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The electron plus positron spectrum from annihilation of Kaluza-Klein dark matter and comparison with recent measurements Dept. Physical Sciences, Ritsumeikan Univ Satoshi Tsuchida, Masaki Mori
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The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

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Page 1: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

The electron plus positron spectrum from annihilation of Kaluza-Klein dark matter

and comparison with recent measurements

Dept. Physical Sciences, Ritsumeikan UnivSatoshi Tsuchida, Masaki Mori

Page 2: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Contents

• Kaluza-Klein Dark Matter

• LKP annihilation modes

• The effects of propagation

• Total positron fraction

• Comparison with recent measurements

• Summary

Page 3: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

We assume the first excited state (LKP) :

Kaluza-Klein Dark Matter

• UED (Universal Extra Dimensions)

Only 1 extra dimension

• Kaluza-Klein dark matter mass

Mass range = 300GeV - 1000GeV

L. Bergstrom et al, Phys. Rev. Lett 94(2005) 131301

Page 4: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

The edge structure is

predicted at the LKP mass

Cheng et al., Phys. Rev. Lett. 89 (2002) 211301

Page 5: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

The predicted edge structure

has not been observed

Page 6: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Positron fractionBy AMS-02 observation…

The positron excess above 10 GeV is reported

M. Aguilar et al., PRL 110. 141102 (2013)

Page 7: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Annihilation modes• Kaluza-Klein dark matter

There are many modes containing the electron as the final products

Line

Electron – Positron Pair (𝑒+𝑒−)

Continuum

Components Branching Ratio

Muon Pair (𝜇+𝜇−) 20 %

Tauon Pair (𝜏+𝜏−) 20 %

Quark Pairs 12 %

Gauge Bosons 1.5 %

Total

L. Bergstrom, Phys. Rev. Lett. 131301 (2005)

Page 8: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

CreationThe energy distribution for Line and Continuum components

when LKP annihilates in the Galactic halo

Page 9: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Flux

• The Electron-Positron Flux

• The Green function for Propagation

By determining the parameters a, b, and c,

the form of propagation is determined

I. V. Moskalenko & A. W. Strong, PRD 60 (1999) 063003

Page 10: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Isothermal model𝜌 = 0.43 GeV/cm3 :

Local DM density

𝑟𝑐 = 2.8 kpc : Core radius

Evans model𝜌 = 0.51 GeV/cm3

𝑟𝑐 = 7.0 kpc

Alternative model𝜌 = 0.38 GeV/cm3

𝑟𝑐 = 0.9 kpc

Upper case 10 kpc

Lower case 4 kpc

Our case 8.5 kpcI. V. Moskalenko & A. W. Strong, PRD 60 (1999) 063003

I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694

Page 11: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Boost factor• Boost factor

The factor which may enhance the signal from LKP

annihilation in the Galactic halo

• Cross Section

The value of boost factor is determined based on this cross section

Cheng et al., Phys. Rev. Lett. 89 (2002) 211301

Page 12: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Line and Continuum Flux

Page 13: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Positron Fraction

Total positron fraction

𝐹𝐿𝐾𝑃 : Flux from LKP annihilation𝐹𝐶𝑜𝑛𝑣 : The “Conventional” Flux𝑓𝐿𝐾𝑃 : Positron fraction for the LKP (=0.5)𝑓𝐶𝑜𝑛𝑣 : Positron fraction for 𝐹𝑐𝑜𝑛𝑣𝐵𝑓 : The Boost Factor

Q. Yuan and X. J. Bi, Phys. Lett. B727, 1 (2013)

I. V. Moskalenko and A. W. Strong, Astrophys. J 493, 694 (1998).

Page 14: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Comparison with recent measurements

𝐵𝑓=2.7 × 102

𝐵𝑓=2.2 × 103

𝐵𝑓=1.5 × 104

𝐵𝑓=3.7 × 104

Page 15: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Boost factor

Boost factor becomes larger

For heavier LKP mass

Page 16: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

By AMS-02 data, 300 GeV LKP mass is not relevant

More strict observation is expected for high energy region

Page 17: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Summary

• The flux from LKP can fit to AMS-02 data for positron excess

• The value of boost factor depends on LKP mass, and it is larger for heavier LKP mass than for lighter

• Light LKP mass, such as 300 GeV, may be excluded, because the edge structure has not been observed by some experimental data

Page 18: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Thank you for listening

Page 19: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Electron plus positron spectrum

M. Di Mauro et al., JCAP 04 (2014) 006

Page 20: The electron plus positron spectrum from annihilation of ......2015/10/29  · I. V. Moskalenko & A. W. Strong, ApJ 493 (1998) 694 Boost factor •Boost factor The factor which may

Positron Fraction

M. Di Mauro et al., JCAP 04 (2014) 006