SearcharxivSearch

arXiv · astro-ph/9901408

Event Rate and Einstein Time Evaluation in Pixel Microlensing

Abstract

It has been shown that a flux--weighted full width at half maximum timescale of a microlensing event can be used in an unbiased estimator of the optical depth. For the first time, this allows a physical parameter to be easily estimated from pixel microlensing data. We derive analytic expressions for the observed rate of pixel lensing events as a function of the full width at half maximum timescale. This contrasts work in the literature which express rates in terms of an ``event duration'' or Einstein time, which require knowledge of the magnification, which is difficult to determine in a pixel event. The full width at half maximum is the most directly measured timescale. We apply these results to possible pixel lensing surveys, using HST for M87, and CFHT for M31. We predict M87 microlensing rates for the HST Advanced Camera and for NGST, and demonstrate that one will be able to probe the stellar IMF. Next, we describe a new method by which a crude measurement of the magnification can be made in the regime of magnifications A~10-100. This in turn gives a crude measurement of the Einstein time. This program requires good photometry and sampling in the low magnification tails of an event, but is feasible with today's technology.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Edward A. Baltz, Joseph Silk. 1999-01-29. Event Rate and Einstein Time Evaluation in Pixel Microlensing. https://doi.org/10.1086/308385

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Deformation procedure for scalar fields in cosmology

This work offers an extension of the deformation procedure introduced in field theory to the case of standard cosmology in the presence of real scalar field in flat space-time. The procedure is shown to work for many models, which give rise to several different cosmic scenarios, evolving under the presence of first-order differential equations which solve the corresponding equations of motion very appropriately.

astro-ph

Dark Energy is the Cosmological Quantum Vacuum Energy of Light Particles-The Axion and the Lightest Neutrino

We uncover the general mechanism producing the dark energy(DE). This is only based on well known quantum physics and cosmology. We show that the observed DE originates from the cosmological quantum vacuum of light particles which provides a continuous energy distribution able to reproduce the data. Bosons give positive contributions to the DE while fermions yield negative contributions. As usual in field theory, ultraviolet divergences are subtracted from the physical quantities. The subtractions respect the symmetries of the theory and we normalize the physical quantities to be zero for the Minkowski vacuum. The resulting finite contributions to the energy density and the pressure from the quantum vacuum grow as log a(t) where a(t) is the scale factor, while the particle contributions dilute as 1/a^3(t), as it must be for massive particles. The DE equation of state P = w(z)H turns to be w(z)<-1 with w(z) asymptotically reaching the value -1 from below.A scalar particle can produce the observed DE through its quantum cosmological vacuum provided:(i)its mass is of the order of 10^{-3} eV = 1 meV,(ii) it is very weakly coupled and (iii) it is stable on the time scale of the age of the universe. The axion vacuum thus appears as a natural candidate. The neutrino vacuum (especially the lightest mass eigenstate) can give negative contributions to the DE. We find that w(z=0) is slightly below -1 by an amount ranging from [-1.5 10^{-3}] to [-8 10^{-3}] and we predict the axion mass to be in the range between 4 and 5 meV. We find that the universe will expand in the future faster than the de Sitter universe, as an exponential in the square of the cosmic time. DE arises from the quantum vacua of light particles in FRW cosmological space time in an analogous way to the Casimir effect in Minkowski spacetime with non trivial boundaries.

astro-ph