2016
DOI: 10.1103/physrevlett.117.241301
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Testing Lorentz Symmetry with Lunar Laser Ranging

Abstract: Lorentz symmetry violations can be parametrized by an effective field theory framework that contains both general relativity and the standard model of particle physics called the standard-model extension (SME). We present new constraints on pure gravity SME coefficients obtained by analyzing lunar laser ranging (LLR) observations. We use a new numerical lunar ephemeris computed in the SME framework and we perform a LLR data analysis using a set of 20721 normal points covering the period of August, 1969 to Dece… Show more

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Cited by 71 publications
(89 citation statements)
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“…Competitive bounds in this sector have been established by various experiments and observations [24,25], such as gravimetry [11][12][13], lunar laser ranging [14][15][16] and astrophysics observations [17,18]. Among these, local gravimetry is the one of the easy-to-access and very precise ground-based method.…”
mentioning
confidence: 99%
“…Competitive bounds in this sector have been established by various experiments and observations [24,25], such as gravimetry [11][12][13], lunar laser ranging [14][15][16] and astrophysics observations [17,18]. Among these, local gravimetry is the one of the easy-to-access and very precise ground-based method.…”
mentioning
confidence: 99%
“…From Figure 1, to make the transfer coefficients as large as possible, different angles are chosen in (a) and (b). Based on Equation (22), the larger transfer coefficients Γ j are, the larger LLI violation signal we will achieve, which means the higher limitation of the LLI violation coefficients k jm we will obtain with the same experimental precision. From Equation (19), as θ is involved in the transfer coefficients, we should choose an appropriate angle to make the fourteen transfer coefficients large simultaneously.…”
Section: Experimental Designmentioning
confidence: 99%
“…For LLI violation in matter-gravity couplings, the best current constraints are obtained at 10 −11 GeV [19]. For LLI violation in the pure-gravity part, the experimental classification falls into three parts: experiments on ground [21], solar system [22], and astrophysical measurements [23,24], in which the different limits for different mass dimensions of LLI violation effects are given. For mass dimension d = 4, the best constraints for violating coefficients are obtained at 10 −12 [22] in solar system.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The LLI violation (LLIv) in gravitational interaction modifies the local Lorentzian transformation property of gravitation, and leads to various anomalous phenomena in gravitational experiments [2,3,[7][8][9][10][11], including lunar laser ranging [12,13], atom interferometry [14], pulsar timing [15][16][17][18][19], cosmic rays [20,21], very long baseline interferometry [22], and short-range experiments in laboratory [23][24][25][26]. In this short contribution, I will focus on the recent limits on LLIv obtained from precision pulsar timing experiments [7,[15][16][17][18][19]27,28] in the theoretical frameworks of parametrized post-Newtonian (PPN) gravity [2,29] and the pure gravity sector of the standard-model extension (SME) [1,6,7].…”
Section: Introductionmentioning
confidence: 99%