Summary paragraph: The origin of the Moon's large-scale topography is important for understanding lunar geology 1 , lunar orbital evolution 2 , and the Moon's orientation in the sky 3 .Previous hypotheses for its origin have included late accretion events 4 , large impacts 5 , tidal effects 6 , and convection processes 7 . However, testing these hypotheses and quantifying the Moon's topography is complicated by the large basins that have formed since the crust crystallized. Here we estimate the low-order lunar topography and gravity spherical harmonics outside these basins and show that the bulk of the degree-2 topography is consistent with a crustbuilding process controlled by early tidal heating throughout the Moon. The remainder of the degree-2 topography is consistent with a frozen tidal-rotational bulge that formed later, at a semimajor axis of 32 Earth radii. The probability of the degree-2 shape having these two separate tidal characteristics by chance is less than 1%. We also infer that internal density contrasts eventually reoriented the Moon's polar axis 36 4°, to the present configuration we observe today. Together, these results link the geology of the near and far sides, and resolve longstanding questions about the Moon's low-order shape, gravity, and history of polar wander.
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Main TextThe theory of equilibrium figures of rotating fluid bodies is a classic problem in geophysics, and it has been helpful in understanding the shapes of the Sun and planets. However, the origin for the Moon's shape has remained an open problem in the last century 2,6,[8][9][10] , and the body's deviations from any simple tidal-rotational (spherical harmonic degree-2) figure are large 11 . This difficulty is surprising given the Moon's presumably simple early thermal history: born hot and quickly cooled, one might expect the Moon to be described by a simple figure of equilibrium.Researchers have traditionally suggested that the Moon's degree-2 spherical harmonic gravity coefficients, which have been used as proxies for the degree-2 shape, are especially large when compared to higher degree coefficients 9,12 . Figure 1 shows a power law or "Kaula's rule" fit to degrees n = 3 to 50 for the Moon's gravity 13 and topography data 14 . The power at degree 2 is 4.5 times and 2.6 times the power expected from extrapolating the best-fit power law, for gravity and topography, respectively, supporting the idea that the degree-2 coefficients are unique. Indeed, the fraction of excess power for topography is greater than the excesses for Venus, Earth, and Mars (SI). Authors have tried to interpret the Moon's strong degree-2 power as a frozen tidalrotational state inherited from when the Moon was closer to the Earth, known as the fossil bulge hypothesis 6 . An open problem, however, has been that the ratio of the C 2,0 and C 2,2 spherical harmonic coefficients is different from the expected value by a factor of 2. 6 (refs. 2,10).Adding to the fossil bulge idea and motivated by tidal processes in Europa's ice shell 15 , GarrickBet...