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Ira Wasserman

Publications and source records attributed to Ira Wasserman.

60 records · Page 4Linked to original sources
arXiv1998

Non-equilibrium effects in steady relativistic $e^+e^-γ$ winds

We consider an ultra-relativistic wind consisting of electron-positron pairs and photons with the principal goal of finding the asymptotic Lorentz factor $γ_{\infty}$ for zero baryon number. The wind is assumed to originate at radius $r_i$ where it has a Lorentz factor $γ_i$ and a temperature $T_i$ sufficiently high to maintain pair equilibrium. As $r$ increases, $T$ decreases and becomes less than the temperature corresponding to the electron mass $m_e$, after which non-equilibrium effects become important. Further out in the flow the optical depth $τ$ drops below one, but the pairs may still be accelerated by the photons until $τ$ falls below $\sim 2\times10^{-5} γ_{i}^{3/4}$. Radiative transfer calculations show that only at this point do the radiation flux and pressure start to deviate significantly from their blackbody values. The acceleration of the pairs increases $γ$ by a factor $\sim 45$ as compared to its value at the photosphere; it is shown to approach $γ_{\infty} \sim 1.4\times 10^3 (r_i/10^6\mbox{cm})^{1/4} γ_{i}^{3/4} T_i/m_e$.

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arXiv1998

Supernova Fallback and the Emergence of a Black Hole

We present the first fully relativistic investigation of matter fallback in a supernova. We investigate spherically symmetric supernova fallback using a relativistic radiation hydrodynamics Lagrangian code that handles radiation transport in all regimes. Our goal is to answer the fundamental question: did SN1987A produce a black hole and, if so, when will the hole become detectable ? We compute the light curve, assuming that a black hole has been formed during the explosion, and compare it with the observations. Our preliminary calculations lack radioactive energy input and adopt a very simple chemical composition (pure hydrogen). As a result, our computed models cannot fit the observed data of SN1987A in detail. Nevertheless, we can show that, during the first hours, the accretion flow is self--regulated and the accretion luminosity stays very close to the Eddington limit. The light curve is completely dominated, during the first few weeks, by the emission of the stellar envelope thermal energy, and resembles that obtained in ``standard'' supernova theory. Only long after hydrogen recombination takes place is there even a chance to actually detect radiation from the accreting black hole above the emission of the expanding envelope. The presence of a black hole is thus not inconsistent with observations to date. Because of the exponential decay of the $^{44}$Ti radioactive heating rate, the date of the emergence of the black hole is not very sensitive to the actual parameters of the models and turns out to be about 1000 years. The bulk of the emission then is expected to be in the visible band, but will be unobservable with present instrumentation. We discuss the implications of our results in connection with the possible emergence of a black hole in other supernovae.

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arXiv1998

The Emergence of a Black Hole in Supernova Explosions

We present results from a fully relativistic investigation of matter fallback in a supernova, assuming that the central compact star is a black hole (BH). Our goal is to answer the following questions: can we infer from the light curve whether a stellar black hole (BH) has formed in the aftermath of a supernova explosion ? Did SN1897A produce a BH and, if so, when will the hole become detectable ? We show that it should not be possible to infer the presence of a BH in the remnant for another several hundred to a thousand years. In the case of SN1987A, we estimate the BH luminosity to be $L\simeq 5\times 10^{34}$ erg s$^{-1}$, which is well below the present day bolometric luminosity of the remnant ($\sim 10^{36}erg/s$; Suntzeff 1997).

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arXiv1996

An adaptive hierarchical particle-mesh code with isolated boundary conditions

This article describes a new, fully adaptive Particle-Multiple-Mesh numerical simulation code developed primarily for simulations of small regions (such as a group of galaxies) in a cosmological context. It integrates the equations of motion of a set of particles subject to their mutual gravitational interaction and to an arbitrary external field. The interactions are computed using a hierarchy of nested grids constructed anew at each integration step to enhance the spatial resolution in high-density regions of interest. Significant effort has gone into supporting isolated boundary conditions at the top grid level. This makes our method also applicable to non-cosmological problems, at the cost of some complications which we discuss. We point out the implications of some differences between our approach and those of other authors of similar codes, in particular with respect to the handling of the interface between regions of different spatial resolution. We present a selection of tests performed to verify the correctness and performance of our implementation. The conclusion suggests possible further improvements in the areas of independent time steps and particle softening lengths.

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arXiv1994

A Potential Cyclotron Line Signature in Low Luminosity X-Ray Sources

Estimates indicate there may be $\simgreat 10^3$ low luminosity X-ray pulsars ($L \simless 10^{34} \rom{erg\;s^{-1}}$) in the Galaxy undergoing ``low-state'' wind accretion in Be/X-ray binary systems, and $\sim 10^8-10^9$ isolated neutron stars which may be accreting directly from the interstellar medium. Despite their low effective temperatures ($kT_e \simless 300 \rom{eV}$), low luminosity accreting neutron stars with magnetic fields $B \sim (0.7-7) \times 10^{12}$ G could emit a substantial fraction ($0.5 - 5\%$) of their total luminosity in a moderately broadened ($E/ΔE \sim 2-4$) cyclotron {\it emission} line which peaks in the energy range $ \sim 5-20\rom{keV}$. The bulk of the thermal emission from these stars will be in the extreme ultraviolet/soft X-ray regime, which is subject to strong interstellar absorption and would be difficult to distinguish from spectra of other types of objects. In sharp contrast, the {\it nonthermal} cyclotron component predicted here will not be strongly absorbed, and consequently it may be the only distinguishing signature for the bulk of these low luminosity sources. We propose a search for this cyclotron emission feature in long pointed observations of the newly discovered candidate isolated neutron star MS0317.7-6477, and the Be/X-ray transient

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