Authors:
(1) Cameron Parker, Sixlotron Institute, University of Texas A & M, Department of Physics and Astronomy, Texas A &M University (Email: [email protected]);
(2) Jetscape cooperation.
Links table
Abstract and 1. Introduction
2. Vaccine systems
3. Medium effects
4. Conclusion and references
3. Medium effects
In this section we use a simplified event pipeline. Since we are not interested in the entire event, only how the means affects its occurrence, we are only studying one plane in the Cuarkon Glon plasma broker. This is done by launching one part in the direction 𝑥 through a specific broker and temperatures (“brick”), bathing on Parton with the material and LBT, then rotating the bathroom with the hybrid. The flow is simulated by adding a specific speed to the thermal Partons in the Hadronization stage. In the following, the longitudinal is defined as in the direction of the bird (𝑥) and is perpendicular to the aircraft.
We first study the effects of the heat Partons presence during the decomposition. We draw the proton to relief as a function of Hadron 𝑝𝑥 for a variety of different brick lengths from 0 (vacuum) to 8 FM. A large proton ratio is known to be a signature from Quark
Reinstalization in the circuit. As shown in the left panel of Figure 3, the proportion of the proton to the bion increases around 1 gev in size with an increase in the size of the brick. This is consistent with the idea that reinstallation with thermal Partons increases in a larger medium.
When a homogeneous longitudinal flow is added in the direction of the jet, the peaks grow in the proportions of the proton to relief and are transferred to 2-2.5 Gev. This can be understood by the flow of thermal islands that add more momentum to the Hadron that re -assemble them. Similar effects can be seen in λ to 𝐾, not explained here.
Then we study the effects of brick flow from brick companies. We spread vertical components of the momentum on aircraft (𝑝𝑦 and 𝑝𝑧) for every Hadron to display the influx effects. The soft Hadron, defined as 2 Gev <𝑝𝑥 10 Gev, shows a great deviation in the direction of flow as shown in Figure 4. This is consistent with expectation. The leading Partons is far from the thermal parties in the phase area, and therefore has a little opportunity to reassemble it.
4. Conclusion
Our study of moderate effects on the jet truce is similarly promising. Using bricks with a flow, we focus all the expected effects, including increasing the bars with average size, turning the peak of Barion/Mason in the momentum with longitudinal flow, and the lateral deviation from the soft hadron with the transverse flow. We intend to advance to heavy flavor and aircraft simulation in full collision 𝐴 + 𝐴.
This work was supported by the American National Science Foundation under the awards 1812431 and 2111568, and under the 2004571 Award through a sub -contract with Wayne State University.
Reference
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