09:30 to 10:00 |
Jan Harms (GSSI) |
The Lunar Gravitational-wave Antenna Future GW detectors like LISA and the proposed Cosmic Explorer and Einstein Telescope will herald a new era of GW science and astronomy. Together with pulsar timing arrays and inflationary probes, a frequency band spanning over 20 decades will be under observation. However, these detectors leave important gaps for GW detections, most notably the decihertz band, which would open exciting possibilities for GW cosmology, multi-messenger astronomy, and fundamental physics. In this talk, we present a new detector concept, the Lunar Gravitational-wave Antenna (LGWA), which measures vibrations of the Moon caused by GWs. The Moon is known to be several orders of magnitude quieter in terms of seismic perturbations than Earth, which is key for the realization of LGWA. It relies on a revolutionary concept for an ultra-sensitive, cryogenic vibration sensor with sub-picometer sensitivity in the decihertz band. An array of at least four seismic stations deployed in a permanently shadowed region at the lunar north or south pole serves to distinguish between GW signals and the seismic background. In this way, LGWA fully exploits the unique lunar environment and has the capability to achieve the first GW observations in the decihertz band.
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10:00 to 10:30 |
Joris van Heijningen (UCLouvain) |
The payload of the Lunar Gravitational-wave Antenna At the heart of the Lunar Gravitational-wave Antenna (LGWA) are cryogenic inertial sensors with sufficient sensitivity in the decihertz band [1,2]. An array of four of these sensors will be deployed in a permanently shadowed region. The Moon is known to be several orders of magnitude quieter than Earth, and the array allows for subtraction techniques to further reduce the extremely weak seismic background predicted from meteoroid impacts and moonquakes. In this way, LGWA becomes a technologically feasible concept fully exploiting and investigating the unique lunar environment and with the capability to achieve the first gravitational-wave observations in the decihertz band. Here, I will present the current technology developments of optical and superconducting inertial sensor readout, a low-vibration sorption cooler to achieve liquid helium temperatures in the payload and further deployment details [3].
[1] JVvH (2020), JINST 15 P06034
[2] JVvH+ (2022), NIM A Vol. 1041, pp. 167231
[3] JVvH+ (2023), arXiv:2301.13685
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10:30 to 11:00 |
Shreevathsa Chalathadka Subrahmanya (University of Hamburg) |
Compact laser interferometry for vibration measurements This talk presents a compact displacement sensor that can be used to measure proof mass motion of Lunar Gravitational Wave Antenna (LGWA). The sensor consists of a fiber-based laser interferometer that uses optical resonators. In principle, such a heterodyne cavity-tracking readout scheme can reach noise levels below 10^(-16) m/rt(Hz) with reasonable cavity and readout configurations. The talk discusses the main noise contributors and how one could expect a sub-femtometer noise floor in such an opto-mechanical readout.
To use this readout for vibration measurements, one basically tracks the heterodyne frequency and retrieves the displacement information. This in turn requires a high dynamic range frequency-tracking system. Such a ‘Phasemeter’ can be realized using Field-Programmable Gate Arrays (FPGAs) with integrated RF data converters. Our progress on the development of such a ‘GHz Phasemeter’ is also presented.
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11:30 to 12:00 |
Surinder P Singh (NPL) |
Fabrication and characterization of superconducting thin films to optimize coil geometries for LGWA actuators |
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12:00 to 12:30 |
Xing Bian (CAS) |
A brief introduction to sensitive vibration sensing based on superconducting effects The LGWA detects mid-frequency gravitational waves by observing the very weak vibration of the moon excited by the tidal force generated by gravitational waves, to meet the scientific goal of this project, the sensitivity of the vibration sensors need to be as high as 10^-15 m s^-2 Hz^-1/2 in the frequency band between 1 mHz~10 Hz. Vibration sensing based on the quantum effects of superconductor can meet this challenging sensitivity requirement with a tabletop scale system, and the permanently shadowed region on the moon where LGWA is to be deployed offers a nature cryogenic environment, making this technology a very competitive candidate for the vibration sensing. This talk will briefly introduce this technology and present some thoughts on its application on LGWA.
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12:30 to 13:00 |
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Discussion |
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14:00 to 14:30 |
Philippe Gläser (TU Berlin) |
Modeling solar illumination and surface temperatures at the lunar poles This presentation deals with the modeling of solar illumination and surface temperatures at the lunar poles.
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14:30 to 15:00 |
Taichi Kawamura (University of Paris City) |
Ambient seismic fields on the Moon Apollo seismic observations revealed that Moon is still seismically active today. However, the seismic environment is very different from Earth and the Moon. In this presentation, we will review the seismic observation made on Moon and discuss the noise environment of Moon. Moon is one of the most seismically quiet environments that we have ever explored. The biggest difference from Earth is that there is no atmosphere and ocean on the Moon. This has significant impact on the noise condition on the Moon and for example, the micro seismic peak that is ubiquitously observed on Earth will not be observed on Moon. The micro seismic peak is excited by oceanic waves and this will mask signals around 4 – 30 seconds period. Observation of that frequency band will be challenging on Earth while it will be almost noise free on Moon. Lack of atmosphere, ocean and human activity make Moon an ideal environment for gravitational wave detection. We will review the observation from Apollo to discuss our current knowledge of the noise environment of Moon. We will also discuss some perspectives for the future with possible launch opportunities that will further inform us with seismic environment of Moon and a new generation seismometer that is now under development for future seismic observations.
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15:30 to 16:00 |
Alberto Sesana (Università di Milano-Bicocca) |
Multiband observation with decihertz GW detectors Following the detection of GW150914, it was soon realized that this source could have been potentially seen by LISA years before merger, opening the possibility of multiband gravitational wave astronomy. Although multiband observations with LISA and ground based detectors are possible, a deciHz band detector would be ideally placed to fulfil the promise of multiband GW astronomy. I will describe some relevant aspects of the science case for multiband GW observations and highlight the potential of LGWA in this respect.
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16:00 to 16:30 |
Seiji Kawamura (Nagoya University, Japan) |
Space gravitational wave antenna DECIGO and B-DECIGO DECi-hertz Interferometer Gravitational-wave Observatory (DECIGO) is a future Japanese space gravitational-wave antenna. There are many science targets that DECIGO aims at, including the detection of primordial gravitational waves, direct measurement of the acceleration of the Universe, the revelation of the formation of massive black holes, and many others. DECIGO consists of four clusters of spacecraft, and each cluster consists of three spacecraft with three Fabry-Perot Michelson interferometers. As a pathfinder/science mission of DECIGO, we plan to launch B-DECIGO to demonstrate technologies necessary for DECIGO and lead to fruitful multimessenger astronomy. B-DECIGO is a small-scale version of DECIGO with a sensitivity good enough to provide frequent detection of gravitational waves. In this talk, I will explain the aimed sciences, the mechanical and optical design, and the current status of DECIGO and B-DECIGO.
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16:30 to 17:00 |
Marco Muccino (INFN LNF) |
Probing Gravity with Next-generation Lunar Laser Ranging (LLR) & Lunar Surface Laser Ranging (LSLR) Next-generation lunar laser retroreflectors from INFN-LNF, MoonLIGHT (Moon Laser Instrumentation for General relativity/geophysics High-accuracy Tests), and from University of Maryland (USA), NGLR (Next-Generation Lunar Retroreflector), are designed to probe weak field – slow motion regime gravity in the Sun-Earth-Moon system through the measurement of Parametrized Post-Newtonian (PPN), Weak & Strong Equivalence Principles (WEP & SEP), Gdot/G, inverse-square law deviations, tests of GR and beyond, and implementation of lunar geodesy/geophysics. Tests have been performed in the last decades by the network of 3 Apollo and 2 Lunokhod laser retroreflector arrays. Imminent lunar surface missions and collaborations with ESA, ASI, NASA, will establish a solid heritage and basis for next-generation lunar reflectors, that will be evolved in the near future for GW detectors on the Moon like LGWA (Lunar Gravitational-wave Antenna), LSGA (Lunar Seismic and Gravitational Antenna) and iLILA (Laser Interferometer Lunar Antenna).
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17:00 to 17:30 |
Tsvi Piran (Hebrew University) |
Jet Gravitational Waves and Lunar Detectors The acceleration of a jet to a relativistic velocity is a source of gravitational energy, jet-GWs, that has been largely left unexplored. Jet-GWs are memory-type signals with an amplitude of h~GE/c^4 d, where E is the energy of the accelerated jet, d is the distance to the source, G is Newton’s constant, and c is the speed of light and a characteristic time scale that depends on the acceleration time, the duration of the jet its opening angle and orientation. Among the most interesting sources of such gravitational waves are Gamma-Ray Bursts (GRBs) whose jets carry typically 10^51 erg. Jet-GWs can reveal how GRB jets are accelerated. Other interesting and less known sources are some Supernovae that harbor hidden jets, these jets don’t manage to penetrate the stars and are choked inside. As such they don’t have only indirect observational signatures. Jet-GW is the best way to directly reveal their existence. Jet-GW from both GRBs and Supernovae are in the deciHz to milliHz range making Lunar gravitational wave detectors best suited ideal for their detection.
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17:30 to 18:00 |
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Discussion |
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19:00 to 20:00 |
Yosio Nakamura (UT Institute of Geophysics) |
What we learned from seismic observations on the moon as a part of the ALSEP (Apollo Lunar Surface Experiment Package) experiments. Three types of seismic experiments, Passive Seismic Experiment (PSE), Active Seismic Experiment (ASE) and Lunar Surface Profiling Experiment (LSPE), were performed during the Apollo lunar landing missions from 1969 to 1972, and another experiment, Lunar Surface Gravimeter (LSG), designed to detect gravitational waves, also provided seismic data. Most of these instruments functioned till they were turned off in September of 1977, giving us continuous seismic data for up to eight years from five Apollo landing sites on the front (earth-facing) side of the moon. Four types of natural seismic events were observed: meteoroid impacts, thermal moonquakes, shallow moonquakes and deep moonquakes, and over 17,000 of those recorded on the PSE mid-period seismometers were catalogued. From these and 9 artificial-impact data, internal structure of the moon, seismic activities inside the moon and streams of meteoroids near the earth-moon system were estimated. The raw data, in the form of bit streams, were archived and are publicly available. Recently, these data were reformatted to standard seismic data format and made available to public. Re-analyses of these data using new analysis techniques and more powerful computers than what were available earlier are providing more detailed information on the interior structure of the moon. It is quite likely that further new information will be extracted from these half-century old data sets. New seismic observations on the moon are being planned to supplement what we now have.
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