“…This is mainly due to a very narrow resonance linewidth, which, depending on the experimental condition, can vary from a few Hz to several KHz. To create the dark state and thus observe a CPT signal that is responsive to changes in the B-field, usually two laser beams from two independent lasers are required [10,14,[19][20][21]. Most commonly, one of the lasers, termed a coupling laser (ω c ), is locked to a given Zeeman sub-level, while the other laser, termed probe (ω p ), is scanned around another sub-level.…”