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Quantum Beats In The 3γ Annihilation Decay Of Positronium Observed By Perturbed Angular Distribution

机译:扰动角分布观察到的正电子3γni没衰变中的量子拍

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We have applied conventional Time Differential Perturbed Angular Correlation (TDPAC) method to observe the anisotropy oscillations in the 3γ annihilation decay of polarized Positronium in a weak magnetic field. The effect, as predicted theoretically and experimentally demonstrated by Barishevsky et al. [V.G. Barishevsky, O.N. Metelitsa, V.V. Tikhomirov, Oscillations of the positronium decay γ-quantum angular distribution in a magnetic field, J. Phys. B: At. Mol. Opt. Phys.22 (1989) 2835], is induced by the coherent admixture of the m = 0 states of ortho-Positronium (o-Ps) and para-Positronium (p-Ps) in interaction with the magnetic field. The following experimental characteristics are to be considered: (i) the oscillation frequency corresponds to the difference in energy of the Ps atom levels in magnetic field and is proportional with H~2; (ii) in a fixed geometry the modulation depth (oscillations amplitude) depends on the mean positron polarization; (iii) privileged angles of the polarization vector, magnetic field and detectors are required for optimizing the observed oscillations amplitude. The normalized difference spectrum function (R(t)) obtained from time spectra measured in vacuum and in different gaseous atmospheres (Ar, H_2, N_2) have the oscillations amplitude constant and we conclude that the Ps atoms are not fully thermalized over a time interval of about 400 ns. The R(t) functions obtained for o-Ps annihilation decays, in dry air or Ar-O mixture, have the oscillations amplitude time dependent due. probably, to the paramagnetism of the Oxygen molecules.
机译:我们已经应用常规的时间微分扰动角相关(TDPAC)方法来观察弱磁场中极化正电子的3γni没衰减的各向异性振荡。正如Barishevsky等人在理论上和实验上所预测的那样,这种效果。 [V.G.俄亥俄州巴里舍夫斯基梅特利察(V.V.)蒂霍米罗夫(Tikhomirov),posit在磁场中的振荡,γ量子角分布,J。Phys。 B:在。大声笑选择。 Phys.22(1989)2835],是由于正正电子(o-Ps)和对正电子(p-Ps)的m = 0状态与磁场相互作用的相干混合而引起的。应考虑以下实验特性:(i)振荡频率对应于磁场中Ps原子能级的能量差,并且与H〜2成比例; (ii)在固定的几何形状中,调制深度(振荡幅度)取决于平均正电子极化; (iii)极化矢量,磁场和检测器的特权角是优化观察到的振荡幅度所必需的。从在真空中和在不同气态大气(Ar,H_2,N_2)中测量的时间谱获得的归一化差异谱函数(R(t))具有振荡振幅常数,我们得出结论,Ps原子在一个时间间隔内未完全热化约400 ns。在干燥空气或Ar-O混合物中,o-Ps hil灭衰减所获得的R(t)函数具有随时间变化的振幅幅度。可能是氧气分子的顺磁性。

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