Characterizing gravitational wave detector networks: from A# to cosmic explorer

Ish Gupta*, Chaitanya Afle, K. G. Arun, Ananya Bandopadhyay, Masha Baryakhtar, Sylvia Biscoveanu, Ssohrab Borhanian, Floor Broekgaarden, Alessandra Corsi, Arnab Dhani, Matthew Evans, Evan D. Hall, Otto A. Hannuksela, Keisi Kacanja, Rahul Kashyap, Sanika Khadkikar, Kevin Kuns, Tjonnie G.F. Li, Andrew L. Miller, Alexander Harvey NitzBenjamin J. Owen, Cristiano Palomba, Anthony Pearce, Hemantakumar Phurailatpam, Binod Rajbhandari, Jocelyn Read, Joseph D. Romano, Bangalore S. Sathyaprakash, David H. Shoemaker, Divya Singh, Salvatore Vitale, Lisa Barsotti, Emanuele Berti, Craig Cahillane, Hsin Yu Chen, Peter Fritschel, Carl Johan Haster, Philippe Landry, Geoffrey Lovelace, David McClelland, Bram J.J. Slagmolen, Joshua R. Smith, Marcelle Soares-Santos, Ling Sun, David Tanner, Hiro Yamamoto, Michael Zucker

*Corresponding author for this work

Research output: Contribution to journalArticleAcademicpeer-review

Abstract

Gravitational-wave observations by the laser interferometer gravitational-wave observatory (LIGO) and Virgo have provided us a new tool to explore the Universe on all scales from nuclear physics to the cosmos and have the massive potential to further impact fundamental physics, astrophysics, and cosmology for decades to come. In this paper we have studied the science capabilities of a network of LIGO detectors when they reach their best possible sensitivity, called A#, given the infrastructure in which they exist and a new generation of observatories that are factor of 10 to 100 times more sensitive (depending on the frequency), in particular a pair of L-shaped cosmic explorer (CE) observatories (one 40 km and one 20 km arm length) in the US and the triangular Einstein telescope with 10 km arms in Europe. We use a set of science metrics derived from the top priorities of several funding agencies to characterize the science capabilities of different networks. The presence of one or two A# observatories in a network containing two or one next generation observatories, respectively, will provide good localization capabilities for facilitating multimessenger astronomy (MMA) and precision measurement of the Hubble parameter. Two CE observatories are indispensable for achieving precise localization of binary neutron star events, facilitating detection of electromagnetic counterparts and transforming MMA. Their combined operation is even more important in the detection and localization of high-redshift sources, such as binary neutron stars, beyond the star-formation peak, and primordial black hole mergers, which may occur roughly 100 million years after the Big Bang. The addition of the Einstein Telescope to a network of two CE observatories is critical for accomplishing all the identified science metrics including the nuclear equation of state, cosmological parameters, the growth of black holes through cosmic history, but also make new discoveries such as the presence of dark matter within or around neutron stars and black holes, continuous gravitational waves from rotating neutron stars, transient signals from supernovae, and the production of stellar-mass black holes in the early Universe. For most metrics the triple network of next generation terrestrial observatories are a factor 100 better than what can be accomplished by a network of three A# observatories.

Original languageEnglish
Article number245001
JournalClassical and Quantum Gravity
Volume41
Issue number24
DOIs
Publication statusPublished - 19 Dec 2024

Bibliographical note

Publisher Copyright:
© 2024 The Author(s).

Funding

We thank the members of the Cosmic Explorer Project and the Scientific Advisory Committee for their input and feedback. We thank Kara Merfeld for pointing out the omission of the assumption for binary neutron stars that leads to more mass-symmetric binaries. I G, A D, B S S, R K, and D S were supported by NSF Grant Numbers AST-2006384, AST-2307147, PHY-2012083, PHY-2207638, PHY-2308886, and PHYS-2309064 to B.S.S. S B acknowledges support from the Deutsche Forschungsgemeinschaft, DFG, Project MEMI number BE 6301/2-1. K G A acknowledges support from the Department of Science and Technology and Science and Engineering Research Board (SERB) of India via the following grants: Swarnajayanti Fellowship Grant DST/SJF/PSA-01/2017-18 and Core Research Grant CRG/2021/004565 K G A, E B and B S S acknowledge the support of the Indo-US Science and Technology Forum through the Indo-US Centre for Gravitational-Physics and Astronomy, grant IUSSTF/JC-142/2019. A B and K K acknowledge support from NSF award PHY-2207264. E B is supported by NSF Grants No. AST-2006538, PHY-2207502, PHY-090003 and PHY-20043, and by NASA Grant Nos. 20-LPS20-0011 and 21-ATP21-0010. E B acknowledges support from the ITA-USA Science and Technology Cooperation program (CUP: D13C23000290001), supported by the Ministry of Foreign Affairs of Italy (MAECI). M B acknowledges support from DOE under Award Number DE- SC0022348 G L acknowledges NSF award PHY-2208014, Nicholas and Lee Begovich, and the Dan Black Family Trust. A Corsi acknowledges support from NSF grant PHYS-2011608. AHN acknowledges support from NSF grant PHY-2309240. OAH and HP acknowledge support by grants from the Research Grants Council of Hong Kong (Project Nos. CUHK 2130822 and 4443086), and the Direct Grant for Research from the Research Committee of The Chinese University of Hong Kong. T G F L acknowledge support by grants from the Research Foundation-Flanders (G086722N, I002123N) and KU Leuven (STG/21/061). D E M, B J J S, and L S acknowledge the support of the Australian Research Council Centre of Excellence for Gravitational Wave Discovery (OzGrav), Project No. CE170100004. C P acknowledges research support from the Italian Istituto Nazionale di Fisica Nucleare (INFN). B J O, A P, and B R acknowledge support from NSF grants PHY-1912625, PHY-2309305, and AST-1907975. JDR acknowledges support from NSF grant PHY-2207270. J R S and G L acknowledge support from NSF Grant 2308985, Nicholas and Lee Begovich, and the Dan Black Family Trust. S V acknowledges support from NSF award PHY-2207387.

FundersFunder number
High Energy Physicshttp://dx.doi.org/10.13039/100006208PHY-2207387
NSFBE 6301/2-1
Deutsche Forschungsgemeinschaft, DFGDST/SJF/PSA-01/2017-18, CRG/2021/004565 K G A
Department of Science and Technology and Science and Engineering Research Board (SERB) of IndiaIUSSTF/JC-142/2019
Indo-US Science and Technology Forum through the Indo-US Centre for Gravitational-Physics and Astronomy20-LPS20-0011, 21-ATP21-0010
NASACUP: D13C23000290001
ITA-USA Science and Technology Cooperation program
Ministry of Foreign Affairs of Italy (MAECI)DE- SC0022348
DOE
Dan Black Family TrustCUHK 2130822, 4443086
Research Grants Council of Hong Kong
Direct Grant for Research from the Research Committee of The Chinese University of Hong KongG086722N, I002123N
Research Foundation-FlandersSTG/21/061
KU LeuvenCE170100004
Australian Research Council Centre of Excellence for Gravitational Wave Discovery
Italian Istituto Nazionale di Fisica Nucleare (INFN)

    Keywords

    • cosmic explorer
    • Einstein telescope
    • gravitational waves
    • next generation

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