The fluxes of the inverse Compton γ-rays expected from synchrotron X-ray nebulae are calculated and the observability of this radiation is discussed. The main emphasis is given to the pulsar driven nebulae (plerions), although the results and conclusions are equally applicable to the extended non-thermal X-ray sources produced by shock-accelerated electrons in the shell-type supernovae remnants. The existence of the non-thermal (synchrotron) component of X-radiation in these objects implies an effective acceleration of electrons up to energies Ee ~ 100B1/2−5€keV TeV (B −5 = B/ 10−5 G; € keV = €/1keV). The inverse Compton scattering of the same electrons on the ambient photon fields may result in observable TeV γ-radiation as well. The 2.7-K microwave background radiation is, as a rule, the dominant target photon field for production of γ-rays. This provides a direct relation, for the given magnetic field, between the typical energies of the synchrotron (€) and inverse Compton (E) photons produced by the same electrons: €keV ≃ 0.07 (E/1 TeV)B − 5. The ratio of relevant energy fluxes at these energies is about fγ( ≥ E)/fx( ≥ € ) ≃ 0.1B−5−2 ξ, where the fx ( ≥ € ) is the energy flux of soft X-rays corrected for absorption, and the factor ξ ≃ 1 is introduced in order to take into account possible differences in the source sizes responsible for the fluxes observed by X-ray and γ-ray detectors. Since the fluxes of X-ray nebulae with angular size less than a few arcmin are typically at the level of fx ≤ 10−11 erg cm−2 s−1, then the detectability of these objects in TeV γ-rays, by current atmospheric Cherenkov telescopes with sensitivities a few times 10 −12 erg cm−2 s−1, would significantly depend on the ambient magnetic field. In particular, the γ-ray observability of these X-ray nebulae becomes problematic even for the lowest possible magnetic field, i.e. B ~ BISM ≃ 3–5 μG. Otherwise, the detection of γ-rays from such sources would require ξ ≫ 1, which implies that in fact the relativistic electrons occupy a significantly larger region around the accelerator than the ≥ 1 arcmin X-ray nebulae resolved by the ROSAT and ASCA satellites. We argue that the invocation of such an hypothesis allows us to explain satisfactorily the flux of TeV γ-rays detected from the direction of the recently discovered faint X-ray nebula around the pulsar PSR B1706 − 44.
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Aharonian et al. (1997) studied this question.