1,440 research outputs found

    A new kind of heterodyne measurement of coherent population trapping in an atomic beam

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    A new heterodyne technique is presented for the simultaneous measurement of dispersion and absorption of atomic transitions useful especially for coherent two photon transitions. This technique is compared with traditional homodyne interferometer and with modern frequency modulation techniques. First results are the properties of a coherent population trapping (CPT) scheme realized in a cesium atomic beam. The measured linewidth of the CPT-resonance is reverse similar, equals 300 kHz (FWHM) with a residual absorption of less than 2 × 10−3 cm−1 and the dispersion is equivalent to a group velocity of vg ≈ c/5000

    A bound on Planck-scale modifications of the energy-momentum composition rule from atomic interferometry

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    High sensitivity measurements in atomic spectroscopy were recently used in Amelino-Camelia et. al. to constraint the form of possible modifications of the energy-momentum dispersion relation resulting from Lorentz invariance violation (LIV). In this letter we show that the same data can be used successfully to set experimental bounds on deformations of the energy-momentum composition rule. Such modifications are natural in models of deformed Lorentz symmetry which are relevant in certain quantum gravity scenarios. We find the bound for the deformation parameter Îș\kappa to be a few orders of magnitude below the Planck scale and of the same magnitude as the next-to-leading order effect found in Amelino-Camelia et. al. We briefly discuss how it would be possible to distinguish between these two scenarios.Comment: 5 pages, some comments and references adde

    Optical resonator with steep internal dispersion

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    We present an optical resonator with modified properties due to a nonabsorbing highly dispersive medium. The steep nonabsorbing dispersion is created with an additional pump field in an atomic beam using the effect of coherent population trapping. The linewidth of such a resonator depends on the slope of the dispersion line, which in turn depends on the atomic density and the intensity of pump and probe field. In the experiments presented here, the cavity linewidth is reduced by a factor of more than 50 relative to the linewidth of the empty resonator. We have studied the influence of the relative intensities of pump and probe field on the line profile. Due to the dispersion of the medium, the resonance frequency is nearly independent of the geometrical length of the resonator

    Improved α4\alpha^4 Term of the Electron Anomalous Magnetic Moment

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    We report a new value of electron g−2g-2, or aea_e, from 891 Feynman diagrams of order α4\alpha^4. The FORTRAN codes of 373 diagrams containing closed electron loops have been verified by at least two independent formulations. For the remaining 518 diagrams, which have no closed lepton loop, verification by a second formulation is not yet attempted because of the enormous amount of additional work required. However, these integrals have structures that allow extensive cross-checking as well as detailed comparison with lower-order diagrams through the renormalization procedure. No algebraic error has been uncovered for them. The numerical evaluation of the entire α4\alpha^4 term by the integration routine VEGAS gives −1.7283(35)(α/π)4-1.7283 (35) (\alpha/\pi)^4, where the uncertainty is obtained by careful examination of error estimates by VEGAS. This leads to ae=1159652175.86(0.10)(0.26)(8.48)×10−12a_e = 1 159 652 175.86 (0.10) (0.26) (8.48) \times 10^{-12}, where the uncertainties come from the α4\alpha^4 term, the estimated uncertainty of α5\alpha^5 term, and the inverse fine structure constant, α−1=137.0360003(10)\alpha^{-1} = 137.036 000 3 (10), measured by atom interferometry combined with a frequency comb technique, respectively. The inverse fine structure constant α−1(ae)\alpha^{-1} (a_e) derived from the theory and the Seattle measurement of aea_e is 137.03599883(51)137.035 998 83 (51).Comment: 64 pages and 10 figures. Eq.(16) is corrected. Comments are added after Eq.(40

    High-accuracy Penning trap mass measurements with stored and cooled exotic ions

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    The technique of Penning trap mass spectrometry is briefly reviewed particularly in view of precision experiments on unstable nuclei, performed at different facilities worldwide. Selected examples of recent results emphasize the importance of high-precision mass measurements in various fields of physics

    White-light cavities, atomic phase coherence, and gravitational wave detectors

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    We propose a new concept to realize optical cavities with large buildup but broadband response (white-light cavities) using atomic phase coherence. We demonstrate that strongly driven double-Λ systems can show negative dispersion without absorption, which is needed in order to compensate for the variation of the wavelength with frequency. Internal buildup profiles and the cavity bandwidth of standard devices and white-light cavities will be briefly compared. These devices may be useful to improve the bandwidth and sensitivity of future generations of laser interferometric gravitational wave detectors

    Improved α4\alpha^4 Term of the Muon Anomalous Magnetic Moment

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    We have completed the evaluation of all mass-dependent α4\alpha^4 QED contributions to the muon g−2g-2, or aÎŒa_\mu, in two or more different formulations. Their numerical values have been greatly improved by an extensive computer calculation. The new value of the dominant α4\alpha^4 term A2(8)(mÎŒ/me)A_2^{(8)} (m_\mu / m_e) is 132.6823 (72), which supersedes the old value 127.50 (41). The new value of the three-mass term A3(8)(mÎŒ/me,mÎŒ/mτ)A_3^{(8)} (m_\mu / m_e, m_\mu / m_\tau) is 0.0376 (1). The term A2(8)(mÎŒ/mτ)A_2^{(8)} (m_\mu / m_\tau) is crudely estimated to be about 0.005 and may be ignored for now. The total QED contribution to aÎŒa_\mu is 116584719.58(0.02)(1.15)(0.85)×10−11116 584 719.58 (0.02)(1.15)(0.85) \times 10^{-11}, where 0.02 and 1.15 are uncertainties in the α4\alpha^4 and α5\alpha^5 terms and 0.85 is from the uncertainty in α\alpha measured by atom interferometry. This raises the Standard Model prediction by 13.9×10−1113.9 \times 10^{-11}, or about 1/5 of the measurement uncertainty of aÎŒa_\mu. It is within the noise of current uncertainty (∌100×10−11\sim 100 \times 10^{-11}) in the estimated hadronic contributions to aÎŒa_\mu.Comment: Appendix A has been rewritten extensively. It includes the 4th-order calculation for illustration. Version accepted by PR

    Probing the quantum-gravity realm with slow atoms

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    For the study of Planck-scale modifications of the energy-momentum dispersion relation, which had been previously focused on the implications for ultrarelativistic (ultrafast) particles, we consider the possible role of experiments involving nonrelativistic particles, and particularly atoms. We extend a recent result establishing that measurements of "atom-recoil frequency" can provide insight that is valuable for some theoretical models. And from a broader perspective we analyze the complementarity of the nonrelativistic and the ultrarelativistic regimes in this research area.Comment: LaTex, 13 page

    Optical Clocks in Space

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    The performance of optical clocks has strongly progressed in recent years, and accuracies and instabilities of 1 part in 10^18 are expected in the near future. The operation of optical clocks in space provides new scientific and technological opportunities. In particular, an earth-orbiting satellite containing an ensemble of optical clocks would allow a precision measurement of the gravitational redshift, navigation with improved precision, mapping of the earth's gravitational potential by relativistic geodesy, and comparisons between ground clocks.Comment: Proc. III International Conference on Particle and Fundamental Physics in Space (SpacePart06), Beijing 19 - 21 April 2006, to appear in Nucl. Phys.

    Nanoporous films with low refractive index for large-surface broad-band anti-reflection coatings

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    Nowadays, nanoporous films are widely employed in biochemical applications or in opto-photonic devices such as displays, solar cells, or light-guiding systems. In particular, the technological feasibility of nanoporous layers with low refractive indices has recently enabled the development of high-efficiency anti-reflection coatings. In this paper, we report on hybrid polymer nanoporous films that can be fabricated in a single coating step with an industrial aqueous-based method on very large surfaces. Both high transparency and low refractive index are simultaneously achieved over the entire visible spectrum. We eventually demonstrate the potential of such films for broadband AR applications by combining them in a graded-index multilayer that reduces the surface reflectivity of a polymer substrate from 10% to few ‰
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