Quantumized photons actually have many characteristics that are different from classical electrom...
Quantumized photons actually have many characteristics that are different from classical electromagnetics. For example, there is no one who is satisfied with the existence of a Phase Operator. The initial intuition is based on the following definition: а-де-іф, and suppose and ф are both Hermitian, because the two correspond to similar amplitudes, one corresponds to similar Phase. Therefore, iT we take Hermitian Conjugate a, we get at-e-ing Note that the order is exchanged, because g and ф are not necessarily able to commute to each other. Under these assumptions, please: 1/2 (A) Prove that g - (n + 1) (B) Prove that ñ-1-e-14hel (C) Through the mathematical formula: and plus part of B's proof n, <p - i In quantum physics [K,p]- ih implies AxAp 2 , so we can speculate that if [ri,oj i is true Δη Δφ-2. However, as mentioned before, the phase itself is not greater than 2π, so Δφ is not greater than 2π, and the uncertainty principle of n and ф that we introduce is not valid. In addition to this, there is a simpler proof, please (D) Through [n'ф-1 , the following formula is obtained: (m-n)<m|фіп- lomn
Quantumized photons actually have many characteristics that are different from classical electromagnetics. For example, there is no one who is satisfied with the existence of a Phase Operator. The initial intuition is based on the following definition: а-де-іф, and suppose and ф are both Hermitian, because the two correspond to similar amplitudes, one corresponds to similar Phase. Therefore, iT we take Hermitian Conjugate a, we get at-e-ing Note that the order is exchanged, because g and ф are not necessarily able to commute to each other. Under these assumptions, please: 1/2 (A) Prove that g - (n + 1) (B) Prove that ñ-1-e-14hel (C) Through the mathematical formula: and plus part of B's proof n,