The oscillator strengths should appear farther down in the output, e.g., using your input file for H2O molecule:

EOMEE-CCSD calculation: CPU 5.06 s wall 3.24 s
Start computing the transition properties
------------------------------------------------------------------------------
The new SOC module will be executed
Authors: Pavel Pokhilko and Evgeny Epifanovsky
SOC 1e and mf integrals are evaluating by libqints...
------------------------------------------------------------------------------
State A: ccsd: 0/A
State B: eomee_ccsd/rhfref/singlets: 1/A
Energy GAP = 0.314615 a.u. = 8.561106 eV
Transition dipole moment (a.u.):
A->B: 0.369590 (X 0.000000, Y -0.369590, Z 0.000000)
B->A: 0.376400 (X 0.000000, Y -0.376400, Z 0.000000)
Oscillator strength (a.u.): 0.029178
Transition angular momentum against gauge origin (a.u.):
A->B: (X -0.115529i, Y 0.000000i, Z 0.149221i)
B->A: (X 0.118861i, Y 0.000000i, Z -0.153525i)
Norm of one-particle transition density matrix:
A->B: 0.957596; B->A: 0.970619
||gamma^AB||*||gamma^BA||: 0.929461

Hello, I want to calculate the resonant auger decay using the EOM-CCSD. The output calculated according to the cvs-ee-states and ip-states instructions used in the Q-chem manual belongs only to the resonant participator decay. How to configure it to calculate the resonance spectator decay? thanks.

In the case of resonant Auger decay, we distinguish between participator and spectator/observer decay. The decay channels for participator decay are 1h states and decay channels for spectator decay are 2h1p states. Both 1h and 2h1p states can be computed by EOM-IP-CCSD, however, the energies of the latter states will be overestimated. The two types of states can be distinguished by analyzing EOM-IP amplitudes: the states with R1^2 close to 1 correspond to participator decay whereas those with R2^2 close to 1 correspond to spectator decay.

Here’s a sample of the rem section of the input for the benzene molecule (for the opitmized structure see J. Chem. Phys., 158, 064109, (2023)):

In the output you will find the first three EOM-IP states with R1^2 close to 1 (participator decay) and the fourth EOM-IP state with R2^2 is close to 1 (spectator/observer decay)