\( \newcommand{\dd}{\mathrm{d}} \) \(
\DeclareMathOperator{\sign}{sign} \) \(
\newcommand{\pvec}[1]{\vec{#1}^{\,\prime}} \) \(
\newcommand{\R}{\mathbb{R}} \)
|
Special
topics in heavy-ion collision dynamics
(Transport and Magnetohydrodynamics Meeting)
\begin{equation*} p^{\mu} \frac{\partial f}{\partial x^{\mu}} + m
\frac{\partial(K^{\mu} f)}{\partial p^{\mu}} = \frac{1}{2}
\frac{g}{(2 \pi \hbar)^3} \int_{\R^3} \frac{\dd^3 \vec{p}_2}{E_2}
\int_{\R^3} \frac{\dd^3 \pvec{p}_1}{E_1'} \int_{\R^3} \frac{\dd^3
\pvec{p}_2}{E_2'} W(p_1',p_2' \leftarrow p_1,p_2) \left (f_1' f_2'
\, \overline{f} \, \overline{f}_2 - f f_1 \overline{f}_1'
\overline{f}_2' \right ) \end{equation*}
|
Venue: PHYS 02.116 and/or via Zoom
Time: Thursdays, 2:15 - 3:15pm
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Summer Semester 2025
Date
|
Speaker
|
Title
|
Presentation |
April 02
12:00 |
David Wagner |
Spin Polarization of Λ hyperons from Dissipative Spin
Hydrodynamics |
Preprint
Talk [pdf] |
April 16
11:00am |
Débora Mroczek |
The high-temperature QCD critical point: modeling and
implementation challenges |
|
| April 24 |
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| May 01 |
May Day |
- |
- |
| May 08 |
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| May 15 |
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| May 22 |
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| May 29 |
Ascension Day |
- |
- |
| June 05 |
|
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| June 12 |
|
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| June 19 |
Corpus Christi |
- |
- |
| June 26 |
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| July 03 |
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| July 10 |
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| July 17 |
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| July 24 |
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CRC-TR 211
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Last updated: April 14, 2025