What do we know about cosmography

Abstract In the present paper, we investigate the cosmographic problem using the bias–variance trade-off. We find that both the z-redshift and the $$y=z/(1+z)$$ y = z / ( 1 + z ) -redshift can present a small bias estimation. It means that the cosmography can describe the supernova data more accurat...

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Main Authors: Ming-Jian Zhang, Hong Li, Jun-Qing Xia
Format: Article
Language:English
Published: SpringerOpen 2017-06-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-5005-4
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spelling doaj-9d9a798f788e45598e5237361d0ed5872020-11-25T02:34:42ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-06-0177711210.1140/epjc/s10052-017-5005-4What do we know about cosmographyMing-Jian Zhang0Hong Li1Jun-Qing Xia2Key Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of ScienceKey Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of ScienceDepartment of Astronomy, Beijing Normal UniversityAbstract In the present paper, we investigate the cosmographic problem using the bias–variance trade-off. We find that both the z-redshift and the $$y=z/(1+z)$$ y = z / ( 1 + z ) -redshift can present a small bias estimation. It means that the cosmography can describe the supernova data more accurately. Minimizing risk, it suggests that cosmography up to the second order is the best approximation. Forecasting the constraint from future measurements, we find that future supernova and redshift drift can significantly improve the constraint, thus having the potential to solve the cosmographic problem. We also exploit the values of cosmography on the deceleration parameter and equation of state of dark energy w(z). We find that supernova cosmography cannot give stable estimations on them. However, much useful information was obtained, such as that the cosmography favors a complicated dark energy with varying w(z), and the derivative $${\text {d}}w/{\text {d}}z <0$$ d w / d z < 0 for low redshift. The cosmography is helpful to model the dark energy.http://link.springer.com/article/10.1140/epjc/s10052-017-5005-4
collection DOAJ
language English
format Article
sources DOAJ
author Ming-Jian Zhang
Hong Li
Jun-Qing Xia
spellingShingle Ming-Jian Zhang
Hong Li
Jun-Qing Xia
What do we know about cosmography
European Physical Journal C: Particles and Fields
author_facet Ming-Jian Zhang
Hong Li
Jun-Qing Xia
author_sort Ming-Jian Zhang
title What do we know about cosmography
title_short What do we know about cosmography
title_full What do we know about cosmography
title_fullStr What do we know about cosmography
title_full_unstemmed What do we know about cosmography
title_sort what do we know about cosmography
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2017-06-01
description Abstract In the present paper, we investigate the cosmographic problem using the bias–variance trade-off. We find that both the z-redshift and the $$y=z/(1+z)$$ y = z / ( 1 + z ) -redshift can present a small bias estimation. It means that the cosmography can describe the supernova data more accurately. Minimizing risk, it suggests that cosmography up to the second order is the best approximation. Forecasting the constraint from future measurements, we find that future supernova and redshift drift can significantly improve the constraint, thus having the potential to solve the cosmographic problem. We also exploit the values of cosmography on the deceleration parameter and equation of state of dark energy w(z). We find that supernova cosmography cannot give stable estimations on them. However, much useful information was obtained, such as that the cosmography favors a complicated dark energy with varying w(z), and the derivative $${\text {d}}w/{\text {d}}z <0$$ d w / d z < 0 for low redshift. The cosmography is helpful to model the dark energy.
url http://link.springer.com/article/10.1140/epjc/s10052-017-5005-4
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