‘æ63‰ñNMLƒZƒ~ƒi[, 2006
ŠJÓúŽž 8th February, 2006, 13:30-15:30 (15:30-discussion)
ŠJÃêŠ Seminar Room on 8th Floor, Main Building at Sengen Site
u‰‰ŽÒ Dr. John E.E. Baglin
Prof. Daryush ILA
Š‘® Research Staff Member Emeritus IBM Almaden Research Center
Executive Director Alabama A&M University Research Institute (AAMURI)
u‰‰‘è–Ú Dr. John E.E. Baglin "Ion Beam Patterning at the Nanometer Scale"
Prof. Daryush ILA "Formation of Nanolayers of Nanomaterials and their applications"
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Dr. John E.E. Baglin

Due to the absence of diffraction limitations, the extensive available process parameter space, and the prospects for one-shot imposition of a projection-reduced master mask nano-pattern, ion beam patterning appears to offer a viable path to large-scale manufacturing of devices and systems based on nanoscale features, while offering robustness, flexibility, high quality of image definition and high throughput. He is one of the pioneers working on nanoscale patterning using ion projection methods, and is collaborating with the NIMS next-step program of quantum beam technology. The lecture covers instrumental techniques and demonstrations for nanoparticle magnetic media and ion lithography in polymers.


Prof. Daryush ILA

Workers at the Center for Irradiation of Materials of Alabama A&M University have used various MeV ion beams to form composites of layers of nanocrystals (NC) in various substrates. The nanolayers (periodic layered films) were produced either by MeV ion implantation followed by thermal annealing and/or by MeV ion irradiation, or by simultaneous deposition of various species followed by thermal annealing and/or by post MeV ion irradiation. The produced multilayer films have a periodic structure consisting of alternating thin film layers of the thicknesses between 20 and 50 Angstroms. The periodic layered thin films were characterized by Rutherford backscattering (RBS) spectrometry. For optical properties we used UV/VIS/IR absorption photo-spectrometry. For thermoelectric properties of nano-layered structure, we fabricated a 3w method to measure thermal conductivity, used a Hall Effect system to measure the electrical conductivity and used a Seebeck coefficient measurement system to completely measure all physical properties of the produced multi-nano-layered structure in order to calculate the Figure of Merit for these nanolayered systems. The systems which we will present as examples for this presentations are 10 to 50 nanolayers of [insulator/metal NC-insulator/insulator/], and [insulator/semiconductor NC-insulator/] This presentation will focus on our last few years efforts on production of variable width optical filters as well as production of highly efficient thermoelectric materials.

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‘æ62‰ñNMLƒZƒ~ƒi[, 2006
ŠJÓúŽž 2006”N2ŒŽ7“úi‰Îj13:30-15:30
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‘æ61‰ñNMLƒZƒ~ƒi[, 2006
ŠJÓúŽž 2006”N2ŒŽ6“úiŒŽj14:00`15:30
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u‰‰‘è–Ú …Ž_‰»•¨—n—Z‰–‚ð—p‚¢‚½Tf-La2CuO4ƒoƒ‹ƒNŽŽ—¿‚̒ቷ‡¬
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La‚̈ꕔ‚ðƒ‰ƒ“ƒ^ƒmƒCƒhLn‚Å’uŠ·‚µ‚½Tf-(La, Ln)2CuO4”––Œ‚Å‚ÍCƒLƒƒƒŠƒAƒh[ƒv–³‚µ‚Å’´“`“±(Tc ` 25K)‚ðŽ¦‚·‚±‚Æ‚ª“à“¡‚ç‚É‚æ‚è•ñ‚³‚êC’–Ú‚ðW‚߂Ă¢‚é[1]DÅ‹ßC‰äX‚ÍCƒAƒ‹ƒJƒŠ‹à‘®…Ž_‰»•¨‚ð—n—Z‰–‚Æ‚µ‚Ä—p‚¢‚Ēቷi350Ž’ö“xj‚Ҭ‚ðs‚¤‚±‚Ƃɂæ‚èCTf\‘¢‚ð—L‚·‚éLa2CuO4‚̃oƒ‹ƒNŽŽ—¿‚𓾂邱‚ƂɬŒ÷‚µ‚½D‚µ‚©‚µ‚È‚ª‚çCŒ»Ý‚̂Ƃ±‚ëC’´“`“±‚ðŠm”F‚·‚é‚É‚ÍŽŠ‚Á‚Ä‚¢‚È‚¢D
Tf- La2CuO4‚ª“¾‚ç‚ꂽ—vˆö‚ÍŽŸ‚̂悤‚Él‚¦‚ç‚ê‚éD’Êí‚ÌŒÅ‘Š”½‰ž–@‚ð—p‚¢‚Ä‚‰·(–ñ1000Ž)‚ÅLa2CuO4‚ð컂·‚邯CCuO6”ª–ʑ̂ð—L‚·‚éT/O\‘¢‚ð‚Æ‚éDT/O\‘¢‚Ì\‘¢‘Š“]ˆÚ‰·“xTd1‚Í250-350ނł ‚éD‚‰·‚Å‚ÍCLa-O–Ê‚ÆCu-O–ʂ̑傫‚³‚͂قړ™‚µ‚¢‚ªC‰·“x‚̒ቺ‚É”º‚¢ƒCƒIƒ“Œ‹‡“I‚ÈLa-O‚Ì•û‚ª‹¤—LŒ‹‡“I‚ÈCu-O‚æ‚è‚àk‚݂₷‚­CƒTƒCƒY‚̃~ƒXƒ}ƒbƒ`‚ª¶‚¸‚éD‚»‚ê‚ð‰ðÁ‚·‚邽‚ßCCuO6”ª–ʑ̂͌X‚«CO\‘¢‚ƂȂéDˆê•ûCLa‚ðƒCƒIƒ“”¼Œa‚̬‚³‚ÈLn‚Å’uŠ·‚µ‚½ê‡‚É‚ÍC–ñ1000Ž‚Ì‚‰·‚Å‚³‚¦‚àƒ~ƒXƒ}ƒbƒ`‚ª‘¶Ý‚·‚éD‚±‚ÌꇂɂÍC’¸“_Ž_‘f‚ªLn-O–Ê‚©‚ç㉺‚ɃVƒtƒg‚µCLn3+-Ln3+ (O2--O2-)‚̃N[ƒƒ“”½”­‚É‚æ‚èCLn-O–Ê‚ªŠg‘å‚·‚邱‚Æ‚ÅCƒ~ƒXƒ}ƒbƒ`‚ð‰ðÁ‚·‚éD‚±‚̂Ƃ«CCu‚Í•½–Ê4”zˆÊ‚ÅCTf\‘¢‚ɂȂéD‚·‚Ȃ킿Cƒ~ƒXƒ}ƒbƒ`‚̉ðÁ–@‚Æ‚µ‚Ä‚ÍO\‘¢‚ɂȂ邩CTf\‘¢‚ƂȂ邩‚ª‚ ‚é‚킯‚¾‚ªCŒ‹»‚ð‘g‚Þ‡¬Žž‚É‚ÍC˜c‚ñ‚¾O\‘¢‚æ‚è‚àTf\‘¢‚ð‚Æ‚é‚Æ‰¼’è‚·‚邯CTd1ˆÈ‰º‚̒ቷ‚Ҭ‚ðs‚¦‚ÎCTf- La2CuO4‚ªì»‰Â”\‚Å‚ ‚Á‚½‚Æl‚¦‚½.

[1] A. Tsukada et al., Solid State Commun. 133 (2005) 427

–â‚¢‡‚í‚¹æ ƒiƒm—ÊŽqƒGƒŒƒNƒgƒƒjƒNƒXƒOƒ‹[ƒv@‚–ì@‹`•Fi“àü 2842j
‘æ60‰ñNMLƒZƒ~ƒi[, 2006
ŠJÓúŽž 23rd January, 2006, 10:00-12:00(10:00-lecture, 11:00-discussion)
ŠJÃêŠ Main conference room on 2nd floor, Sakura Site
u‰‰ŽÒ Prof. J. R. Anderson
Š‘® Dept. of Physics, University of Maryland
u‰‰‘è–Ú Quantum Computing Based on Josephson-Junction Phase Qubits
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Many physical implementations have been proposed for a quantum computer. We have chosen Josephson-junction phase-qubit systems for our investigation since they should be relatively insensitive to charge and flux noise although they will be subject to current noise through the current bias leads. I will introduce the subject of quantum computing by mentioning briefly Shorfs algorithm, which is driving the search for a quantum computer. Then I will discuss our work on single Josephson junctions as phase qubits. Measurements with microwaves applied to one and two-qubit systems will be described. Microwave spectroscopy has provided evidence for the entanglement of two capacitively coupled junctions (a.k.a. qubits).I will also show that this two-junction system, at bias currents corresponding to larger energy separations than used initially, is actually coupled by an LC resonator, which has its own energy levels. We have performed microwave spectroscopy on this three-component system and have observed avoided level-crossings of at least three levels. These results will be compared with theoretical calculations. In addition, Rabi oscillations, observed in single and coupled junctions will be presented. From these measurements and from measurements of escape rates as bias currents through junctions are ramped, we have estimated coherence times. These estimates are being used to compare different techniques for isolating junctions from external sources of decoherence. At the present time we are investigating inductance-junction (LJ) isolation schemes by means of which we have been successful in observing the Rabi oscillations mentioned above. (If time permits, I will discuss a method for state initialization with LJ isolation.) Up to now we have studied no more than two coupled junctions, but we are beginning to investigate multi-qubit systems of three or more junctions. Different schemes for control of qubit coupling will also be compared since it is important to be able to turn the coupling on and off. To conclude, I will discuss the prospects for gate operations and the realization of a Josephson-junction quantum computer.

–â‚¢‡‚í‚¹æ ‹­Ž¥êŒ¤‹†ƒZƒ“ƒ^[@–ØŒË@‹`—Ei“àü 5024j
‘æ59‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 19th December, 2005, 10:30-12:00
ŠJÃêŠ Seminar Room on 8th Floor, Main Building at Sengen Site
u‰‰ŽÒ Associate Prof. Adekunle O Adeyeye
Š‘® Information Storage Materials Laboratory, Department of Electrical and Computer Engineering,
National University of Singapore
u‰‰‘è–Ú Magnetic Nanostructures for Spintronic Applications
ƒAƒuƒXƒgƒ‰ƒNƒg

An exciting development in magnetism has been the use of controlled nanofabrication
techniques such as lithography and other self assembly methods to create nanoscopic
magnetic structures.? Magnetic nanostructures, by virtue of their extremely small size
possess very different properties from their parent bulk material. Ferromagnetic
nanostructures provide an opportunity for the exploration of new physical phenomena and
the development of technologically important devices. One of the main applications of
magnetic nanostructures is in ultra-high density data storage and non-volatile memory.
In this talk, I will present a large area nanofabrication technique we have developed
for synthesizing ferromagnetic nanostructures using deep ultraviolet lithography at
248 nm exposing wavelength . One unique advantage of this technique is the fact that
unlike e-beam lithography, thicker resists can be used to make high aspect ratio
nanostructures.? Using a combination of alternating phase shift masks (alt PSM) and
chrome-less phase lithography (CPL) masks, we have created arrays of ferromagnetic
nanostructures with lateral dimensions well below the conventional resolution limit of
the tool. In alt PSM the adjacent apertures pass the exposing radiation in opposite
phase which results in elimination of 0th diffraction order and the reduction in
separation between the pair of higher orders. Subsequently, we have used electron beam
deposition technique and lift-off method to convert the developed resist patterns into
magnetic Ni80Fe20 and Cobalt nanostructures. Ferromagnetic nanostructures of different
shapes including wire array, complex rings structures and diamond shapes were fabricated.
The uniformity of the nanomagnets was characterized using a scanning electron microscope
(SEM) and atomic force microscopy (AFM). We observed that the structures are uniform,
have the desired shapes and are reproducible over a large area. The magnetic properties
were characterized using vibrating sample magnetometer (VSM) and magnetic force microscopy
(MFM). We observed that the magnetic properties of the fabricated nanostructures are very
different from the reference film and strongly depend on the size and shape of
the nanostructures. This can be attributed to the effect of magnetic shape anisotropy.?
Finally, a simple micromagnetic modeling will be used to aid our understanding of the
magnetization reversal processes in the nanomagnets.
Navab Singh, S. Goolaup and A.O Adeyeye, Nanotechnology, 15, 1539-1544 (2004).

–â‚¢‡‚í‚¹æ ƒiƒm—ÊŽqƒGƒŒƒNƒgƒƒjƒNƒXƒOƒ‹[ƒv@‚–ì@‹`•Fi“àü 2842j
‘æ58‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž 15th December, 2005, 14:00-16:00
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231/232, Namiki Site
u‰‰ŽÒ Prof. Guy Le Lay
Š‘® CRMCN-CNRS and Universite de Provence, LMarseille, France
u‰‰‘è–Ú Self-assembled germanium/silicon nanostructures at silver surfaces
ƒAƒuƒXƒgƒ‰ƒNƒg

In my talk I will present novel germanium or silicon nanostructures obtained by condensing
in situ under ultra-high vacuum Ge or Si onto clean, unreactive, low index surfaces of
silver single crystals. These nanostructures reveal striking aspects and astonishing
features in scanning tunneling microscopy. They are further characterized in great details
by synchrotron radiation surface X-ray diffraction and photoelectron spectroscopy of the
valence bands and core-levels.
With Ge these nanostructures are self-organized assemblies of tetramer nanodots forming
long range ordered superstructures on Ag(100) and Ag(110). Surprisingly, instead,
a long-range ordered substitutional Ag2Ge surface is initially formed on Ag(111) before
the development of an overlayer of nanodots displaying a Moire pattern.
On Ag(100), Si tetramer nanodots develop in a 3x3 superstructure on top of which one
dimensional octagonal or hexagonal ribbons grow and later coalesce. Remarkably, on the
anisotropic Ag(110) surface, single domain, massively parallel arrays of metallic Si
quantized stripes with a magic width of 1.6 nm already develop at room temperature from
highly mobile nanoclusters. They considerably elongate, essentially keeping their width,
upon mild annealing. The quantum states detected in the sp region of the valence band show
a clear dispersion along their lengths. Extremely narrow, two-components,
Si 2p core-levels further indicate that these nanostripes are atomically precise novel
one-dimensional nanoobjects, which are essentially identical and preserve their
perfection up to the macroscopic scale. Upon further growth, perfectly aligned Si nanowires
with an extremely high aspect ratio continue to develop.
These novel nanostructures provide atomically precise new templates that could be eventuallyused, e.g., to align nanotubes or fix individual molecules as in a mould.

–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹Œ¤‹†Š@–ì@³˜ai“àü 4180j
‘æ57‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž

22nd November, 2005, 15:00-16:30

ŠJÃêŠ Nano-Bio Materials Research Build., Room 231/232, Namiki Site
u‰‰ŽÒ Dr. Gunther Lientschnig
Š‘® JSPS Fellow, AIST Nanotechnology Researc Institute Molecular Nanophysics Group
u‰‰‘è–Ú Towards Measuring the Conduction of Single Molecules and Other Nano-objects
ƒAƒuƒXƒgƒ‰ƒNƒg

In order to measure the electrical properties of single molecules or other small nano-objects like metal clusters, the ability to apply a gate voltage is of paramount importance. In the past few years, considerable efforts have been put into fabricating electrode pairs with nanometer-sized gaps on top of a back-gate. Methods that have been employed include electromigration, electrochemical etching, and shadow-evaporation; and interesting results ranging from negative differential conductance, single-electron tunneling behavior, and Kondo resonances have been reported. In this talk, I will report on particularly striking measurement data indicating highly correlated electron transport in devices that were obtained by self-assembling sub-nanometer sized molecules on shadow-evaporated electrodes. Even though there is evidence that it is indeed the molecules that are the active elements in these devices, the possibility that, for example, small metal particles close to the electrodes are responsible for the observed characteristics cannot be ruled out. Like for samples fabricated by all the other means mentioned above, an imaging method with atomic resolution just does not exist and scanning electron microscopy is insufficient to determine their exact geometrical configuration. In the second part of this presentation, I thus will highlight a new fabrication method that allows for the production of freestanding electrodes with no supporting substrate underneath. This has two advantages. On the one hand there is no possibility anymore to have small metal clusters nearby the electrodes, and on the other hand their structure and composition can be determined by transmission electron microscopy (TEM) with atomic resolution. Actually, the electron beam of a TEM machine itself is the main tool to fabricate these electrodes, as it is possible to burn holes into thin, amorphous membranes and to locally melt and shape thin metal films. The sculpting of freestanding electrodes with gaps down to 1 nm seems feasible. The electrodes are surprisingly stable as was demonstrated by trapping a small metal cluster between them in a water-based solution. A single-electron tunneling device was thus fabricated that, after having measured its Coulomb blockade at temperatures down to 4 K, could be visualized with unprecedented resolution. I deem the application of this technique for the electrical characterization of molecules and other nano-objects to be very promising.

–â‚¢‡‚í‚¹æ ƒiƒm“d‹CŒv‘ªƒOƒ‹[ƒv@’†ŽR@’mMi“àü 8481j
‘æ56‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 26th October, 2005, 14:30-
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231/232, Namiki Site
u‰‰ŽÒ Prof. E.V.Chulkov
Š‘® Donostia International Physics Center
u‰‰‘è–Ú ELECTRON AND HOLE DYNAMICS IN BULK METALS AND AT SURFACES
ƒAƒuƒXƒgƒ‰ƒNƒg

Interaction between lattice, electron, and spin subsystems as well as interaction within each of these subsystems is crucial to understand mechanism of single-particle excitation dynamics, i. e. lifetime of excitations.? The lifetime sets the duration of excitation and in combination with the velocity determines the mean free path, a measure of influence of the excitation. Interest to the study of excited particles dynamics is motivated by an important role that excited electrons and holes play in many processes, e.g. in energy, charge, and spin transport in bulk materials, at surfaces, across interfaces, and at nanosystems.
In this presentation theoretical and experimental results on electron and hole dynamics are discussed in terms of different decay mechanisms and different kinds of interactions for bulk electronic states in paramagnetic and ferromagnetic metals, for surface and image states on metal surfaces, for excited states at single adatoms on these surfaces and for quantum well states in adlayers on metals. Of different interactions elastic and inelastic electron-electron (e-e) interaction as well as electron-phonon (e-ph) interaction are discussed. E-ph decay channel is shown to be important for all systems considered being especially important for low-dimensional systems. In the e-e decay channel the electron (hole) decay can be realized via creation of electron-hole pairs or plasmon excitation. In ferromagnetic systems the electron (hole) decay via the Stoner pair excitation or/and excitation of spin waves is made possible. Dimensionality effects in the lifetime of electrons and holes on metal surfaces and the role of screening and intra- (inter-) band transitions are also discussed.

–â‚¢‡‚í‚¹æ ƒiƒm“d‹CŒv‘ªƒOƒ‹[ƒv@’·”ö@’‰ºi“àü 4746j
‘æ55‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 2005”N10ŒŽ18“úi‰Îj16:00-17:00
ŠJÃêŠ •¨Ž¿EÞ—¿Œ¤‹†‹@\@•À–Ø’n‹æ@ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“431/432†Žº
u‰‰ŽÒ –ìŒû@—T@Ž
Š‘® î•ñ’ÊMŒ¤‹†‹@\ŠÖ¼æ’[Œ¤‹†ƒZƒ“ƒ^[? ƒiƒm‹@\ƒOƒ‹[ƒv
u‰‰‘è–Ú —L‹@’Pˆê“dŽqƒgƒ“ƒlƒ‹Ú‡‚Ì“d‹C“`“±“Á«
ƒAƒuƒXƒgƒ‰ƒNƒg

’Pˆê•ªŽq‚Ì\‘¢‚Æ‚»‚Ì“d‹C“`“±‚Ƃ̊֌W‚ð’m‚邱‚Æ‚ÍA•ªŽq‹@”\‚Ì“dŽq‘fŽq‚ւ̉ž—p‚ð–ÚŽw‚·ã‚Å•K—v•s‰ÂŒ‡‚Å‚ ‚éB‰äX‚Í‚±‚ê‚Ü‚ÅAŒÇ—§“±“d«•ªŽq‚ð‰î‚µ‚½“d‹C“`“±‚É‚¨‚¯‚é’Pˆê“dŽqƒgƒ“ƒlƒ‹Œ»Û‚É’…–Ú‚µ‚ÄŒ¤‹†‚ðs‚Á‚Ä‚«‚½B–{u‰‰‚Å‚ÍA—L‹@’´”––Œ‚ð—p‚¢‚Ä컂µ‚½Ï‘w(c)Œ^’Pˆê“dŽqƒgƒ“ƒlƒ‹Ú‡‚Ì“d‹C“`“±“Á«‚É‚¨‚¢‚ÄŠÏ‘ª‚³‚ꂽŒõ—U‹NƒQ[ƒgŒø‰Ê(ƒN[ƒƒ“ƒXƒeƒAƒP[ƒX‚Ì‚µ‚«‚¢’l‚ªŒõƎ˂ɂæ‚èƒVƒtƒg‚·‚錻Û)‚âAƒGƒŒƒNƒgƒƒ}ƒCƒOƒŒ[ƒVƒ‡ƒ“–@‚ð—p‚¢‚Ä컂µ‚½‰¡Œ^•ªŽqÚ‡‚É‚¨‚¯‚é’Pˆê“dŽqƒgƒ‰ƒ“ƒWƒXƒ^“Á«‚Ȃǂð•ñ‚·‚éB

–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹—§‘Ì”z’uƒOƒ‹[ƒv@ŽáŽR —Ti“àü4403j
‘æ54‰ñNMLƒZƒ~ƒi[, 2006
ŠJÓúŽž 2005”N10ŒŽ14“úi‹àj13:30-14:30
ŠJÃêŠ •¨Ž¿EÞ—¿Œ¤‹†‹@\@•À–Ø’n‹æ@ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“2F@232†Žº
u‰‰ŽÒ ]–{@Œ°—Y@Ž
Š‘® ’·‰ª‹Zp‰ÈŠw‘åŠw‘åŠw‰@HŠwŒ¤‹†‰È
u‰‰‘è–Ú Œõ”½‰ž«‰t»Þ—¿’†‚ł̌õ—U‹NˆÙ•û«ŠiŽq‚ÌŒ`¬‚ƉñÜ“Á«
ƒAƒuƒXƒgƒ‰ƒNƒg

Ǝ˕Όõ‚Ɉˑ¶‚µ‚½ŒõŠwˆÙ•û«‚ð—U‹N‚Å‚«‚é”}Ž¿’†‚Å‚ÍA•ÎŒõƒzƒƒOƒ‰ƒ€‚Ì‹L˜^‚ª‰Â”\‚ƂȂèAŽQÆŒõ‚̕Όõó‘Ԃ̕ω»‚É‚æ‚Á‚Ä‹L˜^î•ñ‚ªÄ¶‚³‚ê‚éB–{Œ¤‹†‚Å‚ÍAÆŽËŽ‡ŠOŒõ‚̕Όõ•ûŒü‚ɉž‚¶‚½•ªŽq”zŒü‚ðˆÀ’肵‚Ä—U‹N‚Å‚«‚é‰t»‚•ªŽq‚ð—p‚¢‚ĕΌõƒzƒƒOƒ‰ƒ€‚Ì‹L˜^‚ðŽŽ‚Ý‚½BŒ‹‰Ê‚Æ‚µ‚ÄA•ÎŒõî•ñ‚͉t»•ªŽq‚ÌÄ”z—ñ‚É‚æ‚éŒõŠwˆÙ•û«•ª•z‚Æ‚µ‚Ä‹L˜^‚³‚êA“üŽËŒõ‚̕Όõó‘Ԃ͕ϊ·‚³‚ê‚ĉñÜ‚³‚ꂽB‚±‚̕Όõ•ÏŠ·‹@”\‚É’–Ú‚µAƒzƒƒOƒ‰ƒ€‚Ìd‚Ë‘‚«‚ðs‚Á‚½‚Æ‚±‚ëA—lX‚ȕΌõ•ÏŠ·‚𓯎ž‚É“¾‚邱‚Æ‚ª‚Å‚«‚½B‚Ü‚½A‰äX‚ÍŒõˆÙ«‰»”½‰ž‚ðŽ¦‚·Þ—¿‚Æ‚µ‚Ä’m‚ç‚ê‚éƒAƒ]ƒxƒ“ƒ[ƒ“‚ð—p‚¢‚ĕΌõƒzƒƒOƒ‰ƒ€‚Ì‹L˜^‚ðŽŽ‚Ý‚½B’ᕪŽq‰t»‚Æ‚•ªŽq‰t»‚Ì•¡‡‘̂ɃAƒ]F‘f‚ðƒh[ƒv‚µA•ÎŒõ•Ï’²‚ðÆŽË‚µ‚½‚Æ‚±‚ëA‰~•¡‹üÜ‚à’¼ü•¡‹ü܂Ɠ™‚µ‚¢Œø—¦‚Å—U‹N‚·‚邱‚ƂɬŒ÷‚µ‚½B‚Ü‚½A‚±‚ê‚ç‚ÌŽÀŒ±Œ‹‰Ê‚ɂ‚¢‚ăWƒ‡[ƒ“ƒY–@‚ð—p‚¢‚½‰ðÍ‚ðs‚¢A—˜_“I‚Éà–¾‚·‚邱‚Æ‚ª‚Å‚«‚½B

–â‚¢‡‚í‚¹æ Œ´ŽqƒGƒŒƒNƒgƒƒjƒNƒXƒOƒ‹[ƒv@’·’Jì@„i“àü4734j
‘æ53‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 11th October, 2005, 11:00-
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231, 232, Namiki Site
u‰‰ŽÒ Dr. Claus Ascheron
Š‘® Springer-Verlag
u‰‰‘è–Ú Scientific Creativity and Productivity
ƒAƒuƒXƒgƒ‰ƒNƒg

It is the aim of every scientist to work creatively and productively.

In the presentation the following topics are discussed:

  1. What is scientific creativity?
  2. Innate creativity
  3. Everyday creativity
  4. Personal qualities for successful working
  5. Influence of the working style on productivity and creativity
  6. Influence of personal working conditions
  7. Social factors
  8. Role of competition and criticism
  9. Knowledge as a basis for creativity
  10. Role of stress
Creativity of different hours of the day.
–â‚¢‡‚í‚¹æ Œ´ŽqƒGƒŒƒNƒgƒƒjƒNƒXƒOƒ‹[ƒv@‘åì@—SŽii“àü4739j
‘æ52‰ñNMLƒZƒ~ƒi[, 2006
ŠJÓúŽž 20th September, 2005, 14:00-15:00
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231, 232, Namiki Site
u‰‰ŽÒ Dr. Achim Walter Hassel
Š‘® Max-Planck Institute for Microstructure PhysicsHead of the Research group "Electrochemistry and Corrosion" Department of Interface Chemistry and Surface Engineering,
Max-Planck-Institut fur Eisenforschung
u‰‰‘è–Ú Self organised nanostructures from directionally solidified eutectics
ƒAƒuƒXƒgƒ‰ƒNƒg

Nanostructures show improved properties when compared to conventional materials, and open the possibility of their application in fields such as high activity catalysts, chemical and biological sensors, and magnetoelectronic and optoelectronic devices. For the fabricated nanostructures to show reproducible patterns and characteristic within individual samples, a method must be developed that allows the production of self-organised nanostructures (SONS). These structures present identical physical characteristics and are well organised into the matrix, thus making them ideal candidates for use in arrays for nanosensing or nanoelectronic devices. The production of such SONS is presented in this work by use of directional solidification of eutectics. One of the crucial factors in the synthesis of nanowires is the microstructural control governed by the kinetics of solidification process. Therefore, the thermodynamic aspects of eutectic growth were investigated during this study. Initially, the principles of crystallisation were applied to eutectic growth in order to derive main variables that control the process (Figure 1).

Then, the influence of each variable on the microstructure was analysed, as well as the correlation between them. Finally, the applicability of the thermodynamic analysis was demonstrated on the pseudobinary NiAl-Re eutectic system. For this purpose, NiAl-1.5at%Re eutectic alloys were directionally solidified using a constant growth rate, V, and different temperature gradients, G, as well as with a constant temperature gradient and different growth rates in the Bridgman-type directional solidification furnace. The interphase spacing, l, was measured from transverse sections of the specimen. The variations of l with respect to G and V were determined by using linear regression analysis. In addition, the dependence of l on the undercooling, ĢT, was also analysed. Moreover, the variations of ĢT with V at constant G, and with G at constant V were investigated. The results obtained in this work have been compared with the Jackson?Hunt theory of eutectic growth. The selective etching of one of the eutectic components allowed the fabrication of highly ordered nanostructures. Thus, oxidation of the NiAl matrix in acidic solutions (HCl:H2O2, H2SO4) resulted in the formation of faceted rhenium nanowires, which can subsequently be applied for the preparation of nanodisc electrode arrays by embedding the nanowires into a polymer and grinding until the wires are exposed (Figure 2). The selective etching of the rhenium wires, on the other hand, was achieved by electrochemical polarisation of the sample at 0.4 V in neutral acetate buffer, yielding the formation of nickel and aluminium oxides (which passivate the alloy surface) wherein the rhenium is dissolved as perrhenate. The obtained nanopores remain electrochemically active, enabling their use in the deposition of alternative metals (gold, platinum) for the formation of nanoelectrodes arrays (Figure 2). The reduction on the electrode area inherent in the use of such nanoelectrodes increases the signal-to-noise ratio, thus favouring the system application in analytical sensors.
–â‚¢‡‚í‚¹æ ƒiƒm“d‹CŒv‘ªƒOƒ‹[ƒv@’†ŽR@’mMi“àü8481j
‘æ51‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 2005”N10ŒŽ4“úi‰Îj 10:00-12:00
ŠJÃêŠ •¨Ž¿EÞ—¿Œ¤‹†‹@\@÷’n‹æ@2Fƒ[ƒ~ƒi[ƒ‹Žº
u‰‰ŽÒ ¬‹v•Û@Ll Ž
Š‘® ’}”g‘åŠw”—•¨Ž¿‰ÈŠwŒ¤‹†‰È
u‰‰‘è–Ú ƒƒ]ƒXƒRƒsƒbƒNƒ`ƒƒƒlƒ‹‚É‚¨‚¯‚鎥‘©ƒtƒ[ƒ_ƒCƒiƒ~ƒNƒX
ƒAƒuƒXƒgƒ‰ƒNƒg

ƒƒ]ƒXƒRƒsƒbƒNƒ`ƒƒƒlƒ‹‚ɕ‚¶ž‚ß‚½‘æ“ñŽí’´“`“±‘̂̎¥‘©ƒtƒ[“Á«‚ð‚²Ð‰î‚·‚éB’´“`“±‘̂̃sƒ“Ž~‚ß“Á«‚Ì‹­Žã‚ð—˜—p‚µ‚½‰äX‚̃tƒ[ƒ`ƒƒƒlƒ‹‚Å‚ÍAŽ¥ê‚̑傫‚³‚¾‚¯‚ÅAƒ`ƒƒƒlƒ‹“à‚ÌŽ¥‘©ŠiŽq‚ÌŒú‚³‚ð‹Í‚©‚P‘w‚©‚ç\”‘w‚܂ŧŒä‚Å‚«‚邾‚¯‚łȂ­Aƒ`ƒƒƒlƒ‹“à‚ÌŽ¥‘©ŠiŽq\‘¢‚ðA’˜‚µ‚½‹K‘¥ŠiŽqó‘Ô‚©‚痂ꂽƒAƒ‚ƒ‹ƒtƒ@ƒXó‘Ԃ܂Ōn““I‚ɕω»‚³‚¹‚邱‚Æ‚ª‚Å‚«‚éB‰äX‚ÍAƒ‚[ƒhƒƒbƒNƒeƒNƒjƒbƒN‚ðŽg‚Á‚ÄAŠOŽ¥ê‚ɑ΂µ‚Ä1‘w‚¸‚ŠK’ió‚ÉŒú‚³‚ª‘‰Á‚·‚鎥‘©ŠiŽq‚̬’·‰ß’ö‚âA‹Í‚©”‘w‚ÌŽ¥‘©ŠiŽq‚ªŽ¦‚·€ˆêŽŸŒ³“I‚ȃtƒ[“Á«A—‚ê‚½Ž¥‘©Œn‚ªŽ¦‚·ƒWƒƒƒ€ƒtƒ[“Á«‚Ȃǃƒ]ƒXƒRƒsƒbƒNƒXƒP[ƒ‹‚É‚¨‚¯‚éV‚µ‚¢“®“I“Á«‚ðŽÀŒ±“I‚É–¾‚ç‚©‚É‚µ‚Ä‚«‚½Bu‰‰‚Å‚ÍAŒvŽZ‹@ƒVƒ…ƒ~ƒŒ[ƒVƒ‡ƒ“ASTM‚ÌŒ‹‰Ê‚à‡‚í‚¹‚Ä‚²Ð‰î‚µ‚½‚¢B
Leiden‘åŠwKamerling OnnesŒ¤‹†ŠP.H.Kes ‹³Žö•À‚Ñ‚ÉR.Besseling”ŽŽm‚Ƃ̋¤“¯Œ¤‹†‚Å‚ ‚éB

Žå‚ÈŽQl•¶Œ£@
N. Kokubo R. Besseling, V. M. Vinokur and P.H. Kes, Phys. Rev. Lett. 88, 247004 (2002).
N. Kokubo, R. Besseling, and P.H. Kes Phys. Rev. B 69, 064504 (2004).
R. Besseling, N. Kokubo, and P. H. Kes Phys. Rev. Lett. 91, 177002 (2003).

–â‚¢‡‚í‚¹æ ƒiƒm—ÊŽq—A‘—ƒOƒ‹[ƒv@‰FŽ¡@i–çi“àü5512j
‘æ50‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 31st? August, 2005, 13:30-14:30
ŠJÃêŠ Main Conference room on the 2nd floor, Sakura Site
u‰‰ŽÒ Dr. Malik Maaza
Š‘® Chairman, NANOsciences AFrican NETwork
u‰‰‘è–Ú Nanomaterials in South Africa
ƒAƒuƒXƒgƒ‰ƒNƒg

Nanosciences, the recent emerging global & multipolar discipline, represent a new integrated approach to materials sciences & engineering. Research at the nano-scale frontier is unified by the human society need to develop knowledge, techniques & expertise on the fundamental atomic & molecular interactions fitting with the new millennium socio-economic pressures. Within the South African landscape, the scientific & industrial community has recently established its nanoscience initiative so called SANi: South African Nanotechnology initiative. Key laboratories have established nanomaterials oriented programs.Within the Japan-South African S&T bilateral agreement, this seminar is intended to present an overview on the nanomaterials activities carried out at the Nanosciences Laboratories of the Materials Research Group of iThemba LABS, a National facility of the National Research Foundation in the Cape region, South Africa.

–â‚¢‡‚í‚¹æ ‹­Ž¥êŒ¤‹†ƒZƒ“ƒ^[@Œ´ŒcŽqiext.5440j
‘æ49‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 227th May, 2005, 14:00-15:00
ŠJÃêŠ Nano-Bio Materials Research Build., Room 431-432, Namiki Site
u‰‰ŽÒ Benjamin Cho
Š‘® Dept. of Materials Science & Engineering, University of Illinois at Urbana-Champaign
u‰‰‘è–Ú Effect of phosphorus doping on morphology, surface segregation, and film growth kinetics of homoepitaxial GS-MBE Si(001) from Si2H6 and PH3
ƒAƒuƒXƒgƒ‰ƒNƒg

The effects of P doping at concentrations Cp = 3~1019 cm-3 on the growth kinetics, surface morphological evolution, and D2 desorption of Si(001):P layers grown at temperatures Ts = 500-900 ‹C by gas-source molecular-beam epitaxy from Si2H6 and PH3 have been investigated. With increasing PH3:Si2H6 flux ratio JP/Si, we observe a decrease in the Si (001) growth rate RSi:P, accompanied by increased surface roughening and pit formation. At constant JP/Si, film growth rates increase with increasing growth temperature Ts. Incorporated P concentrations Cp in Si(001) layers initially increase with increasing Ts, reach a maximum at 700 ‹C, and decrease at Ts > 700 ‹C. In-situ isotopically tagged D2 temperature programmed desorption (TPD) measurements of both as-deposited Si(001):P and P-adsorbed Si(001) reveal ƒÀ1 and ƒÀ2 peaks due to D2 desorption from Si monohydride and dihydride species, respectively, as well as the formation of a third peak ƒÀ3 corresponding to D2 desorption from Si:P dimers. TPD spectra of phosphorus-adsorbed Si display a decrease in the total surface dangling bond density following P adsorption, with ƒÆp reaching a maximum of `1 ML at Tads = 600 ‹C. From measurements of ƒÆp as a function of Cp we obtain a P surface segregation enthalpy ƒ¢Hs= -0.86 eV. We model surface coverage and incorporated dopant concentration using a simple transition-state kinetic model, together with measured kinetic parameters, which results in an excellent fit to the experimental data.

–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹—§‘Ì”z’uG@‘å–Ñ—˜Œ’Ž¡i“àü8878j
‘æ48‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 2005”N7ŒŽ25“úiŒŽj 16:00-17:00
ŠJÃêŠ •¨Ž¿EÞ—¿Œ¤‹†‹@\@•À–Ø’n‹æ ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“2F (231A232†Žº)
u‰‰ŽÒ _“c »\ Ž
Š‘® Max-Planck Institute for Microstructure Physics’}”g‘åŠw”—•¨Ž¿‰ÈŠwŒ¤‹†‰ÈAŠwÛ•¨Ž¿‰ÈŠwŒ¤‹†ƒZƒ“ƒ^[
u‰‰‘è–Ú ƒƒ]ƒXƒRƒsƒbƒN’´“`“±‘̂ɂ¨‚¯‚éV‚µ‚¢‰QŽ…‚ÌŠÏ‘ª
ƒAƒuƒXƒgƒ‰ƒNƒg

u‰Qv‚ÍŽ©‘RŠE‚Ì—lX‚Èê–ʂŌ©‚ç‚ê‚é••Õ“I‚ÈŒ»Û‚Å‚ ‚éFð‚𔲂¢‚½…‘…‚Ì…A––å‚̉Q’ªA‚‚ނ¶•—A‘ä•—A—³ŠªcB‰Q‚Í—ÊŽq—ÍŠw‚Ì¢ŠE‚Å‚àŒ©‚ç‚ê‚éF‘æ‚QŽí’´“`“±‘ÌA’´—¬“®‘ÌAƒ{[ƒY|ƒAƒCƒ“ƒVƒ…ƒ^ƒCƒ“‹ÃkŒnB—ÊŽq—ÍŠw“I‚ȉQ‚ÍŒn‚ð“Á’¥•t‚¯‚é’˜ƒpƒ‰ƒƒ^‚ÌˆÊ‘Š•Ï‰»‚Å‚ ‚ç‚킳‚êA”g“®ŠÖ”‚̈ꉿ«‚ɑΉž‚µ‚ÄˆÊ‘Š‚Í‰Q‚Ì’†S‚ÌŽü‚è‚Å2np•ω»‚·‚éBƒGƒlƒ‹ƒM[‚ªÅ¬‚ɂȂéðŒ‚©‚ç’Êí‚Ín = 1‚̉Q‚ªŠÏ‘ª‚³‚ê‚é‚̂ł ‚邪A“ÁŽê‚Ȋ‹«‰ºA—Ⴆ‚΃TƒCƒY‚ª’´“`“±ƒRƒq[ƒŒƒ“ƒX’·‚⎥êN“ü[‚³‚Æ“¯’ö“x‚̃ƒ]ƒXƒRƒsƒbƒN’´“`“±‘̂ɂ¨‚¢‚Ä‚ÍA‰Qi’´“`“±‘Ì‚ÌꇂÍu‰QŽ…v‚ƂȂéj‚ÌŽü‚è‚ÅˆÊ‘Š‚ª2p‚Ì•¡””{•ω»‚·‚é‹‘å‚ȉQ‚Ì‘¶Ý‚ª—\Œ¾‚³‚ê‚Ä‚¢‚éB‚Ü‚½•¡”‚̉QŽ…‚ª‡‘Ì‚µ‚½‚èA”z’u‚ð•Ï‚¦‚½‚è‚·‚邱‚Æ‚à‹N‚±‚肤‚éB–{u‰‰‚Å‚ÍA‚±‚̂悤‚ÈV‚µ‚¢‰QŽ…ó‘Ô‚ðЉ‚邯‚Æ‚à‚ÉAŋ߉äX‚Ìs‚Á‚½‹‘å‚ȉQŽ…‚Ì‘¶Ý‚ðØ–¾‚·‚éŽÀŒ±‚ɂ‚¢‚Äq‚ׂéBƒƒ]ƒXƒRƒsƒbƒN’´“`“±‘̂̂à‚ÂV‚µ‚¢•¨—Œ»Û‚ÌŠg‚ª‚è‚É‹»–¡‚ðŽ‚Á‚Ä‚¢‚½‚¾‚¯‚ê‚ÎK‚¢‚Å‚·B

–â‚¢‡‚í‚¹æ ƒiƒm“d‹CŒv‘ªƒOƒ‹[ƒv@“à‹´@—²i“àü4150j
‘æ47‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 14th June, 2005, 15:00-17:00
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231-232, Namiki Site
u‰‰ŽÒ Prof. Ignatius Tsong
Š‘® Max-Planck Institute for Microstructure PhysicsDepartment of Physics & Astronomy, Arizona State University
u‰‰‘è–Ú Nucleation and growth of epitaxial ZrB2(0001) on Si(111) for III-nitride applications
ƒAƒuƒXƒgƒ‰ƒNƒg

Silicon, which is abundant, cheap, and non-toxic, would be an ideal substrate material for III-nitrides.? Unfortunately, Si not only has a large lattice mismatch with GaN, it also absorbs visible and UV light.? In addition, the mismatch between the thermal expansion coefficients of Si and that of GaN is also large.? We have shown that the solution to these deficiencies lies in the use of a buffer layer of ZrB2(0001) on Si(111).? The in-plane lattice constant of ZrB2(0001), a = 3.169 A, has only 0.6% mismatch with that of GaN(0001) where a = 3.189 A; and a perfect match with that of Al0.26Ga0.74N.? The thermal expansion coefficients along the [1010] on the basal plane are also well matched between ZrB2 and GaN.? We report in situ and real-time studies of the epitaxial growth behavior of ZrB2(0001) on Si(111) using LEED and LEEM, and ex situ studies of the surface morphology and interfacial mismatch using AFM and XTEM.? The interface between ZrB2(0001) and Si(111) is modeled theoretically by first-principles density functional theory calculations.? The most favorable interface consists of the ZrB2(0001) growing on a Si(111)-(ã3xã3)B surface with Zr-Si bonds at the interface.? The ZrB2 buffer layer is metallic and highly reflective, thus serving the dual role of providing electrical contact and eliminating any loss of emitted light from the active nitride layer.? Applications of the ZrB2/Si(111) substrate system for III-nitride growth show luminescence from band-edge emission comparable to or better than nitride layers grown on conventional sapphire substrates.

–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹Œ¤‹†Š@–ì@³˜ai“àü4180j
‘æ46‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 23rd May, 2005, 16:00-16:30 (-17:00 discussion)
ŠJÃêŠ Nano-Bio Materials Research Build., Room 431, Namiki Site
u‰‰ŽÒ Dr. Laura Lazzarini
Š‘® CNR-IMEM, Parma, Italy
u‰‰‘è–Ú Structural characterization of strain-balanced (SB) InGaAs/InGaAs/InP multi-quantum wells (MQWs) for thermophotovoltaic devices
ƒAƒuƒXƒgƒ‰ƒNƒg

SB epitaxy is very critical when the well and barrier misfit is of the order of 1% resulting in the onset of the wavy growth mode. TEM, HRXRD, AFM, XRT, were used to study the separate role of the well/barrier misfit strain and the growth temperature on the wavy growth onset in SB MQWs by varying the well and barrier misfit in the 0.5%-1.5% range. An empirical model to predict the maximum number of layers that can be grown without modulations and defects, as a function of the elastic energy per period and of the growth temperature is presented.
The preliminary results on the optical study of quasi-1D SnO2 single nanostrings grown on Al2O3, SiO2 and Si substrates for gas sensors and visible LEDs will be also shown.

–â‚¢‡‚í‚¹æ ƒiƒm“dŽqŒõŠwÞ—¿ƒOƒ‹[ƒv@ŠÖŒû—²Žji“àü4297j
‘æ46‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 23rd May, 2005, 15:00-16:00
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231, Namiki Site
u‰‰ŽÒ Prof. Giancarlo Salviati
Š‘® CNR-IMEM, Parma, Italy
u‰‰‘è–Ú CL and PL studies on the interplay of polarization fields and free carrier screening in III-Nitrides QWs and QDs
ƒAƒuƒXƒgƒ‰ƒNƒg

At first, a short introduction is given on the Italian National Research Council and on the main projects carried out at IMEM. ?
The interplay of polarization fields and free carrier screening in In x Ga 1-x N/GaN (0.3<x<0.7) MQWs are studied by combining photoluminescence and cathodoluminescence. Efficient field screening is demonstrated in CL steady-state high-injection conditions and in PL time-resolved experiments at the maximum excitation density. Under recovered nearly flat band conditions, quantum confinement effects are revealed and a high and possibly composition-dependent bowing parameter is extrapolated.

–â‚¢‡‚í‚¹æ ƒiƒm“dŽqŒõŠwÞ—¿ƒOƒ‹[ƒv@ŠÖŒû—²Žji“àü4297j
‘æ45‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 27th May, 2005, 14:00-15:00
ŠJÃêŠ Nano-Bio Materials Research Build., Room 431, Namiki Site
u‰‰ŽÒ Dr. Peter Werner
Š‘® Max-Planck Institute for Microstructure Physics
u‰‰‘è–Ú SiGe nanostructures designed for efficient light emission
ƒAƒuƒXƒgƒ‰ƒNƒg

Low-dimensional semiconductor structures, in particular quantum dots (QD) have attracted
continuously increased interest from the viewpoints of both fundamental physics and device
applications. The concept of Stranski-Krastanov growth mechanism can successfully be
applied to generate self-assembled nano-structures not only for III-V heterostructures,
such as InAs/GaAs. Also the strained SiGe/Si system has become a subject of numerous
investigations (see, e.g. [1] and references there in). However, Si and Ge are
characterized by a fundamental indirect band gap in real space as well as in k-space,
which strongly reduces the recombination efficiency of carriers and, therefore,
the luminescence.
? Our approach on an effective light-emitting Si-Ge diode is based on a heterostructure,
which consists of a multi-quantum well structure including stacked Ge islands. The light,
wavelength of which is in the range of 1.5 to 1.6 ƒÊm, is emitted i) with higher intensity
compared to previously described structures and ii) at room temperature.
The heterostructure has grown by molecular beam epitaxy (MBE) as schematically seen Fig.1.
It consists of periodic pairs of thin Ge and Si layers, where the Ge layers have a thickness
of about 0.5 to 0.8 nm (less than the so-called critical Stranski-Krastanov thickness) and
a Si spacer of 5 nm, respectively.

–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹—§‘Ì”z’uƒOƒ‹[ƒv@ŽáŽR@—Ti“àü4403j
‘æ44‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 26th April, 2005, 14:00-15:30
ŠJÃêŠ Nano-Bio Materials Research Build., Room 231-232, Namiki Site
u‰‰ŽÒ

Dr. Stefan Foelsch

Š‘® Paul-Drude-Institut for Solid State Electronics, Berlin, Germany
u‰‰‘è–Ú Assembly and spectroscopy of atomic-scale surface structures by low-temperature STM: From monatomic chains to single-molecule/quantum wire contacts
ƒAƒuƒXƒgƒ‰ƒNƒg

Aside from local surface characterization, low-temperature scanning
tunneling microscopy (LT-STM) allows to manipulate adsorbed atoms and
molecules with atomic-scale precision. This combined approach makes
LT-STM a powerful experimental tool to explore fundamental electronic
processes in low-dimensional systems because it permits both to direct
and to probe quantum confinement. The experiments discussed in this talk
employ a Cu(111) substrate surface onto which straight monatomic chains
?(interatomic spacing 255 pm) are assembled from single Cu adatoms. We
find that these atom chains exhibit chain-localized states trapped in
the pseudogap of the Cu bulk bands and thus represent a clear-cut model
case of a one-dimensional quantum box. The concept of STM-based
manipulation can be also extended to construct Cu chain structures of
advanced complexity such as kinked and branched chains. Finally, the
attachment of single organic molecules will be addressed and the local
structure of these single-molecule/metal model junctions is discussed.

–â‚¢‡‚í‚¹æ Œ´ŽqƒGƒŒƒNƒgƒƒjƒNƒXƒOƒ‹[ƒv@ŸNˆä@—ºi“àü4736j
‘æ43‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 11th April, 2005, 14:30-16:30
ŠJÃêŠ Seminar Room on 8th Floor, Main Building at Sengen Site,
u‰‰ŽÒ 1. Ms. Jana Vejpravova
2. Prof. Vladimir Sechovsky
Š‘® 1. Faculty of Mathematics and Physics, Charles University
2. Faculty of Mathematics and Physics, Charles University
u‰‰‘è–Ú 1. Sol-gel fabricated CoFe2O4 nanocomposites: synthesis, characterization and magnetic properties
2. Physics of UCoAl - an itinerant 5f-electron metamagnet
ƒAƒuƒXƒgƒ‰ƒNƒg

J. Vejpravova

? Well-defined CoFe2O4 nanoparticles embedded in an amorphous SiO2 matrix have been
synthesized by the conventional sol-gel method, characterized by high-resolution electron
microscopy and investigated by Mossbauer 57Fe spectroscopy and magnetic measurements.
The mean particle diameter increases from 3 to 15 nm consistently with the temperature of
the subsequent annealing, which varied from 800 to 1100 Ž, respectively. At low
temperatures the magnetization curves show hysteresis. The maximum value of coercive field
HC ` 2.5 T (at 2 K) has been observed for the sample with largest particles. At elevated
temperatures the composites exhibit superparamagnetic behavior with the blocking
temperature TB. The value of TB increases with the mean particle size from ` 80 to 350 K, respectively. At temperatures above TB, the magnetization curves show no hysteresis and
follow the expected universal Langevin scaling of M/MS vs. ƒÊ0H/T. The results will be
analyzed and discussed within the Neel theory of supeparamagnetism.

Physics of UCoAl - an itenerant 5f-electron metamagnet
V. Sechovsky

? Physics of UCoAl as an archetype of the itinerant 5f-electron metamagnetism will be
discussed. The ground state of UCoAl is paramagnetic but the c-axis susceptibility is
exchange enhanced and shows a broad maximum Tmax = 20 K. At lower temperatures this
compound undergoes a metamagnetic transition to a ferromagnetic state with a U moment
of 0.3 ƒÊB. The critical field of the transition is low, Bc < 1 T, but the magnetic
field should be applied along the c-axis. In the basal plane a Pauli paramagnetic behavior
is observed. The low-temperature resistivity of UCoAl in zero field is proportional to
T5/3 but in the metamagnetic state resistivity data exhibit the T2 dependence.
The critical parameters Tmax and Bc are very sensitive to external pressure and alloying.
Both, Tmax and Bc values are increasing with increasing pressure and at a high enough
pressure the metamagnetism is suppressed and a conventional paramagnetism is promoted.
The resistivity data can be approximated by the aTƒ¿ dependence, where the exponent ƒ¿
increases with pressure with a tendency to a linear temperature dependence of resistivity.
On the other hand, application of a c-axis uniaxial stress yields reduction of the critical
field Bc. When the Bc value crosses zero a spontaneous magnetic moment (ferromagnetism)
emerges and the T2 scaling of low-temperature is observed.
A scenario for UCoAl will be discussed considering pressure and alloying effects on the
5f-ligand hybridization, which involves both, the 5f-electron moment formation and thehybridization mediated exchange interactions.

–â‚¢‡‚í‚¹æ ƒiƒm•¨«ƒOƒ‹[ƒv –kàV‰p–¾@i“àü2818j
‘æ42‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 15th March, 2005, 10:00-12:00
ŠJÃêŠ Main Conference Room on 2nd Floor, Sakura Site, NIMS
u‰‰ŽÒ Prof. Fritz C. Herlach
Š‘® Katholieke Universiteit Leuven and Huazhong University of Science and Technology
u‰‰‘è–Ú State of the art of pulsed magnets
ƒAƒuƒXƒgƒ‰ƒNƒg

The design and operation of modern pulsed magnets will be reviewed.?
This is focused on the Leuven design with optimized fibre composite
reinforcement, and on the development of new materials, both strong wires and fibre composites.
The reason for building dual magnet systems will be explained, with the respective advantages
and limitations.? As an example, the European ARMS magnet will be discussed.?A survey of existing and new magnet laboratories will be given.

–â‚¢‡‚í‚¹æ ƒiƒm•¨«ƒOƒ‹[ƒv ‚‘@³@i“àü5416j
‘æ41‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 2005”N3ŒŽ7“úiŒŽj 14:00`15:00
ŠJÃêŠ •¨Ž¿EÞ—¿Œ¤‹†‹@\@•À–Ø’n‹æ@ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“ (231,232†Žº)
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‘æ40‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 2005”N2ŒŽ8“úi‰Îj 14:30`15:30
ŠJÃêŠ •¨Ž¿EÞ—¿Œ¤‹†‹@\@•À–Ø’n‹æ@ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“ (231ƒZƒ~ƒi[Žº)
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ƒAƒuƒXƒgƒ‰ƒNƒg

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–â‚¢‡‚í‚¹æ ƒiƒm“d‹CŒv‘ªƒOƒ‹[ƒv@’†ŽR@’mMi“àü4129j
‘æ39‰ñNMLƒZƒ~ƒi[, 2005
ŠJÓúŽž 2005”N”N1ŒŽ28“úi‹àj 10:00`11:30
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–â‚¢‡‚í‚¹æ ‹­Ž¥êŒ¤‹†ƒZƒ“ƒ^[@–،ˋ`—Ei“àü5024j
‘æ38‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž December 15th, 2004, 14:00-15:00
ŠJÃêŠ Nano-Bio Materials Research Bld. 4F Seminor Room, Namiki Site
u‰‰ŽÒ Prof. Norifumi FUJIMURA
Š‘® Department of Applied Material Science, Graduate School of Engineering, Osaka Prefecture University
u‰‰‘è–Ú Development of Multi-Functional Materials for Future Devices
ƒAƒuƒXƒgƒ‰ƒNƒg

The magnetoelectric effect presumed to exist by Pierre Curie? - i.e. the induction of a
magnetization by means of an electric field and induction of a polarization by means of a
magnetic field - attracted a great deal of interest in 1960s-70s. In recent years, relevant
studies on magnetic ferroelectrics or dielectric magnets, which are called as multiferroic
materials have come to the fore again. Magnetic Semiconductors, on the other hand,
are getting recognized as one of the most important spintronics materials from the first
discovery of III-V diluted magnetic semiconductors.
Here, I review the recent status of multiferroics in addition to the development of Si
based DMS. Eventually, the concept of multiferroic-DMS gate FETs will be described.
We have developed YMnO3 based ferroelectric gate FETs to overcome the retention problem
of the transistor. After the brief introduction of ferroelectric gate FET and the
advantage of material for the device, the dielectric anomalies at around Neel point of
YMnO3 epitaxial films deposited by pulsed laser deposition method are described.
The relationship between the magnetic structure and the dielectric properties are discussed
in terms of the temperature dependences of magnetization and dielectric permittivity.
The control of ferroelectric domain switching by applying external magnetic field is also
presented. I will also briefly touch to the results on newly developed Ba(Fe,Zr)O3 [10]
and Ba(Co,Mn)O3 dielectric ferromagnets. As a IV group DMS material, I introduce the Cedoped Si films, which shows large magneto-resistance and ferromagnetic behavior.

–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹—§‘Ì”z’uG@’m‹ž –L—Ti“àü4725)
‘æ37‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž 2004”N12ŒŽ9“ú(–Ø) 14:00`16:00 (15:00‚©‚çƒfƒBƒXƒJƒbƒVƒ‡ƒ“)
ŠJÃêŠ •À–Ø’n‹æ ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“ 2ŠK 231/232Žº
u‰‰ŽÒ ‰zì F”Í ‹³Žö
Š‘® ‘åã“d‹C’ÊM‘åŠw ƒGƒŒƒNƒgƒƒjƒNƒXŠî‘bŒ¤‹†Š
u‰‰‘è–Ú •úŽËŒõ‚ð—˜—p‚µ‚½Œõ“dŽqŒ°”÷‹¾‚ÌV“WŠJLEEM/PEEM‚ð—p‚¢‚½•\–ÊŒ¤‹†‚Æ•úŽËŒõPEEM‚Ì•ª‰ð”\Œüã‚ÌŽŽ‚Ý
ƒAƒuƒXƒgƒ‰ƒNƒg ’áƒGƒlƒ‹ƒM[“dŽqŒ°”÷‹¾(LEEM)‚ÆŒõ“dŽqŒ°”÷‹¾(PEEM)‚ÍAV‚µ‚¢•\–Ê“dŽqŒ°”÷‹¾‚Æ‚µ‚Ä’–Ú‚ðW‚߂Ă¢‚éB“Á‚É“®“I‚É•\–ʂ̉ߒö‚ðŠÏŽ@‚Å‚«‚邱‚ÆA‹y‚ÑA¡‚܂œ¾‚ç‚ê‚È‚©‚Á‚½î•ñ‚ÌŒ°”÷‘œ‚ª“¾‚ç‚ê‚é“™‚̑傫‚È’·Š‚ª‚ ‚éB
–{u‰‰‚Å‚ÍALEEMEPEEM‚ÌŠT—vA“¾‚ç‚ꂽÅV‚ÌŒ‹‰ÊA•À‚Ñ‚ÉAŽû·•Ⳃɂæ‚é‚•ª‰ð”\‰»‚ÌŽŽ‚Ý‚É‚Â‚¢‚ÄÚׂðq‚ׂéB
–â‚¢‡‚í‚¹æ ƒiƒmƒ}ƒeƒŠƒAƒ‹Œ¤‹†Š Š’· Â–ì ³˜a (“àü 4180)
‘æ36‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž 2004”N12ŒŽ7“ú(‰Î) 10:00`11:00
ŠJÃêŠ •À–Ø’n‹æ ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“ 4ŠK 431/432Žº
u‰‰ŽÒ Prof. A.J. Fisher
Š‘® Department of Physics and Astronomy and London Centre for Nanotechnology, University College London
u‰‰‘è–Ú New approaches to quantum information processing in condensed matter
ƒAƒuƒXƒgƒ‰ƒNƒg I will discuss some of the constraints on quantum information processing in condensed phases arising from (1) the technological limits of fabrication and measurement, and (2) the more fundamental competition between coherent and incoherent evolution of a quantum system, as expressed in the fluctuation-dissipation theorem [1]. I will describe how a new approach to the optical control of entangling interactions between quantum bits [2,3] may be able to optimize these constraints, and potentially produce relatively robust quantum gates in familiar semiconducting materials.
(1) Quantum computing in the solid state: the challenge of decoherence. A.J. Fisher, Phil. Trans. Roy. Soc. A 361 1441-1450 (2003).
(2) Optically driven silicon-based quantum gates with potential for high-temperature operation. A M Stoneham, A J Fisher and P T Greenland. J. Phys.: Condens. Matter 15 L447-L451 (2003).
(3) Avoiding entanglement loss when two-qubit quantum gates are controlled by electronic excitation. R. Rodriquez, A,J. Fisher, P.T. Greenland and A.M.Stoneham. J. Phys.: Conden. Matt. 16 2757-2772 (2004)
–â‚¢‡‚í‚¹æ ƒiƒmƒA[ƒLƒeƒNƒ`ƒƒ[ƒOƒ‹[ƒv ŽO–Ø ˆêŽi
ŒvŽZÞ—¿‰ÈŠwŒ¤‹†ƒZƒ“ƒ^[ ‘å–ì —²‰›
ICYS David Bowler
‘æ35‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž 2004”N11ŒŽ25“ú(–Ø) 11:00`12:00
ŠJÃêŠ çŒ»’n‹æ Œ¤‹†–{ŠÙ 8ŠK ƒZƒ~ƒi[Žº
u‰‰ŽÒ Dr. Herve Menard
Š‘® Department of Physics, University of York, Heslington
u‰‰‘è–Ú An improved metastable de-excitation pectrometer using laser-cooling techniques
ƒAƒuƒXƒgƒ‰ƒNƒg Details of a new approach for performing metastable de-excitation spectroscopy will be presented. A beam of metastable (23S) helium atoms, produced in a hollow cathode dc discharge, is collimated and subsequently focused using Doppler cooling of the 23S1-23P2 transition at 1083 nm, forming an intense probe of up to 1~1012 atomss-1cm-2. The large distance between the source and the sample means that the beam is relatively free of UV photons and 21S metastable atoms, removing the need for quench lamps and chopper wheels. As well as providing a clean high intensive source, the well defined nature of the beam is a necessary step towards using more sophisticated laser-cooling techniques with the ultimate aim to producing a metastable helium microscope. Examples of MDS and UPS spectra from Si(111) and Cu(111) will be shown.
–â‚¢‡‚í‚¹æ ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“ƒOƒ‹[ƒv ŽR“à ‘× (029-851-3354 “àü6667)
‘æ34‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž 2004”N11ŒŽ24“ú(…) 14:30`15:30
ŠJÃêŠ •À–Ø’n‹æ ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“2F 232†Žº
u‰‰ŽÒ ‚é ‘å•ã Ž
Š‘® ‹ž“s‘åŠw‘åŠw‰@—ŠwŒ¤‹†‰È‰»ŠwêU(‰»ŠwŒ¤‹†Š)
u‰‰‘è–Ú STM‚É‚æ‚é—L‹@•ªŽq‘½‘w–Œ¬’·‰Šú‰ß’ö‚ÌŒ¤‹†
ƒAƒuƒXƒgƒ‰ƒNƒg —L‹@•ªŽq‚ÌŒ‹»¬’·‚É‚¨‚¢‚ÄAƒGƒsƒ^ƒLƒVƒƒƒ‹¬’·‚ͬ’·‹@\Ž©‘̗̂‰ð‚ª‹‚ß‚ç‚ê‚Ä‚¢‚邯“¯Žž‚Ƀiƒmƒtƒ@ƒuƒŠƒP[ƒVƒ‡ƒ“‚ւ̉ž—p‚àŠú‘Ò‚³‚ê‚éB‚»‚±‚ÅAŠî”Âã‚Ì‘æˆê‘w‚̋NJî•ñ‚ðŠÏŽ@‚Å‚«‚éSTM (Scanning Tunneling Microscopy)‚É‚æ‚èAƒGƒsƒ^ƒLƒVƒƒƒ‹¬’·‚ÉÅd—v‚Å‚ ‚邯l‚¦‚ç‚ê‚éŠî”Âã‚ł̑æˆê‘w‚ª·‚ñ‚ɉðÍ‚³‚ê‚Ä‚«‚½B‚µ‚©‚µA‘æˆê‘w‚©‚炳‚ç‚ɬ’·‚·‚é‰ß’ö‚Å‚ÌA\‘¢•ω»A\‘¢ŠÉ˜aA”zŒü•ω»AŒ`‘Ԃ̕ω»‚Ȃǂɂ‚¢‚Ä‚ÌÚׂȒmŒ©‚Í­‚È‚¢B‚»‚±‚ÅA–{Œ¤‹†‚ł͑æˆê‘w‚ɂ‚­‘æ“ñ‘w‚ðSTM‚ÅŠÏŽ@‚·‚邱‚ƂƂµ‚½B‚Ü‚¸A‘æˆê‘w‚Æ‘æ“ñ‘w‚Ì•ªŽq‚ª“¯‚¶‚Å‚ ‚éhomo-epitaxy‚ɂ‚¢‚ÄA’·½óƒWƒAƒZƒ`ƒŒƒ“•ªŽq‚ð—p‚¢‚ÄŒ¤‹†‚ðs‚Á‚½B‚±‚±‚łͬ’·‰ß’ö‚ð—eˆÕ‚É‚»‚ÌêŠÏŽ@‚Å‚«‚éŒÅ‰tŠE–ʬ’·–@‚ð‘I‘ð‚µ‚½B‚»‚ÌŒ‹‰ÊA‘æ“ñ‘wˆÈ~‚Ì\‘¢‚Í‘æˆê‘w‚Æ“¯‚¶‚Å‚ ‚é‚à‚Ì‚ÌA‚»‚ÌŒ`‘Ô‚ª‘S‚­ˆÙ‚Ȃ邱‚Æ‚ª–¾‚ç‚©‚ƂȂÁ‚½B‘æˆê‘w‚Ì•½‹ÏƒhƒƒCƒ“ƒTƒCƒY‚ª”\nm‚Å‚ ‚é‚̂ɑ΂µA‘æ“ñ‘wˆÈ~‚ł͔•Snm‚Æ‹‘å‚È‚à‚̂ƂȂÁ‚½‚̂ł ‚éB‚±‚ê‚Í^‹óö’…–Œ‚É•C“G‚·‚é‚©‚»‚êˆÈã‚̃TƒCƒY‚Å‚ ‚èA^‹óö’…–@‚Ȃǂɂ¨‚¯‚é—L‹@•ªŽq‚Ì”M—ò‰»‚╪‰ð‚ð‹N‚±‚³‚È‚¢ŒÅ‰tŠE–ʬ’·–@‚ÅŽÀŒ»‚Å‚«‚½B‚Ü‚½A“¯‚¶’·½ó•ªŽq‚̃XƒeƒAƒŠƒ“Ž_‚ÌꇂàA‘æ“ñ‘w‚ª‘åƒhƒƒCƒ“‚ðŒ`¬‚·‚邱‚Ƃ𖾂炩‚É‚µ‚½B“¯Žž‚ÉAƒXƒeƒAƒŠƒ“Ž_‚ł͑æˆê‘w‚Æ‘æ“ñ‘w‚Ì\‘¢‚ªˆÙ‚Ȃ邱‚Ƃ𖾂炩‚É‚µ‚½B‚±‚ê‚ÍAŠE–ʂł̃Gƒsƒ^ƒLƒVƒƒƒ‹¬’·‚É‚¨‚¯‚é˜c‚݂̊ɘa‚ª‹}s‚És‚í‚ꂽ‚½‚߂ł ‚邯Œ‹˜_‚µ‚½B‚³‚ç‚ÉA‘æˆê‘w‚Æ‘æ“ñ‘w‚Ì•ªŽq‚ªˆÙ‚È‚éhetero-epitaxy‚̉Šú‰ß’ö‚ɂ‚¢‚Ă̌¤‹†‚ðs‚Á‚½B‚±‚±‚ł̓wƒeƒ‚Ȭ’·‚ÌŒn‚Æ‚µ‚Ä’·½óƒWƒAƒZƒ`ƒŒƒ“‚âƒAƒ‹ƒJƒ“‘æˆê‘wã‚ÉCu-phthalocyanine‚Ì‘æ“ñ‘w‚𬒷‚³‚¹‚½B¬’·‚Ì’†ŠÔó‘Ô‚Æ‚µ‚Ä‘æˆê‘w‚ðbuffer-layer‚Æ‚µ‚½“ÁˆÙ‚È\‘¢‘ÌŒ`¬‚ªŒ©‚ç‚êACu-phthalocyanine•ªŽq‚ªˆêŽŸŒ³“I‚É”z—ñ‚µ‚½\‘¢‚âƒ_ƒCƒ}[‰»‚µ‚½ó‘Ô‚ª\’z‚³‚ꂽB‚»‚̂悤‚Èó‘Ô‚ðŒo‚ÄA”zŒü‚É—h‚炬‚ð‚à‚Á‚½¬‚³‚È“ñŽŸŒ³ƒhƒƒCƒ“‚Æ‚µ‚Ĭ’·‚µAÅI“I‚É‚Íbuffer-layer‚Époint-on-line®‡‚µ‚½‘å‚«‚ÈCu-phthalocyanine“ñŽŸŒ³‘w‚ª¬’·‚·‚邱‚Ƃ𖾂炩‚É‚µ‚½B‘æˆê‘w‚̬’·‚É”ä‚ׂ邯‘½—l‚Ȭ’·‚ªŒ©‚ç‚ꂽ‚ªA‚±‚ê‚ÍA‘½—l‚È•ªŽqŠÔ‘ŠŒÝì—p‚Æbuffer-layer‚Æ‚Ì‘ŠŒÝì—p‚𔽉f‚µ‚½‚à‚̂ł ‚éB‚Ü‚½A‚±‚Ì‘ŠŒÝì—p‚ð—˜—p‚·‚ê‚΂³‚Ü‚´‚Ü‚È\‘¢‘Ì‚ð\’z‚Å‚«‚邱‚Æ‚ðˆÓ–¡‚µ‚Ä‚¢‚éB
–â‚¢‡‚í‚¹æ Œ´ŽqƒGƒŒƒNƒgƒƒjƒNƒXƒOƒ‹[ƒv ‘åì —SŽi (029-851-3354 “àü4739)
‘æ33‰ñNMLƒZƒ~ƒi[, 2004
ŠJÓúŽž 2004”N11ŒŽ17“ú(…) 10:30`12:00
ŠJÃêŠ •À–Ø’n‹æ ƒiƒmE¶‘ÌÞ—¿Œ¤‹†“ 431Žº
u‰‰ŽÒ Dr. Roberto Li Voti
Š‘® Dipartimento di Energetica, Universit di Roma "La Sapienza"
u‰‰‘è–Ú Inverse problems in Photoacoustic and Photothermal science
ƒAƒuƒXƒgƒ‰ƒNƒg Nondestructive evaluation of materials surface by photothermal and photoacoustic techniques with pulsed lasers has been the subject of many studies in the last few years. In this seminar, different kinds of inverse problems related to these experimental techniques will be introduced and their theoretical treatment shall be discussed.
–â‚¢‡‚í‚¹æ ƒiƒm•¨«ƒOƒ‹[ƒv ”—“c ˜a² (029-851-3354 “àü4184)
‘æ5‰ñNMLŒ¤‹†Œð—¬‰ï, 2004
ŠJÓúŽž 2004”N10ŒŽ26“ú(‰Î) 13:30`16:00
ŠJÃêŠ •À–Ø’n‹æ ‹¤“¯Œ¤‹†“ 4ŠK ‘å‰ï‹cŽº
”­•\ŽÒ 13:30-14:20  ƒiƒm—ÊŽqƒGƒŒƒNƒgƒƒjƒNƒX‚f  ‰H‘½–ì‹B  uBi-2212ŒÅ—LƒWƒ‡ƒZƒtƒ\ƒ“Ú‡v
14:20-15:10  ƒoƒCƒIƒiƒmƒ}ƒeƒŠƒAƒ‹‚f  rìG—Y  u¶‘Ì•ªŽq‚̃iƒm—ÍŠw‘ª’è‚ÌŒ»ó‚Æ“W–]v
15:10-16:00  ‹ÉŒÀêƒiƒm‹@”\‚f  “¡“c‘å‰î  u‘–¸ƒgƒ“ƒlƒ‹Œ°”÷‹¾‚É‚æ‚éƒiƒm‹@”\E•¨«’Tõv
–â‚¢‡‚í‚¹æ ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“ƒOƒ‹|ƒvŠÝ–{’¼Ž÷ (029-851-3354 “àü5433)
‘æ4‰ñNMLŒ¤‹†Œð—¬‰ï, 2004
ŠJÓúŽž 2004”N8ŒŽ3“ú(‰Î) 13:30`16:00
ŠJÃêŠ •À–Ø’n‹æ ‹¤“¯Œ¤‹†“ 4ŠK ‘å‰ï‹cŽº
”­•\ŽÒ 13:30-14:20  ƒiƒmƒ}ƒeƒŠƒAƒ‹—§‘Ì”z’u‚f  ŽáŽR—T  u—L‹@•ªŽq‚ð—p‚¢‚½’Pˆê“dŽq‘fŽq‚Æ‚»‚ÌŒõ§Œäv
14:20-15:10  ƒiƒm—ÊŽq—A‘—‚f  ‰FŽ¡i–ç  uBETSŒnŽ¥«—L‹@“`“±‘̂̒´“`“±v
15:10-16:00  Œ´ŽqƒGƒŒƒNƒgƒƒjƒNƒX‚f  Ž›•”ˆê–í  uŒ´ŽqƒXƒCƒbƒ`‚ÌŠJ”­‚Æ‚»‚Ì»•i‰»“W–]v
–â‚¢‡‚í‚¹æ ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“ƒOƒ‹|ƒvŠÝ–{’¼Ž÷ (029-851-3354 “àü5433)
‘æ3‰ñNMLŒ¤‹†Œð—¬‰ï, 2004
ŠJÓúŽž 2004”N3ŒŽ9“ú(‰Î) 13:30`16:00
ŠJÃêŠ ÷’n‹æ Œ¤‹†“ 2ŠK ‘å‰ï‹cŽº
”­•\ŽÒ 13:30-14:20  ƒiƒm“d‹CŒv‘ª‚f  Vƒ–’J‹`—²  u‘½’Tj‘–¸ƒgƒ“ƒlƒ‹Œ°”÷‹¾‚ÌŠJ”­‚Æ¡Œã‚Ì“WŠJv
14:20-15:10  ƒiƒm“dŽqŒõŠwÞ—¿‚f  ‹yì‰pr  u—L‹@E‚•ªŽqƒiƒmŒ‹»‘n»‚Ìŋ߂̌¤‹†“®Œü‚Æ¡Œã‚Ì“WŠJv
15:10-16:00  ƒiƒmƒA[ƒLƒeƒNƒ`ƒƒ[‚f  â–{Œª“ñ  uŒõˆÙ«‰»”½‰ž‚ð—˜—p‚µ‚½‚•ªŽq–Œ‚Ì”zŒü§Œä‚Æ‚»‚̉ž—p“WŠJv
–â‚¢‡‚í‚¹æ ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“ƒOƒ‹|ƒvŠÝ–{’¼Ž÷ (029-851-3354 “àü5433)
‘æ2‰ñNMLŒ¤‹†Œð—¬‰ï, 2004
ŠJÓúŽž 2004”N1ŒŽ14“ú(‰Î) 13:30`16:00
ŠJÃêŠ ÷’n‹æ Œ¤‹†“ 2ŠK ‘å‰ï‹cŽº
”­•\ŽÒ 13:30-14:20  ƒiƒmƒtƒ@ƒuƒŠƒP[ƒVƒ‡ƒ“‚f  ŠÔ‹{L–¾  uŽ¥«ƒiƒm—±ŽqŒ¤‹†‚É‚¨‚¯‚éV‚½‚ÈŽ‹“_‚Æ¡Œã‚Ì“W–]v
14:20-15:10  ƒiƒmƒLƒƒƒ‰ƒNƒ^ƒŠƒ[[ƒVƒ‡ƒ“‚f  ŽOΘa‹M  u“dŽqü‚ð—˜—p‚µ‚½ƒiƒm\‘¢ì»‚ÌŒ»ó‚Æ“W–]v
15:10-16:00  ƒiƒmƒVƒ“ƒZƒVƒX‚f  Dmitri Golberg  uSynthesis, Structural Analysis and Electrical Property Measurements of Composite Nanotubes in the B-C-N Ceramic Systemv
–â‚¢‡‚í‚¹æ ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“ƒOƒ‹|ƒvŠÝ–{’¼Ž÷ (029-851-3354 “àü5433)
‘æ1‰ñNMLŒ¤‹†Œð—¬‰ï, 2004
ŠJÓúŽž 2003”N11ŒŽ26“ú(‰Î) 13:30`16:00
ŠJÃêŠ ÷’n‹æ Œ¤‹†“ 2ŠK ‘å‰ï‹cŽº
”­•\ŽÒ 13:30-14:20  ƒiƒm•¨«‚f  –kàV‰p–¾  uV‹KŽ¥« —ÊŽq‹@”\Þ—¿ŠJ”­‚ÌŒ»ó‚Æ“W–]v
14:20-15:10  ƒiƒmƒfƒoƒCƒX‚f  –ì“c•Ži  u‰t“HƒGƒsƒ^ƒLƒVƒB‚É‚æ‚é—ÊŽqƒhƒbƒg‘n»‚ÌŒ»ó‚Æ“W–]v
15:10-16:00  ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“‚f  •“c—Ç•F  u‹à‘®ƒiƒm—±Žq‚Ì”ñüŒ`ŒõŠw“Á«‚Æ‚»‚̉ž—p“WŠJv
–â‚¢‡‚í‚¹æ ƒiƒmƒtƒ@ƒ“ƒNƒVƒ‡ƒ“ƒOƒ‹|ƒvŠÝ–{’¼Ž÷ (029-851-3354 “àü5433)

  NML seminar, 2003

Date
5th August, 2003, 13:30`15:00 idiscussion 15:00`j
Place
Special Meeting Room, 3rd Floor of Administration Office at
Sengen Sitei“Á•ʉï‹cŽºAçŒ»Ž––±“‚RŠKj
Lecturer
Prof. Mark E. Welland
Affiliation
Interdisciplinary Research Center for Nanotechnology
University of Cambridge, UK.
Title Recent Activities in Interdisciplinary Research Center for
Nanotechnology of University of Cambridge.
Introduction
Professor Mark E. Welland is a distinguished researcher
in the field of nanotechnology and has been appointed as a director of
newly-established Interdisciplinary Research Center (IRC) for
nanotechnology of University of Cambridge. He is now promoting
variety of research project in nano- and bio-related science and
technology. In this seminar, he will introduce selected topics from those
projects.
reference
http://www.nanoscience.cam.ac.uk/ (IRC for nanotechnology)
Host
Tomonobu Nakayama (Electro Nano-Characterization Group, phone 0298-859-2563)
–â‚¢‡‚킹æ
ƒiƒm“d‹CŒv‘ªƒOƒ‹[ƒv’†ŽR’mMi“àü2563j




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