Figure 3
From: Generation of macroscopic Schrödinger cat state in diamond mechanical resonator
(a–g) Represent the Husimi Q function (
with αQ = x + iy the arbitrary complex number and 
the mechanical phonon state) of SCS at the different times t = 0, 9, 17, 28, 39, 47, 56. The upper and lower panel represent the non-dissipative case (κ = 0) and dissipative case (κ = 0.02), respectively. The other parameters are the same as the Fig. 2(a).
