在LHC上用ALICE探测器测量了$\sqrt{s}$ = 7 TeV质子-质子碰撞中中的中快度（$\left | y \right |<0.5$）奇异和双奇异重子共振（$Σ(1385)^{\pm}$，$Ξ(1530)^{0}$）的产生.横向动量谱的非弹性碰撞相比，QCD启发的模型，在一般underpredict的数据。对在$Ξπ$通道中衰变的$ϕ(1860)$五夸克的搜索已经进行，但没有看到任何证据。
英文摘要：
The production of the strange and double-strange baryon resonances ($Σ(1385)^{\pm}$, $Ξ(1530)^{0}$) has been measured at mid-rapidity ($\left | y \right |<0.5$) in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ALICE detector at the LHC. Transverse momentum spectra for inelastic collisions are compared to QCD-inspired models, which in general underpredict the data. A search for the $ϕ(1860)$ pentaquark, decaying in the $Ξπ$ channel, has been carried out but no evidence is seen.
ψ(2S) production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}$= 13 TeV and p--Pb collisions at $\sqrt{s_{\mathrm{NN}}}$= 8.16 TeV with ALICE at the LHC
Heavy Flavour decay muon production at forward rapidity in pp collisions at \sqrt{s}= 7 TeV and in Pb-Pb collisions at \sqrt{s_{NN}}=2.76 TeV with the ALICE experiment
Measurement of azimuthal correlations of D mesons and charged particles in pp collisions at $\sqrt{s}=7$ TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
Characterizing system dynamics with two-particle transverse momentum correlations in pp collisions at $\sqrt{s} = 7\;\text{TeV}$ and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$
Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV and Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV
Reference heavy flavour cross sections in pp collisions at sqrt(s) = 2.76 TeV, using a pQCD-driven sqrt(s)-scaling of ALICE measurements at sqrt(s) = 7 TeV
Measurements of long-range azimuthal anisotropies and associated Fourier coefficients for $pp$ collisions at $\sqrt{s}=5.02$ and $13$ TeV and $p$+Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ATLAS detector
用ATLAS方法测量了LHC上$\sqrt{s} = 5.02$和$13$ TeV $pp$碰撞以及$\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV $p$ +Pb碰撞的两粒子关联。测量的相关函数作为相对方位角$Δϕ$，和赝快度分离$Δη$的函数，使用带电粒子的赝快度间隔$|η|{<}2.5$内检测。方位角调制的相关函数的长程分量，与$|Δη|{>}2$，研究使用模板拟合过程，以消除“背靠背”的相关函数，主要是从硬散射过程中产生的贡献。除了在先前的测量中观察到的椭圆$\cos{(2Δϕ)}$调制之外，$pp$相关函数还表现出显著的$\cos{(3Δϕ)}$和$\cos{(4Δϕ)}$调制。与$n =$ $2$ - $4$的相关函数的$\cos{(nΔϕ)}$调制相关联的傅立叶系数$v_{n,n}$被测量为带电粒子多重性和带电粒子横向动量的函数。傅立叶系数被观察到与$\cos{(nϕ)}$调制的每事件单粒子的方位角分布是兼容的。测量的单粒子傅立叶系数$v_n$作为一个函数的带电粒子多重性，和带电粒子的横向动量$n {=} $ $2$ - $4$。本分析中使用的积分光度为$\sqrt{s}=13$ TeV $pp$数据的$64$ $\mathrm{nb^{-1}}$、$\sqrt{s}=5.02$ TeV $pp$数据的$170$ $\mathrm{nb^{-1}…
