han_2000_apl
... contribution from the rapidly varying component (molecular lines). If the absorption crosssection is known then the gas concentration can be derived by using the Beer-Lambert law.1 To detect water vapor, which has narrow absorption lines at the THz frequency range, a narrowband THz wave source is d ...
... contribution from the rapidly varying component (molecular lines). If the absorption crosssection is known then the gas concentration can be derived by using the Beer-Lambert law.1 To detect water vapor, which has narrow absorption lines at the THz frequency range, a narrowband THz wave source is d ...
Quantum Optics and Photonics
... the range of diode lasers for this rubidium system, potentially allowing inexpensive and practical systems in the future. While this scheme is much simpler than the one employed in sodium, it is still necessary to introduce a detuning (typically 80 MHz) between the two pump beams to provide the symm ...
... the range of diode lasers for this rubidium system, potentially allowing inexpensive and practical systems in the future. While this scheme is much simpler than the one employed in sodium, it is still necessary to introduce a detuning (typically 80 MHz) between the two pump beams to provide the symm ...
![[HMIM][Br9]: a Room-temperature Ionic Liquid Based on a](http://s1.studyres.com/store/data/016911324_1-ac5688316a1e3a6c1ba364df016e5832-300x300.png)
Quantum theory of spin waves in finite chiral spin chains
... We address first the case of a simple chain with firstnearest-neighbors exchange and DM interactions. In spite of its simplicity, we shall see that this simple model captures the essence of the physical behavior of the spin waves in the more realistic case described in the next subsection. The first ...
... We address first the case of a simple chain with firstnearest-neighbors exchange and DM interactions. In spite of its simplicity, we shall see that this simple model captures the essence of the physical behavior of the spin waves in the more realistic case described in the next subsection. The first ...
Heterodynedetected timedomain measurement of I2 predissociation
... contributions to the excited state signal will decay with different time constants. In the present case, however, we find 12v::= TI ::=200 fs. This result implies that vibrational dephasing results predominantly from population decay of both excited state vibronic levels involved in the vibrational ...
... contributions to the excited state signal will decay with different time constants. In the present case, however, we find 12v::= TI ::=200 fs. This result implies that vibrational dephasing results predominantly from population decay of both excited state vibronic levels involved in the vibrational ...
laser spectroscopy
... The hyperfine structure of both 85Rb and 87Rb will be observed in this experiment; however, it is the hyperfine structure of 87Rb that will be studied. The split of energy levels by the hyperfine interaction is shown in the right column of Figure 3 for 87Rb. These levels are known as hyperfine level ...
... The hyperfine structure of both 85Rb and 87Rb will be observed in this experiment; however, it is the hyperfine structure of 87Rb that will be studied. The split of energy levels by the hyperfine interaction is shown in the right column of Figure 3 for 87Rb. These levels are known as hyperfine level ...
Visible light optical coherence correlation spectroscopy
... spL2048-140km with 2048 pixels, Basler). As illustrated in Fig. 1, the illumination and detection beams do not overlap in the aperture plane of the objective: any specular reflected light from the glass slide is blocked by the diaphragm Fdet . The interferometer was conceived with a minimum number o ...
... spL2048-140km with 2048 pixels, Basler). As illustrated in Fig. 1, the illumination and detection beams do not overlap in the aperture plane of the objective: any specular reflected light from the glass slide is blocked by the diaphragm Fdet . The interferometer was conceived with a minimum number o ...
