The Electric Dipole and the Nuclear Quadrupole Moment of Methyl Bromide in the Ground Vibrational State

A set of high-resolution Stark measurements at millimeter-wave frequencies is reported for CH₃⁷⁹Br and CH₃⁸¹Br. These results are analyzed together with previous data available in the literature to find new sets of molecular (rotational, hyperfine, and dipole moments) constants for both isotopic species. A particular improvement is obtained in the evaluation of the dipole moments, whose values are μ(79) = 1.82171 (26) 0, μ(8l) = 1.82185 (26) D, and for the hyperfine-structure parameters, which are estimated by assuming the most recent model for centrifugal distortion (M. R. Aliev and J. T. Hougen, J. Mol. Spectrosc.106, 110-123 (1984)), obtaining eqQ⁷⁹₀ = 577.1088 (57) MHz, χ⁷⁹_J = −0.63 (16) kHz, χ⁷⁹_K = 12.6 (16) kHz and eqQ⁸¹₀ = 482.1030 (94) MHz, χ⁸¹_J = −0.57 (17) kHz, χ⁸¹_K = 9.3 (22) kHz.     

Electric Dipole Moment Function of the OH Molecule

The electric dipole moment function of the OH radical in the ground electronic state is constructed for internuclear distances R [0, ]. The electric dipole moment function is represented as a piecewise continuous function satisfying physically exact asymptotes and experimental values of the electric dipole moment and its derivatives for equilibrium positions of nuclei of the radical. The Padé form for the electric dipole moment function of the OH radical is also approximated. Electric dipole moment functions obtained are compared with the results of ab initio calculations.     

氢原子的固有电偶极矩

用经典力学和双波量子力学计算了氢原子的固有电偶极矩。双波量子理论算得的结果在经典极限下与经典力学的结果一致。普通量子力学对氢原子Stark效应中表现出来的电偶极矩难以做出很好的解释，因为一个波函数描述的是系综而不是单个粒子。经典力学和双波量子力学可描述单个粒子的行为，对永久电偶极矩的计算和解释显得自然而合理。     

铯原子永久电偶极矩研究

从理论方面和实验方面论述,铯原子可能有大的永久电偶极矩。     

The A (3Pi1) State of ClF

The A(3Pi1) state of ClF is studied (1) in emission from the beta(1(3)P2) ion-pair state in a high-pressure discharge, (2) from its role in perturbations of the B(3Pi0(+)) and A'(3Pi2) states, and (3) in direct absorption from the X(1Sigma+) ground state. The last of these is obtained via a UV-labeling technique and represents the first observation of the A <-- X transition. The emission spectrum yields extensive assignments for the 0-4, 0-5, and 1-4 bands of beta --> A, with both e and f lines identified. The well-known perturbation in v = 7 of the B state is attributed to interaction with v = 9 of A. A newly identified perturbation in B(6) involves coupling with A(8). The known perturbation in B(8) may involve A(11), but other assignments cannot be ruled out. Approximate potential curves are derived for all three valence states and used to compute the vibrational factors for the perturbations, permitting extraction of the electronic coupling strengths. The B-A coupling elements are within approximately 10% of expectations for rotation-electronic coupling within a Hund's case (a) 3Pi manifold, but the strength of the perturbation between A(5) and A'(6) is only about 30% of predictions for this model. Copyright 1999 Academic Press.     

W-Boson Electric Dipole Moment Generated at the Two-Loop Level

We calculate the W-boson electric dipole moment in the Weinberg-Higgs model in which the Cp violation is mediated by charged Higgs boson exchange and compare our results with other works.     

The (1)(3)Pi Electronic State of LaF

Rotational studies of bands of the infrared systems (1)(3)Pi-->(1)(3)Delta and (1)(3)Pi(1)-->X(1)Sigma(+) of lanthanum monofluoride were carried out with the aim of characterizing the (1)(3)Pi state, assuming the previous representations of X(1)Sigma(+) and (1)(3)Delta (1-3). The vibrational levels of (1)(3)Pi involved in the analyzed transitions were v=0, 1, 2 of the Omega=0 component, v=0, 1 of the Omega=1 component, and v=0 of the Omega=2 component. Perturbations were observed in both systems which were ascribed to spin-uncoupling interactions between (1)(3)Pi(2)(v=0) and (1)(3)Pi(1)(v=1) levels. A 9x9 matrix representation at equilibrium of the complex of interacting levels (v=0, 1, 2) was constructed, each diagonal v-block corresponding to a triplet model of the rovibrational (3)Pi Hamiltonian. The wavenumbers of some 1910 lines in the two systems were simultaneously fitted (rms error of the fit of about 0.0053 cm(-1)), thus yielding a consistent set of accurate spectroscopic constants for the (1)(3)Pi state; the spin-uncoupling interaction parameter was determined as B(Pi)(0, 1)=0.010917(13) cm(-1). Copyright 2001 Academic Press.     

Electric Dipole Moment of W-boson Through Neutral Higga-Boson Exchange

We compute the electric dipole moment generated at two-loop for the W-boson in the Weinberg-Higgs model in which the CP violation is mediated by neutral Higgs-boson exchange. We also compare our results with the others relative to the problem in the literature     

Self-Rotation of Particles with a Photoinduced Electric Dipole Moment

Technical Physics - We consider the realization of rotation of particles with a photoinduced dipole moment in the absence of an external field source. The effects considered here are based on the...     

Improvement of the Spectroscopic Constants of the PF(A(3)Pi) State and Assignment of the PF(A-X) Transition Dipole Function

High-resolution laser-excitation spectra were acquired for the v'=3-7 levels of the PF(A(3)Pi(0,1,2)<--X(3)Sigma(-)) transition from PF(X(3)Sigma(-)) molecules generated in a discharge flow reactor. These results were combined with lower resolution excitation spectra for the v'=8-11 levels and with existing high-resolution data in the literature for v'=0 and 1 to assign improved spectroscopic constants for PF(A(3)Pi(0,1,2)). The abnormal vibrational energy level spacings for all spin components of the PF(A(3)Pi) state are evidence for a homogeneous interaction with another (3)Pi state. The Lambda-doublet separation in the PF((3)Pi(0)) substate increases with vibrational level, which is taken as evidence for interaction with the PF(b(1)Sigma(+)) state. Laser-induced fluorescence spectra from individual v'=0-5 levels were used to obtain vibrational band intensities of the A-X transition. The strong dependence of the transition dipole on the r-centroid is consistent with the reduction in the radiative lifetimes with increasing v' level. The similarity between the isovalent PF(A(3)Pi) and SO(A(3)Pi) states is noted and the bond dissociation energy of PF(X(3)Sigma(-)) is discussed. Copyright 2001 Academic Press.     

铯原子永久电偶极矩实验研究

圆柱形电容器中充铯蒸气,测量不同温度下电容量的变化,这变化与铯原子数度成正比。本实验得出铯原子永久电偶极矩edCs>2.4e×10-8cm。     

The Orientation of the Phosphorescence Dipole Moment of Erythrosine B Within Its Molecular Frame

For an unequivocal interpretation of time-resolved phosphorescence depolarization measurements on dye molecules in biophysical systems, the orientation of the transition dipole moments within the frame of the dye has to be known. The goal of this work is to find the orientation of the phosphorescence dipole moment of erythrosine B within its molecular frame. To this end, we first determine four difference angles, exciting a molecule in two of its absorption bands and measuring the fluorescence and phosphorescence anisotropy for each excitation wavelength. The next step is to position the transition dipole moments within the molecular frame, combining the results of angle-resolved fluorescence depolarization measurements with the measured difference angles. It is shown that the phosphorescence dipole moment is tilted out of the plane of the molecule. Additionally, we find that the phosphorescence dipole moment is located above the fluorescence dipole moment and not above the absorption dipole moment. This induces an extra difference angle between the absorption and the phosphorescence dipole moments which in the past has been interpreted erroneously as a larger tilt out of the plane of the molecule.     

Search for the Electric Dipole Moment of a Deuteron Using a Storage Ring

Physics of Atomic Nuclei - One of the alternatives to the Standard Model (SM) of elementary particles is the supersymmetry theories; the electric dipole moment (EDM) of elementary particles can...     

The Electric Dipole Moment of the CO2–CO van der Waals Complex

Radiofrequency transitions withinK= 2 asymmetry doublets have been observed for the CO₂–CO van der Waals complex. A Stark effect measurement on theJ= 2,K= 2 transition provides an electric dipole moment of μ = 0.2493(1) D. Combining this result with the permanent moment of CO, μ_CO= 0.1098 D, gives a change of moment on complex formation of Δμ = 0.140 D. The sign of Δμ is such that the CO end of the complex is more positive than CO₂. The origin of Δμ should not be attributed to any single mechanism, and several different contributions to Δμ are discussed.     

Submillimeter-Wave Spectroscopy of CO in the a(3)Pi State

Submillimeter-wave absorption spectrum of CO in electronically excited a(3)Pi state was observed in the 540-830 GHz region by using a phase-locked BWO spectrometer. New rotational transitions up to J = 9-8 in the vibrational excited states up to v = 5 were analyzed accompanied with previous observations in the RF and millimeter-wave regions. A multivibrational states fit among a' (3)Sigma(+) (v = 0-3) and a(3)Pi (v = 0-7) states was performed in order to analyze overall perturbation between the a(3)Pi and a' (3)Sigma(+) states. As a result, the deperturbed rotational parameters were derived precisely to improve the RKR potential. Copyright 2000 Academic Press.     

Dipole Moment Function of Hydrogen Halides

A new semi-empirical method for constructing the dipole moments of diatomic molecules as functions of the internuclear distance R $\varepsilon$ [0, ∞) is suggested. The dipole moment is described by a piecewise continuous function specified by a power-law polynomial with the asymptotic μ(R) → R ³ for small R, the dipole moment and its derivatives for equilibrium positions of nuclei in the molecule, and the results of ab initio calculations of the dipole moment for large R. The method is hydrogen halide molecules.     

High-Resolution Study of the BaI A(2)Pi Electronic State

Near-infrared and visible spectra of the A(2)Pi-X(2)Sigma(+), C(2)Pi(1/2)-A(2)Pi(1/2), C(2)Pi(1/2)-B(2)Sigma(+), and C(2)Pi(1/2)-X(2)Sigma(+) band systems of the BaI molecule were recorded by using Fourier transform spectroscopy (FTS). The spectra were produced from the chemiluminescent reaction Ba + I(2) and also by using laser-induced fluorescence (LIF) technique in which the laser sources were a Ti:sapphire single-mode laser, a dye single-mode laser, and a Kr(+) multimode ion laser. Resolved rotational data, originating from 19 vibrational levels (0 相似文献   

The Millimeter- and Submillimeter-Wave Spectrum and the Dipole Moment of Ethylenimine

The 0(0)(0) bands of the ?(2)B(2)-&Xtilde;(2)A(1) and &Btilde;(2)B(1)-&Xtilde;(2)A(1) systems of SrNH(2) were observed at Doppler-limited resolution using a Broida oven source and laser-induced fluorescence detection. A full rotational analysis of both transitions was performed including K(a) levels up to 5 and J levels up to 55. The &Btilde;(2)B(1) state was found to be extensively perturbed and only some of the subbands could be analyzed. The ?(2)B(2) and &Btilde;(2)B(1) states undergo a strong Coriolis-type interaction which results in extremely large spin-rotation splittings in both states, effectively splitting all levels with K(a)(') not equal 0 into two well-separated spin components. Copyright 2000 Academic Press.