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Seminari A.A. 2012-2013 |
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I Seminari si svolgono il martedì alle 14:30 nell'aula 311
del Dipartimento di Matematica
(salvo diversa indicazione)
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Relatore |
Titolo |
Data |
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2012-13/
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Omar Maj
Max-Planck Inst. für Plasmaphys. Garching |
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02 Luglio 2013 (ore 14:00) |
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Marco Brambilla
Max-Planck Inst. für Plasmaphys. Garching |
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11 Giugno 2013 |
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Mustapha Mourragui
Université de Rouen |
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16 Maggio 2013 (giovedì) |
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Mustapha Mourragui
Université de Rouen |
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15 Maggio 2013 (mercoledì) |
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Bruno Coppi
MIT |
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14 Maggio 2013 (ore 15:00) |
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Francesco Califano
Università di Pisa |
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14 Maggio 2013 (ore 14:00) |
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Alain Messager
CPT - CNRS Marseille |
Phase transitions in the long range XXZ model |
07 Maggio 2013 (ore 15:30) |
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Carlo Marchioro
Università di Roma "La Sapienza" |
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07 Maggio 2013 |
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Milos Zahradnik
Charles University Prague |
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30 Aprile 2013 (ore 15:00) |
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Daniela Grasso
CNR e Politecnico di Torino |
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30 Aprile 2013 (ore 14:00) |
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Yuri Kondratev
Universität Bielefeld |
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23 Aprile 2013 |
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Israel Michael Sigal
Toronto University |
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12 Aprile 2013 (venerdì) |
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Errico Presutti
Università di Roma "Tor Vergata" |
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09 Aprile 2013 |
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Giovanni Gallavotti
INFN Roma1 e Accademia dei Lincei |
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05 Marzo 2013 |
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Alessandro Pizzo
UC Davis |
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23 Ottobre 2012 (ore 16:00) |
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Zhituo Wang
Paris XI - Orsay |
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26 Settembre 2012 (mercoledì) |
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Joel Lebowitz
Rutgers University |
Three easy (to state) open problems (that have worried me for many years) |
24 Settembre 2012 (lunedì 16:00 aula F) |
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Manuel de Llano
UNAM |
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21 Settembre 2012 (venerdì) |
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A recent reexamination of BCS theory leads one to devise a
generalized BEC formalism (GBEC) that is essentially a boson-fermion (BF)
gas model containing three new ingredients: i) Cooper pairs (CPs),
in contrast to BCS pairs, as real bosons; ii) BF vertex interactions
(analogous to electron-phonon vertex interactions in metals) and
iii) two-hole CPs (2hCPs) along with two-electron CPs (2eCPs) on an
equal footing. In addition to the usual normal phase at very high
temperatures T, three condensed phases emerge at low T: two pure
BECs of 2eCPs and of 2hCPs, as well as a mixed phase of both kinds of CPs.
BCS theory is precisely recovered with a mixed phase of equal numbers
of both kinds of CPs. Substantially higher Tcs than BCS theory are
predicted and, in contrast to the well-known BCS exponential rise of Tc
from zero, the GBEC scheme exhibits a linear rise as function of doping
as eminently observed in high-Tc superconductors. Ultracold fermionic
atoms are briefly discussed, especially around the so-called unitarity
range where the two-fermion scattering length can diverge. |
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