Article

Electromagnetically induced transparency: the thickness of the vapor column is of the order of a light wavelength

Journal of the Optical Society of America B (Impact Factor: 2.21). 01/2007; 24(8):1829-1838. DOI: 10.1364/JOSAB.24.001829

ABSTRACT Electromagnetically induced transparency (EIT) effect has been studied using an extremely thin cell (ETC) with the thickness of an Rb vapor column of the order of light wavelength λ(780nm) and varying in the range of 0.5λ–2.5λ . Λ-systems on the D2 line of Rb85 and Rb87 have been studied experimentally. Along with EIT resonance, we study the peculiarities of velocity-selective optical pumping/saturation (VSOP) resonances, which accompany the EIT resonance and, as a rule, are spectrally broader. It is demonstrated that size-conditioned strongly anisotropic contribution of atoms with different velocities in an ETC causes several dramatic differences of the EIT and VSOP resonances formation in the ETC as compared with an ordinary 1–10cm long cell. Particularly, in the case of the ETC, the EIT linewidth and contrast dramatically depend on the coupling laser detuning from the exact atomic transition. A theoretical model taking into account the peculiarities of transmission spectra when L=nλ and L=(2n+1)λ/2 (n is an integer) has been developed. The experimental transmission spectra are well described by the theoretical model developed. The possibility of EIT resonance formation when atomic column thickness is of the order of L=0.5λ and less is theoretically predicted

0 Bookmarks
 · 
150 Views
  • Source
    [Show abstract] [Hide abstract]
    ABSTRACT: We observe and investigate, both experimentally and theoretically, electromagnetically-induced transparency experienced by evanescent fields arising due to total internal reflection from an interface of glass and hot rubidium vapor. This phenomenon manifests itself as a non-Lorentzian peak in the reflectivity spectrum, which features a sharp cusp with a sub-natural width of about 1 MHz. The width of the peak is independent of the thickness of the interaction region, which indicates that the main source of decoherence is likely due to collisions with the cell walls rather than diffusion of atoms. With the inclusion of a coherence-preserving wall coating, this system could be used as an ultra-compact frequency reference.
    Optics Express 03/2013; 21(6):6880-8. · 3.55 Impact Factor
  • [Show abstract] [Hide abstract]
    ABSTRACT: The Electromagnetically Induced Transparency (EIT) effect in a Λ-systemformed by Cs atoms (6S1/2−6P3/2−6S1/2)confined in an extremely thin cell (ETC) (atomic column thickness L varies in the range of 800 nm–3 μm is studied both experimentally and theoretically. It is demonstrated that when the coupling laser frequency is in exact resonance with the corresponding atomic transition, the EIT resonance parameters weakly depend on L, which allows us to detect the effect at L=λ=852 nm. EIT process reveals a striking peculiarity in case of the coupling laser detuned by Δ fromthe atomic transition, namely the width of the EIT resonance rapidly increases upon an increase in Δ (an opposite effect is observed in centimeter-scale cells). The strong broadening of the EIT resonance for large values of detunings Δ is caused by the influence of atom-wall collisions on dephasing rate of coherence. The influence of the coupling laser on the velocity selective optical pumping/saturation resonances formed in ETC has beenalso studied. The theoretical model well describes the observed results.
    Optics Communications. 01/2012; 285:2090.
  • Source
    [Show abstract] [Hide abstract]
    ABSTRACT: The electromagnetically induced transparency (EIT) on the atomic D 1 line of rubidium is studied using a nanometric-thin cell with atomic vapor column length in the range of L=400–800 nm. It is shown that the reduction of the cell thickness by four orders as compared with an ordinary cm-size cell still allows to form an EIT resonance for L=λ=794 nm with the contrast of up to 40%. Further reduction of thickness to L=λ/2 leads to significant reduction of EIT contrast, verifying that the key parameter for EIT in wavelength-scale-thickness cells is not the value of L itself but L/λ ratio. Remarkable distinctions of EIT formation in nanometric-thin and ordinary cells are demonstrated. Well-resolved splitting of the EIT resonance in a magnetic field for L=λ can be used for magnetometry with nanometric spatial resolution. The presented theoretical model well describes the observed results
    Applied Physics B 01/2011; · 1.78 Impact Factor

Full-text (2 Sources)

View
103 Downloads
Available from
May 20, 2014