Symbols Latin letters proposition,number à=品(oi+) annihilation operator annihilation operator of the k-th mode of the electromagnetic field =√亮(oi-) creation operator creation operator of the k-th mode of the electromagnetic field lai) A number A() Airy function vector potential A(r,1)=∑kk vector potential operator x akuk(r)e-iant +agu(r)ea! apparatus b proposition,number (polarization)state vector(along the direction b) bi) element vector of a discrete basisb) number,intensity of the magnetic field B=h/8π21 rotational constant of the rigid rotato B=V×A classical magnetic field =(益) magnetic field operator xiker-t)ie-i(kr-on)b speed of light.proposition cj.cj generic coefficients of the j-th element of given discrete expansion coefficient of the basis elementa) coefficient of the basis element coefficients of the expansion of a state vector in stationary state at an initial moment to =0Symbols Latin letters a proposition, number aˆ = m 2h¯ω ωxˆ + ı ˆ x˙  annihilation operator aˆk annihilation operator of the k-th mode of the electromagnetic field aˆ † = m 2h¯ω ωxˆ − ıˆ x˙  creation operator aˆ † k creation operator of the k-th mode of the electromagnetic field |a (polarization) state vector (along the direction a)  a j  element of a discrete vector basis  a j   A number A(ζ ) Airy function A vector potential Aˆ (r, t) = k ck × aˆkuk(r)e−ıωkt + ˆa† ku∗ k(r)eıωkt  vector potential operator A apparatus |A ket describing a generic state of the apparatus b proposition, number |b (polarization) state vector (along the direction b)  bj  element vector of a discrete basis  b j   B number, intensity of the magnetic field B = h/8π2I rotational constant of the rigid rotator B = ∇ × A classical magnetic field Bˆ (r, t) = ı k hk¯ 2cL30 1 2 × aˆkeı(k·r−ωkt) − ˆa† ke−ı(k·r−ωkt)  bλ magnetic field operator c speed of light, proposition c j , c  j generic coefficients of the j-th element of a given discrete expansion ca j coefficient of the basis element  a j  cb j coefficient of the basis element  bj  c (0) n coefficients of the expansion of a state vector in stationary state at an initial moment t0 = 0