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1. ${\mathrm{\Lambda }}_c^{+}$ production in $pp$ and in $p$ -Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV

   https://doi.org/10.1103/PhysRevC.104.054905  

   Acharya, S.; Adamová, D.; Adler, A.; Adolfsson, J.; Aglieri Rinella, G.; Agnello, M.; Agrawal, N.; Ahammed, Z.; Ahmad, S.; Ahn, S. U.; et al (November 2021, Physical Review C)
2. Production of $\eta$ and ${\eta }^{\prime }$ mesons in $pp$ and $p\mathrm{Pb}$ collisions

   https://doi.org/10.1103/PhysRevC.109.024907  

   Aaij, R; Abdelmotteleb, A_S W; Abellan_Beteta, C; Abudinén, F; Ackernley, T; Adeva, B; Adinolfi, M; Adlarson, P; Agapopoulou, C; Aidala, C A; et al (February 2024, Physical Review C)

   The production of 𝜂 and 𝜂′ mesons is studied in proton-proton and proton-lead collisions collected with the LHCb detector. Proton-proton collisions are studied at center-of-mass energies of 5.02 and 13TeV and proton-lead collisions are studied at a center-of-mass energy per nucleon of 8.16TeV. The studies are performed in center-of-mass (c.m.) rapidity regions 2.5<𝑦c.m.<3.5 (forward rapidity) and −4.0<𝑦c.m.<−3.0 (backward rapidity) defined relative to the proton beam direction. The 𝜂 and 𝜂′ production cross sections are measured differentially as a function of transverse momentum for 1.5<𝑝T<10GeV and 3<𝑝T<10GeV, respectively. The differential cross sections are used to calculate nuclear modification factors. The nuclear modification factors for 𝜂 and 𝜂′ mesons agree at both forward and backward rapidity, showing no significant evidence of mass dependence. The differential cross sections of 𝜂 mesons are also used to calculate 𝜂/𝜋0 cross-section ratios, which show evidence of a deviation from the world average. These studies offer new constraints on mass-dependent nuclear effects in heavy-ion collisions, as well as 𝜂 and 𝜂′ meson fragmentation. 

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3. $\varphi$ meson production in $p+\mathrm{Al},$ $p+\mathrm{Au},$ $d+\mathrm{Au},$ and ${}^3\mathrm{He}+\mathrm{Au}$ collisions at $\sqrt{s_{NN}}=200\mathrm{GeV}$

   https://doi.org/10.1103/PhysRevC.106.014908  

   Acharya, U.; Adare, A.; Aidala, C.; Ajitanand, N. N.; Akiba, Y.; Alfred, M.; Andrieux, V.; Apadula, N.; Asano, H.; Azmoun, B.; et al (July 2022, Physical Review C)
4. Measurement of $\varphi$ -meson production in $\mathrm{Cu}+\mathrm{Au}$ collisions at $\sqrt{s_{NN}}=200$ GeV and $\mathrm{U}+\mathrm{U}$ collisions at $\sqrt{s_{NN}}=193$ GeV

   https://doi.org/10.1103/PhysRevC.107.014907  

   Abdulameer, N. J.; Acharya, U.; Aidala, C.; Ajitanand, N. N.; Akiba, Y.; Akimoto, R.; Alexander, J.; Alfred, M.; Alibordi, M.; Aoki, K.; et al (January 2023, Physical Review C)
5. Measurement of $\omega$ meson production in $pp$ and $p$ -Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV

   https://doi.org/10.1103/ls6w-x1bb  

   Acharya, S; Agarwal, A; Aglieri_Rinella, G; Aglietta, L; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, S U; Ahuja, I; et al (October 2025, Physical Review C)

   We present the measurement of the $p_{\mathrm{T}}$ -differential production cross section of $\omega$ mesons in and $p$ -Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV at midrapidity by ALICE. In addition, the first measurement of the nuclear modification factor $R_{p\mathrm{Pb}}$ for $\omega$ mesons at LHC energies is presented, complementing the existing measurements of lighter neutral mesons such as the ${\pi }^0$ and $\eta$ . Within the measured $p_{\mathrm{T}}$ range, the $R_{p\mathrm{Pb}}$ of $\omega$ mesons is compatible with no cold nuclear matter effects within the uncertainties, consistent with previous measurements at lower energies. The $\omega /{\pi }^0$ ratio is presented for both collision systems, showing no collision system dependence within the uncertainties. The comparison to previously published $\omega /{\pi }^0$ ratios at lower and higher collision energies in collisions suggests a decreasing trend of the ratio above $p_{\mathrm{T}}$ = 4 GeV/ $c$ with increasing collision energy. The data in both collision systems are compared to predictions from PYTHIA 8, EPOS LHC, and DPMJET event generators, revealing significant shortcomings in these models’ ability to describe the production of $\omega$ mesons. 

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