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Laser Physics Letters

Beating in free polarization decay

Гольдорт Вениамин Гершевич, Ледовских Дмитрий Васильевич, Хворостов Евгений Борисович, Н. Н. Рубцова

Published Dec 10, 2007• 5 citations
Publisher

Abstract

Free polarization decay formed by Stark switching technique in a presence of 9P(32) CO2 laser low intensity radiation in a low pressure gas 13CH3F is investigated as a function of Stark field strength. Rotation transition R(4,3) of vibrational mode 0 ↔ 1 ν3 was used. The beatings between free polarization signals originating from transitions with different magnetic quantum numbers appeared as periodic peaks with the period inversely proportional to the Stark field strength. The weighted difference between permanent dipole moments of upper and lower vibration states is estimated from these data, in agreement with known values of permanent dipole moments.

DOI
10.1002/lapl.200710118

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Physical Review A•Oct 1, 1979•8 citations
Free polarization decay formed by Stark switching technique in a presence of 9P(32) CO2 laser low intensity radiation in a low pressure gas 13CH3F is investigated as a function of Stark field strength. Rotation transition R(4,3) of vibrational mode 0 ↔ 1 ν3 was used. The beatings between free polarization signals originating from transitions with different magnetic quantum numbers appeared as periodic peaks with the period inversely proportional to the Stark field strength. The weighted difference between permanent dipole moments of upper and lower vibration states is estimated from these data, in agreement with known values of permanent dipole moments.
Transient signals of optical nutations and free polarization decay arising in a gas 13CH3F (rotational transition R(4,3) of vibration mode 0–1 ν3 ) at the step-wise switch of electric field in the presence of resonant radiation of CO2 laser are investigated. In the limit of low intensity of radiation the peaks of free polarization decay are observed; the frequency of their appearance is proportional to the electric field strength. The number of observable peaks of free polarization decay decreases at laser intensity growth, and free polarization decay signal becomes indistinguishable at a background of optical nutations at high laser intensity. At high laser intensity the signal of transient optical nutations dominates. Results of calculations are in qualitative agreement with experimental data
Free polarization decay and photon echo were studied experimentally in polar gas 13CH3F at the transition R(4,3) of vibrational mode 0 yields 1 (nu) 3 by Stark switching of molecular levels under irradiation by CW CO2 laser at 9P(32) line. Application of 4.5 mcs pulse to the Stark electrodes inside the gas cell allows to detect the free polarization decay signal, combined with the optical nutation. The sign of the signal corresponds to the increase of absorption in the limit of low intensity (not over 0.01 W/cm2) saturating radiation. Exciting intensity growth till the level of 6.0 W/cm2 implies decrease of signal absolute value, till the change of its sign, while the oscillation of the free polarization decay signal reveals remarkable frequency shift. Such behavior is attributed to the combined action of the dynamic Stark effect of CW radiation field and the levels splitting by the Stark voltage. Two shorter (of about 0.1 and 0.2 mcs) Stark pulses, applied to the gas, generate the photon echo signals detected by the same heterodyne technique. The study of the variations of photon echo parameters versus exciting radiation intensity is in progress.
The possibility of controlling the processes of the free-polarization decay and photon echo in a gas by means of resonant CW radiation has been shown. The photon echo and free-polarization decay are formed using the method of the Stark switching of levels in a low-intensity radiation field in the presence of an orthogonally polarized strong field. The experiments in the gas at the R(4, 3) transition in the vibrational band 0 ↔ 1 v3 13CH3F in the presence of radiation from a CW CO2 laser and the calculations by the evolution operator method show a strong effect of the high-intensity radiation field on the photon echo and free-polarization decay to its complete suppression.
Coherent transient phenomena can be generated by the abrupt changes of parameters either of the electromagnetic field or of the matter. Comparative analysis of these two approaches, made on the base of experimental research in molecular gases SF6, 15NH3, HFCO and 13CH3F, excited by the radiation of CW CO2 and 13CO2 lasers, is presented. The first approach of photon echo (and its modifications) generation, based on electro-optic pulses formation from the resonant CW exciting radiation, has proven to be successful for intense infrared molecular transitions. The coherent responses are sufficiently powerful to be applied in high resolution spectroscopy, the spectral markers creation ,and molecular collisions investigations. However, this technique is not very effective for the free polarization decay investigations. Another approach based on the Stark switching molecular levels of polar gas, irradiated by CW laser, was demonstrated for free polarization decay and photon echo generation in 13CH3F. Free polarization decay has shown the pronounced frequency shift because of dynamic Stark effect in the CW radiation field. This specific feature of coherent transients, created by Stark switching, limits the high resolution spectroscopy by the low intensity range of exciting radiation. From other viewpoint, it gives unique possibility to investigate coherent transients generated at the dressed molecular levels.
The authors study the phenomenon of coherent Raman beats in 15N^{15}\mathrm{N}15NH3{\mathrm{H}}_{3}H3​ using a CO2{\mathrm{O}}_{2}O2​ laser and Stark switching. In particular, a three-level system in which the two upper levels always remain split by a few MHz is prepared by switching the transitions into resonance with a short Stark pulse whose bandwidth is large enough to coherently excite both transitions. When one of the coherently excited levels remains in resonance with the laser after the Stark pulse, this system exhibits a qualitatively new effect which has not been seen heretofore. For Stark shifts on the order of the upper-state splitting or smaller, the Raman beat is amplitude modulated at a frequency related to the optical nutation frequency. This is interpreted as being due to an interaction between the two-photon coherent Raman beat process and a single-photon optical nutation process which occurs simultaneously. Numerical calculations as well as a simple analytic model are presented to support this interpretation. By reducing the laser power, one can make the modulation of the Raman beat disappear. From the Raman signal in this regime the permanent electric dipole moment of 15N^{15}\mathrm{N}15NH3{\mathrm{H}}_{3}H3​ in an excited vibrational state is determined and the Raman beat decay rate measured. By comparing the latter result with a delayed optical nutation measurement we show that phase-changing collisions are negligible for the transition studied.