Radiative cascade of highly excited hydrogen atoms in strong magnetic... Türker Topçu and Francis Robicheaux 兲
... 兩m兩 from 200 to 40 and observed that the motion in states with 兩m兩 ⬃ 200− 80 are adiabatically separable to the extent where no more than 50% of the energy levels are overtaken by the nonadiabatic couplings. As they decreased 兩m兩 further down to 兩m兩 ⬃ 40 the energy spectrum experienced a transition ...
... 兩m兩 from 200 to 40 and observed that the motion in states with 兩m兩 ⬃ 200− 80 are adiabatically separable to the extent where no more than 50% of the energy levels are overtaken by the nonadiabatic couplings. As they decreased 兩m兩 further down to 兩m兩 ⬃ 40 the energy spectrum experienced a transition ...
Indistinguishability and improper mixtures
... The error in d’Espagnat’s argument has “caused some confusion in the theory of measurement,” in Jammer’s phrase (Ref. 15, pp. 479-80, footnote), referring to the argument of Refs. 2 and 4) — but in the sense opposite to that meant by Jammer. The “confusion” referred to is the repeated rediscovery of ...
... The error in d’Espagnat’s argument has “caused some confusion in the theory of measurement,” in Jammer’s phrase (Ref. 15, pp. 479-80, footnote), referring to the argument of Refs. 2 and 4) — but in the sense opposite to that meant by Jammer. The “confusion” referred to is the repeated rediscovery of ...
Chapter 24 Physical Pendulum
... How good is this approximation? If the pendulum is pulled out to an initial angle θ 0 that is not small (such that our first approximation sin θ ≅ θ no longer holds) then our expression for the period is no longer valid. We shall calculate the first-order (or higherorder) correction to the period of ...
... How good is this approximation? If the pendulum is pulled out to an initial angle θ 0 that is not small (such that our first approximation sin θ ≅ θ no longer holds) then our expression for the period is no longer valid. We shall calculate the first-order (or higherorder) correction to the period of ...
Free-Space distribution of entanglement and single photons over
... bounded by 2 in any local realistic theory. However quantum mechanical predictions violate this limit with a maximum value of S = 2 2 ≈ 2.828 . In our experiment, typically measuring over a time of 221 s with 7058 coincidence-events in total, we found S = 2.508±0.037, demonstrating the violation of ...
... bounded by 2 in any local realistic theory. However quantum mechanical predictions violate this limit with a maximum value of S = 2 2 ≈ 2.828 . In our experiment, typically measuring over a time of 221 s with 7058 coincidence-events in total, we found S = 2.508±0.037, demonstrating the violation of ...