A cold Rydberg gas, with its atoms prepared initially all in the excited state <span style="white-space:nowrap;">|<em>n</em><sub>0</sub>></span> , with <em>n</...A cold Rydberg gas, with its atoms prepared initially all in the excited state <span style="white-space:nowrap;">|<em>n</em><sub>0</sub>></span> , with <em>n</em><sub>0 </sub><span style="white-space:nowrap;">»</span>1, contains an excessive amount of energy, and presumably is to relax by the Penning-type <em>molecular auto-ionization</em> (<em>MAI</em>), in which a portion of excess energy of one atom is given to another near-by atom and ionizing it. Its complementary process, the <em>resonant energy transfer</em> (<em>RET</em>), is discussed, in which the excess energy of one atom is used on another to form a hyper-excited atomic state <span style="white-space:normal;">|</span><em style="white-space:normal;">n</em><sub style="white-space:normal;"><em>a</em></sub><span style="white-space:normal;">></span> with <em>n</em><sub><em>a</em></sub><span style="white-space:nowrap;">»</span><em style="white-space:normal;">n</em><sub style="white-space:normal;">0</sub>. This process is always present, provided certain resonance energy conditions are satisfied. In this report, the <em>n</em><sub>0</sub> and density dependences of the RET rates are studied in detail, employing a simple model: 1) at low densities, the RET is mediated by the dipole-dipole coupling <em>V</em><sub><em>dd</em></sub> and its rates are generally much smaller than that of MAI, especially for small <em>n</em><sub>0</sub>. But 2) as the density increases, our model shows that the rates become of comparable magnitude or even larger than the MAI rates. The<em> V</em><sub><em>dd</em></sub> is no longer adequate. We, then construct a semi-empirical potential to describe the RET process. 3) At high densities, we show that the atomic orbital of <span style="white-space:normal;">|</span><em style="white-space:normal;">n</em><sub style="white-space:normal;"><em>a</em></sub><span style="white-space:normal;">></span> overlaps with that of neighboring atoms, and the electron-electron potential becomes prominent, resulting in much higher rates.展开更多
文摘A cold Rydberg gas, with its atoms prepared initially all in the excited state <span style="white-space:nowrap;">|<em>n</em><sub>0</sub>></span> , with <em>n</em><sub>0 </sub><span style="white-space:nowrap;">»</span>1, contains an excessive amount of energy, and presumably is to relax by the Penning-type <em>molecular auto-ionization</em> (<em>MAI</em>), in which a portion of excess energy of one atom is given to another near-by atom and ionizing it. Its complementary process, the <em>resonant energy transfer</em> (<em>RET</em>), is discussed, in which the excess energy of one atom is used on another to form a hyper-excited atomic state <span style="white-space:normal;">|</span><em style="white-space:normal;">n</em><sub style="white-space:normal;"><em>a</em></sub><span style="white-space:normal;">></span> with <em>n</em><sub><em>a</em></sub><span style="white-space:nowrap;">»</span><em style="white-space:normal;">n</em><sub style="white-space:normal;">0</sub>. This process is always present, provided certain resonance energy conditions are satisfied. In this report, the <em>n</em><sub>0</sub> and density dependences of the RET rates are studied in detail, employing a simple model: 1) at low densities, the RET is mediated by the dipole-dipole coupling <em>V</em><sub><em>dd</em></sub> and its rates are generally much smaller than that of MAI, especially for small <em>n</em><sub>0</sub>. But 2) as the density increases, our model shows that the rates become of comparable magnitude or even larger than the MAI rates. The<em> V</em><sub><em>dd</em></sub> is no longer adequate. We, then construct a semi-empirical potential to describe the RET process. 3) At high densities, we show that the atomic orbital of <span style="white-space:normal;">|</span><em style="white-space:normal;">n</em><sub style="white-space:normal;"><em>a</em></sub><span style="white-space:normal;">></span> overlaps with that of neighboring atoms, and the electron-electron potential becomes prominent, resulting in much higher rates.