# Analysis of the Spectral Intensities and Ratios of Electrons and Positrons in Cosmic Rays

## Abstract

The observations of the total electronic component and the positron fraction in cosmic rays by the FERMI, HESS, ATIC, and PAMELA instruments are studied with analytical propagation models, both for a set of discrete sources and for a spatially smooth source distribution. The positron fraction over the entire energy range of is shown to fit with the nested leaky box model. We derive the spectrum of electrons in cosmic rays arising from direct acceleration by the sources and discuss the narrow spectral feature in the spectrum.

electrons, positrons, dark matter

## 1 Introduction

Progressive improvements of detectors since the pioneering efforts in the 1960s have led to improved measurements of the spectrum of the electronic component and positron fraction by the FERMI, HESS, ATIC, and PAMELA instruments [1-5]. These measurements have stimulated great excitement, not only because of their importance to cosmic ray studies, but also because of the possible interpretation of some of the features from signals from the annihilation of dark matter in the Galaxy. We reproduce the observed total electronic spectrum and the positron fraction in fig. 1 and fig. 2 respectively.

In section II, we show that these observations help us in distinguishing between the leaky box [6] and the nested leaky box models [7]. It is the difference in the kinematics of the reactions producing secondary ‘light’ nuclei and positrons that helps in distinguishing amongst these models. We show that the positron fraction observed by PAMELA may be fit well with the nested leaky box model. We begin section III by deriving the spectrum of electrons resulting from direct acceleration in the cosmic ray sources by subtracting the secondary electrons and positrons from the spectrum of the total electronic component. After this, the rest of the section is devoted to a discussion of this primary electron spectrum in terms of a set of discrete sources of cosmic rays sprinkled throughout the Galaxy. The analysis indicates that we need the closest source to be no more than 200 pc from the solar system, which in turn implies that there are about 5000 sources accelerating cosmic rays in the Galaxy. The contrast between the spectra expected from a discrete set of sources and from sources spatially distributed smoothly throughout the Galaxy plays an important role in analyzing signatures from the annihilation of dark matter in the Galaxy. This aspect is discussed in section IV. It would be appropriate to note here that the theoretical considerations of cosmic ray transport with exponential pathlength distributions [6][8] and its analysis in terms of a set of discrete sources sprinkled over the galaxy [7][9] started three or four decades ago. The recent improved measurements constitute a testing ground for these early ideas on cosmic ray physics.

## 2 Positron Fraction in Cosmic Rays and the Leaky Box Models

The observations of decreasing ratios of secondaries to primaries like B/C and (V+Ti+Sc)/Fe with increasing energy per nucleon in cosmic rays could be incorporated into the original leaky box model (A and B) [6] by letting the mean residence time depend on energy in such a way as to reproduce the observations [11]. A viable alternative to this idea was the nested leaky box model (C) [7] in which the energy dependant part of the ratio (proportional to ) was attributed to the spallation in the matter constrained in a cocoon-like region surrounding the sources and the resident time in the Galaxy was assumed independent of energy. With observations of the ratios limited to a finite range of energies, it became customary to extrapolate the residence times as a simple power law, decreasing as . Even though the observations to date allow beyond some tens of GeV/n, this alternative had not been discussed earlier. These three possibilities and their corresponding fit to the secondary to primary ratios are shown in fig. 3 for the B/C ratio. The (V+Ti+Sc)/Fe ratio can be fit similarly. The three models presented here are characterized by mean residence times as noted below:

(1) |

(2) |

(3) |

where is a constant.

Consider now the injection of cosmic rays by sources with the spectral form

(4) |

When spallation and energy loss during transport could be neglected, the three models led to the following equilibrium spectra of cosmic rays in the Galaxy:

Note that does not depend upon [7].

Unless itself is a function of energy so that eq. 5B reproduces the observed spectra of the nuclear component that is a simple power law, model B is not viable. Model A requires and predicts increasing anisotropy with energy of cosmic rays, and model C requires and generates constant anisotropy at all energies.

The observations of the positron fraction provides a clear way of choosing amongst these three models. The reason for this is related to the fact that in the spallation process that generates the secondary cosmic ray nuclei like B in collisions of the primary C nuclei, the daughter nuclei will emerge with the same energy per nucleon as the parents. On the other hand, the production of positrons proceeds through the production of mesons (mainly pions) in the collision of the primary nuclei which follow the decay chain , followed by . In this process, the positrons and the secondary electrons carry, on the average, only a small fraction of the energy/nucleon of the primary. As a consequence of this, the production spectrum of positrons (and secondary electrons) in all the three models are nearly identical. The fact that low energy cosmic rays spend more time in the cocoon surrounding the sources plays no role as the and secondaries are generated only by the high energy part of the nucleon spectrum. Now the equilibrium spectrum of secondary and predicted by the three models simply follow the product of the production rate, and the residence time at low energies. At very high energies, all the models predict steeper spectra :

(5) | |||||

where and is defined in eq. 10. In fig. 2 we show the positron fraction

(6) |

with the positron spectrum as given in eq. 6 for the three models, and the spectrum of the total electronic component is taken to be the smooth fit to the data shown in fig. 1. Note that only model C provides a good fit over the entire range of the PAMELA observations. Thus, the observed positron fraction resolves the degeneracy amongst models developed to understand the nuclear secondaries and suggests that the nested leaky box model may provide a closer approximation to cosmic ray transport in the Galaxy [12].

## 3 Spectrum of Electrons Generated by Cosmic Ray Sources

The nucleonic component in the primary cosmic rays consists mainly of protons with a small fraction of neutrons which come in bound to He and other nuclei. As a consequence, the production of positrons is favored over that of electrons in cosmic ray secondaries:

(7) |

The lower value of is favored by the theoretical estimates based on the data on nuclear interactions obtained at accelerators [13], and the larger value is favored by the observations of the ratio generated by cosmic rays in the atmosphere [14]. The loss of energy by energetic cosmic ray electrons due to inverse Compton scattering and synchrotron emission in the magnetic fields prevalent in the propagation volume is given by

(8) |

(9) | |||||

Noting that the scattering of starlight by the very high energy electrons is described by the Klein-Nishina formula, the effect of starlight may be neglected, and only the microwave background contributes to in eq. 10. Taking and , we get . Adopting the nested leaky box model, the spectrum of the secondary positrons and electrons is given by [8]

In fig. 1, we show the total secondary component , with the normalization for determined from a smooth fit to the PAMELA data and , i.e. . We also show the secondary component for . Subtracting this (for ) from the total spectrum of the electronic component, we get the spectrum due to the sources,

(11) |

In an attempt to understand this spectrum, we assume diffusive transport of cosmic rays and write the differential equation describing the transport as

(12) |

Note that here we have simplified the form of the Green’s function by introducing an escape term in place of the boundary condition demanding that the cosmic ray density vanish at the planar surfaces of the thick cosmic ray disk of the Galaxy. The Green’s function is given by

(13) |

This along with the subsidiary eq. 9 is adequate to describe the transport of the electronic component of cosmic rays. Note that for a smooth and uniform distribution of sources , the Green’s function in eq. 14 integrates to the simple leaky box model.

Suppose we have a source situated at a distance which is continuously emitting cosmic ray electrons with a spectrum

(14) |

the observed spectrum is given by

(15) |

We display in fig. 4 this spectrum for various values of . Note that for , , and , one can obtain a reasonable fit to the high energy part of the primary electron spectrum g(E).

However, it is appropriate to add the contributions of all the sources situated at different distances to obtain their net contribution to . Assuming that the source is at an average distance of , we sum their contributions and compare with the primary electron spectrum in fig. 5. We see that irrespective of the choice of parameters, the high energy part of is not reproduced by the theoretical expectation . This difference becomes particularly large for much larger than . Thus we may expect that the distance to the nearest source and the typical spacing between the sources is . The difference between the contribution of the discrete sources and the fit to is also shown in fig. 5, and the difference with the data points is shown in fig. 6.

## 4 Narrow Spectral Features in the Primary Electron Spectrum

The narrow spectral feature displayed in figs. 5 and 6 has been ascribed in toto or in part to products of dark matter annihilation (see [15] for references). In this section, we discuss two input spectra, one a -function in energy and the other a flat spectrum , such as that expected for acceleration at planar shocks of high Mach number.

### 4.1 -function Input Spectrum

Here, the injection spectrum , the spectrum after time , (without leakage), and for a spatially smooth source and leakage lifetime are given by

(16) |

(17) |

(18) |

The spectrum peaks at for , and there is no sharp peak at (see fig. 6). A -function input from discrete sources leads to an observed spectrum

(18) |

For large , this spectrum displays a peak at

(19) |

For small , the peak will be sharp near , but with increasing , the peak will shift to lower energies and will become broader. We display in fig. 7 some examples of the spectra generated by -function inputs at various and show the sum, , over the sources at various distances in fig. 5.

### 4.2 Shock Acceleration

Planar shocks of high Mach number yield

(20) |

resulting in an equilibrium spectrum

(21) |

which can reproduce as shown in fig. 6.

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