Issue 
A&A
Volume 567, July 2014



Article Number  A101  
Number of page(s)  7  
Section  Astrophysical processes  
DOI  https://doi.org/10.1051/00046361/201322664  
Published online  22 July 2014 
Estimates of relativistic electron and proton energy densities in starburst galactic nuclei from radio measurements
^{1} INAFTrieste, via G.B. Tiepolo 11, 34143 Trieste, Italy
email: persic@oats.inaf.it
^{2} INFNTrieste, via A. Valerio 2, 34127 Trieste, Italy
^{3} School of Physics & Astronomy, TelAviv University, 69978 Tel Aviv, Israel
^{4} Center for Astrophysics & Space Sciences, University of California at San Diego, La Jolla CA 92093, USA
Received: 13 September 2013
Accepted: 12 May 2014
The energy density of energetic protons, U_{p}, in several nearby starburst nuclei (SBNs) has been directly deduced from γray measurements of the radiative decay of π^{0} produced in interactions with ambient protons. Lack of sufficient sensitivity and spatial resolution makes this direct deduction unrealistic in the foreseeable future for even a moderately distant SBN. A more viable indirect method for determining U_{p} in starforming galaxies is to use its theoretically based scaling to the energy density of energetic electrons, U_{e}, which can be directly deduced from radio synchrotron and possibly also nonthermal hard Xray emission. In order to improve the quantitative basis and diagnostic power of this leptonic method we reformulate and clarify its main aspects. Doing so we obtain a basic expression for the ratio U_{p}/U_{e} in terms of the proton and electron masses and the powerlaw indices that characterize the particle spectral distributions in regions where the total particle energy density is at equipartition with that of the mean magnetic field. We also express the field strength and the particle energy density in the equipartition region in terms of the region’s size, mean gas density, IR and radio fluxes, and distance from the observer, and determine values of U_{p} in a sample of nine nearby and local SBNs.
Key words: astroparticle physics / ISM: magnetic fields / cosmic rays / galaxies: magnetic fields / galaxies: starburst
© ESO, 2014
1. Introduction
Supernovae (SNe) are thought to be the main drivers of particle acceleration via the FermiI diffusive shock mechanism (e.g., Gaisser 1990). The radiative yields of relativistic electrons and protons have been measured in the radio to TeV regions.
Proton interactions with ambient gas protons produce neutral pions (π^{0}), whose decay into γ rays is the most significant signature of the main component of cosmic rays (CRs). Measurement of this emission yields the essential ingredient in the energetics of galactic nonthermal particles, and together with synchrotron and Compton emissions by relativistic electrons, allows us to relate diverse phenomena such as star formation (SF) and SN rates, efficiency of particle acceleration, and magnetic field strength. The high SF rates and dense gas in starburst nuclei (SBNs) make these regions prime targets for exploring this relation between stellar and nonthermal quantities.
In a SBN with Hnuclei number density n and volume V, the integrated hadronic γray emission from π^{0} decay is (1)with the integral emissivity measured in units of photon s^{1}(Hatom)^{1}(eV/cm^{3})^{1}, and q_{p} the spectral index of the proton powerlaw distribution (Drury et al. 1994). The value of U_{p} can be determined from the measured value of if n(r) is known. In steady state the spectrospatial particle distributions can be calculated by numerically solving a convectiondiffusion equation which includes all the relevant energy losses (e.g., Paglione et al. 1996; Torres 2004). Normalizing the particle distributions based on their measured radiative yields estimates their energy densities. In particular, measurement of the π^{0}decay γray emission is the most direct way to determine U_{p}.
Improving the physical basis for a reliable extraction of the proton energy density, U_{p}, from γray measurements is well motivated and timely, in light of recent satellite and groundbased observations. These include the detection of three nearby starburst galaxies, NGC 253, NGC 3034 (M 82), and NGC 5945, in the GeV (Ackermann et al. 2012) and TeV (Acero et al. 2009; Acciari et al. 2009; Lenain et al. 2010) regions. Measured fluxes from these galaxies agree with earlier theoretical predictions (NGC 253: DomingoSantamaría & Torres 2005; Rephaeli et al. 2010; NGC 3034: Persic et al. 2008; de Cea et al. 2009; NGC 4945: Lenain et al. 2010) based on convectiondiffusion models for proton and electron propagation and energy losses. While there were appreciable differences in the models treated in those works, predicted values for U_{p} in the SBNs of the three galaxies were around 250 eV cm^{3}.
Even though most of the CR energy is in protons, the level of the unbeamed hadronic emission in most SBNs is not high enough to obtain a reliable estimation of U_{p} from the measurement of hadronic γray emission. This is the main reason why, with current detector sensitivities, γray emission was detected (as we just noted) in only three nearby starburst galaxies. It is therefore important to reformulate the leptonic route for estimating particle energy densities, testing its viability in these three starburst galaxies, and applying the insight gained from applications of both methods to these nearby galaxies to improve the precision with which U_{p} and U_{e} can be determined in SBNs.
Starting with estimates of the duration of a starburst phase, and of the relevant timescales for particle acceleration, energy loss, and advection, we show that particle distributions can be in steady state in a SBN. We continue with the usual assumptions in order to relate the proton and electron densities by charge neutrality, and energy densities through equipartition with the mean magnetic field. Doing so we reformulate the hadronic and leptonic methods for determining particle energy densities from measurements of radio and γray emission, and refine the expressions for the protontoelectron density and energy density ratios. We then obtain an expression for the equipartition magnetic field and particle energy densities in a SBN in terms of an assumed (theoreticallybased) value of the spectral index of the proton density, and basic measured parameters characterizing the region, i.e., size, gas density, IR luminosity, radio flux, radio spectral index, and distance from the observer.
In Sect. 2 we assess the viability of the standard assumption that particle distributions attain a steady state, and the likelihood of reaching energy equipartition with the mean magnetic field in the SBN. The basic expressions for protontoelectron (p/e) ratios and for U_{p} in terms of the electron synchrotron flux are written in Sect. 3. In Sect. 4 these expressions are applied to a sample of nearby and local SBNs. We conclude with a discussion and a summary in Sect. 5.
2. Energy loss and propagation timescales
The benchmark timescale for enhanced stellar activity in a SBN, i.e., the duration of the starburst phase, is typically estimated to be t_{SB} ~ 10^{8} yr. This characteristic time sets the scale for the assessment of temporal nonvariability of particle distributions. Specifically, particle densities may attain a steady state if their characteristic acceleration and weighted energyloss (by collisions and through propagation out of the SBN) timescales are considerably shorter than t_{SB}. If so, and if the acceleration and energy loss timescales are comparable, the particle (spectral) densities are in a steady state.
Acceleration in a SN remnant (SNR) by the FermiI process occurs on a timescale t_{acc} ≡ E/Ė = (ΔE/E)^{1}Δt = β^{1}Δt = (30 /β_{0.033}) Δt ~ 3 × 10^{5} yr, where Δt ~ 10^{4} yr is a typical SNR lifetime, and β_{0.033} is the speed of the SN shock in units of 0.033 c = 10^{4} km s^{1}. Clearly, particle acceleration to all relevant energies occurs on a relatively short timescale.
Protons lose energy mainly by protonproton (pp) interactions and escape out of the SBN, on a characteristic timescale . The two terms on the r.h.s. are the energyloss timescales for, respectively, pp interactions, t_{pp} = (σ_{pp}cn)^{1} with σ_{pp} the corresponding total cross section, and particle removal, , with t_{adv} the timescale for advection in a largescale outflow (i.e., a galactic wind) and t_{diff} the diffusion timescale. In the energy range 10 − 10^{5} GeV, it is σ_{pp} ~ 50 mb, so that yr. For a homogeneous distribution of SNe in a SBN of radius r_{s}, the advection timescale for transfer of particles out of the disk midplane region in a fast (v_{adv} ~ 1000 km s^{1}) SBdriven wind^{1} is t_{adv} = 5 × 10^{4}(r_{s}/ 0.2 kpc)(v_{out}/ 1000 km s^{1})^{1} yr. Particle diffusion is likely to be dominated by randomwalk through the tangled magnetic fields in the SBN. In this dense region the field coherence scale is expected to be much smaller than in the disk (where the smallscale cellular structure has a coherence scale ~ 100 pc), so scaling to a value of 3 pc, the characteristic diffusion time of protons in the SBN is t_{diff} = 1.3 × 10^{5}(r_{s}/ 0.2 kpc)^{2}(λ/ 3 pc)^{1} yr, a value comparable to t_{adv}. From , we get t_{p} ~ 3 × 10^{4} yr for fiducial parameter values typical for SBNs.
Protontoelectron energy density ratios, κ.
The electron energy loss timescale is determined by Coulomb, bremsstrahlung, synchrotron and Compton processes, and escape out of the SBN, , respectively. Limiting the discussion here to electron energies higher than a threshold value γ_{1} below which Coulomb losses become relevant (see Sect. 4), we can ignore this nonradiative process in the estimation of the weighted mean energyloss time. The bremsstrahlung cooling time for electrons traveling through ionized gas with number density n is t_{br} = 4.4 × 10^{7}n^{1} yr. The synchrotronCompton time for electrons traversing a region with disordered magnetic field B with energy density U_{B} = B^{2}/ (8π), and IR energy density U_{IR} = L_{IR}/ (4πr^{2}c), is yr. Under typical SBN conditions, which are fully specified in Sect. 4 (see also Fig. 1), the weighted energy loss time for high energy electrons is t_{e} ~ 4.3 × 10^{4} yr for γ ~ 10^{3}.
Fig. 1 Energy loss rates of an electron of energy γm_{e}c^{2} due to Coulomb, bremsstrahlung, and synchrotronCompton processes in a typical (M 82like) SBN environment: B = 100 μG, L_{IR} = 10^{44} erg s^{1}, r_{s} = 0.2 kpc, n = 100 cm^{3}, n_{e} = 200 cm^{3}. 

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Since typical acceleration and energyloss times are much shorter than the SB duration, particle spectral densities can attain steady state at levels that are proportional to the respective ratios of the energyloss time to the acceleration time. More generally, in a state of hydrostatic and virial equilibrium, it is likely that in the minimumenergy configuration, the energy densities of particles and magnetic fields, which are tightly coupled dynamically and energetically in the SN environment, are in energy equipartition (e.g., Longair 1981). Generally, the denser and more radiatively intense the environment, the tighter is the coupling between all degrees of freedom, including nonthermal particles and magnetic fields. Physical processes that couple nonthermal particles and thermal gas are Coulomb interactions (i.e., ionization, electronic excitations, and bremsstrahlung), Compton scattering, and excitation of magnetic turbulence (e.g., Alfvén waves) by nonisotropic particle distributions. Particle coupling to magnetic fields is particularly strong because of the high field strength in a SBN and its disordered morphology, affecting both particle energy distribution and transport properties. Under such conditions, particlefield energy equipartition would be expected.
3. Particle and field energy densities
In repeated crossings of the shock region, fast electrons and protons in the ambient SNR gas gain energy from their initial fiducial kinetic energy T_{0} ≃ 10 keV (in the Maxwellian tail) to a very high value, O(10^{5}) GeV. In the immediate vicinity of the acceleration sites, and before energy losses substantially modify their initial distributions, the particles’ spectral densities are usually assumed to have a powerlaw (in momentum p) form, N_{j}(p) = N_{0,j}p^{− qj} with j = e,p for, respectively, electrons and protons; in general, q_{e} ≠ q_{p}. If the gas of nonthermal electrons and protons is approximated as an electrically neutral plasma, then (2)The basic energymomentum relation yields dp/ dT = (T/c^{2} + m)(T^{2}/c^{2} + 2Tm)^{− 1 / 2}, and using N_{j}(T) = N_{j} [ p(T) ] dp/ dT, an explicit expression for N_{j}(T) is obtained (e.g., Schlickeiser 2002): (3)The respective normalization can now be obtained by performing the integration in Eq. (2): (4)The p/e number density ratio, ζ = N_{p}(T) /N_{e}(T), can now be explicitly written (5)When it is assumed that q_{p} = q_{e} = q (e.g., at injection), simpler limiting expressions for this ratio are obtained (e.g., Schlickeiser 2002): (6)The general expression for the p/e energy density ratio, (7)can also be written as: (8)In order to explore the relevant range of values of this ratio, we computed κ for several representative values of q_{p} and q_{e} (see Table 1). An approximate expression for κ can be obtained by considering only proton and electron energies higher than the respective particle mass (where the particle spectra, N_{j}(T), are singlepowerlaw in energy): (9)which for q_{p} = q_{e} = q reduces to (10)This expression for the energy density ratio (Eq. (10)) is analogous to the highenergy limit of the number density ratio in Eq. (6) (see also Persic & Rephaeli 2014).
Determining U_{p} from the theoretically predicted value of κ and U_{e}, which is deduced from the measured radio flux, obviously requires knowledge of the mean magnetic field in the emitting region, B. To overcome this (implied) indeterminacy, the assumption of field and particle energy equipartition is commonly made. In addition, the contribution of secondary electrons (from π^{−} decay)^{2} to the (steady state) electron density has to be included.
While the exact form of the particle steadystate spectral density does not generally have a single powerlaw form (e.g., Rephaeli 1979), the radiative yields are largely by protons and electrons with energies higher than a few Gev, for which Coulomb losses (which flatten the spectral density) are subdominant. In this limit, the total electron spectral density can be approximated by (11)where the electron Lorentz factor γ is in the range γ_{1} ≤ γ ≤ γ_{2}, N_{e,0} is a normalization factor of the primary electrons, and χ is the secondarytoprimary electron ratio. The electron spectral index is q_{e} ≥ 2, with the minimal value of 2 corresponding to the strongshock limit of the FermiI acceleration mechanism.
Ignoring the contribution of lowenergy electrons with γ<γ_{1}, the electron energy density is . For q_{e}> 2, (12)For a population of electrons described by Eq. (11), traversing a homogeneous magnetic field of strength B that permeates a region of (spherically equivalent) radius r_{s} located at a distance d from the observer, and emitting a 5 GHz synchrotron radiation flux of f_{5} Jy, the standard synchrotron formula (e.g., Blumenthal & Gould 1970) yields (13)where quantities are expressed in c.g.s. units, the factor a_{qe} is defined and tabulated (in, e.g., Blumenthal & Gould 1970), and . From Eqs. (12) and (13) we derive (14)Since U_{e} includes both primary and secondary electrons, the rough assumption that both populations can be characterized with nearly the same powerlaw index^{3} means that the primary electron energy is U_{e}/ (1 + χ). Denoting the primary p/e energy density ratio (see Sect. 3) by κ(q_{p},q_{e}), the proton energy density is (15)Since tight coupling is expected in the very dense environment of SBN, particle and magnetic field energy densities can be assumed to be close to equipartition (see Eq. (21)). If so, we can express the field in terms of the total particle energy density; this leads to (16)In general, q_{e}, q_{p}, χ, γ_{1}, γ_{2}, and κ need to be known (or assumed) in order to compute U_{p}. The value of q_{e} is readily deduced from measurements of the (nonthermal) radio spectral index, α, through the relation q_{e} = 2 α + 1.
Starburst galaxies: data and results for highenergy activity.
3.1. Proton spectral index
The proton spectral index has been measured in the nearby starburst galaxies NGC 253, NGC 3034, and NGC 4945, as q_{p} ≃ 2.2 (Ackermann et al. 2012). As we discuss below, it can be expected that this value also characterizes proton spectra in other starburst galaxies.
Suprathermal particles injected into a supernova shock have a powerlaw spectrum with index q = (R + 2) / (R − 1), where R is the shock compression ratio, defined as the downstream to upstream density, ρ_{d}/ρ_{u}. In an ideal gas, , where γ is the ratio of the gas specific heats, M_{u} = v_{u}/c_{s} is the shock Mach number, and c_{s} is the sound speed. Since , clearly . The temperature of the upstream medium, T_{u}, is nearly two orders of magnitude higher (T ~ 10^{6 − 7} K) in SB regions than in more quiescent galactic disks (T ~ 10^{4 − 5} K) (Heckman & Lehnert 2000; Fujita et al. 2009). Therefore, for a given shock velocity v_{u}, during the Sedov phase of SNR the Mach number is smaller in the SBN than in the disk, so that the compression ratio of a strong shock in the SBN is expected to be R ≃ 3.6, somewhat lower than the more typical (Galactic) value R ≃ 4. This lower value implies an injection index in the range 2.0 ≤ q ≤ 2.3 (Fujita et al. 2009).
3.2. Electron secondarytoprimary ratio
The secondarytoprimary electron ratio χ depends on the injection p/e number ratio, ζ, and on the gas density, which determines the effectiveness of pp interactions that yield charged and neutral pions. An electron is produced in the decay , followed by ; a positron is produced in the decay π^{+} → μ^{+} + ν_{μ}, followed by . The pp branching ratios are such that in 2/3 of these interactions e^{±} are produced.
The mean free path of an energetic proton for pp interactions in a gas with density n is λ_{pp} = (σ_{pp}n)^{1}. The pp cross section for protons with kinetic energy of a few TeV is σ_{pp} ≈ 50 mb = 5 × 10^{26} cm^{2} (Baltrusaitis et al. 1984), so that the probability for a proton to undergo pp interactions during its 3D random walk through a region of radius r_{s} is then . Given the injection p/e ratio, ζ, and the above branching ratio, the secondarytoprimary electron ratio is (17)In a typical SBN with r_{s} = 0.2 kpc, n = 200 cm^{3}, and q = 2.2–2.3), estimated values of χ are ~ 0.6–1, in agreement with results from more detailed numerical models (e.g., Paglione et al. 1996; DomingoSantamaría & Torres 2005; De Cea et al. 2009; Rephaeli et al. 2010).
3.3. Equipartition magnetic field
As we have already noted, it is quite likely that in their equilibrium minimumenergy configuration particles and magnetic fields, which are tightly coupled dynamically and energetically in the SN environment, are in energy equipartition. We assume that equipartition is indeed attained during the starburst phase, and use it to determine the mean magnetic field in the SBN region. The starting point is an estimate of the electron energy density from the measured radio flux, which we obtain by integrating the electron spectral energy density over the interval [ γ_{1},γ_{2} ].
For consistency with the assumed powerlaw form of the electron spectral density, we take the lowenergy limit γ_{1} to be the value of the Lorentz factor at which the sum of the Coulomb (or electronic excitation, in ionized gas) and bremsstrahlung loss rates equals the synchrotronCompton loss rate. This is also based on the fact that even for the relatively high values of the magnetic field in SBN, the measured radio emission (upon which our normalization of the electron density is based) samples electrons with γ> 10^{3}.
The Coulomb (electronic excitation) loss rate (e.g., Rephaeli 1979) is (18)where n_{e} is the (thermal) electron number density.
The closely related bremsstrahlung loss rate for a H+He plasma with solar abundances, that also includes the contribution of ee scatterings, is (Gould 1975) (19)where n denotes the number density of Hnuclei. The reported expression for neutral plasma holds for γ ≥ 100; at lower γ the ionized and neutral cases essentially overlap (Gould 1975).
The higher order (in γ) synchrotronCompton loss rate (e.g., Blumenthal & Gould 1970) is (20)where ρ_{IR} is the energy density of the (dominant) IR radiation field in the SBN region.
Equating the sum of the first two loss rates with the latter yields an estimate of γ_{1}. In Fig. 1 we display the energyloss rates, expressed in Eqs. (18)–(20), for typical SBN parameters. In our numerical estimates (see Table 2) we use the second of Eq. (19) for the mostlyneutral SBNs in Arp 220 and Arp 299A, and the first for the other, mostlyionized SBNs.
Whereas the dependence of the electron energy density on γ_{1} is appreciable, since γ_{2}> 10^{5} the exact value of the upper end of the γ integral is of little significance for the range of values of q_{e} of interest here; in our calculations we take γ_{2} = 10^{5}.
With both U_{e} and U_{p} determined, the mean field strength is deduced from (21)where η = 1 in equipartition, but somewhat lower, η = 3 / 4, in strictly minimumenergy configuration (Longair 1981)^{4}. In terms of the particle p/e energy density ratio, κ, the particlefield coupling condition is B^{2}/ 8π = ηU_{p} [ 1 + (1 + χ) /κ ], so that (22)Given the values of n, the size of the SBN region, and the IR energy density (which is computed from the L_{IR} and the region size), as listed in Table 2, the expression for B in the last equation (with η = 1) can be inserted in Eq. (20), and using the other two loss rate equations, the value of γ_{1} can be deduced. This value of γ_{1} is then substituted in the equation for B to obtain the equipartition value of the mean field. We note that in most cases the corresponding synchrotron frequency, MHz, where the radio spectrum is expected to curve to a flatter slope for decreasing frequencies, is comparable to our reference frequency of 5 GHz.
4. Proton energy densities in SBNs
In starburst galaxies SF is very intense in a relatively small nuclear region (the SBN) with effective radius r_{s} ≈ 0.2 kpc – with , where R_{sb} and h_{sb} are the radius and height of the region. By contrast, lowintensity SF quiescently proceeds throughout the galactic disk (as in normal, i.e., nonstarburst, spirals, such as the Galaxy).
For a sample of local SBNs, values of U_{p} and B were calculated using the relevant observational quantities in Table 2, starting with the radio flux and spectral index. Because of appreciable observational uncertainties, mostly in the values of the gas density and the size of the emitting region, and because of modeling uncertainties, the derived values of B and U_{p} are also uncertain, typically by a factor which we estimate to be ~1.4 and ~2. While our results for these two quantities would not seem to be that precise, it should be emphasized that some of the uncertainties are inherent given the basic difficulties in determining the size and density of the SBN, the limited spatial resolution, and the rudimentary level of the spectral γray measurements. We note that, in light of these substantial uncertainties, the (modeling) uncertainty in B, when the latter is calculated assuming energy equipartition as compared to minimum energy, is relatively insignificant. For example, for the two wellstudied nearby starburst galaxies, NGC 253 and NGC 3034 (M 82), values of B are only ~ 15% lower in the minimum energy configuration compared to the equipartition values (listed in Table 2). The CRderived results are stable over much of the ISM parameter space of SBNs (Boettcher et al. 2013).
Our electronbased estimates of the proton energy densities are in agreement with γray measurements of π^{0}decay emission for the three galaxies NGC 253, NGC 3034, and NGC 4945 for which such emission was detected. The results for the very compact SBNs of Arp 220 and Arp 299A represent extreme cases; small source regions and relatively hard electron spectra result in high magnetic fields and high CR energy densities, B ~ 0.2 mG and U_{p} ~ 500 eV cm^{3}. However, it is questionable whether in such extreme environments, with conditions that are more typical of SNRs, steady state and equipartition are actually attained (e.g., Torres 2004). The unusually high values of γ_{1} derived for these highly compact nuclei may signal, in fact, a breakdown in our assumptions, the most critical one being particlefield equipartition.
5. Discussion
Active SF leads to particle acceleration by SN shocks. Considerations of the acceleration, relevant energy losses, and starburst timescales, indicate that relativistic proton and electron distributions reach steady state during most of the starburst phase. Given the tight coupling between the particles and magnetic fields in the dense plasma, it is quite likely that energy equipartition is achieved in the SBN region. With an assumed theoretically motivated p/e ratio, the assumption of equipartition provides the requisite relation to determine particle energy densities and the mean field from spectral radio measurements.
Essential to this radiobased method is a reliable estimate of the p/e energy ratio, κ. Adopting the common assumption of an overall electrically neutral nonthermal plasma, we derived an approximate expression for this ratio as a function of the electron and proton spectral indices, q_{e} and q_{p}. We note that, in the limit of q_{e} = q_{p} = q (e.g., at injection), κ ≃ (m_{p}/m_{e})^{(3 − q) / 2}; this simple relation is supplementary to the analogous, wellknown p/e number ratio, N_{p}/N_{e} = (m_{p}/m_{e})^{(q − 1) / 2} (e.g., Schlickeiser 2002). Even though the assumptions of singleindex steadystate spectra and particlefield equipartition may be unrealistic, at our present knowledge of the SBN environment relaxing any of these simplifications necessarily leads to a more parameterrich formalism that will invariably result in arbitrariness in guessing parameter values in what is essentially an underdetermined problem.
For the determination of q_{p}, we have assumed that SBN γray spectra (in the observed Fermi/LAT and IACT energy ranges) are dominated by emission from π^{0}decay owing to the much higher SF rate and mean (target) gas density in the SBN than in the (rest of the) disk. The theoretical expectation of proton injection index in the range 2.0 ≤ q ≤ 2.3 is fully consistent with the measured value q_{p} ≃ 2.2. Because of the lack of spatial information on the distribution of γray emission in the nearby starburst galaxies, our expectation on the respective contributions of the SBN and disk regions is based on theoretical predictions, particularly our own detailed numerical modeling of the emission in M 82 and NGC 253 (using a modified version of the GALPROP code: Persic et al. 2008 and Rephaeli et al. 2010; see also DomingoSantamaría & Torres 2005 for NGC 253). These analyses do suggest that while the relative contribution of the disk is not negligible, it comprises only a small fraction due to further steepening of the particle spectra in the disk. However, given the uncertainty in the exact values of both the measured and predicted powerlaw indices, there is also an uncertainty in the relative contributions of the SBN and disk.
Our work here improves on our earlier discussion and partial implementation of the radiobased method for determining electron and proton energy densities in active regions of SF (Persic & Rephaeli 2010). We do so by accounting for electron radiative losses, by using a more accurate calculation of the p/e ratio, and basing our approach on insight gained from our previous implementation of a modified version of the GALPROP code that fully accounts for both spectral and spatial evolution of proton and electron distributions in the SB region and throughout the disk (Persic et al. 2008; Rephaeli et al. 2010). Our general approach and its quantitative implementations for predicting the highenergy spectra of the starburst galaxies NGC 253 and NGC 3034 have been validated by good agreement with γray measurements (Acero et al. 2009; Acciari et al. 2009; Ackermann et al. 2012).
Following on previous work (Beck & Krause 2005), in a recent paper Lacki & Beck (2013, hereafter LB13) discussed the validity of fieldparticle equipartition in a SB environment, accounting for secondary electrons and strong energy losses. While their main conclusions on deducing U_{p} from radio measurements do agree with ours (in both Persic & Rephaeli 2010 and this work), there are substantial differences between our respective treatments. First, we start with the electron spectrum as deduced from radio measurements, including the contribution of secondary electrons to the emission. We then use an analytically derived primary p/e energy density ratio (using the relevant parameter values) to compute U_{p}. In contrast, the starting point of the LB13 analysis is the proton energy density, which they take to be related to the electron energy density by the same factor, 75, for all the galaxies in their sample. Second, whereas we assume electric neutrality of the accelerated particles to determine the primary p/e ratios for different electron and proton spectral indices, LB13 start from an assumed universal p/e number density ratio, which they adjust by accounting for the electrons’ energy losses. Third, we compute the secondarytoprimary electron mumber ratio by using the primary p/e number ratio, the mean proton free path in a gas with a given density, and the branching ratios in pp interactions, whereas LB13 estimate this ratio by scaling the injection p/e ratio by 1/6 the value of the estimated fraction of the proton energy that goes into π^{±}. These differences in approach and implementation led to substantially different results for U_{p} and B (listed in our Table 2 and their Table 3). Whatever the details, it should be noted that for the nearby starburst galaxies NGC 253, NGC 3034, and NGC 4945 our estimated U_{p} and B agree with results of direct measurements. This agreement suggests that the equipartition assumption, which we made to derive CR and B energy densities, is globally verified in these SBNs, at least as an average property. For NGC 3034 this suggestion was made early on by Völk et al. (1990) on the condition that ζ(>1 GeV) ~ 10^{2}, a condition that is consistent with our procedure, see Eq. (6).
If the agreement between radio estimates and γray measurements of U_{p} and B in SBNs is further validated and established, the radio method for reliable estimation of proton energy densities will be particularly useful for distant (z ≳ 1) galaxies whose intense SF is exemplified (albeit at lower levels) by the nearby starburst galaxies, but whose faint γray fluxes are not detectable with current or upcoming instruments, whereas their <0.1 mJy radio fluxes are (e.g., Tozzi et al. 2009).
Theoretical expectation is that powerlaw indices of proton and electron source spectra are nearly identical. Under typical interstellar medium (ISM) conditions, electrons lose energy more efficiently than protons, resulting in a relative steepening of the electron spectrum. Secondary electrons (and positrons, produced in π^{±} decays following pp collisions) initially have a slightly flatter spectrum (by Δq ≃ 0.2) than the parent proton spectrum for energies ≳1 GeV, but then their spectrum steepens due to severe energy losses. Detailed numerical models of emission from starburst galaxies show that primary and secondary electrons have roughly similar spectral shapes at energies ~ 10 MeV–1 TeV (e.g., DomingoSantamaría & Torres 2005; De Cea del Pozo et al. 2009; Rephaeli et al. 2010). Therefore, in the relatively small SBN region, where energetic particles have not yet ventured out too far from their acceleration sites, it is quite reasonable (for our purposes here) to characterize their spectra with the same index. After all, from a practical point of view, both primary and secondary electrons contribute to the main observable upon which we base our analysis – radio emission – which is described by a singleindex powerlaw spectrum.
Energy equipartition may be attained (over time) under conditions of tight coupling of the main matter and energy components of a physical environment in its minimum energy configuration. The electromagnetic emission of a SBN that directly comes from relativistic particles manifests itself in the radio and in γ rays. The total energy density in the SBN responsible for such nonthermal emission is U = U_{CR} + U_{B}. As noted in Sect. 2, under physical conditions prevailing in a SBN the particles and the Bfield behave like relativistic fluids tightly coupled with each other. Their equilibrium configuration most likely corresponds to a state of minimum energy, which is achieved for U_{B} = ηU_{CR} with η = 3 / 4 (Longair 1981). Clearly, this minimumenergy condition is very close to equipartition (η = 1), so at equilibrium the particle energy density nearly equals the field energy density.
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All Tables
All Figures
Fig. 1 Energy loss rates of an electron of energy γm_{e}c^{2} due to Coulomb, bremsstrahlung, and synchrotronCompton processes in a typical (M 82like) SBN environment: B = 100 μG, L_{IR} = 10^{44} erg s^{1}, r_{s} = 0.2 kpc, n = 100 cm^{3}, n_{e} = 200 cm^{3}. 

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