|
@  @@@½¬18Nx€¬Κρο@ϋͺ\vO@@@@ |
||
|
ϊ@ϊ@F@QOOUNPQPSϊiΨj`PUϊiyj |
||
|
κ@@F@WH²δΫοcκ@ |
||
 |
||
|
vO(Nov./29jPDF(16KB) 
AuXgNg(Nov./29jPDF(636KB) |
||
 @PQPSϊiΨj |
||
A-14-1 (Porous 4He)@Chair; M. Imada |
||
10:30-10:40 |
Opening | |
10:40-10:55 |
l \η (K. Shirahama) | |
| Quantum Phenomena in 4He Confined in Nano-porous Structures | ||
11:00-11:15 |
ιΨ@ (M. Suzuki) | |
| Simultaneous Measurements of an Ultrasound and a Torsional Oscillator for 4He in a Nano-porous Glass | ||
11:20-11:35 |
ac MY (N. Wada) | |
| 4He and 3He Quantum Fluids Realized in N -Dimensional Nanopores | ||
11:40-11:55 |
΄ εγ (D. Takahashi) | |
| Property of Surface Electrons on Rotating Superfluid 4He | ||
12:00-13:20 |
Lunch | |
A-14-2 (Anisotropic superconductors I)@Chair; K. Miyake |
||
13:20-13:45 |
M. Sigrist | |
| Theoretical discussion of Superconductivity in Materials without Inversion Symmetry | ||
13:50-14:05 |
²‘ Ί (N.K. Sato) | |
| Magnetism and superconductivity in the ferromagnet UGe2 | ||
14:10-14:25 |
Ξc ρ (K. Ishida) | |
| Measurements of Knight Shift and Spontaneous Field in Superconducting State of Sr2RuO4 | ||
14:30-14:45 |
rc _Ν (H. Ikeda) | |
| Magnetic properties in the normal and superconducting states in Sr2RuO4 | ||
14:50-15:05 |
VJ@κ (K. Tenya) | |
| Anisotropy of the Upper Critical Field in Sr2RuO4 | ||
15:10-15:30 |
Break | |
A-14-3 (3He; Anisotropic superfluid with boundaries as in aerogel)@ Chair; Y. Maeno |
||
15:30-15:45 |
Ξμ CZ (S. Ishikawa) | |
| Superfluid 3He in aerogel and in a narrow cylinder | ||
15:50-16:05 |
rc ²ξ (R. Ikeda) | |
| Theoretical Study of Superfluid Helium-three in Aerogels | ||
16:10-16:25 |
Φ‘ Κ (M. Saito) | |
| Investigation of Phase Transition in Submicron Superfluid 3He Film | ||
16:30-16:45 |
iδ F (K. Nagai) | |
| Surface Enhancement of Spin Susceptibility in Superfluid 3He-B | ||
16:50-17:05 |
Ό΄@Ύ (A. Matsubara) | |
| Visualization of Vortex Lattice in Rotating Superfluid 3He-A | ||
A-14-4 (Anisotropic superconductors II)@Chair; M. Ogata |
||
17:30-17:45 |
cRμv (Y. Tanaka) | |
| Odd-frequency pairing state in superconducting junctions | ||
17:50-18:05 |
σμ Χ° (Y. Asano) | |
| Josephson Spin Current in Triplet Superconductor Junctions | ||
18:10-18:25 |
Ύc K₯ (Y. Ohta) | |
| Spin-Triplet Superconductivity and Excitation Spectra in the Two-Chain Hubbard Models | ||
18:30-18:45 |
‘R υq (H. Yokoyama) | |
| Superconductor as Doped Mott Insulator in 2D Hubbard Model | ||
18:50-20:10 |
Dinner | |
Informal discussion |
||
20:10-22:00 |
Panel Discussion: Outlook of Super Clean Project Shirahama, Wada, Maeno, Miyake, Tsubota, Ueda, Ishimoto, Fukuyama, Kono (10min. each) |
|
|
@PQPTϊiΰj |
||
A-15-1 (Quantum vortex, dynamics)@Chair; M. Ueda |
||
8:40-8:55 |
Ψc@½ (M. Tsubota) | |
| Quantum Turbulence `Another Da Vinci Code` | ||
9:00-9:15 |
ξμ pY (H. Yano) | |
| Generation of Quantum Turbulence by a Vibrating Wire in Superfluid 4He | ||
9:20-9:35 |
΄c «ξ (K. Harada) | |
| Millimeter-wave Spectroscopy of the (He)n-HCN clusters | ||
9:40-9:55 |
c Yκ (Y. Okuda) | |
| Crystal growth of solid 4He in the quantum limit | ||
10:00-10:15 |
²XΨ L (Y. Sasaki) | |
| Field Induced First Order Phase Transition near Absolute Zero Between Nuclear Antiferromagnetic Phases of Solid 3He | ||
10:20-10:40 |
Break | |
A-15-2 (Frustration & Spin liquid I)@Chair; N. Kawakami |
||
10:40-10:55 |
Ξ{ pF (H. Ishimoto) | |
| Two-dimensional 3He film on graphite in high magnetic field | ||
11:00-11:15 |
δ@Χ (T. Momoi) | |
| Octupolar order in the multiple spin exchange model on a triangular lattice | ||
11:20-11:35 |
ν Gκ (H. Tsunetsugu) | |
| Magnetic Properties of Spin Nematic State | ||
11:40-12:50 |
Poster Preview I; P01-P56, 1minute each Chair; H. Fukuyama |
|
12:50-14:10 |
Lunch | |
14:10-15:20 |
Poster Preview II; P57-P113, 1 minute each Chair; K. Shirahama |
|
15:20-17:50 |
Poster Session | |
A-15-3 (Frustration & Spin liquid II)@Chair; K. Kubo |
||
17:50-18:05 |
ψ΄ rΖ (T. Hikihara) | |
| Magnetic phase diagram of spin-1/2 two-leg ladder with four-spin ring exchanges | ||
18:10-18:25 |
μΊ υ (H. Kawamura) | |
| Novel ordering of frustrated 2D triangular and 3D pyrochlore systems | ||
18:30-18:45 |
βδ O (T. Sakai) | |
| Ring Exchange Induced Charge Stripes in 2D t-J Model | ||
18:50-19:05 |
L ΐO (Y. Hatsugai) | |
| Quantum and Topological Orders of Quantum Liquids: use of Berry Connection and Entanglement Entropy with Bulk-Edge Correspondence | ||
19:20- |
Banquet | |
|
@PQPUϊiyj |
||
A-16-1 (BEC, Optical lattice)@Chair; M. Tsubota |
||
9:00-9:15 |
γc ³m (M. Ueda) | |
| Symmetry Breaking in Dilute Bose-Einstein Condensates | ||
9:20-9:35 |
½μ τη (T. Hirano) | |
| Dynamics of atomic Bose-Einstein condensates with internal degrees of freedom | ||
9:40-9:55 |
¬c ΉF (M. Machida) | |
| Numerical Observation of Kolmogorov Spectrum in Rotating BEC I. Time Evolution of Energy Spectrum and Vortex Dynamics | ||
10:00-10:15 |
μγ ₯Y (N. Kawakami) | |
| Correlated Fermions in Optical Lattice with Harmonic Confinement | ||
10:20-10:35 |
΄ `N (Y. Takahashi) | |
| Quantum Simulation Using Quantum Degenerate Ytterbium Atoms in Optical Lattices | ||
10:40-11:00 |
Break | |
A-16-2 (2D 3He)@Chair; H. Ishimoto |
||
11:00-11:15 |
R@ ° (H. Fukuyama) | |
| Zero-Point Vacancies Doped into a Two-Dimensional Gapless Spin-Liquid | ||
11:20-11:35 |
Ψ δv (T. Takagi) | |
| A γ7xγ7 phase of the second adsorbed 3He layer on a graphite | ||
11:40-11:55 |
¬` ³j (M. Ogata) | |
| A Model Calculation of 3He on Two-Dimensional Graphite | ||
12:00-12:15 |
ͺ{ O (T. Okamoto) | |
| Spin Polarization in Strongly Correlated 2D Systems in Semiconductors | ||
12:20-12:35 |
ΰVc ΐχ (A. Sawada) | |
| Novel Quantum Phases in the Bilayer Quantum Hall Regime | ||
12:40-14:00 |
Lunch | |
A-16-3 (Mott physics, MI transitions, quantum criticality)@ Chair; H. Fukuyama |
||
14:00-14:15 |
μc κi (K. Kanoda) | |
| Recent results on Mott criticality in 2D organics | ||
14:20-14:35 |
Ί ΆF (F. Nakamura) | |
| Novel quantum phenomena in single-layered ruthenates under pressure | ||
14:40-14:55 |
Ψ pT (H. Takagi) | |
| Charge transport at quantum critical point in gcleanh NiS2 pyrite | ||
15:00-15:15 |
cΊ λj (M. Tamura) | |
| Valence Bond States and Pressure-Induced Superconductivity in Quantum Triangular Antiferromagnets, [Pd(dmit)2] Salts | ||
15:20-15:35 |
‘c ³r (M. Imada) | |
| Topology transition vs. symmetry breaking at quantum end point of 1st-order transition | ||
15:40-16:00 |
Closing H.Fukuyama | |
