We consider a class of ordinary differential equations describing one-dimensional analytic systems with a quasiperiodic forcing term and in the presence of damping. In the limit of large damping, under some generic nondegeneracy condition on the force, there are quasiperiodic solutions which have the same frequency vector as the forcing term. We prove that such solutions are Borel summable at the origin when the frequency vector is either any one-dimensional number or a twodimensional vector such that the ratio of its components is an irrational number of constant type. In the first case the proof given simplifies that provided in a previous work of ours. We also show that in any dimension d, for the existence of a quasiperiodic solution wi...
We consider a class of ordinary differential equations describing one-dimensional systems with a qua...
We consider a class of ordinary differential equations describing one-dimensional systems with a qua...
We consider a class of differential equations, x ̈ + γx ̇ + g(x) = f(ωt), with ω ∈ Rd, describing o...
We consider a class of ordinary differential equations describing one-dimensional analytic systems w...
We consider a class of ordinary differential equations describing one-dimensional analytic systems ...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We study the behaviour of one-dimensional strongly dissipative systems subject to a quasi-periodic f...
We consider a class of singular ordinary differential equations describing analytic systems of arbit...
We study the behaviour of one-dimensional strongly dissipative systems subject to a quasi-periodic f...
We consider a class of ordinary differential equations describing one-dimensional quasi-periodically...
We consider a class of singular ordinary differential equations describing analytic systems of arbit...
We consider a class of ordinary differential equations describing one-dimensional quasi-periodically...
We consider a class of ordinary differential equations describing one-dimensional systems with a qua...
We consider a class of ordinary differential equations describing one-dimensional systems with a qua...
We consider a class of differential equations, x ̈ + γx ̇ + g(x) = f(ωt), with ω ∈ Rd, describing o...
We consider a class of ordinary differential equations describing one-dimensional analytic systems w...
We consider a class of ordinary differential equations describing one-dimensional analytic systems ...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We consider a class of second order ordinary differential equations describing one-dimensional syste...
We study the behaviour of one-dimensional strongly dissipative systems subject to a quasi-periodic f...
We consider a class of singular ordinary differential equations describing analytic systems of arbit...
We study the behaviour of one-dimensional strongly dissipative systems subject to a quasi-periodic f...
We consider a class of ordinary differential equations describing one-dimensional quasi-periodically...
We consider a class of singular ordinary differential equations describing analytic systems of arbit...
We consider a class of ordinary differential equations describing one-dimensional quasi-periodically...
We consider a class of ordinary differential equations describing one-dimensional systems with a qua...
We consider a class of ordinary differential equations describing one-dimensional systems with a qua...
We consider a class of differential equations, x ̈ + γx ̇ + g(x) = f(ωt), with ω ∈ Rd, describing o...