Issue 
A&A
Volume 592, August 2016



Article Number  A52  
Number of page(s)  8  
Section  Astrophysical processes  
DOI  https://doi.org/10.1051/00046361/201628116  
Published online  22 July 2016 
Do asteroids evaporate near pulsars? Induction heating by pulsar waves revisited
^{1} Sorbonne Universités, UPMC Univ. Paris 6 et CNRS, UMR 7095, Institut d’Astrophysique de Paris, 98bis bd Arago, 75014 Paris, France
email: kotera@iap.fr
^{2} Department of Astronomy & Astrophysics, Kavli Institute for Cosmological Physics, The University of Chicago, Chicago, IL 60637, USA
^{3} LUTH, Observatoire de Paris, PSL Research University, CNRS, Université Paris Diderot, 5 place Jules Janssen, 92190 Meudon, France
email: fabrice.mottez@obspm.fr
^{4} Observatoire Astronomique, Université de Strasbourg, 11 rue de l’Université, 67000 Strasbourg, France
Received: 12 January 2016
Accepted: 26 April 2016
Aims. We investigate the evaporation of closeby pulsar companions, such as planets, asteroids, and white dwarfs, by induction heating.
Methods. Assuming that the outflow energy is dominated by a Poynting flux (or pulsar wave) at the location of the companions, we calculate their evaporation timescales, by applying the Mie theory.
Results. Depending on the size of the companion compared to the incident electromagnetic wavelength, the heating regime varies and can lead to a total evaporation of the companion. In particular, we find that inductive heating is mostly inefficient for small pulsar companions, although it is generally considered the dominant process.
Conclusions. Small objects like asteroids can survive induction heating for 10^{4} yr at distances as small as 1 R_{⊙} from the neutron star. For degenerate companions, induction heating cannot lead to evaporation and another source of heating (likely by kinetic energy of the pulsar wind) has to be considered. It was recently proposed that bodies orbiting pulsars are the cause of fast radio bursts; the present results explain how those bodies can survive in the pulsar’s highly energetic environment.
Key words: minor planets, asteroids: general / stars: winds, outflows / binaries: close / pulsars: general
© ESO, 2016
1. Introduction
Pulsars are highly magnetized, rapidly rotating neutron stars (NS) that lose their energy principally via electromagnetic cooling, which results in their spindown. The pulsar outflow comprises a lowfrequency (ω = 2π/P, with P the pulsar spin period) Poynting fluxdominated component (also called the pulsar wave), a relativistic wind, and highenergy radiation from the magnetosphere. The energy of the outflow is believed to be dominated by Poynting flux close to the star, and by relativistic particles farther out (as observed in particular in the case of the Crab pulsar). However, the location of this transition remains a puzzle to the community (see, e.g., Kirk et al. 2009, for a review).
Pulsars are often observed to evolve in multiple systems, and evaluating the amount of energy absorbed by the companions is paramount to understanding their evolution and emission. The most common companions are white dwarfs (Savonije 1987; Manchester et al. 2005; Ransom et al. 2014) or Mdwarfs (Roberts 2013), but smaller objects such as planets, asteroids, or comets can also orbit pulsars (Wolszczan & Frail 1992; Thorsett et al. 1993; Bailes et al. 2011). The existence of asteroid belts around pulsars has been invoked by several authors to explain timing irregularities (Shannon et al. 2013), antiglitches (Huang & Geng 2014), or burst intermittency (Cordes & Shannon 2008; Deneva et al. 2009; Mottez et al. 2013b).
Asteroids around pulsars could also be at the origin of fast radio bursts (FRBs). These brief radio signals (typically 5 ms at a given frequency) are dispersed in frequency (as for pulsar signals), but with a dispersion corresponding to cosmological distances (e.g., Champion et al. 2016, and references therein). Going against the mainstream scenarios involving the collapse of massive objects, Mottez & Zarka (2014) proposed that FRBs could be emitted by bodies orbiting extragalactic pulsars (see also Dai et al. 2016). Highly collimated waves would be produced by the magnetic wake of these objects immersed in the relativistic pulsar wind. The collimation would enable their detection even at distances of hundreds of Mpc. This model can naturally produce the repeating bursts reported by Spitler et al. (2016) in the presence of an asteroid belt.
For massive companions, the standard scenario stipulates that old neutron stars are spun up to periods <10 ms in close binary systems by transfer of mass and angular momentum by the lowmass companion (Alpar et al. 1982). This accretion process leads to the production of Xrays detected as lowmass Xray binaries. In particular, the socalled black widow (dwarf companion with mass m ~ 0.002−0.07 M_{⊙}) and redback (Mdwarf companion with mass m ~ 0.1−0.4 M_{⊙}) pulsars illustrate the importance of energy absorption by companions on the evolution of binary systems. These systems have very lowmass secondaries and orbital periods of less than 10 h. Early studies pointed out that these pulsars should theoretically evaporate their companion by highenergy radiation (Ruderman et al. 1989) and/or by Roche lobe overflow. At the time of their discovery, it was assumed that black widows provided the missing link between lowmass Xray binaries and isolated millisecond pulsars.
Since pulsar environments can evaporate white dwarves and Mstars orbiting them, it may seem surprising that smaller planets and asteroids could be maintained in a solid state at similar distances to the neutron star. In the present paper, we propose an explanation for their survival.
To date, it has been confirmed that two pulsars (PSR B1257+12 and PSR B162026) host planets. PSR B1257+12 hosts three planets at distances on the order of the astronomical unit (in the pulsar wind) with orbital periods in the range of days and weeks (Wolszczan & Frail 1992). The distances are therefore greater than in close binary systems (orbital periods in the range of hours) such as black widow and redback systems, which can provide an explanation to the stability of the planets. PSR B162026 is a neutron starwhite dwarf binary, that was confirmed to host a Jovian mass companion orbiting at 23 AU (Sigurdsson et al. 2003). The distant orbit makes this system illsuited for our framework, and could explain by itself why the companion has not been evaporated. On the other hand and if confirmed, the suspected belt of asteroids at a small distance from PSR 1931+24, with an orbital period ranging in minutes (Cordes & Shannon 2008; Deneva et al. 2009; Mottez et al. 2013a,b) is puzzling and would require an alternative justification for its survival. PSR J17191438 presents an orbiting candidate planet (Bailes et al. 2011). Its Jovian mass companion has a short orbital period of ~2.2 h, implying a compact orbital distance of ~0.95 R_{⊙}, and a minimum mean density of 23.3 g cm^{3}. This density suggests that it may be an ultralowmass carbon white dwarf rather than a planet. The evaporation timescale of this companion should also be investigated.
At distances within a few lightcylinder radii from the neutron star, there is a general agreement that most of the energy outflowing from the pulsar is under the form of the Poynting flux associated with the pulsar wave (Kirk et al. 2009). The pulsar wave is the electromagnetic structure created by the rotation of the neutron star magnetic field at the pulsar spin frequency (with an inclination angle i ≠ 0 relative to the spin axis). Outside the lightcylinder, this corresponds to a lowfrequency spherical wave propagating at a velocity ~c and of wavelength equal to two lightcylinder radii (Deutsch 1955). On the scale of a companion radius, this wave can be considered a plane wave. Because the pulsar wave constitutes the main flux of energy out of the pulsar, we consider that it is potentially the main source of heat for pulsar companions. In the remaining sections, we investigate the physical parameters that control the efficiency of the pulsar companion heating by the pulsar wave.
2. Companion heating by induction: model
All numerical quantities are denoted Q_{x} ≡ Q/ 10^{x} in cgs units unless specified otherwise.
2.1. Energy flux of the pulsar wind
The energy loss rate (or luminosity) of a pulsar with moment of inertia I, rotation period P, radius R_{⋆}, dipole magnetic field strength B_{⋆}, and corresponding period derivative Ṗ reads (e.g., Shapiro & Teukolsky 1983) (1)The energy flux in the pulsar wind at distance a, large compared to the pulsar light cylinder radius, R_{L} = cP/ (2π) ~ 4.8 × 10^{8} cm P_{3}, can then be written (Arons & Tavani 1993) (2)where f_{p} = ΔΩ_{p}/ (4π) is the fraction of the sky into which the pulsar wind is emitted. We note that this flux can also be expressed as F_{w} = cB^{2}(1 + σ_{B})/ (4πσ_{B}); the magnetization parameter is defined as σ_{B} ≡ B^{2}/ [4πc^{2}(n_{i}m_{i} + κ_{±}m_{±}n_{±})], i.e., the ratio of the magnetic energy flux to the kinetic energy flux in the comoving wind frame. Here B, n_{i}, m_{i}, and n_{±} and m_{±} are respectively the magnetic field strength, the number density, the mass of ions, and pairs of the cold plasma, and κ_{±} the pair multiplicity. In this work, we assume that the wind is Poyntingflux dominated (σ_{B} ≫ 1) in the region where the companion is located. It can be demonstrated that this is valid out to the termination shock for a supersonic, radially expanding ideal magnetohydrodynamics (MHD) wind. In more realistic situations, the dissipation to kinetic energy could happen earlier, but all models predict a Poyntingflux dominated wind close to the star (e.g., Kirk et al. 2009).
The companion at a distance a can intercept a fraction f of this flux, provided that it falls in the wind beam and absorbs a flux, F_{abs} = fQ_{abs}F_{w}, which can be written in terms of absorbed luminosity: (3)Here, Q_{abs} is the energy absorption efficiency. Using the magnetization parameter σ defined above, this quantity can be decomposed into two components: the absorption of energy from the pulsar wave, characterized by an efficiency Q_{em}, and the absorption of kinetic energy from the pulsar wind, of efficiency Q_{kin}, (4)The next two sections are devoted to the evaluation of Q_{em} ~ Q_{abs} for a Poyntingflux dominated case when σ_{B} ≫ 1.
2.2. Absorption properties of a body in an electromagnetic wave
The absorption properties of a spherical body in an electromagnetic wave can be modeled by the Mie theory (van de Hulst 1981). Two parameters govern the regime in which absorption or scattering occurs: the ratio of the size of the body to the incident wavelength (5)and the complex refractive index of the medium N = N_{r} + N_{i}, where N_{r} and N_{i} are real.
2.2.1. Refractive index of the companion
Companions orbiting a 10 ms pulsar at a distance a = 1 R_{⊙} see an alternating magnetic field of amplitude B ≤ 10 G with a 100 Hz frequency^{1}. The electric field induced by the pulsar wind (v ~ c) is E ≤ 10^{5} V/m. This is less than the electric strength encountered in most materials (larger than 10^{6} V/m). Therefore, the companions are not ionized by the electric field induced by the pulsar wave. Similar conditions are met for companions orbiting standard pulsars (P ~ 1 s) beyond the light cylinder. Therefore, the usual approximations and textbook data can be used to estimate the electromagnetic properties of the constituents of pulsar companions.
The refractive index can be calculated using the Maxwell equations and the material equation J = σE where J is the current density and σ is a scalar conductivity (Born & Wolf 1980). The dispersion equation reads (6)where ω = 2π/P, k is the wave number, and ϵ and μ the dielectric permittivity and magnetic permeability of the medium, respectively. The refractive index N defined by N^{2} ≡ k^{2}c^{2}/ω^{2} can be written (7)Pulsars rarely spin faster than with a millisecond period, thus ω ≲ 6 × 10^{3} s^{1} (a strict lower bound on the spin is given by Haensel et al. 1999). For low electromagnetic frequencies (up to infrared frequencies), σ is real in any kind of material. For companions made of degenerate matter, the electrical conductivity can be estimated as σ ~ 10^{24} s^{1}ρ^{2/ 3}T^{1}, for densities ranging from ρ ~ 10^{6−12} g cm^{3}, and T the stellar temperature (Canuto & Solinger 1970). White dwarfs typically have ρ ~ 10^{9} g cm^{3} and T ~ 10^{4−7} K. For T = 10^{5} K, σ ~ 10^{22} s^{1}. To date, the planets orbiting pulsars that have been discovered could be either lowmass white dwarfs made of degenerate matter, or made of ordinary matter. For T = 10^{5} K, σ ~ 10^{25} s^{1}. Smaller objects such as asteroids could be modeled as silicate rock or as ferrous metals. The conductivity of sea water is on the order of σ ~ 10 Mho m^{1} ~ 10^{10} s^{1}. In metals, σ ~ 10^{6}−10^{7} Mho m^{1} ~ 10^{17} s^{1}. For solid rocks in the terrestrial crust, σ ~ 10^{3} Mho m^{1} ~ 10^{6} s^{1}, but in some conductive belts (for instance between the African Rift and Namibia) σ ~ 10^{1} Mho m^{1} (Gough 1989).
In all materials, the permittivity ϵ is of order unity, rarely exceeding 100. For instance, waterfree iron ore has ϵ ~ 5 and iron oxides ϵ ~ 2.
Given the above estimates, one can neglect the real part of N^{2} in our framework. The real and imaginary parts of N can then be extracted from Eq. (7): (8)For example, for a companion made of iron (or any other ferromagnetic material), μ> 10^{3} and N_{r} ≫ 10^{3}. For solid rocks in the terrestrial crust, μ ~ 1 and N_{r} ~ 10^{3} for a P = 1 s pulsar and N_{r} ~ 30 for a P = 1 ms pulsar.
For white dwarfs, the very large conductivity σ implies N_{r} ≫ 10^{6}.
Fig. 1
Absorption coefficient Q_{abs} as a function of the size ratio x = R/cP and of the refractive index N_{r} of the companion in the Metallic regime (N = N_{r} = −N_{i}). Overlayed are the contours of the analytical approximation, in black for Region 1 (xN_{r} ≪ 1, Eq. (10)) and in white for Region 2 (xN_{r} ≫ 1, Eq. (9)). The grayshaded region corresponds to parameters outside the confidence range of the computation with Damie. 
2.2.2. Absorption coefficient
Here we compute the absorption coefficient Q_{abs}, defined in Eq. (3) as the proportion of energy absorbed by the companion, relative to the flux of incident energy of the wave through the section of the companion. We perform a numerical computation of Q_{abs} using a version of the Damie code, based on Lentz (1976)^{2}. We have tested the program with real and complex values of N^{2}, and compared the results with analytical approximations given in van de Hulst (1981) for various regions of the (x,N) parameter space. We find that numerical and analytical methods give consistent values within an error of <21%. This level of agreement is sufficient for our purpose as we are mostly interested in orderofmagnitude estimates, given the uncertainties of our other parameters.
Figure 1 shows the value of the absorption coefficient computed with Damie as a function of the size parameter x = R/ (cP) and of the refractive index N, in the socalled Metallic regime, where N = N_{r} = −N_{i} for values of N larger than one.
As expected, for large objects (x ≳ 1), Q_{abs} ~ 1. This means that all the flux received from the pulsar wave is absorbed. The values x ≳ 1 correspond to planetsized and white dwarfsized objects (R ≥ 1000 km) in a millisecond pulsar wind (cP = 3000 km for P = 10 ms). For such objects, taking into account the Mie theory does not modify the heating rate.
On the other hand, for smaller objects with x< 1, the level of absorption is reduced by orders of magnitude. For instance, for a kilometersized asteroid orbiting a standard pulsar (P = 1 s), x = 3 × 10^{6}. If it is made of rocks, N_{r} ~ 30, and it can be read Q_{abs} ~ 10^{8}. A value Q_{abs} ~ 10^{12} is even reached when N_{r} ~ 10^{3}.
For x ≪ 1, van de Hulst (1981) gives an analytical expression for the absorption coefficient (we note, however, the corrected typo in the numerator) (9)The absorption coefficient computed with Eq. (9) is plotted in Fig. 1 (white contours). For small values of x, this approximation is numerically unstable. An approximation for the parameter space where N_{r}x ≪ 1 called “Region 1” was proposed (van de Hulst 1981): (10)As shown in Fig. 1 (black contours), this approximation is valid for the smallest values of N_{r}x. The domain corresponding to xN_{r} ≥ 1 was denoted “Region 2” by van de Hulst (1981). For xN_{r} ≫ 1, Eq. (9) can be approximated as (11)Region 2 corresponds roughly to planets and white dwarfs, while Region 1 corresponds to planetesimals, asteroids, and comets^{3}.
White dwarfs, with N_{r} ≫ 10^{6}, are hence highly reflective bodies, as confirmed by the Mie theory. Indeed, Q_{abs} → 0 (Eq. (11)). If the pulsar outflow is under the form of a pulsar wave while it reaches the white dwarf, it should not absorb any energy and should not evaporate. This goes against the existence of black widow systems. It thus seems likely that the outflow is not Poyntingflux dominated as it reaches the white dwarf companion. One possible scenario is that the pulsar wave energy is dissipated by plasma heating, in the dense plasma surrounding the evaporating white dwarf.
3. Effects on the evaporation of companions
We discuss in this section the impact of Q_{abs} on the evaporation rate of pulsar companions. A simple energy balance gives the evaporation timescale of the companions as (12)where t_{ev} is the minimum time of evaporation, E_{abs} is the total energy absorbed at time t, E_{rad} the total radiated energy, E_{g} the gravitational binding energy, and E_{c} the cohesive energy^{4}. Two regimes will be distinguished in this paper. For massive, degenerate companions the cohesive energy can be neglected (Sect. 3.1), while for lowmass companions it dominates (Sect. 3.2). Gravitational and cohesive energies are of the same order of magnitude for bodies about the mass of the Earth. In both cases, we neglect the radiative cooling, but we will include it in a more refined treatment in a future paper.
3.1. Ablation and evaporation of massive companions (degenerate and nondegenerate)
For massive companions, the dominant process for evaporation is the gravitational escape of the gas. The evaporation timescale, t_{ev}, results from the balance between the energy flux input from the pulsar wave and the rate of gravitational escape of the heated material (van den Heuvel & van Paradijs 1988). The luminosity available to drive the wind of a companion of mass M and radius R located at a distance a from the pulsar is then (1/ 2)Ṁv^{2} = Q_{abs}(f/f_{p})(R/ 2a)^{2}L_{p}. Assuming that the wind velocity is on the order of the escape velocity v = (2GM/R)^{1/ 2} from the surface of the companion, the gravitational binding energy of the companion reads (13)and the evaporation timescale For low values of M when the star is degenerate, the massradius relation follows roughly R/R_{⊙} = 0.013(1 + X)^{5/ 3}(M/M_{⊙})^{− 1/ 3}, where X is the hydrogen fraction; the evaporation time can then be expressed(16)The spindown luminosity is on the order of L_{p} ~ 10^{35}erg s^{1} for a typical millisecond pulsar with R_{⋆} = 10 km, P = 10 ms, B = 10^{8} G, and on the order of L_{p} ~ 10^{31}erg s^{1} for a standard pulsar with P = 1000 ms, B = 10^{12} G (see Eq. (1)).
Gravitational (t_{ev,g}) and cohesive (t_{ev,c}) evaporation timescales due to induction heating for various pulsar and companion parameters.
This equation is analogous to those in van den Heuvel & van Paradijs (1988). These estimates can be applied to PSR B1957+20, a benchmark black widow system suspected of ablating its companion (e.g., Phinney et al. 1988; Kluzniak et al. 1988; Arons & Tavani 1993; Callanan et al. 1995; Khechinashvili et al. 2000; Stappers et al. 2003; Reynolds et al. 2007; van Kerkwijk et al. 2011). PSR B1957+20 has a period of P = 1.61 ms, and its dwarf companion of mass M = 0.021 M_{⊙} orbits at a distance a = 2.1 R_{⊙} (P_{orb} = 9.2 h), hence yr. However, as argued at the end of Sect. 2.2.1, the high refractive index of white dwarfs implies that Q_{abs} ≪ 1, thus t_{ev,WD} ≫ 10^{6}yr. The conclusions derived in van den Heuvel & van Paradijs (1988), namely that the evaporation of the companion (strongly dependent on R_{⋆} and X) takes only a few million years, remain valid only if the absorbed energy is principally kinetic (Eq. (4)). The same conclusions apply for PSR J17191438 (period P = 5.7 ms), if its companion is indeed an ultralowmass carbon white dwarf with M = 0.015 × 10^{3}M_{⊙}, R = 4.2 × 10^{4} km, and a = 0.95 R_{⊙}.
For planet companions made of ordinary matter, the mass/radius relationship simply reads M = (4π/ 3)R^{3}ρ, where ρ is the average density. The evaporation time can then be expressed (17)This equation can be applied to the planets orbiting PSR 1257+12. The results are given in Table 1 for two values of the refractive index N_{r} that correspond to planets made of rocks and to more metallic planets. We find that the closest planet can survive a few million years. The two other planets can reach a billion years. This estimate neglects the thermal energy radiated by the planet; therefore, the evaporation time through Poynting flux absorption may be underestimated.
If the companion of PSR J17191438 is actually a nondegenerate planet with minimum mean density ρ = 23.3 g cm^{3}, then x ≫ 1, but with N_{r} ≲ 100, implying Q_{abs} ≳ 10^{2} and for f = f_{p} = 1, which is compatible with the observation of the companion.
3.2. Evaporation of small nondegenerate companions
In the case of small objects like asteroids, Eq. (17) fails because the dominant process for evaporating the body is no longer gravitational escape but heating, melting, and evaporation.The cohesive energy can be expressed as (18)with K the cohesive factor that depends on the material (Kittel 1998). In particular, the cohesive factor of iron is K_{iron} = 7.4 × 10^{10} erg/g (and the orders of magnitude are similar for rock).
Equating with E_{g}, the cohesive energy starts to dominate for a masstosize ratio of M/R ≲ 10^{18} g cm^{1}. For ordinary matter, this constraint can then be expressed in terms of companion size as (19)In this regime, the evaporation timescale can be calculated (20)which leads to (21)For small objects, and when the pulsar energy is mostly in the form of Poynting flux, Q_{abs} is low and has a strong influence on the evaporation time. The comparison of t_{ev,g} and t_{ev,c} shows, as expected, that when small bodies have melted and vaporized, the gravitational escape that follows is very fast.
Fig. 2
Contours of evaporation timescales (in yrs) of nondegenerate pulsar companions (t_{ev,g} and t_{ev,c}, Eqs. (17) and (21)) as a function of the companion radius R and its distance a to the pulsar in solar radii, for pulsar spin periods and magnetic fields as indicated (left to right: P = 1,10,100 ms and B = 10^{8},10^{8},10^{12} G), for conductivity times magnetic permeability σμ = 10^{6}s^{1} and density ρ = 1 g cm^{3}. The white dotted line delimits the region where the cohesive energy dominates over gravitational energy (for small companions) for evaporation. The white region indicates evaporation times t_{ev}< 10 yr and yellow regions t_{ev}> 10^{12} yr. 
Figure 2 shows the evaporation timescales of nondegenerate pulsar companions (t_{ev,g} and t_{ev,c}, Eqs. (17) and (21)), for three spin periods. For small companions, on the lefthand side of the white dotted line, the cohesive energy dominates over gravitational energy for evaporation. The green contours indicate evaporation timescales shorter than ~10^{6} yr. A few typical examples are also given in Table 1 for companions made of rock (Cols. 8, 9) and for a more metallic composition (Cols. 10, 11).
The table shows that small nondegenerate bodies at one solar radius from a 1 ms pulsar evaporate in less than a few years. We note that for P = 1–100 ms and N_{r} ~ 100, the fastest evaporation occurs for R ~ 100 km, and not for the smallest companions. We also note also the strong dependency of the evaporation time on the pulsar period P. An asteroid at the same distance of a 10 ms pulsar can survive a few 10^{7} yr. At 1 AU (200 R_{⊙}), it is definitively stable.
Figure 3 demonstrates that N_{r}, namely the chemical composition of the companion, has a strong influence on the evaporation timescale. An asteroid (R ~ 1 km) made of rock (N_{r} ~ 100 or μσ = 10^{6} s^{1}) has an optimal lifetime. More resistive (N_{r} ~ 10), or more metallic asteroids (N_{r} ≳ 10^{3}) evaporate over a shorter timescale. For N_{r} ≲ 100, the distance a remains constant for small size ratios x (black line in Fig. 3). This stems from the change in the dependency of Q_{abs} over x (and thus over R), as shown in Fig. 1 for small x and low N_{r}.
The comparison between Cols. 8, 9 and 10, 11 of Table 1 confirms that kilometersize companions are more stable against evaporation when made of rock (μσ = 10^{6} s^{1}) than for a more metallic refractive index μσ = 10^{7} s^{1}. On the other hand, the table and Fig. 2 show that for R ≥ 100 km the evaporation timescale increases with the conductivity of the companion.
Mottez et al. (2013b) proposed that the intermittency of PSR 1931+24 can be explained by the existence of a stream of small bodies of kilometer or subkilometer sizes close to the pulsar (a = 0.14 R_{⊙}). We calculate that these asteroids would evaporate in about one Gyr. If the Mie theory were not taken into account, such asteroids would not survive a year. A billion years being a long timescale compared to the migration time in the pulsar wind magnetic field (10 000 yr, Mottez & Heyvaerts 2011), the evaporation caused by induction does not invalidate the model of Mottez et al. (2013b).
The last lines in Table 1 refers to planets discovered near PSR 1257+12 (Wolszczan 1994). Because of their size, the Mie theory still has an influence on the vaporization rate, with Q_{abs}< 0.06. If it is made of rock, 1257+21a should evaporate in 10^{5} yr. With a more metallic composition, it could last a few million years. The other two planets are stable for 10^{8} yr, or more if they are metallic.
Fig. 3
Influence of companion composition on evaporation timescale. The contours of t_{ev} = 10^{6}yr (solid lines) and t_{ev} = 10^{12} yr (dashed lines) are represented as a function of companion distance a and size R for P = 10 ms, B = 10^{8} G, and an indicative (and conservative) density ρ = 1 g cm^{3}, and for various companion refractive indices as indicated in the legend (increasing from right to left): σμ = 10^{4−14} s^{1}, corresponding to N_{r} = 10^{1−6}. 
Fig. 4
Amplitude of the pulsar wind magnetic field for a) a surface dipole field l = 1,m = 1; b) quadrupole l = 2,m = 2; and c)l = 3,m = 3. Panels a) to c) are plotted with the same color scale. On these panels, the spiral structure is the pulsar wave. Comparison ratio a, see Eq. (22) for modes d) l = 2,m = 2; e)l = 3,m = 2; and f) l = 3,m = 3. Panels d) to f) are plotted with the same color scale. 
4. Effect of multipole magnetic field components
We have considered the case of a star with a dipole magnetic field. In terms of spherical harmonics analysis, it has longitudinal and azimuthal components l = 1, m = 0, and m = 1. Only the m = 1 component participates in the pulsar wave and produces a monochromatic frequency spectrum, but we know that neutron star magnetic fields can have multipole components l> 1. The components with azimuthal numbers m> 1 induce shorter wavelengths cP/m, i.e., 2πR_{L}/m. In all the above inductive heating rates, a multipole term of azimuthal number m can be accounted for by replacing the ratio of the size of the body to the incident wavelength x by x_{m} = mx. If they had the same amplitude, multipole m> 1 terms would contribute more efficiently to the companion heating than the m = 1 wave for small bodies where x ~ 1. Therefore, it is important to evaluate the contribution of multipole terms of the neutron star magnetic field to the pulsar wind.
Bonazzola et al. (2015) have computed the vacuum solution of the electromagnetic field surrounding a pulsar. The solutions have a complex structure at distances less than the light cylinder radius with an amplitude that decreases faster for higher values of l. At greater distances, it has the characteristic Parker spiral wave structure dominated by the azimuthal component B_{φ} ∝ r^{1}. Beyond the light cylinder, the ratio of amplitudes of the various modes does not vary much on average. To illustrate this, we have plotted in Fig. 4 a few vacuum field solutions corresponding to the same maximum amplitude B_{0} (on the star surface). The amplitude B of the magnetic field in the equatorial plane is plotted up to distances r = 11R_{L} for the dipole solution (panel a), for the quadrupole solution l = 2m = 2 (panel b)^{5}, and for l = 3,m = 3 (panel c). For comparison of magnetic amplitudes, we define the ratio where the maximum is computed for any radius larger than R. This definition is intended to avoid a divergent ratio when the two functions reach their minimum for different values of R that would not be pertinent to what we want to compare. The ratios a_{2,2},a_{3,2}, and a_{3,3} are plotted respectively in panels d)–f). We can see from a_{2,2} that beyond a distance 2R_{L}, the contributions of l = 1,m = 1 (dipole) and l = 2,m = 2 modes with the same maximum magnetic field on the star’s surface are comparable, although larger with the dipole. For larger values of l, the dipole term is dominant by a factor exceeding 10^{2}. This means that the contribution of a large amplitude quadrupole term to the heating of a pulsar companion cannot be neglected, implying that companions of radius R/ 2 twice as small can absorb an energy comparable to that of a Rsized body in the dipole case. Higher multipole terms should not have an important influence in our example.
We note that the above computation does not take into account the contribution of the plasma to the evolution of the wave amplitude into the wind; it should be considered a firstorder approximation.
5. Conclusion and discussion
In this paper, we have assessed the efficiency of the inductive heating of pulsar companions caused by the pulsar Poyntingflux electromagnetic wave. Inductive heating is generally considered to be the dominant heating process, for instance when the evaporation of black widow companions is considered (van den Heuvel & van Paradijs 1988). It is commonly assumed that the whole flux carried by the pulsar wave is absorbed by the companion. Taking into account the Mie theory, we have shown that this assumption fails for objects with radius R smaller than the pulsar wavelength cP, P being the pulsar spin period. The rate of absorption of the wave energy decreases by many orders of magnitude for small objects like asteroids or planetesimals. This is especially true with standard P = 1 s pulsars because of their long wavelength. One consequence is that asteroids, considered to be objects that should quickly evaporate, do not always do so even at very close distances (1 R_{⊙}) of a 1 speriod pulsar.
The conclusion regarding kilometersized asteroids at short distances from pulsars cannot be generalized to any kind of pulsar. For instance, bodies orbiting a P = 1 ms pulsar at 1 R_{⊙} would not last a year.
The behavior of small objects orbiting a pulsar is important because it can explain the intermittency of their radioemissions. For instance, Cordes & Shannon (2008) proposed a model where small rocks (metersized) falling on a pulsar cause intermittency during the few seconds in which they evaporate. For metric objects, Q_{abs} derived from the Mie theory is so low that these rocks should not evaporate.
The survival of small bodies around pulsars is a prerequisite of the theory developed by Mottez & Zarka (2014) to explain the origin of FRBs. In that model, asteroids immersed in the pulsar relativistic wind produce collimated magnetic wakes, that can be observed at cosmological distances and lead to radio bursts similar to the observed signals. An asteroid belt could also be invoked to account for the repeating FRB reported by Spitler et al. (2016; see also Dai et al. 2016).
We have assumed in this paper that the wind was Poyntingflux dominated at the location of the companion. For objects made of ordinary matter, the consistency of our evaporation timescales compared to the observations seems to validate a posteriori this hypothesis. If a nonnegligible fraction of the wind energy were kinetic, a heating process by highenergy particle irradiation would have to be considered. This process would evaporate most closeby companions, whatever their size, as has been calculated and observed for black widow and redback systems (e.g., Phinney et al. 1988; Kluzniak et al. 1988; Arons & Tavani 1993). In this case, the energy absorption coefficient Q_{kin} can be taken as ~1 at firstorder approximation. A more thorough evaluation of Q_{kin} would require calculating the cascading interactions of particles, which is beyond the scope of this study. Models considering simultaneously inductive heating, sputtering by the wind, and blackbody Xrays will be developed in forthcoming papers. From Eqs. (4) and (21), one can then infer that in order to avoid heating by particles, the fraction of kinetic energy in the wind has to be lower than Q_{em}, the absorption coefficient of the Poynting flux given by the Mie Theory (denoted Q_{abs} by abuse of notation throughout this paper, see values in Fig. 1 and Table 1). This implies a magnetization of σ_{B}> 1/Q_{em}−1. As Q_{em} ≪ 1 over a large parameter space, as is demonstrated in this paper, a very low fraction of kinetic energy in the wind and thus a very high magnetization is required for the survival of objects close to the pulsar.
We note that we have also argued in this work that, because of their high refractive index to the pulsar wave, the observed ablation of white dwarfs and Mstars in back widow and redback systems can only be explained if the absorbed energy is principally kinetic.
From an electromagnetism point of view, one can understand these two regions as different regimes of penetration of the magnetic field inside the object. In Region 2, the inductive currents do not penetrate deep under the surface (the resistive skindepth is shallow). For Region 1, the skindepth is approximately the entire size of the object, and the magnetic field can be considered as roughly uniform over it.
Cohesive energy is the energy required to form separated neutral atoms in their ground electronic state from the solid at a given temperature under a given pressure (Kittel 1998).
Acknowledgments
This work was nurtured by Jean Heyvaerts’ notes on the Mie theory and by the inspiring discussions we had with him. His great insight and input were very much missed during the completion of the project. K.K. thanks S. Phinney for fruitful discussions that led to her involvement in this project. This work was supported by the Programme National des Hautes Énergies. K.K. acknowledges financial support from the PERSU fellowship at Sorbonne Universités, from the Labex ILP (reference ANR10LABX63, ANR11IDEX000402), as well as from the NSF grant NSF PHY1412261 and the NASA grant 11APRA0066 at the University of Chicago, and the grant NSF PHY1125897 at the Kavli Institute for Cosmological Physics.
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All Tables
Gravitational (t_{ev,g}) and cohesive (t_{ev,c}) evaporation timescales due to induction heating for various pulsar and companion parameters.
All Figures
Fig. 1
Absorption coefficient Q_{abs} as a function of the size ratio x = R/cP and of the refractive index N_{r} of the companion in the Metallic regime (N = N_{r} = −N_{i}). Overlayed are the contours of the analytical approximation, in black for Region 1 (xN_{r} ≪ 1, Eq. (10)) and in white for Region 2 (xN_{r} ≫ 1, Eq. (9)). The grayshaded region corresponds to parameters outside the confidence range of the computation with Damie. 

In the text 
Fig. 2
Contours of evaporation timescales (in yrs) of nondegenerate pulsar companions (t_{ev,g} and t_{ev,c}, Eqs. (17) and (21)) as a function of the companion radius R and its distance a to the pulsar in solar radii, for pulsar spin periods and magnetic fields as indicated (left to right: P = 1,10,100 ms and B = 10^{8},10^{8},10^{12} G), for conductivity times magnetic permeability σμ = 10^{6}s^{1} and density ρ = 1 g cm^{3}. The white dotted line delimits the region where the cohesive energy dominates over gravitational energy (for small companions) for evaporation. The white region indicates evaporation times t_{ev}< 10 yr and yellow regions t_{ev}> 10^{12} yr. 

In the text 
Fig. 3
Influence of companion composition on evaporation timescale. The contours of t_{ev} = 10^{6}yr (solid lines) and t_{ev} = 10^{12} yr (dashed lines) are represented as a function of companion distance a and size R for P = 10 ms, B = 10^{8} G, and an indicative (and conservative) density ρ = 1 g cm^{3}, and for various companion refractive indices as indicated in the legend (increasing from right to left): σμ = 10^{4−14} s^{1}, corresponding to N_{r} = 10^{1−6}. 

In the text 
Fig. 4
Amplitude of the pulsar wind magnetic field for a) a surface dipole field l = 1,m = 1; b) quadrupole l = 2,m = 2; and c)l = 3,m = 3. Panels a) to c) are plotted with the same color scale. On these panels, the spiral structure is the pulsar wave. Comparison ratio a, see Eq. (22) for modes d) l = 2,m = 2; e)l = 3,m = 2; and f) l = 3,m = 3. Panels d) to f) are plotted with the same color scale. 

In the text 
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