Table B1.

Temporal evolution of the spectral parameters. Each parameter in the leftmost column evolves as a power law in time, with the power-law index in the coasting and accelerating regimes given in the centre and right columns, respectively.

QuantityCoasting (f > γ2)Accelerating (f < γ2)
νm20|$\frac{s-\ell }{\ell +2}$|
νm3|$\frac{-4(s-\ell )}{s+2}$||$\frac{-(s-\ell )}{\ell +2}$|
νc−2(k − 1)|$-2(k-1) + \frac{5(s-\ell )}{\ell +2}$|
Lν, max2(k − 1) + ℓ|$(k-1)+s -\frac{3(s-\ell )}{\ell +2}$|
Lν, max3|$(k-1) + \ell + \frac{s-\ell }{s+2}$||$(k-1)+s-\frac{2(s-\ell )}{\ell +2}$|
QuantityCoasting (f > γ2)Accelerating (f < γ2)
νm20|$\frac{s-\ell }{\ell +2}$|
νm3|$\frac{-4(s-\ell )}{s+2}$||$\frac{-(s-\ell )}{\ell +2}$|
νc−2(k − 1)|$-2(k-1) + \frac{5(s-\ell )}{\ell +2}$|
Lν, max2(k − 1) + ℓ|$(k-1)+s -\frac{3(s-\ell )}{\ell +2}$|
Lν, max3|$(k-1) + \ell + \frac{s-\ell }{s+2}$||$(k-1)+s-\frac{2(s-\ell )}{\ell +2}$|
Table B1.

Temporal evolution of the spectral parameters. Each parameter in the leftmost column evolves as a power law in time, with the power-law index in the coasting and accelerating regimes given in the centre and right columns, respectively.

QuantityCoasting (f > γ2)Accelerating (f < γ2)
νm20|$\frac{s-\ell }{\ell +2}$|
νm3|$\frac{-4(s-\ell )}{s+2}$||$\frac{-(s-\ell )}{\ell +2}$|
νc−2(k − 1)|$-2(k-1) + \frac{5(s-\ell )}{\ell +2}$|
Lν, max2(k − 1) + ℓ|$(k-1)+s -\frac{3(s-\ell )}{\ell +2}$|
Lν, max3|$(k-1) + \ell + \frac{s-\ell }{s+2}$||$(k-1)+s-\frac{2(s-\ell )}{\ell +2}$|
QuantityCoasting (f > γ2)Accelerating (f < γ2)
νm20|$\frac{s-\ell }{\ell +2}$|
νm3|$\frac{-4(s-\ell )}{s+2}$||$\frac{-(s-\ell )}{\ell +2}$|
νc−2(k − 1)|$-2(k-1) + \frac{5(s-\ell )}{\ell +2}$|
Lν, max2(k − 1) + ℓ|$(k-1)+s -\frac{3(s-\ell )}{\ell +2}$|
Lν, max3|$(k-1) + \ell + \frac{s-\ell }{s+2}$||$(k-1)+s-\frac{2(s-\ell )}{\ell +2}$|
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