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   https://doi.org/10.1103/PhysRevLett.130.212301  

   Aboona, B. E.; Adam, J.; Adams, J. R.; Agakishiev, G.; Aggarwal, I.; Aggarwal, M. M.; Ahammed, Z.; Aitbaev, A.; Alekseev, I.; Anderson, D. M.; et al (May 2023, Physical Review Letters)
2. Observation of $\mathrm{\Lambda }$ Hyperon Local Polarization in $p$ -Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=8.16\mathrm{TeV}$

   https://doi.org/10.1103/6ywq-gm61  

   Hayrapetyan, A; Tumasyan, A; Adam, W; Andrejkovic, J W; Benato, L; Bergauer, T; Chatterjee, S; Damanakis, K; Dragicevic, M; Hussain, P S; et al (September 2025, Physical Review Letters)

   The polarization of the $\mathrm{\Lambda }$and $\overline{\mathrm{\Lambda }}$hyperons along the beam direction has been measured in proton-lead ( $p\text{-Pb}$) collisions at a center-of-mass energy per nucleon pair of 8.16 TeV. The data were obtained with the CMS detector at the LHC and correspond to an integrated luminosity of $186.0\pm 6.5{\mathrm{nb}}^{-1}$. A significant azimuthal dependence of the hyperon polarization, characterized by the second-order Fourier sine coefficient $P_{z,\mathrm{s}2}$, is observed. The $P_{z,\mathrm{s}2}$values decrease as a function of charged particle multiplicity, but increase with transverse momentum. A hydrodynamic model that describes the observed $P_{z,\mathrm{s}2}$values in nucleus-nucleus collisions by introducing vorticity effects does not reproduce either the sign or the magnitude of the $p\text{-Pb}$results. These observations pose a challenge to the current theoretical implementation of spin polarization in heavy ion collisions and offer new insights into the origin of spin polarization in hadronic collisions at LHC energies. 

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3. Measurement of the Prompt $D^0$ Nuclear Modification Factor in $p\text{−}\mathrm{Pb}$ Collisions at $\sqrt{s_{NN}}=8.16\mathrm{TeV}$

   https://doi.org/10.1103/PhysRevLett.131.102301  

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4. Normal State ${}^{17}\mathrm{O}$ NMR Studies of ${\mathrm{Sr}}_2{\mathrm{RuO}}_4$ under Uniaxial Stress

   https://doi.org/10.1103/PhysRevX.9.021044  

   Luo, Yongkang; Pustogow, A.; Guzman, P.; Dioguardi, A. P.; Thomas, S. M.; Ronning, F.; Kikugawa, N.; Sokolov, D. A.; Jerzembeck, F.; Mackenzie, A. P.; et al (May 2019, Physical Review X)
5. First $\beta$ -Delayed Two-Neutron Spectroscopy of the $r$ -Process Nucleus ${}^{134}\mathrm{In}$ and Observation of the $i_{13/2}$ Single-Particle Neutron State in ${}^{133}\mathrm{Sn}$

   https://doi.org/10.1103/l24v-5m31  

   Dyszel, P; Grzywacz, R; Xu, Z Y; Kitamura, N; Karny, M; Korgul, A; Madurga, M; Neupane, S; Algora, A; Andreyev, A N; et al (October 2025, Physical Review Letters)

   This manuscript reports on the direct observation of a $\beta$-delayed two-neutron emission in a study of ${}^{134}\mathrm{In}$at the ISOLDE Decay Station using neutron spectroscopy. We also report on the first measurement in ${\beta }^{-}$decay of the long-sought $13/2^{+}$excited state in ${}^{133}\mathrm{Sn}$, attributed to be the neutron single-particle $i_{13/2}$orbital. The observation of sequential neutron emission is used to extract the relative population of the $i_{13/2}$state, which was found to be much smaller than the predictions of the statistical model. The experiment was possible because of the innovative use of a neutron array with neutron discrimination and interaction tracking capabilities. This is the first study of the details of the two-neutron emission for a nucleus, which belongs to the $r$-process path. Understanding $\beta$-delayed two-neutron emission probabilities is essential to validate models used in astrophysical $r$-process nucleosynthesis calculations. Observing two-neutron emissions in ${\beta }^{-}$decay paves the way for new experiments to study energy and angular correlations for $\beta$-delayed multineutron emitters. 

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