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Table 2.

Summary of the results for the three filaments considered.

System nISM γMPD γesc ΔB ϵ R/d0
cm−3 μG ×10−3
Guitar 0.6 1.2 × 108 1.2 × 107 78 6 0.5

Lighthouse 0.07 4.0 × 109 8 × 107 26 19 2

J2030+4415 4.0 5 × 108 ≲4 × 107(Lf/pc) 40 < ΔB < 181

Notes. Here, nISM is the ambient number density, γMPD the Lorentz factor associated with the pulsar MPD, γesc the Lorentz factor of the particles producing the instability, ΔB the amplified magnetic field in the filament, ϵ the fraction of the pulsar power carried by the escaping particles, and R/d0 the radius of the filament base, in terms of the bow shock standoff distance, d0. For J2030+4415 it is only possible to define a range for the amplified field, since there are indications that the filament formed only tevent ∼ 32 yrs ago and its present wf might not be determined by synchrotron losses. A lower limit comes from asserting that X-ray emission must be produced by particles with γ ≤ γMPD, while an upper limit is derived from the condition tevent < τsync (see main text). From the maximum magnetic field, through Eq. (8) one also determines an upper limit of γesc, which depends on Lf, since the feature might not be in its final form.

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