 |
Di, 08:30–10:30 |
ZHG 002 |
GR 5: Schwarze Löcher – Lösungen I |
08:30 None PP T a |
PP 08:30 T a |
|
|
08:30 None PP T b |
PP 08:30 T b |
|
Di, 08:30–10:30 |
ZHG 011 |
T 2: Hauptvorträge 2 |
08:30 None Q PP a |
Q 08:30 PP a |
|
|
08:30 None Q PP b |
Q 08:30 PP b |
|
Di, 09:00–19:00 |
ZHG 003 |
MP 19: Poster (durchgehend Di - Do) |
09:00 None PPP W a |
PPP 09:00 W a |
|
|
09:00 None PPP W b |
PPP 09:00 W b |
|
Di, 09:15–10:30 |
ZHG 003 |
MP 1: Quanteninformation I |
09:15 None PPP P a |
PPP 09:15 P a |
|
|
09:15 None PPP P b |
PPP 09:15 P b |
|
Di, 11:00–11:45 |
ZHG 011 |
PV 1: PV I |
11:00 None P P a |
P 11:00 P a |
|
|
11:00 None P P b |
P 11:00 P b |
|
Di, 11:00–11:45 |
ZHG 011 |
MP 2: Plenarvortrag 1: G. Herten, LHC Highlights |
11:00 None PPP PP a |
PPP 11:00 PP a |
|
|
11:00 None PPP PP b |
PPP 11:00 PP b |
|
Di, 11:45–12:30 |
ZHG 011 |
PV 2: PV II |
11:45 None P PP a |
P 11:45 PP a |
|
|
11:45 None P PP b |
P 11:45 PP b |
|
Di, 11:45–12:30 |
ZHG 011 |
MP 3: Plenarvortrag 2: M. Ansorg, Rotierende relativistische Sterne |
11:45 None PPP Q a |
PPP 11:45 Q a |
|
|
11:45 None PPP Q b |
PPP 11:45 Q b |
|
Di, 14:00–15:30 |
ZHG 002 |
GR 6: Hauptvorträge Schwarze Löcher I |
14:00 None PP TP a |
PP 14:00 TP a |
|
|
14:00 None PP TP b |
PP 14:00 TP b |
|
Di, 14:00–16:20 |
ZHG 011 |
T 6: Eingeladene Vorträge 1 |
14:00 None Q QPP a |
Q 14:00 QPP a |
|
|
14:00 None Q QPP b |
Q 14:00 QPP b |
|
Di, 14:00–16:20 |
ZHG 010 |
T 7: Eingeladene Vorträge 2 |
14:00 None Q QPPP a |
Q 14:00 QPPP a |
|
|
14:00 None Q QPPP b |
Q 14:00 QPPP b |
|
Di, 14:15–14:55 |
ZHG 003 |
MP 4: HV Quantenmechanik: S. Warzel |
14:15 None PPP R a |
PPP 14:15 R a |
|
|
14:15 None PPP R b |
PPP 14:15 R b |
|
Di, 15:00–15:50 |
ZHG 003 |
MP 5: Quantenmechanik |
15:00 None PPP RP a |
PPP 15:00 RP a |
|
|
15:00 None PPP RP b |
PPP 15:00 RP b |
|
Di, 15:30–16:10 |
ZHG 002 |
GR 7: Schwarze Löcher – Lösungen II |
15:30 None PP TPP a |
PP 15:30 TPP a |
|
|
15:30 None PP TPP b |
PP 15:30 TPP b |
|
Di, 16:30–17:10 |
ZHG 003 |
MP 6: HV Quantenfeldtheorie: D. Buchholz |
16:30 None PPP RQ a |
PPP 16:30 RQ a |
|
|
16:30 None PPP RQ b |
PPP 16:30 RQ b |
|
Di, 16:40–18:00 |
ZHG 002 |
GR 8: Schwarze Löcher – Bahnen |
16:40 None PP TPPP a |
PP 16:40 TPPP a |
|
|
16:40 None PP TPPP b |
PP 16:40 TPPP b |
|
Di, 16:45–19:00 |
VG 3.103 |
T 11: QCD (Theorie) 1 |
16:45 None Q T a |
Q 16:45 T a |
|
|
16:45 None Q T b |
Q 16:45 T b |
|
Di, 16:45–18:45 |
VG 3.102 |
T 16: Beyond the Standard Model (Theorie) 2 |
16:45 None Q TR a |
Q 16:45 TR a |
|
|
16:45 None Q TR b |
Q 16:45 TR b |
|
Di, 16:45–19:00 |
VG 3.101 |
T 21: Astroteilchenphysik, Kosmologie / Neutrinophysik (Theorie) |
16:45 None Q TT a |
Q 16:45 TT a |
|
|
16:45 None Q TT b |
Q 16:45 TT b |
|
Di, 16:45–18:55 |
ZHG 009 |
T 26: QCD 2 |
16:45 None Q X a |
Q 16:45 X a |
|
|
16:45 None Q X b |
Q 16:45 X b |
|
Di, 16:45–18:30 |
ZHG 104 |
T 33: Top-Quark: Produktion 2 |
16:45 None Q ZRP a |
Q 16:45 ZRP a |
|
|
16:45 None Q ZRP b |
Q 16:45 ZRP b |
|
Di, 16:45–18:45 |
ZHG 105 |
T 38: Top-Quark: Eigenschaften 2 |
16:45 None Q \PP a |
Q 16:45 \PP a |
|
|
16:45 None Q \PP b |
Q 16:45 \PP b |
|
Di, 16:45–19:05 |
ZHG 004 |
T 40: CP-Verletzung 1 |
16:45 None Q \PR a |
Q 16:45 \PR a |
|
|
16:45 None Q \PR b |
Q 16:45 \PR b |
|
Di, 16:45–18:05 |
ZHG 101 |
T 45: Higgs-Physik 2 |
16:45 None Q \RPP a |
Q 16:45 \RPP a |
|
|
16:45 None Q \RPP b |
Q 16:45 \RPP b |
|
Di, 16:45–19:00 |
ZHG 011 |
T 46: Higgs-Physik 3 |
16:45 None Q \S a |
Q 16:45 \S a |
|
|
16:45 None Q \S b |
Q 16:45 \S b |
|
Di, 16:45–19:15 |
ZHG 010 |
T 51: Supersymmetrie 2 |
16:45 None Q \TPP a |
Q 16:45 \TPP a |
|
|
16:45 None Q \TPP b |
Q 16:45 \TPP b |
|
Di, 16:45–19:15 |
VG 2.102 |
T 59: Spurdetektoren und Spurrekonstruktion |
16:45 None Q ` a |
Q 16:45 ` a |
|
|
16:45 None Q ` b |
Q 16:45 ` b |
|
Di, 16:45–19:00 |
ZHG 001 |
T 64: Halbleiterdetektoren: Forschung und Entwicklung 2 |
16:45 None Q dP a |
Q 16:45 dP a |
|
|
16:45 None Q dP b |
Q 16:45 dP b |
|
Di, 16:45–19:05 |
ZHG 005 |
T 69: Halbleiterdetektoren: Modulbau und Test |
16:45 None Q dR a |
Q 16:45 dR a |
|
|
16:45 None Q dR b |
Q 16:45 dR b |
|
Di, 16:45–18:45 |
VG 1.102 |
T 72: Kalorimeter 2 |
16:45 None Q f a |
Q 16:45 f a |
|
|
16:45 None Q f b |
Q 16:45 f b |
|
Di, 16:45–18:45 |
VG 0.111 |
T 75: Experimentelle Methoden 2 |
16:45 None Q h a |
Q 16:45 h a |
|
|
16:45 None Q h b |
Q 16:45 h b |
|
Di, 16:45–18:50 |
VG 1.103 |
T 81: Beschleunigerphysik 3 |
16:45 None Q jPP a |
Q 16:45 jPP a |
|
|
16:45 None Q jPP b |
Q 16:45 jPP b |
|
Di, 16:45–18:45 |
VG 1.104 |
T 82: Beschleunigerphysik 4 |
16:45 None Q jQ a |
Q 16:45 jQ a |
|
|
16:45 None Q jQ b |
Q 16:45 jQ b |
|
Di, 16:45–19:10 |
ZHG 008 |
T 90: Gammaastronomie 2 |
16:45 None Q oP a |
Q 16:45 oP a |
|
|
16:45 None Q oP b |
Q 16:45 oP b |
|
Di, 16:45–19:00 |
ZHG 007 |
T 95: Neutrinoastronomie 2 |
16:45 None Q qP a |
Q 16:45 qP a |
|
|
16:45 None Q qP b |
Q 16:45 qP b |
|
Di, 16:45–19:05 |
ZHG 006 |
T 100: Kosmische Strahlung 2 |
16:45 None Q qPQPP a |
Q 16:45 qPQPP a |
|
|
16:45 None Q qPQPP b |
Q 16:45 qPQPP b |
|
Di, 16:45–19:05 |
ZHG 102 |
T 108: Niederenergie-Neutrinophysik/Suche nach Dunkler Materie 3 |
16:45 None Q sP a |
Q 16:45 sP a |
|
|
16:45 None Q sP b |
Q 16:45 sP b |
|
Di, 16:45–19:05 |
ZHG 103 |
T 109: Niederenergie-Neutrinophysik/Suche nach Dunkler Materie 4 |
16:45 None Q t a |
Q 16:45 t a |
|
|
16:45 None Q t b |
Q 16:45 t b |
|
Di, 16:45–18:50 |
VG 0.110 |
T 114: Experimentelle Techniken der Astroteilchenphysik 2 |
16:45 None Q vQ a |
Q 16:45 vQ a |
|
|
16:45 None Q vQ b |
Q 16:45 vQ b |
|
Di, 17:15–18:05 |
ZHG 003 |
MP 7: Quantenfeldtheorie |
17:15 None PPP RQP a |
PPP 17:15 RQP a |
|
|
17:15 None PPP RQP b |
PPP 17:15 RQP b |
