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V. V. Nahorna

Publications and source records attributed to V. V. Nahorna.

3 recordsLinked to original sources

Electron spectral shape of the third-forbidden $β$-decay of $^{87}$Rb measured using a Rb$_2$ZrCl$_6$ crystal scintillator

In recent years, interest in experimental studies of $β$-decay electron spectra -- often referred to as $β$ spectra -- has been growing. This is particularly true for $β$ transitions where the electron spectra are sensitive to the effective value of the weak axial coupling, $g_{\rm A}$. Such measurements serve as important benchmarks for nuclear physics calculations and can also be used to characterize background in astroparticle physics experiments. In this work, a dedicated experiment has been carried out to investigate the spectral shape of the third-forbidden $^{87}$Rb $β$-decays, with the goal of estimating the effective $g_{\rm A}$ value for this transition and of deriving the T$_{1/2}$ value. This was done by comparing the experimental spectral shape with the estimates from various phenomenological models. The $^{87}$Rb source was embedded directly within the detector material of a new Rb$_2$ZrCl$_6$ crystal scintillator; the data taking was performed deep underground at Gran Sasso National Laboratory. The obtained experimental half-life value for the studied process is T$_{1/2} = 5.08(13) \times$ 10$^{10}$ yr; while a $g_{\rm A}$ value in the range 0.4 to 0.6 is obtained when accounting for uncertainties and depending on the model adopted as discussed in detail in the text.

nucl-ex↗

Scintillating properties of Cs${_2}$ZrCl${_6}$ crystals in the temperature range of 5-300 K

A new comprehensive study on the Cs${_2}$ZrCl${_6}$ (CZC) crystal scintillating properties under different types of irradiation was performed over a wide temperature range from 5 to 300 K. The light yield (LY) at room temperature (RT), measured under irradiation by 662 keV $γ$ quanta of $^{137}$Cs, was evaluated to be 53,300 $\pm$ 4,700 photons/MeV corresponding to approximately 71% of its estimated absolute value. The maximum light emission was observed in the temperature interval 135-165 K, where the LY reached 56,900 photons/MeV and 19,700 photons/MeV for $γ$ quanta and $α$ particles, respectively. The quenching factor (QF) for $α$ particles increases smoothly from QF = 0.30 at RT to QF = 0.36 at 135 K. The shape of scintillation pulses induced by $α$ particles is characterized by three time-constants (0.3, 2.5 and 11.8 $μ$s at RT), whereas the average pulse of $γ$ induced events is characterized by two time-constants (1.3 and 11.5 $μ$s at RT). At the same time, scintillating properties and pulse-shape discrimination capability of the CZC exhibit an acute deterioration at temperatures below 135 K. The optimal operating conditions to maximize the scintillating performance of undoped CZC crystals are discussed.

physics.ins-det↗

Luminescence of the Cs2ZrCl6 under high pressure

The luminescence and Raman spectra of the Cs2ZrCl6 crystal in a wide range of pressures were studied in this work for the first time. Luminescence measurements were performed up to 10 GPa, while the Raman spectra were measured up to 20 GPa. The luminescence data revealed a linear blue shift of the emission maximum from about 2.5 eV at ambient pressure to 3.1 eV at 5 GPa and a strong intensity quenching. The indirect-to-direct bandgap transition at about 5 GPa, a phenomenon previously predicted only theoretically, was used to explain the strong quenching of the luminescence. This model was confirmed by fitting luminescence intensity data and analysis of the luminescence decay kinetics, which exhibited a shortening of the pulse decay time with the pressure increase. Raman spectra confirmed the stability of Cs2ZrCl6 up to 20 GPa and showed no evidence of the pressure-induced structural phase transitions. An energetic scheme of excitonic levels, which takes into account the indirect-to-direct band gasp transition, was proposed to explain the rapid luminescence quenching with increasing pressure.

cond-mat.mtrl-sci↗