Design and performance of a collimated beam projector for telescope transmission measurement using a broad-band light source

Author:

Sommer K1ORCID,Cohen-Tanugi J12ORCID,Plez B1ORCID,Betoule M3ORCID,Bongard S3ORCID,Le Guillou L3ORCID,Neveu J34ORCID,Nuss E1,Sepulveda E3,Souverin T3,Moniez M4ORCID,Stubbs C W56ORCID

Affiliation:

1. Laboratoire Univers et Particules de Montpellier, Université de Montpellier, CNRS , F-34095 Montpellier , France

2. Laboratoire de Physique de Clermont, Université Clermont Auvergne, CNRS , F-63000 Clermont-Ferrand , France

3. LPNHE, CNRS/IN2P3 & Sorbonne Université , 4 place Jussieu, F-75005 Paris , France

4. IJCLab, Université Paris-Saclay, CNRS , F-91405 Orsay , France

5. Department of Physics, Harvard University , 17 Oxford street, Cambridge, MA 02143 , USA

6. Department of Astronomy, Harvard University, and Center for Astrophysics , 60 Garden Street, Cambridge, MA 02143 , USA

Abstract

Abstract Type Ia supernovae are the most direct cosmological probe to study dark energy in the recent Universe, for which the photometric calibration of astronomical instruments remains one major source of systematic uncertainties. To address this, recent advancements introduce collimated beam projectors (CBPs), aiming to enhance calibration by precisely measuring a telescope’s throughput as a function of wavelength. This work describes the performance of a prototype portable CBP. The experimental set-up consists of a broad-band Xenon light source replacing a more customary but much more demanding high-power laser source, coupled with a monochromator emitting light inside an integrating sphere monitored with a photodiode and a spectrograph. Light is injected at the focus of the CBP telescope projecting a collimated beam onto a solar cell whose quantum efficiency has been obtained by comparison with a NIST-calibrated photodiode. The throughput and signal-to-noise ratio achieved by comparing the photocurrent signal in the CBP photodiode with the one in the solar cell are computed. We prove that the prototype, in its current state of development, is capable of achieving 1.2 per cent and 2.3 per cent precision on the integrated g and r bands of the Zwicky Transient Facility photometric filter system, respectively, in a reasonable amount of integration time. Central wavelength determination accuracy is kept below ∼0.91 and ∼0.58 nm for g and r bands, respectively. The expected photometric uncertainty caused by filter throughput measurement is approximately 5 mmag on the zero-point magnitude. Several straightforward improvement paths are discussed to upgrade the current set-up.

Funder

CEA

CNES

Publisher

Oxford University Press (OUP)

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