In special relativity, such a relationship exists between energy and time as a result of the Robertson–Schrödinger relation. In harmonic analysis, viewing a function and its Fourier transform as conjugate variables on the time-frequency domain will result in the inequality that the infinite integral of the squares of the time and position of the function multiplied by that of its Fourier transform is greater than 1 over 16 pi squared, resulting in a formalized statement of this principle. The most famous version of this principle results when one notes that the wave functions of the momentum and position are Fourier transform pairs, resulting in serious complications in experimentation at the particle level. For 10 points, what is this physical principle whose quan
In special relativity, such a relationship exists between energy and time as a result of the Robertson–Schrödinger relation. In harmonic analysis, viewing a function and its Fourier transform as conjugate variables on the time-frequency domain will result in the inequality that the infinite integral of the squares of the time and position of the function multiplied by that of its Fourier transform is greater than 1 over 16 pi squared, resulting in a formalized statement of this principle. The most famous version of this principle results when one notes that the wave functions of the momentum and position are Fourier transform pairs, resulting in serious complications in experimentation at the particle level. For 10 points, what is this physical principle whose quantum analog was formulated by a student of Niels Bohr in 1926?
In special relativity, such a relationship exists between energy and time as a result of the Robertson–Schrödinger relation.
{uncertainty} principle [do not accept “Heisenberg Uncertainty Principle”]