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- W1991867785 abstract "We present a detailed description of new observations of parity nonconservation in the ${6}^{2}$${P}_{1/2}$ensuremath{rightarrow}${7}^{2}$${P}_{1/2}$ transition (293 nm) in atomic $_{{mathrm{}}^{2}{mathrm{}}_{81}^{05}}mathrm{Tl}$. Linearly polarized 293-nm photons, polarization ensuremath{varepsilon}^, are absorbed by ${6}^{2}$${P}_{1/2}$ atoms in crossed E and B fields. The transition probability for each Zeeman component contains a pseudoscalar term, proportional to ensuremath{varepsilon}^ensuremath{cdot}Bensuremath{varepsilon}^ensuremath{cdot}Eifmmodetimeselsetexttimesfi{}B, arising from interference between the parity-nonconserving E1 amplitude ${mathrm{scrE}}_{P}$ and the Stark E1 amplitude ensuremath{beta}E. This is detected by observation of fluorescence at 535 nm accompanying the decay ${(7}^{2}$${P}_{1/2}$ensuremath{rightarrow}) ${7}^{2}$${S}_{1/2}$ensuremath{rightarrow}${6}^{2}$${P}_{3/2}$. Systematic corrections, due to imperfect linear polarization and misaligned E and B fields, are determined precisely by auxiliary experiments and found to be small. Our final result: Im[${mathrm{scrE}}_{P/ensuremath{beta}}$]${ensuremath{Vert}}_{mathrm{expt}}$=-(1.73ifmmodepmelsetextpmfi{}0 .26ifmmodepmelsetextpmfi{}0.07) mV/cm, where the first uncertainty is statistical, and the second is systematic, is compared with results of other experiments and with theoretical estimates based on the standard SU(2)ifmmodetimeselsetexttimesfi{}U(1) electroweak model." @default.
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- W1991867785 date "1985-10-01" @default.
- W1991867785 modified "2023-09-27" @default.
- W1991867785 title "Parity nonconservation in atomic thallium" @default.
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- W1991867785 doi "https://doi.org/10.1103/physreva.32.2196" @default.
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