“…The energy difference between permitted states ∆E n,n+1 ≈ I p,A Φ 0 ≈ 4 10 −21 J (5) at the real amplitude I p,A ≈ 2 µA of the persistent current of a real ring measured even near superconducting transition T ≈ 0.99T c ≈ 1.24 K [11] corresponds to the value ∆E n,n+1 /k B ≈ 300 K exceeding strongly the temperature of measurements T ≈ 1.24 K. According to (4) and (5) the persistent current and the spectrum discreteness diminish ∆E n,n+1 ≈ I p,A Φ 0 = Φ 0 q /mr(sn s ) −1 → 0 with pair density decrease 1/(sn s ) −1 → 0. Both the persistent current I p,A = q /2mr(sn s ) −1 and the energy difference ∆E n,n+1 equal zero when pair density is zero n s,A = 0 at least in a ring segment l A , Fig.1, because 1/(sn s ) −1 ≈ sln s,A n s,0 /(ln s,A + l A n s,0 − l A n s,A ) = 0.…”