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arxiv: 2606.28071 · v1 · pith:SUVKQMKHnew · submitted 2026-06-26 · 🌀 gr-qc · astro-ph.CO· astro-ph.IM

Construction of Sensitivity Curves for Dynamic LISA and Taiji

Hong-Yu Shi , Yong Tang This is my paper

Pith reviewed 2026-06-29 03:26 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.COastro-ph.IM
keywords gravitational wave detectorsLISATaijisensitivity curvesorbital dynamicsdirectional dependenceMichelson interferometermillihertz band
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The pith

Dynamic LISA and Taiji sensitivity curves vary by 20% from static approximations at low frequencies, producing 70% shifts in directional source counts.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper builds direction-dependent sensitivity curves for LISA and Taiji by incorporating their full heliocentric orbital motion over one year. It derives analytic expressions for the Michelson-channel response under an adiabatic unequal-arm configuration and shows that the static equilateral-triangle model misses systematic angular variations. These variations reach roughly 20% at low frequencies and translate into 70% differences in the number of detectable gravitational-wave sources depending on sky position, with bigger effects at higher frequencies. Accurate forecasts of total source populations and binary parameter estimation therefore require the dynamic treatment. A reader cares because mission planning and data analysis for millihertz gravitational waves rest on these sensitivity maps.

Core claim

The central claim is that the direction-dependent response of dynamic LISA and Taiji, obtained from an analytic time-dependent heliocentric orbital model and adiabatic unequal-arm interferometer, produces sensitivity curves whose low-frequency values differ by roughly 20% from the static approximation; this difference induces about 70% variation in the directional distribution of detectable GW sources, with larger discrepancies at higher frequencies, so that fully dynamic curves are required for reliable source-count predictions and parameter inference.

What carries the argument

Analytic expressions for angular-dependent sensitivity in the Michelson interferometric channel, built from the time-dependent heliocentric orbital model and adiabatic unequal-arm configuration

If this is right

  • Total predicted counts of detectable gravitational-wave sources must be recalculated with direction-dependent dynamic curves.
  • Parameter estimation for binary systems will shift when the correct angular sensitivity is used instead of the static average.
  • Sky maps of sensitivity display a quadrant-like pattern at low frequencies that is absent in static models.
  • Discrepancies between dynamic and static predictions grow at higher frequencies within the millihertz band.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Earlier population studies that relied on static sensitivity maps may have under- or over-estimated detection rates for sources clustered in particular sky regions.
  • Mission design trade-offs for sky coverage could be re-evaluated once the dynamic quadrant pattern is folded into exposure calculations.
  • The same orbital-modeling approach could be applied to other proposed heliocentric interferometers to test whether similar 20% corrections appear.

Load-bearing premise

The adiabatic unequal-arm interferometer configuration together with the analytic time-dependent heliocentric orbital model accurately captures the instrument response over a full year.

What would settle it

Direct numerical integration of the exact time-dependent arm-length responses over one full orbit, compared against the analytic sensitivity curves; systematic differences exceeding 5% at low frequencies would falsify the model.

Figures

Figures reproduced from arXiv: 2606.28071 by Hong-Yu Shi, Yong Tang.

Figure 1
Figure 1. Figure 1: FIG. 1. (left) Schematic illustration of the heliocentric triangular constellation. (right) Coordinate [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Direction-dependent sensitivity curves in the [PITH_FULL_IMAGE:figures/full_fig_p010_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Ratios relative to the static sky-averaged sensitivity curve. The red line denotes the [PITH_FULL_IMAGE:figures/full_fig_p011_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Directional dependence of sensitivity for dynamic Taiji at [PITH_FULL_IMAGE:figures/full_fig_p012_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Static equal-arm sky-averaged amplitude sensitivities of the [PITH_FULL_IMAGE:figures/full_fig_p013_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Dynamic responses and amplitude sensitivities of the [PITH_FULL_IMAGE:figures/full_fig_p014_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Dynamic responses and sensitivities for 42 sky directions, compared with the correspond [PITH_FULL_IMAGE:figures/full_fig_p015_7.png] view at source ↗
read the original abstract

Space-based gravitational-wave (GW) laser interferometers, including LISA and Taiji, are designed to observe gravitational waves in the millihertz band and are expected to open up a frequency range that is otherwise inaccessible. The sensitivity and response of these instruments are central to their scientific goals, mission design and parameter estimation capabilities. However, they are commonly modeled as static, equilateral triangular constellations, an approximation that neglects both orbital motion and directional dependence. In this work, we systematically examine the direction-dependent response and sensitivity of dynamic LISA-like detectors over an entire year of heliocentric orbit. Based on an analytical, time-dependent heliocentric orbital model and an adiabatic unequal-arm interferometer configuration, we construct direction-dependent sensitivity curves in the Michelson interferometric channel for dynamic LISA and Taiji. We obtain analytic expressions for the angular-dependent sensitivity and demonstrate the emergence of a quadrant-like pattern in sky maps at low frequencies. We show that, relative to the static approximation, the low-frequency sensitivity varies by roughly $20\%$, which in turn produces about a $70\%$ variation in the directional dependence of the number of detectable GW sources, with even larger discrepancies at higher frequencies. Therefore, for accurate predictions of the total GW source counts and reliable parameter inference for binary systems, it is necessary to employ fully dynamic, direction-dependent sensitivity curves.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The paper constructs analytic, direction-dependent sensitivity curves for dynamic LISA and Taiji using a time-dependent heliocentric orbital model and an adiabatic unequal-arm Michelson interferometer configuration. It reports that, relative to the static equilateral approximation, low-frequency sensitivity varies by ~20%, producing ~70% variation in the directional dependence of detectable GW sources (with larger discrepancies at higher frequencies), and concludes that fully dynamic curves are required for accurate source counts and parameter estimation.

Significance. If the analytic model is shown to be faithful, the result demonstrates that the common static approximation introduces non-negligible errors in sky-dependent sensitivity, directly affecting forecasts of resolvable binary populations and inference. The provision of closed-form angular expressions and the emergence of a quadrant pattern in low-frequency sky maps would be a concrete, usable advance for mission planning and data analysis pipelines.

major comments (1)
  1. [Abstract (methods paragraph)] Abstract (methods paragraph): The quoted 20% low-frequency sensitivity variation and 70% source-count variation rest entirely on the fidelity of the adiabatic unequal-arm configuration plus analytic heliocentric orbital model. No comparison to the static limit, no numerical time-domain validation, and no error budget for neglected orbital perturbations are described; without these checks the central percentages cannot be confirmed to be physical rather than artifacts of the chosen analytic setup.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for highlighting the need to strengthen the validation of the analytic model. We address the single major comment below.

read point-by-point responses

  1. Referee: [Abstract (methods paragraph)] Abstract (methods paragraph): The quoted 20% low-frequency sensitivity variation and 70% source-count variation rest entirely on the fidelity of the adiabatic unequal-arm configuration plus analytic heliocentric orbital model. No comparison to the static limit, no numerical time-domain validation, and no error budget for neglected orbital perturbations are described; without these checks the central percentages cannot be confirmed to be physical rather than artifacts of the chosen analytic setup.

    Authors: The abstract explicitly states the comparison to the static equilateral approximation, and the main text (Sections 3 and 4) derives and quantifies the ~20% low-frequency variation and the resulting ~70% directional source-count variation using the same analytic expressions for both the dynamic and static cases. The heliocentric orbital model and adiabatic unequal-arm Michelson configuration follow standard treatments in the LISA literature. We nevertheless agree that the manuscript would benefit from explicit numerical time-domain validation and an error budget for neglected perturbations (e.g., small eccentricities). We will add a dedicated subsection presenting such comparisons and error estimates in the revised version. revision: yes

Circularity Check

0 steps flagged

No circularity; derivation uses external orbital and interferometer models

full rationale

The paper derives direction-dependent sensitivity curves from an analytical time-dependent heliocentric orbital model and adiabatic unequal-arm interferometer configuration, treated as standard external inputs from orbital mechanics and interferometry. No equations or results reduce to self-defined quantities, fitted parameters renamed as predictions, or load-bearing self-citations. The reported 20% sensitivity variation and 70% source-count variation are computed outputs of these models, not inputs. The central claim is self-contained against external benchmarks like standard LISA response functions.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only; no explicit free parameters, axioms, or invented entities are stated. The orbital model and adiabatic approximation are treated as given inputs from prior literature.

pith-pipeline@v0.9.1-grok · 5771 in / 1040 out tokens · 38845 ms · 2026-06-29T03:26:01.819518+00:00 · methodology

discussion (0)

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