

Inst. for Phys. Sci. & Tech. and Department of PhysicsUniversity of Maryland

Cosmic SIG

Page 2: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

CosmicSIG Eun-Suk Seo 2

They influence- evolution and shape of galaxies- state of interstellar medium- interstellar chemistry- evolution of species on Earth- and even the weather …

- Highest-energy particles known to mankind- Made in some of the most extreme

environments of the Universe- Energy density is comparable to thermal

energies, magnetic fields

Cosmic Rays: Why Care?

Presenter
Presentation Notes
P4-04 muon demo;
Page 3: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

Search for Existence of Antimatter in the Universe

The Big Bang was preceded by vacuum.

Nothing exists in a vacuum.

After the Big Bang there must have been

equal amounts of matter and antimatter.

Where is the antimatter?

CosmicSIG 3Eun-Suk Seo

Page 4: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

• Weakly Interacting Massive Particles (WIMPS) could comprise dark matter.

• This can be tested by direct search for various annihilating products of WIMP’s in the Galactic halo.

χ χ

q q

Indirect Detection

Direct Detection

Parti

cle C

ollid

ers

rmv

rGMm 2

2 =r

GMv =2

rv

Search for Dark Matter

CosmicSIG Eun-Suk Seo 4

Page 5: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

Search for Antimatter & Dark MatterNovel Cosmic Origin

CosmicSIG 5

1979: first observation of antiprotons (Golden et al,1979 , Bogomolov et al.1979)

1981: Anomalous excess (Buffington et al.)1987: LEAP, PBAR1988: ASTROMAG proposal1989: MASS1991: ASTROMAG shelved1992: IMAX1993: BESS, TS931994: CAPRICE, HEAT1995: AMS proposal1998: AMS-01 (Discovery STS-91)2000/2: Heat-pbar2004: BESS-Polar I2006-present PAMELA (Polar-orbit) 2007: BESS-Polar II2011-present: AMS-02 (Endeavour

STS -134)Eun-Suk Seo

Page 6: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

• Original BESS instrument was flown nine times between 1993 and 2002.

• New BESS-Polar instrument flew from Antarctica in 2004 and 2007– Polar–I: 8.5 days observation– Polar–II 24.5 day observation, 4700 M events7886 antiprotons detected: no evidence of primary

antiprotons from evaporation of primordial black holes.

− +

β−1

Rigidity

Abe et al. PRL, 108, 051102, 2012

Kinetic Energy (GeV)

Antip

roto

n Fl

ux (m

-2sr

-1s-

1 GeV

-1)

BESS-PolarII

Balloon–borne Experiment with a Superconducting Spectrometer

CosmicSIG 6Eun-Suk Seo

Page 7: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

Alpha Magnet Spectrometer

• Search for dark matter by measuring positrons, antiprotons, antideuterons and γ-rays with a single instrument

• Search for antimatter on the level of < 10-9

Launch for ISS on May 16, 2011AMS

Aguilar et al., PRL 110, 141102, 2013

CosmicSIG Eun-Suk Seo 7

Accardo et al., PRL 113, 121101, 2014Aguilar et al., PRL 113, 121102, 2014

"With AMS and with the LHC to restart in the near future at energies never reached before, we are living in very exciting times for particle physics as both instruments are pushing boundaries of physics,” said CERN Director-General Rolf Heuer.

Page 8: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

High Energy Antiprotons

CosmicSIG Eun-Suk Seo 8

Wino Dark Matter, Decaying Gravitino Dark Matter…?? Ibe et al. arXiv:1504.05554v1 [hep-ph] 2015Hamaguchi et al. arXiv:1504.05937v1 [hep-ph] 2015

“It is urgent to address first one of the main current limitations in the field of charged CRs, namely the determination of the propagation parameters.”

Giesen et al.arXiv:1504.04276v1[astro-ph.HE] 2015Evoli et al. arXiv:1504.05175v1 [astro-ph.HE] 2015

AMS Days at CERN, April 15-17, 2015

Page 9: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

CosmicSIG Eun-Suk Seo

γ < 200 GeV/n = 2.77 ± 0.03γ > 200 GeV/n = 2.56 ± 0.04

CREAM C-Fe

He

γCREAM = 2.58 ± 0.02

γAMS-01 = 2.74 ± 0.01

9

PAMELA (Adriani et al., Science 332, 69, 2011)

(Ahn et al., ApJ 714, L89, 2010)

Yoon et al. ApJ 728, 122, 2011; Ahn et al. ApJ 714, L89, 2010

CREAM-IγP = 2.66 ± 0.02γHe = 2.58 ± 0.02

It provides important constraints on cosmic ray acceleration and propagation models, and it must be accounted for in explanations of the e+e- anomaly and cosmic ray “knee.”

AMS-02 (Choutko et al., #1262; Haino et al. #1265, ICRC, Rio de Janeiro, 2013)

CREAM spectra harder than prior lower energy measurements

Page 10: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

Spectral Hardening Confirmed

CosmicSIG Eun-Suk Seo 10

Aguilar et al., PRL 115, 211101, 2015

Aguilar et al., PRL 114, 171103, 2015

Aguilar et al., PRL 113, 121102, 2014

Page 11: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

• Building on the success of balloon flights, the payload has been transformed for accommodation on the ISS (NASA’s share of JEM-EF).− Increase the exposure by an order of magnitude

• ISS-CREAM (CREAM for the ISS) will measure cosmic ray energy spectra from 1012 to >1015 eV with individual element precision over the range from protons to iron to:

- Probe cosmic ray origin, acceleration and propagation. - Search for spectral features from nearby/young sources, acceleration

effects, or propagation history.

Mass: 1392 kg Power: 550 WNominal data rate: ~350 kbps

To be installed on the ISS by Space X-12

JEM-EF #2

E. S. Seo et al, Advances in Space Research, 53/10, 1451, 2014

CosmicSIG 11Eun-Suk Seo

Delivered to KSC, August 2015

CREAM Cosmic Ray Energetics And Mass

Page 12: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

CosmicSIG Eun-Suk Seo 12

Page 13: Cosmic SIG - NASA€¦ · −1. Rigidity . Abe et al. PRL, 108, 051102, 2012. Kinetic Energy (GeV) Antiproton Flux (m-2. sr-1. s-1. GeV-1) BESS-Polar. II. Balloon–borne Experiment

BESS

ATIC

Cosmic Ray Science Interest

Elemental Charge

CosmicSIG Eun-Suk Seo 13

CREAM

AMS

&

ground based Indirect measurements

Session J13 CosmicSIGRm 250F

10:45 AM -12:30 PM