Unless we ignore the unobservable global phase, it is not possible to express qiskit's $U_1(\lambda)$ gate $$\begin{pmatrix}1 & 0 \\ 0 & e^{i\lambda}\end{pmatrix}$$ for arbitrary $\lambda$ in terms of $R_x$, $R_y$ and $R_z$. Note that the three rotation gates have unit determinant
$$
\det R_x(\theta) = \det \begin{pmatrix} \cos\frac{\theta}{2} & -i\sin\frac{\theta}{2} \\ -i\sin\frac{\theta}{2} & \cos\frac{\theta}{2}\end{pmatrix} = 1\\
\det R_y(\theta) = \det \begin{pmatrix} \cos\frac{\theta}{2} & -\sin\frac{\theta}{2} \\ \sin\frac{\theta}{2} & \cos\frac{\theta}{2}\end{pmatrix} = 1\\
\det R_z(\theta) = \det \begin{pmatrix} e^{-i\theta/2} & 0 \\ 0 & e^{i\theta/2}\end{pmatrix} = 1
$$
for all $\theta$. Since determinant of a product is a product of determinants, any product of $R_x$, $R_y$ and $R_z$ also has unit determinant. On the other hand, $\det U_1(\lambda) = e^{i\lambda}$.
In other words, $R_x(\theta), R_y(\theta), R_z(\theta)\in SU(2)$ for all $\theta$, but $U_1(\lambda)\notin SU(2)$ unless $\lambda = 2\pi k$ for some $k\in\mathbb{Z}$ (in which case $U_1(2\pi k) = I$).
However, if we ignore the global phase then $U_1(\lambda) = e^{i\lambda/2} R_z(\lambda)$ is equivalent to $R_z(\lambda)$.
RZ
gate is equal toU1
because the global phase is ignored. So if you docircuit = QuantumCircuit(1); circuit.rz(lambda)
that would implement a u1($\lambda$). $\endgroup$u1
is already the "most basic" gate and cannot be further decomposed. $\endgroup$