2013
DOI: 10.1016/j.asr.2012.09.017
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Numerical simulation of time delay interferometry for a LISA-like mission with the simplification of having only one interferometer

Abstract: In order to attain the requisite sensitivity for LISA, laser frequency noise must be suppressed below the secondary noises such as the optical path noise, acceleration noise etc.In a previous paper (Dhurandhar et al., Class. Quantum Grav., 27, 135013, 2010), we have found a large family of second-generation analytic solutions of time delay interferometry with one arm dysfunctional, and we also estimated the laser noise due to residual time-delay semi-analytically from orbit perturbations due to Earth. Since ot… Show more

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Cited by 31 publications
(42 citation statements)
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“…For this, we considered all known 492 asteroids with diameter greater than 65 km to obtain an improved ephemeris framework ---CGC 2, and calculated the perturbations due to these 492 asteroids on the ASTROD spacecraft [77]. More recently, we apply different variants of CGC 2 ephemeris framework to study the ASTROD I orbit design/optimization/simulation [78], the ASTROD-GW orbit design/optimization [79], and the numerical Time Delay Interferometry (TDI) for space gravitational-wave mission concepts ASTROD-GW [80], LISA [81] and eLISA [82].…”
Section: Solar System Ephemeridesmentioning
confidence: 99%
“…For this, we considered all known 492 asteroids with diameter greater than 65 km to obtain an improved ephemeris framework ---CGC 2, and calculated the perturbations due to these 492 asteroids on the ASTROD spacecraft [77]. More recently, we apply different variants of CGC 2 ephemeris framework to study the ASTROD I orbit design/optimization/simulation [78], the ASTROD-GW orbit design/optimization [79], and the numerical Time Delay Interferometry (TDI) for space gravitational-wave mission concepts ASTROD-GW [80], LISA [81] and eLISA [82].…”
Section: Solar System Ephemeridesmentioning
confidence: 99%
“…Time delay interferometry is considered for ASTROD in 1996 [27,28] and has been worked out for LISA much more thoroughly since 1999. [29,30] In our recent papers, we have worked out various TDI configurations numerically for ASTROD-GW, [31][32][33][34] LISA [35] and eLISA/NGO [36] and compared them with one another. [21] These second generation TDIs all satisfy their respective requirements.…”
Section: Introductionmentioning
confidence: 99%
“…where a Newton and a 1PN are the Newtonian and first-order post-Newtonian acceleration from the major celestial bodies in the solar system considered as point mass, a fig is the acceleration due to the figure effects from the Sun, Earth and Moon, and a asteroid is the acceleration from Newtonian perturbation of the 340 asteroids. The explicit interactions in our CGC ephemeris framework are fully described in references [24,36,37]. The thruster needs to provide acceleration a thruster a thruster = a traj  a traj (10) to maintain the constant arm length trajectories.…”
Section: Thruster Accelerationmentioning
confidence: 99%