Journal articles: 'Electric Dipole Moment of the electron'

1

Leigh, R. G., S. Paban, and R. M. Xu. "Electric dipole moment of electron." Nuclear Physics B 352, no. 1 (March 1991): 45–58. http://dx.doi.org/10.1016/0550-3213(91)90128-k.

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2

Bernreuther, Werner, and Mahiko Suzuki. "The electric dipole moment of the electron." Reviews of Modern Physics 63, no. 2 (April 1, 1991): 313–40. http://dx.doi.org/10.1103/revmodphys.63.313.

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3

Ayazi, Seyed Yaser, and Yasaman Farzan. "Electron electric dipole moment from Lepton Flavor Violation." Journal of High Energy Physics 2007, no. 06 (June 4, 2007): 013. http://dx.doi.org/10.1088/1126-6708/2007/06/013.

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4

Bernreuther, Werner, and Mahiko Suzuki. "Erratum: The electric dipole moment of the electron." Reviews of Modern Physics 64, no. 2 (April 1, 1992): 633. http://dx.doi.org/10.1103/revmodphys.64.633.

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5

GOULD, HARVEY. "ELECTRON ELECTRIC DIPOLE MOMENT EXPERIMENT WITH SLOW ATOMS." International Journal of Modern Physics D 16, no. 12b (December 2007): 2337–42. http://dx.doi.org/10.1142/s0218271807011395.

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Discovering an electron electric dipole moment (e-EDM) would uncover new physics requiring an extension of the Standard Model. e-EDMs, large enough to be discovered by new experiments are now common predictions in extensions of the Standard Model, including extensions that describe baryogenesis, dark matter, and neutrino mass. A cesium slow-atom e-EDM experiment (which is similar to an atomic clock) can improve the sensitivity to the e-EDM. And, as with an atomic clock, it could be more sensitive in microgravity than on Earth. As a first step an Earth-based demonstration Cs fountain e-EDM experiment has been carried out at LBNL.

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6

Choi, Kiwoon, and Jooyoo Hong. "Electron electric dipole moment and θ>QCD." Physics Letters B 259, no. 3 (April 1991): 340–44. http://dx.doi.org/10.1016/0370-2693(91)90838-h.

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7

Lindroth, E., B. W. Lynn, and P. G. H. Sandars. "Order α2theory of the atomic electric dipole moment due to an electric dipole moment on the electron." Journal of Physics B: Atomic, Molecular and Optical Physics 22, no. 4 (February 28, 1989): 559–76. http://dx.doi.org/10.1088/0953-4075/22/4/004.

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8

Heo, Jae Ho, and Wai-Yee Keung. "Electron electric dipole moment induced by octet-colored scalars." Physics Letters B 661, no. 4 (March 2008): 259–62. http://dx.doi.org/10.1016/j.physletb.2008.02.021.

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9

Ibrahim, Tarek, and Pran Nath. "Neutron and electron electric dipole moment inN=1supergravity unification." Physical Review D 57, no. 1 (January 1, 1998): 478–88. http://dx.doi.org/10.1103/physrevd.57.478.

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10

Abdullah, K., C. Carlberg, E. D. Commins, Harvey Gould, and Stephen B. Ross. "New experimental limit on the electron electric dipole moment." Physical Review Letters 65, no. 19 (November 5, 1990): 2347–50. http://dx.doi.org/10.1103/physrevlett.65.2347.

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11

Frank, M. "Doubly Charged Higgsinos and the EDM of the Electron." Modern Physics Letters A 12, no. 40 (December 28, 1997): 3131–37. http://dx.doi.org/10.1142/s0217732397003241.

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We study the contribution of the doubly charged higgsino to the electric dipole moment of the electron in a left–right extension of the standard supersymmetric model. The CP violation comes from the trilinear scalar interaction terms in the selectron mixing matrix. We find that this contribution can be quite large, of the same order of magnitude as the electric dipole moment of the electron in the MSSM, and reachable by future experiments.

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12

MUKHOPADHYAYA, BISWARUP, and SATYANANAYAN NANDI. "GAUGE SINGLETS AND THE DIPOLE MOMENT OF THE ELECTRON." Modern Physics Letters A 05, no. 27 (October 30, 1990): 2267–70. http://dx.doi.org/10.1142/s0217732390002596.

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It is shown that models containing both SU(2) singlet fermions and a singlet Higgs have interesting effects on the electric dipole moment of the electron. Unlike the neutron dipole moment, there is no QCD suppression in this case. It is thus possible to find useful constraints on models that include both these kinds of singlets.

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13

Петров, А. Н., and Л. В. Скрипников. "Интерференция между E1- и M1-амплитудами перехода из состояния H в C молекулы ThO." Журнал технической физики 126, no. 4 (2019): 414. http://dx.doi.org/10.21883/os.2019.04.47508.346-18.

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AbstractThe systematic error in experiments concerning searching for the electric dipole moment of an electron due to the Stark interference between the E 1 and M 1 amplitudes of the transition from the $${{H}^{3}}{{\Delta }_{1}}$$ state to $${{C}^{1}}\Pi $$ of a ThO molecule has been calculated. The calculations show that the error is about three orders of magnitude lower than the current limitation on the electric dipole moment of electron.

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14

Mosyagin, N. S., M. G. Kozlov, and A. V. Titov. "Electric dipole moment of the electron in the YbF molecule." Journal of Physics B: Atomic, Molecular and Optical Physics 31, no. 19 (October 14, 1998): L763—L767. http://dx.doi.org/10.1088/0953-4075/31/19/002.

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15

Liu, Jiang. "Electric dipole moment of the electron in left-right models." Nuclear Physics B 271, no. 3-4 (January 1986): 531–39. http://dx.doi.org/10.1016/s0550-3213(86)80024-4.

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16

Fleig, Timo, and Malaya K. Nayak. "Electron electric dipole moment and hyperfine interaction constants for ThO." Journal of Molecular Spectroscopy 300 (June 2014): 16–21. http://dx.doi.org/10.1016/j.jms.2014.03.017.

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17

Bowser-Chao, David, Darwin Chang, and Wai-Yee Keung. "Electron Electric Dipole Moment fromCPViolation in the Charged Higgs Sector." Physical Review Letters 79, no. 11 (September 15, 1997): 1988–91. http://dx.doi.org/10.1103/physrevlett.79.1988.

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18

Murthy, S. A., D. Krause, Z. L. Li, and L. R. Hunter. "New limits on the electron electric dipole moment from cesium." Physical Review Letters 63, no. 9 (August 28, 1989): 965–68. http://dx.doi.org/10.1103/physrevlett.63.965.

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19

Barr, S. M., and A. Zee. "Electric dipole moment of the electron and of the neutron." Physical Review Letters 65, no. 1 (July 2, 1990): 21–24. http://dx.doi.org/10.1103/physrevlett.65.21.

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20

Barr, S. M., and A. Zee. "Electric Dipole Moment of the Electron and of the Neutron." Physical Review Letters 65, no. 23 (December 3, 1990): 2920. http://dx.doi.org/10.1103/physrevlett.65.2920.

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21

Fabbrichesi, Marco, Paul M. Fishbane, and Richard E. Norton. "Heavy leptons and the electric dipole moment of the electron." Physical Review D 37, no. 7 (April 1, 1988): 1942–49. http://dx.doi.org/10.1103/physrevd.37.1942.

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22

Chang, D., W. Y. Keung, and T. C. Yuan. "Two-loop bosonic contribution to the electron electric dipole moment." Physical Review D 43, no. 1 (January 1, 1991): R14—R16. http://dx.doi.org/10.1103/physrevd.43.r14.

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23

Zee, A. "Electric Dipole Moment of the Electron andCPNonconservation in Muon Decay." Physical Review Letters 55, no. 22 (November 25, 1985): 2382–85. http://dx.doi.org/10.1103/physrevlett.55.2382.

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24

DZUBA, V. A., and V. V. FLAMBAUM. "PARITY VIOLATION AND ELECTRIC DIPOLE MOMENTS IN ATOMS AND MOLECULES." International Journal of Modern Physics E 21, no. 11 (November 2012): 1230010. http://dx.doi.org/10.1142/s021830131230010x.

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We review the current status of the study of parity and time invariance violation in atoms, nuclei and molecules. We focus on parity nonconservation (PNC) in cesium (CS) and three of the most promising areas of research: (i) PNC in a chain of isotopes, (ii) search for nuclear anapole moments, and (iii) search for permanent electric dipole moments (EDMs) of atoms and molecules, which in turn are caused by either an electron EDM or nuclear T, P-odd moments such as a nuclear EDM or nuclear Schiff moment.

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25

Maroulis, George. "Electrical Properties for HCO+ and NNH+ from Fourth-Order Møller-Plesset Perturbation Theory." Zeitschrift für Naturforschung A 43, no. 5 (May 1, 1988): 419–29. http://dx.doi.org/10.1515/zna-1988-0505.

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Electric multipole moments and static polarizabilities are reported for HCO+ and NNH+ . Both molecular ions are of great importance to interstellar matter chemistry. All properties were calculated from the energy of the molecule in the presence of distant electric charges. Electron correlation effects were taken into account via SDQ-MPPT(4), fourth-order Møller-Plesset Perturbation Theory with single, double and quadrupole substitutions from the reference SCF wavefunction. With the exception of the dipole moment, values for the other properties studied in this work appear in the literature for the first time. The dipole moment (relative to the centre of mass) and the axial and perpendicular components of the dipole polarizability are 1.515 ea0, 13.39 and 6.88 e2a2Eh+1 respectively for HCO+ and 1.328 ea0, 13.81 and 5.70 e2a20Eh-1 for NNH+ .

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26

Chubukov, Dmitry V., Leonid V. Skripnikov, Vasily N. Kutuzov, Sergey D. Chekhovskoi, and Leonti N. Labzowsky. "Optical Rotation Approach to Search for the Electric Dipole Moment of the Electron." Atoms 7, no. 2 (June 7, 2019): 56. http://dx.doi.org/10.3390/atoms7020056.

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The P , T -odd Faraday effect (i.e., rotation of the polarization plane of light propagating through a medium in presence of the external electric field due to P , T symmetry violating interactions) is considered for several atomic species: Ra, Pb, Tl, Hg, Cs, and Xe. Corresponding theoretical simulation of P , T -odd Faraday experiment, with already achieved intracavity absorption spectroscopy characteristics and parameters, is performed. The results show that the magnetic dipole transitions in the Tl and Pb atoms as well as the electric dipole transitions in the Ra, Hg and Cs atoms are favorable for the observation of the P , T -odd Faraday optical rotation. The estimation of the rotation angle of the light polarization plane demonstrates that recently existing boundaries for the electron electric dipole moment can be improved by one-two orders of magnitude.

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27

Binh, D. T., Vo Van On, and H. N. Long. "Bounds on dipole moments of tau-neutrino from single photon searches in SU(4)L × U(1)X model at CLIC and ILC energies." International Journal of Modern Physics A 34, no. 11 (April 20, 2019): 1950062. http://dx.doi.org/10.1142/s0217751x19500623.

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We investigate the dipole moments of the tau-neutrino at high-energy and high luminosity at linear electron–positron colliders, such as CLIC or ILC through the analysis of the reaction [Formula: see text] in the framework of the [Formula: see text] model. The limits on dipole moment were obtained for integrated luminosity of [Formula: see text] and mass ranging from 0.25 to 1.0 TeV. The estimated limits for the tau-neutrino magnetic and electric dipole moments at 95% of confidence level are [Formula: see text] and [Formula: see text] improved by 2–3 orders of magnitude compared to L3 and complement previous studies on the dipole moments.

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28

Talman, Richard. "Prospects for Electric Dipole Moment Measurement Using Electrostatic Accelerators." Reviews of Accelerator Science and Technology 10, no. 01 (August 2019): 267–301. http://dx.doi.org/10.1142/s1793626819300147.

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Electrostatic accelerators have played a glorious role in physics, especially for low energy atomic and nuclear physics and electron microscopy. But circular accelerators have depended almost exclusively on the far greater bending force possible with static magnetic, rather than electric, fields. There is a potential exception to this magnetic bending monopoly for experimental high energy elementary particle physics — it is the possibility of measuring the electric dipole moments (EDMs) of charged elementary particles, such as proton, deuteron, or electron, using an electrostatic storage ring. Any such non-zero EDM would demonstrate violation of both parity (P) and time-reversal (T) invariance. One way of understanding the preponderance of matter over anti-matter in the present-day universe pre-supposes the existence of violations of P and T substantially greater than are allowed by the “standard model” of elementary particle physics. This provides the leading motivation for measuring EDMs. Currently, only upper limits are known for these EDMs. The very same smallness that makes it important to determine them makes their measurement difficult. Accepting as obvious the particle physics motivation, this paper concentrates on the accelerator physics of the (not very) high energy electrostatic accelerators needed for EDM measurements. Developments already completed are emphasized. Impressive advances have been made in the diagnostic tools, spin control and polarimetry that will make EDM measurement possible. Ring design for minimizing spin decoherence and limiting systematic EDM errors is presented. There have, however, been worrisome indications from low energy rings, concerning beam current limitations. A prototype ring design is proposed for investigating and addressing this concern.

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29

Augenbraun, Benjamin L., Zack D. Lasner, Alexander Frenett, Hiromitsu Sawaoka, Calder Miller, Timothy C. Steimle, and John M. Doyle. "Laser-cooled polyatomic molecules for improved electron electric dipole moment searches." New Journal of Physics 22, no. 2 (February 19, 2020): 022003. http://dx.doi.org/10.1088/1367-2630/ab687b.

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30

Commins, Eugene D., Stephen B. Ross, David DeMille, and B. C. Regan. "Improved experimental limit on the electric dipole moment of the electron." Physical Review A 50, no. 4 (October 1, 1994): 2960–77. http://dx.doi.org/10.1103/physreva.50.2960.

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31

Ettefaghi, M. M., and Z. Zeinali. "Screening of electron electric dipole moment through the Foldy-Wouthuysen representation." Iranian Journal of Physics Research 15, no. 1 (July 1, 2015): 53–62. http://dx.doi.org/10.18869/acadpub.ijpr.15.1.53.

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32

Nieves, José F., Darwin Chang, and Palash B. Pal. "Electric dipole moment of the electron in left-right-symmetric theories." Physical Review D 33, no. 11 (June 1, 1986): 3324–28. http://dx.doi.org/10.1103/physrevd.33.3324.

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33

Kobayashi, M., T. Kugo, and T. Tokunaga. "Electric Dipole Moments of Dyon and 'Electron'." Progress of Theoretical Physics 118, no. 5 (November 1, 2007): 921–34. http://dx.doi.org/10.1143/ptp.118.921.

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34

NG, DANIEL, and JOHN N. NG. "A NOTE ON MAJORANA NEUTRINOS, LEPTONIC CKM AND ELECTRON ELECTRIC DIPOLE MOMENT." Modern Physics Letters A 11, no. 03 (January 30, 1996): 211–16. http://dx.doi.org/10.1142/s0217732396000254.

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The electric dipole moment of the electron, de, is known to vanish up to three-loop in the standard model with massless neutrinos. However, if neutrinos are massive Majorana particles, we obtain the result that de induced by leptonic CKM mechanism is nonvanishing at two-loop order, and it applies to all massive Majorana neutrino models.

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35

Spackman, M. A., and P. G. Byrom. "Molecular electric moments and electric field gradients from X-ray diffraction data: model studies." Acta Crystallographica Section B Structural Science 52, no. 6 (December 1, 1996): 1023–35. http://dx.doi.org/10.1107/s0108768196008294.

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Model X-ray data sets, with and without the inclusion of experimental thermal motion parameters, have been computed via Fourier transformation of ab initio molecular electron densities for 12 different molecular crystals. These datasets were then analysed with three different multipole models of varying sophistication and, from the multipole functions, molecular dipole and second moments, as well as electric field gradients (EFG's), at each nuclear site were computed and compared with results obtained from the original ab initio wavefunctions. The results provide valuable insight into the reliability of these properties, extracted in the same way from experimental X-ray data. Not all molecular systems display identical trends, but a general pattern is discernible. Specifically, dipole moments are typically underestimated by a small but significant amount (~ 10–15%), the trace of the second moment tensor is well determined but overestimated by a few per cent and electric field gradients at protons are confirmed to be well within reach of a careful charge density analysis of X-ray diffraction data.

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36

Garcia, L. F., W. Gutiérrez, and I. D. Mikhailov. "One-Electron Conical Nanotube in External Electric and Magnetic Fields." Journal of Nanomaterials 2017 (2017): 1–12. http://dx.doi.org/10.1155/2017/5658796.

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The effects of variation of the aperture angle on spectral and magnetic properties of one-electron nanotube of the axially symmetrical conical shape in the presence of the electric and magnetic fields have been investigated based on a numerical solution of the Schrödinger equation in the effective mass approximation. We show that the energy spectrum and the magnetic dipole moment of the structure are changed dramatically with increase of the cone’s aperture angle due to the interplay between the diamagnetic and centrifugal forces, which push the electron at opposite directions. Particularly, the energy levels close to the ground state become quasi-degenerate, owing to a change of the hidden symmetry, induced by the magnetic field in this structure, when its morphology is converted from the cylindrical type to the conical one and the Aharonov-Bohm oscillations of the ground state energy and of the magnetic dipole moment are quenched. We found additionally that any weak electric field breaks this hidden symmetry, splits quasi-degenerate state, and restores the Aharonov-Bohm oscillations.

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37

Howard, S. T., J. P. Foreman, and P. G. Edwards. "Substituent effects on basicity in Group 15 compounds: an analysis based on proton affinities, charge distributions, and dipole polarizabilities." Canadian Journal of Chemistry 75, no. 1 (January 1, 1997): 60–67. http://dx.doi.org/10.1139/v97-009.

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Ab initio calculations on a series of trisubstituted amines, phosphines, and arsines are presented at the MP2/6-311G(d,p) level. Specifically, the species studied are XH3, XF3, and X(Me)3, where X = N, P, or As. The influence of the substituents on the proton affinity is analyzed in terms of the charge distribution, its topology, some one-electron properties (dipole moments, electric field gradients), and dipole polarizabilities. An atoms-in-molecules. decomposition of the charge distribution, energetics, and polarizabilities also proves informative. There seems to be no straightforward way of rationalizing the basicities of these compounds on the basis of electrostatic properties (i.e., properties of the charge distribution in the unprotonated bases). However, substituent effects on basicities can be correlated with response properties, such as the molecular (and atoms-in-molecules) polarizability tensors, and the amount of charge that a substituent group or atom donates on protonation. Key words: quantum chemistry, proton affinity, electron density, lone pairs, polarizability, basicity, dipole moment, electric field gradient.

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38

Medveď, Miroslav, Ivan Černušák, Stanislav Kedžuch, and Jozef Noga. "Electric Properties of Cyanoborane Isomers." Collection of Czechoslovak Chemical Communications 70, no. 8 (2005): 1055–81. http://dx.doi.org/10.1135/cccc20051055.

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Cyanoborane isomers and their acyclic and cyclic oligomers serve as useful models for studying properties of molecules with alternating electron-rich and electron-deficient groups. Static electric properties including electronic dipole moment, polarizability, first and second hyperpolarizabilities of three stable isomeric monomers - boranylmethanenitrile, borazirene and 1-(methanylidyne)borazan-1-ium-2-ide - have been calculated at the MP2, CCSD and CCSD(T) levels using various basis sets. In addition, frequency-dependent (hyper)- polarizabilities of the most stable isomer have been evaluated via the CCSD response theory.

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39

Kawski, A., D. Gloyna, P. Bojarski, J. Czajko, and J. Gadomska-Lichacz. "The Effect of ω-Substituted Acceptors in 4-Dimethylamino-trans-Styrenes on the Polarity in the Ground and Excited Singlet State." Zeitschrift für Naturforschung A 45, no. 11-12 (December 1, 1990): 1230–34. http://dx.doi.org/10.1515/zna-1990-11-1202.

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ABSTRACTThe electric dipole moment in the ground (μg) and in the first excited singlet state (μe) of co-substituted acceptors in 4-dimethylamino-trans-styrenes (Z = P(S)Ph2 , P(O)Ph2 , SO2CH3 ) were determined by solvatochromic and thermochromic methods. The obtained values of μe and μg and the values for Z = CN and Z = NO 2 known from the literature [2] fulfill the linear relation between the dipole moments (μe or μg and the Hammett constants σp of the substituents. On pincreasing the electron-acceptor power of Z, μe grows faster than μg

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40

Sauer, B. E., J. J. Hudson, D. M. Kara, I. J. Smallman, M. R. Tarbutt, and E. A. Hinds. "Prospects for the measurement of the electron electric dipole moment using YbF." Physics Procedia 17 (2011): 175–80. http://dx.doi.org/10.1016/j.phpro.2011.06.034.

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41

Kim, Y. J., C.-Y. Liu, S. K. Lamoreaux, and G. Reddy. "Experimental search for the electron Electric Dipole Moment using solid state techniques." Journal of Physics: Conference Series 312, no. 10 (September 23, 2011): 102009. http://dx.doi.org/10.1088/1742-6596/312/10/102009.

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42

Bijlsma, M., B. J. Verhaar, and D. J. Heinzen. "Role of collisions in the search for an electron electric-dipole moment." Physical Review A 49, no. 6 (June 1, 1994): R4285—R4288. http://dx.doi.org/10.1103/physreva.49.r4285.

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43

Skripnikov, L. V., A. N. Petrov, and A. V. Titov. "Communication: Theoretical study of ThO for the electron electric dipole moment search." Journal of Chemical Physics 139, no. 22 (December 14, 2013): 221103. http://dx.doi.org/10.1063/1.4843955.

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44

Nataraj, H. S., B. K. Sahoo, B. P. Das, R. K. Chaudhuri, and D. Mukherjee. "The electron electric dipole moment enhancement factors of Rubidium and Caesium atoms." Journal of Physics: Conference Series 80 (September 1, 2007): 012050. http://dx.doi.org/10.1088/1742-6596/80/1/012050.

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45

Nath, Pran. "CPviolation via electroweak gauginos and the electric dipole moment of the electron." Physical Review Letters 66, no. 20 (May 20, 1991): 2565–68. http://dx.doi.org/10.1103/physrevlett.66.2565.

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46

Vutha, A. C., W. C. Campbell, Y. V. Gurevich, N. R. Hutzler, M. Parsons, D. Patterson, E. Petrik, et al. "Search for the electric dipole moment of the electron with thorium monoxide." Journal of Physics B: Atomic, Molecular and Optical Physics 44, no. 7 (March 14, 2011): 079803. http://dx.doi.org/10.1088/0953-4075/44/7/079803.

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47

Vutha, A. C., W. C. Campbell, Y. V. Gurevich, N. R. Hutzler, M. Parsons, D. Patterson, E. Petrik, et al. "Search for the electric dipole moment of the electron with thorium monoxide." Journal of Physics B: Atomic, Molecular and Optical Physics 43, no. 7 (March 19, 2010): 074007. http://dx.doi.org/10.1088/0953-4075/43/7/074007.

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48

Gunion, J. F., and R. Vega. "The electron electric dipole moment for a CP-violating neutral Higgs sector." Physics Letters B 251, no. 1 (November 1990): 157–62. http://dx.doi.org/10.1016/0370-2693(90)90246-3.

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49

Hoogeveen, F. "The standard model prediction for the electric dipole moment of the electron." Nuclear Physics B 341, no. 2 (September 1990): 322–40. http://dx.doi.org/10.1016/0550-3213(90)90182-d.

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50

Kao, Chung, and Rui-Ming Xu. "Charged-Higgs-loop contribution to the electric dipole moment of the electron." Physics Letters B 296, no. 3-4 (December 1992): 435–39. http://dx.doi.org/10.1016/0370-2693(92)91345-a.

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Journal articles on the topic 'Electric Dipole Moment of the electron'

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