Open Access
Table D.1
Notations used along this work and their designations in order of appearance in the text.
Symbol | Definition | Reference |
---|---|---|
e | Planet eccentricity | Sect. 1 |
eAR | Critical eccentricity for asynchronous rotation | Sect. 1 |
Mp | Planet mass | Sect. 2 |
Rp | Planet radius | Sect. 2 |
Hoc | Ocean depth | Sect. 2 |
ρoc | Ocean density | Sect. 2 |
n⋆ | Planet mean motion | Sect. 2 |
n⋆ | Orbital angular momentum of the planet | Sect. 2 |
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Planetocentric reference frame | Sect. 2 |
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Reference frame co-rotating with the planet | Sect. 2 |
Ω | Spin vector | Sect. 2 |
Ω | Rotation rate of the planet | Sect. 2 |
t | Time | Sect. 2 |
r | Radial coordinate (spherical coordinates) | Sect. 2 |
θ | Colatitude (spherical coordinates) | Sect. 2 |
φ | Longitude (spherical coordinates) | Sect. 2 |
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Spherical unit-vector basis | Sect. 2 |
g | Planet surface gravity | Sect. 2 |
ρp | Planet mean density | Sect. 2 |
Moc | Mass of the ocean | Sect. 2 |
Mc | Mass of the solid part | Sect. 2 |
Rc | Radius of the solid part | Sect. 2 |
ρc | Mean density of the solid part | Sect. 2 |
σR | Rayleigh drag frequency | Sect. 2 |
τR | Typical timescale of core-ocean coupling by viscous friction | Sect. 2 |
r⋆ | Star-planet distance | Eq. (1) |
M⋆ | Mass of the host star | Eq. (1) |
Û⋆ | Gravitational potential of the host star | Eq. (1) |
^ | Symbol used to highlight real quantities | Eq. (1) |
˜ | Symbol used to highlight complex quantities | Eq. (1) |
ÛT | Real tidal gravitational potential | Eq. (2) |
ℜ | Real part of a complex number | Eq. (3) |
ℑ | Imaginary part of a complex number | Eq. (3) |
i | Imaginary number | Eq. (3) |
UT | Complex tidal gravitational potential | Eq. (3) |
l | Latitudinal degree (spherical harmonics) | Eq. (3) |
m | Longitudinal degree (spherical harmonics) | Eq. (3) |
s | Eccentricity degree | Eq. (3) |
σ | Forcing frequency | Eq. (3) |
σm,s | Forcing tidal frequency of the mode associated with the doublet ![]() |
Eq. (3) |
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Normalised associated Legendre functions | Eq. (3) |
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Eq. (3) |
a | Semi-major axis of the planet | Eq. (4) |
Al,m,s | Dimensionless eccentricity functions | Eq. (4) |
δl,k | Kronecker symbol | Eq. (5) |
δs<0 | Coefficient equal to 1 for s < 0, 0 otherwise | Eq. (5) |
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Unnormalised associated Legendre functions | Eq. (5) |
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Hansen coefficients | Eq. (5) |
σ2,s | Forcing frequency of the degree-s eccentricity term | Eq. (6) |
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Degree-s component of the perturbing tidal potential | Eq. (7) |
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Semidiurnal component of the perturbing tidal potential | Eq. (8) |
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Degree-1 eccentricity component of the perturbing tidal potential | Eq. (9) |
σ2,1 | Forcing frequency of the degree-1 eccentricity component | Eq. (9) |
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Degree-3 eccentricity component of the perturbing tidal potential | Eq. (10) |
σ2,3 | Forcing frequency of the degree-3 eccentricity component | Eq. (10) |
etrans | Transition eccentricity | Sect. 3.1 |
μ | Effective unrelaxed shear modulus of the solid core | Sect. 3.2 |
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Stress tensor | Eq. (12) |
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Strain tensor | Eq. (12) |
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Complex shear modulus of the solid part | Eq. (13) |
Γ | Gamma function | Eq. (14) |
α | Rheological exponent of the material in the Andrade model | Eq. (14) |
τM | Maxwell relaxation time of the material | Eq. (14) |
η | Viscosity of the material | Eq. (14) |
τA | Andrade time of the material in the Andrade model | Eq. (14) |
PT | Tidal period | Sect. 3.2 |
β | Andrade parameter | Sect. 3.2 |
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Gravitational Love number of the degree-l mode | Eq. (15) |
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Displacement Love number of the degree-l mode | Eq. (15) |
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Gravitational load Love number of the degree-l mode | Eq. (15) |
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Displacement load Love number of the degree-l mode | Eq. (15) |
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Dimensionless effective rigidity | Eq. (16) |
Al | Dimensionless rigidity coefficient associated with the degree-l component | Eq. (17) |
ξc | Vertical displacement of the oceanic floor | Sect. 3.3 |
V | Velocity vector of the horizontal component of tidal flows | Sect. 3.3 |
Vθ | Latitudinal component of the velocity field | Sect. 3.3 |
Vφ | Longitudinal component of the velocity field | Sect. 3.3 |
ξoc | Vertical displacement of the ocean surface | Sect. 3.3 |
η | Variation of the ocean thickness | Sect. 3.3 |
∂X | Partial derivative with respect to X | Eq. (18) |
Ψ | Perturbed potential encompassing the gravitational forcing and coupling with the solid part | Eq. (18) |
∇h | Horizontal gradient operator | Eq. (20) |
∇h ⋅ | Horizontal divergence operator | Eq. (21) |
Ψm,σ | Fourier component of the perturbed potential | Eq. (22) |
Vm,σ | Fourier component of the velocity vector | Eq. (22) |
ηm,σ | Fourier component of the vertical variation of the ocean depth | Eq. (22) |
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Degree-l component of Ψm,σ expanded in series of associated Legendre functions | Eq. (23) |
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Degree-l component of Vm,σ expanded in series of associated Legendre functions | Eq. (23) |
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Degree-l component of ηm,σ expanded in series of associated Legendre functions | Eq. (23) |
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Complex tidal frequency | Eq. (24) |
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Complex spin parameter | Eq. (24) |
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Laplace’s tidal operator | Eq. (27) |
n | Degrees of Hough functions | Eq. (29) |
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Degree-n component of Ψm,σ expanded in series of Hough functions | Eq. (29) |
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Degree-n Hough function | Eq. (29) |
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Eigenvalue associated with the degree-n Hough function | Eq. (30) |
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Equivalent depth of the degree-n Hough mode | Eq. (31) |
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Coefficients of Hough functions expanded in series of the ![]() |
Eq. (32) |
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Coefficients of the ![]() |
Eq. (33) |
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Overlap coefficients weighting the degree-n component of the oceanic tidal torque | Eq. (34) |
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Tilt factor associated with the tidal gravitational forcing of the perturber | Eq. (35) |
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Tilt factor associated with the distortion of the oceanic layer | Eq. (36) |
σn,k | Complex characteristic frequencies of the planet | Eq. (41) |
kh ;n | Horizontal wavenumber of the degree-n Hough mode | Eq. (41) |
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Component of the force vector inducing the tidal perturbation | Eq. (42) |
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Tidal torque exerted on the planet | Eq. (44) |
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Quadrupolar component of the effective gravitational Love number of the planet | Eq. (45) |
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Tidal torque exerted on the solid part in absence of oceanic layer | Eq. (46) |
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Quadrupolar tidal Love number of the solid part in absence of oceanic layer | Eq. (47) |
A2 | Dimensionless rigidity coefficient associated with the l = 2 component | Eq. (48) |
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Tidal torque exerted on the ocean in case of solid part of infinite rigidity | Eq. (49) |
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Complex eigenfrequency of the degree-n Hough mode in the positive-frequency range | Eq. (50) |
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Complex eigenfrequency of the degree-n Hough mode in the negative-frequency range | Eq. (50) |
σn | Characteristic frequency of the degree-n surface gravity mode | Eq. (54) |
σmax ;n | Frequency at which the resonant peak of a mode reaches a maximum | Eq. (56) |
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Maximum of ![]() |
Eq. (58) |
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Degree-s eccentricity frequency associated with a peak | Sect. 4.3 |
Ωeq ;s | Rotation rate corresponding to the degree-s spin-orbit resonance | Sect. 4.3 |
P⋆ | Orbital period of the planet | Sect. 4.4 |
M⊙ | Mass of the Sun | Sect. 4.4 |
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Spin parameter associated with the semidiurnal tidal component | Eq. (62) |
γs | Parameter controlling the existence of asynchronous states in the case of pure oceanic tide | Eq. (65) |
X | Normalised frequency | Eq. (69) |
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Dimensionless constant | Eq. (69) |
uα | Maximum of the polynomial function defined by Eq. (69) | Eq. (71) |
Prot | Rotation period of the planet | Sect. 6.1 |
Hoc ;s | Ocean depth associated with the resonance of the degree-s eccentricity component | Sect. 6.1 |
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Constant factor in the expression of the solid tidal torque in the non-resonant regime | Eq. (73) |
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Tidal torque exerted on the planet | Eq. (75) |
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Torque due to triaxiality | Eq. (75) |
∙ | Time derivative | Eq. (75) |
A, B, C | Principal moments of inertia of the planet (in increasing magnitude) | Eq. (76) |
γ2,s | angle associated with the degree-s perturbation component | Eq. (76) |
ϑ | Planet rotation angle | Eq. (76) |
M | Planet mean anomaly | Eq. (76) |
.. | Second order time derivative | Eq. (78) |
Δ | Width of the resonance | Eq. (79) |
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Even component of the tidal torque | Eq. (81) |
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Odd component of the tidal torque | Eq. (82) |
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Capture probability of the s∕2 spin-orbit resonance | Eq. (83) |
ΔP | Normalised width of the 1:1 spin-orbit resonance | Eq. (84) |
γ | Logarithm of the ocean depth | Sect. 8 |
Č | Normalised moment of inertia | Sect. 8 |
τev | Evolution timescale of the planet spin rotation | Eq. (89) |
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Eccentricity and mean anomaly function | Eq. (B.1) |
v | True anomaly | Eq. (B.1) |
N | Order of the fast Fourier transform (FFT) in the calculation of Hansen coefficients | Appendix B |
K | Truncation index of the series of Hansen coefficients calculated using the FFT method | Appendix B |
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Complex triaxial torque | Eq. (C.2) |
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