A Precise Photometric Ratio via Laser Excitation of the Sodium Layer II: Two-photon Excitation Using Lasers Detuned from 589.16 nm and 819.71 nm Resonances

TL;DR

This paper presents a two-photon excitation method using detuned lasers to generate a brighter sodium-based artificial star with a precise photometric ratio, enhancing calibration accuracy for astronomical and atmospheric measurements.

Contribution

It introduces a novel two-photon excitation technique with lower power lasers to produce a brighter artificial star with a precise photon ratio, improving calibration methods.

Findings

Achieves approximately 1000 times brighter LPRS with <30 W lasers.

Provides a method for precise 1:1 photon ratio in yellow and near-infrared emissions.

Requires polarization filters to reduce Rayleigh backscatter in telescope imaging.

Abstract

This article is the second in a pair of articles on the topic of the generation of a two-color artificial star (which we term a "laser photometric ratio star," or LPRS) of de-excitation light from neutral sodium atoms in the mesosphere, for use in precision telescopic measurements in astronomy and atmospheric physics, and more specifically for the calibration of measurements of dark energy using type Ia supernovae. The two techniques respectively described in both this and the previous article would each generate an LPRS with a precisely 1:1 ratio of yellow (589/590 nm) photons to near-infrared (819/820 nm) photons produced in the mesosphere. Both techniques would provide novel mechanisms for establishing a spectrophotometric calibration ratio of unprecedented precision, from above most of Earth's atmosphere, for upcoming telescopic observations across astronomy and atmospheric physics. The technique described in this article has the advantage of producing a much brighter (specifically, brighter by approximately a factor of 1000) LPRS, using lower-power (<30 W average power) lasers, than the technique using a single 500 W average power laser described in the first article of this pair. However, the technique described here would require polarization filters to be installed into the telescope camera in order to sufficiently remove laser atmospheric Rayleigh backscatter from telescope images, whereas the technique described in the first article would only require more typical wavelength filters in order to sufficiently remove laser Rayleigh backscatter.