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1.
W.J. Zakrzewski 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,29(2):217-219
In this talk we introduce a Weierstrass-like system of equations corresponding to CP
N
-1 fields in two dimensions. Then using this representation we introduce a vector in R
N
2-1 and treating this vector as the radius vector of a surface immersed in R
N
2-1 we discuss to what extent the associated metric describes the geometry of the CP
N
-1 maps. We show that for the holomorphic maps - the correspondence is exact; while for the more general fields we have to go
beyond the Weierstrass system and add extra terms.
Received 1st August 2001 / Received in final form 18 October 2001 Published online 2 October 2002
RID="a"
ID="a"Work done in collaboration with M. Grundland e-mail: w.j.zakrzewski@durham.ac.uk 相似文献
2.
M. Jourdan N. Blümer H. Adrian 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,33(1):25-30
Superconducting SrTiO
3 - δ
was obtained by annealing single crystalline SrTiO3 samples in ultra high vacuum. An analysis of the V
(
I
) characteristics revealed very small critical currents I
c
which can be traced back to an unavoidable doping inhomogeneity. R
(
T
) curves were measured for a range of magnetic fields B at I
≪
I
c
, thereby probing only the sample regions with the highest doping level. The resulting curves B
c2
(
T
) show upward curvature, both at small and strong doping. These results are discussed in the context of bipolaronic and conventional
superconductivity with Fermi surface anisotropy. We conclude that the special superconducting properties of SrTiO
3 - δ
can be related to its Fermi surface and compare this finding with properties of the recently discovered superconductor MgB2.
Received 4 December 2002 / Received in final form 10 March 2003 Published online 23 May 2003
RID="a"
ID="a"e-mail: jourdan@uni-mainz.de 相似文献
3.
4.
H. Gayvallet J.-C. Géminard 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,30(3):369-375
We have studied the temperature dependent resistivity ρ(
T
) of La2-xSrxCuO4 epitaxial thin films in the doping range 0.045 ⩽
x
⩽ 0.25 in pulsed magnetic fields up to 50 T. The zero-field resistivity ρ(
T
) of these samples in the pseudogap regime, can be scaled onto one single universal curve in a broad temperature range by using
a linear transformation of both temperature and resistivity. The high field data ρ(
T
) reveal a metal to insulator transition (MIT) at low temperatures, well into the overdoped regime. For samples having k
F
l
< 1, with kF the Fermi wave vector and l the mean free path, this low temperature insulating behavior of the resistivity is described by the variable range hopping
conductivity (VRH). For samples with k
F
l
> 1, the divergence follows ρ(
T
) ∼
ln
(1/
T
) or a power law, depending upon the Sr-content. We further found that the residual conductivity at the minimum in ρ(
T
), appearing due to the MIT, follows a linear behavior with respect to the Sr-content. It is argued that the unusual MIT in
compounds with k
F
l
> 1, is most probably associated with the pseudogap and the behavior of charge stripes at low temperatures.
Received 4 January 2002 / Received in final form 7 May 2002 Published online 14 October 2002
RID="a"
ID="a"e-mail: liesbet.weckhuysen@fys.kuleuven.ac.be 相似文献
5.
The synthesis and characterization of the new ligands L
1
, L
2
and L
4
are described with the series of four europium complexes of formula [EuL
n
(TTA)3] in which TTA refers to 2-thenoyltrifluoroacetonate and L
n
to tridentate ligands with nitrogen containing heterocyclic structure, such as a 2,6-bis(3-methyl-pyrazolyl)-4-(p-toluyl-ethynyl)-triazine for L
1
, or terpyridines functionalized at the 4′ position by a phenyl-vinylene for L
2
, a p-dimethylamino-phenylene for L
3
, or a p-aminophenyl-ethynylene for L
4
. The spectroscopic properties of the ligands and of the complexes are studied by means of UV–Vis absorption spectroscopy,
as well as steady-state and time-resolved luminescence spectroscopy. All complexes display europium centred luminescence upon
ligand excitation. Careful examination of the excitation spectra revealed differences in the ligand based sensitization efficiencies.
For complexes of L
1
and L
2
, excitation of europium is mainly achieved through the TTA moieties and the photo-physical studies on [EuL
1
(TTA)3] evidenced a weaker coordination of the bispyrazolyltriazine tridentate ligand, resulting from a partial decomplexation upon
dilution. Complexes of L
3
and L
4
display intense excitation through the tridentate units, which extend down to 460 nm in the visible region. In the case of
L
3
, selective excitation reveals the presence of a ligand-centred emission band at 520 nm which is likely ascribed to a L
3
centred charge transfer state. 相似文献
6.
S. Pokrant J.A. Becker 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,16(1):165-168
Magnetic properties of isolated DyN clusters are studied in a molecular beam performing Stern-Gerlach experiments. The magnetizations μ
z
of DyN are measured in dependence of the magnetic field strength B
= 0-1.6 T and at nozzle temperatures T
n
= 18 K and T
n
= 300 K. At room temperature the magnetization augments linear with the field following a simple paramagnetic model. At T
n
= 18 K the magnetization curves saturate at field strengths B
≥0.8 T. To explain the magnetization process at low temperatures two models are discussed: A model for adiabatic magnetization
based on cluster rotation effects and a modified van-Vleck model.
Received 30 November 2000 相似文献
7.
B. Gorshunov C.A. Kuntscher P. Haas M. Dressel F.P. Mena A.B. Kuz'menko D. van der Marel T. Muranaka J. Akimitsu 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,21(2):159-161
Far-infrared reflectivity studies on the polycrystalline intermetallic compound MgB2 with a superconducting transition temperature T
c
= 39 K were performed at temperatures 20 K to 300 K. We observe a significant raise of the superconducting-to-normal state reflectivity
ratio below 70
cm
-1
, with a maximum at about 25-30
cm
-1
, which gives a lower estimate of the superconducting gap of 2Δ(0)
≈ 3-4 meV.
Received 7 March 2001 and Received in final form 18 April 2001 相似文献
8.
T. Koga H. Matsuyama J. Molina Molina J.S. Dehesa 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1999,7(1):17-23
Electron-pair intracule (relative motion) and extracule (center-of-mass motion) densities are studied in both position and
momentum spaces for the
1
P and
3
P terms of the group 2 atoms Be (atomic number Z
=4), Mg (Z
=12), Ca (Z
=20), Sr (Z
=38), Ba (Z
=56), and Ra (Z
=88). In position space, the
1
P
-
3
P difference in the intracule densities shows that the probability of a small interelectronic distance is larger in the triplet
for all the six atoms, as reported for the lightest Be atom in the literature. The position-space extracule density clarifies
that the triplet electrons are more likely to be at opposite positions with respect to the nucleus than the singlet electrons
for all the atoms. In momentum space, the singlet generally has a larger probability of a small relative momentum between
two electrons as a na?ve manifestation of the Fermi hole in the triplet. The extracule density in momentum space shows that
the
1
P term has a distribution larger in a large center-of-mass momentum region than the
3
P term.
Received: 26 August 1998 / Received in final form: 1 February 1999 相似文献
9.
M. Vogel K. Hansen A. Herlert L. Schweikhard 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,21(2):163-166
The dimer dissociation energies of gold cluster ions Au
+
n
, n
= 9, 11, 13, 15 have been determined with an extension of a recently developed model-independent method. Monomer-dimer decay
pathway branching ratios provide the energy dependent process which is needed in this method. The measured values are D
2
(
Au
+
9
) = 3.66(8)(9) eV, D
2
(
Au
+
11
) = 4.27(11)(8) eV, D
2
(
Au
+
13
) = 4.50(9)(7) eV and D
2
(
Au
+
15
) = 4.29(10)(6) eV.
Received 13 May 2002 / Received in final form 22 July 2002 Published online 24 September 2002
RID="a"
ID="a"e-mail: manuel.vogel@uni-mainz.de 相似文献
10.
T. Zabel M.E. Garcia K.H. Bennemann 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1999,7(2):219-227
The absorption spectra of small Ag
+
n clusters are calculated at finite vibrational temperature by using a microscopic tight-binding RPA method. We consider free
clusters with sizes between n
= 3 and n
=13 and take into account explicitly the degrees of freedom corresponding to the 4
d-electrons. We analyze the optical absorption as a function of the cluster size. We show that the contribution of the d-electrons has an important influence on the size dependence of the energy of the Mie plasmon. We also perform ensemble averages
to obtain the absorption spectra for different vibrational temperatures. We obtain relatively good agreement with experiment
for a temperature . The dynamics of the 4
d-electrons, which shows in small clusters an incipient delocalized character for n
>7, yields an important contribution to the absorption spectrum already for n
=13. We find that the strength of this contribution can be controlled by varying the vibrational temperature.
Received: 4 January 1999 / Received in final form: 12 May 1999 相似文献
11.
J. Li C.H. Sow X.S. Rao C.K. Ong D.N. Zheng 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,32(4):471-476
In this research, c-axis oriented epitaxial anatase TiO 2 thin films were grown on SrTiO 3 (100) substrates using a ceramic Ti 0.95 Co 0.05 O 2 target by Pulsed Laser Deposition (PLD). The film growth processes were monitored by reflective high energy electronic diffraction (RHEED). Microstructure, conductivity, and magnetism of these doped films are found strongly affected by the oxygen pressure and substrate temperature Ts. Grown at a Ts around 750 ° C in an oxygen pressure of 0.2 mbar, the dopants are found existing as oxide inclusions. The doped film thus behaves as an insulator and shows diamagnetism in a magnetic field parallel to the film surface. However, in the doped film grown at a reduced temperature of 630 ° C in a vacuum, no impurity phase can be identified. The film shows a saturated magnetic moment of 0.16μ B / Co and a fairly good conductivity at room temperature. It is then concluded that nonequilibrium growth at lower temperatures in vacuum is essential for a high solubility of Co in the TiO 2 lattice and thus the ferromagnetism. 相似文献
12.
M.P. Lissitski A. Naddeo C. Nappi A. Tagliacozzo V.N. Gubankov R. Monaco M. Russo 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,32(3):309-314
Measurements of differential resistance in a superconductor-degenerate semiconductor junction Nb
-
n
+ +
GaAs at T
= 1.6 K show close similarity to those for a conventional superconductor-insulator- normal metal junction, except for the position
of the minimum which is located at 3.6 meV. Using a simple model for the charge screening at the Schottky barrier, we give
an argument why this minimum is by far displaced with respect to the superconducting gap energy ( Δ
g
= 1.5 meV for bulk Nb). We argue that a rebuilding of the density of states takes place at the barrier, due to the imperfect metal
screening in the degenerate semiconductor. Energy states close to the degenerate semiconductor Fermi energy are depleted at
the barrier and are not available for tunneling, up to an energy Eg which adds to the superconducting gap Δ
g
.
Received 11 November 2002 / Received in final form 21 February 2003 Published online 11 April 2003
RID="a"
ID="a"e-mail: c.nappi@cib.na.cnr.it 相似文献
13.
14.
N. Magneron Y. Luspin G. Hauret E. Philippot 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,3(1):7-15
Transverse and pseudo-transverse elastic waves have been studied in several scattering geometries in order to investigate
the temperature dependences of C
E
66
and C
E
14
over the range 300-1100 K, including the transitions near 860 K. These results complete those on C
E
44
we have obtained in a previous work. All these constants display discontinuities at the lock-in transition. In the phase, the results are analysed in term of lowest order couplings between strains (e) and the order parameter (Q). The main features are described by the lowest order biquadratic e2Q2 coupling, in particular for C
E
44
in a large temperature range. However, it appears that a contribution of the next coupling term arises for C
E
66
below K and that the first two lowest order terms have to be taken into account even just below the lock-in transition in the case
of C
E
14
. The temperature dependence of Q has been deduced and it can be well described in the framework of Landau's theory.
Received: 2 October 1997 / Received in final form: 3 December 1997 / Accepted: 29 January 1998 相似文献
15.
S.I. Themelis Y. Komninos C.A. Nicolaides 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,18(3):277-293
This paper discusses theory and results on 1P0 doubly excited states (DES) in He and in H- of very high excitation, up to the N
= 25 manifold. Our calculations employed full configuration interaction (CI) with large hydrogenic basis sets and produced correlated
wavefunctions for the four lowest roots at each hydrogenic manifold by excluding open channels and the small contribution
of series belonging to lower thresholds. The suitability of the hydrogenic basis sets for such calculations is justified,
apart from their practicality, by the fact that, by computing from them natural orbitals, the results were shown to be the
same with those of earlier multiconfigurational Hartree-Fock (MCHF) calculations on low-lying DES. In total, 160 states were
computed, most of them for the first time. Their energy spectrum should be of use to possible future photoabsorption experiments.
For certain low-lying DES up to N
= 13, for which previous reliable results are available, comparison of the calculated energies shows good agreement. The correlated
wavefunctions contain systematically chosen single and double excitations from each hydrogenic manifold of interest. From
their analysis, we determined the “goodness" of different quantum numbers and the geometry (average angles and radii) as a
function of excitation. For the Sinano lu-Herrick (
K
,
T
) classification scheme, whose basis is a restricted CI with hydrogenic functions and which has thus far been tested only on
low-lying DES, we established that, whereas T remains a good index as energy increases, K does not. Consequently, a more flexible than K quantum number is needed in order to account for most of the additional correlation. This number, represented by F
=
N
-
K
- 1, where N and K are not good numbers anymore, produces consistently a much higher degree of purity than the (
K
,
T
) scheme does, especially as N increases and as the relative significance of various virtual excitations due to electron correlation increases. Among the
four states of each manifold, in all cases in H- and in most cases in He, the three are of the intrashell type and one is of the intershell type with (
F
,
T
) = (0, 0). The lowest intrashell states and the lowest intershell states exhibit a wide angle geometry tending to 180
°
as N
↦∞.
Received 10 September 2001 and Received in final form 12 November 2001 相似文献
16.
V.V. Savkin A.N. Rubtsov T. Janssen 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,31(4):525-531
The classical two-dimensional discrete frustrated φ
4
model is studied by Monte Carlo simulations. The correlation function is obtained for two values of a parameter d that determines the frustration in the model. The ground state is a ferro-phase for d
= - 0.35 and a commensurate phase with period N
= 6 for d
= - 0.45. Mean field predicts that at higher temperature the system enters a para-phase via an incommensurate state, in both cases. Monte Carlo data for d
= - 0.45 show two phase transitions with a floating-incommensurate phase between them. The phase transition at higher temperature
is of the Kosterlitz-Thouless type. Analysis of the data for d
= - 0.35 shows only a single phase transition between the floating-fluid phase and the ferro-phase within the numerical error.
Received 16 December 2002 / Received in final form 17 January 2003 Published online 6 March 2003
RID="a"
ID="a"e-mail: vladimir@shg.ru 相似文献
17.
M. Gómez Berisso P. Pedrazzini J.G. Sereni O. Trovarelli C. Geibel F. Steglich 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,30(3):343-349
We present electrical resistivity and specific heat measurements of alloys on the Rh rich side of the phase diagram of the
Ce(Rh1-xPdx)2Si2 system. We compare these results with those obtained at intermediate and low Rh concentrations. The analysis of the concentration
and temperature dependence of the entropy and of the scaling behaviour of C
el
(
T
) and ρ(
T
) clearly confirm a separation of the magnetic phase diagram into two regions: the region x
≤0.3, showing a concentration independent characteristic temperature for the 4
f-electrons with T
0
≈ 45
K, while for x
> 0.3, T0 decreases to T
0
(
x
= 1) ≈ 15
K. At low Pd-content, TN decreases very rapidly from T
N
= 36
K in pure CeRh2Si2 to T
N
= 18
K at x
= 0.1. With higher Pd concentration TN stabilizes at T
N
≈ 15
K whereas the magnitude of the anomalies in C
el
(
T
) and in the susceptibility around TN are further reduced and disappear at x
≈ 0.3. This differs from the behavior found on the Pd-rich side, where TN decreases continuously to zero with increasing Rh content. The pronounced differences observed between both phase boundaries
and the drastic effect of doping on the Rh rich side suggest an itinerant character in CeRh2 Si2, in contrast with the localized character of CePd2Si2. Further evidence for the itinerant character of CeRh2Si2 is given by the ρ(
T
) dependence observed for x
≤0.3, which scales with ρ(
T
) of the prototype itinerant compound YCo2.
Received 31 December 2001 / Received in final form 6 July 2002 Published online 19 December 2002
RID="a"
ID="a"e-mail: berisso@cab.cnea.gov.ar 相似文献
18.
M. Putti E. Galleani d'Agliano D. Marrè F. Napoli M. Tassisto P. Manfrinetti A. Palenzona C. Rizzuto S. Massidda 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,25(4):439-443
We report measurements of the resistivity, ρ, and the Seebeck coefficient, S
, of a MgB2 sintered sample, and compare S with theoretical calculations based on precise electronic structure calculations. ρ is fitted well by a generalized Bloch-Grüneisen equation with a Debye temperature Θ
R
of 1050 K. S is given by the sum of a diffusive and a phonon drag term and the behavior in the temperature region T
c
<
T
< 0.1Θ
R
follows the relationship AT+BT3. The phonon drag term indicates a strong electron-phonon interaction. The diffusive term, compared with calculations, suggests
that σ bands give the main contribution to the Seebeck effect.
Received 16 November 2001 and Received in final form 21 December 2001 相似文献
19.
U.D. Rapol A. Krishna V. Natarajan 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,23(2):185-188
We demonstrate a technique to measure hyperfine structure using a frequency-stabilized diode laser and an acousto-optic modulator
locked to the frequency difference between two hyperfine peaks. We use this technique to measure hyperfine intervals in the
5
P
3/2
state of 85Rb and obtain a precision of 20 kHz. We extract values for the magnetic-dipole coupling constant A
= 25.038(5) MHz and the electric-quadrupole coupling constant B
= 26.011(22) MHz. These values are a significant improvement over previous results.
Received 6 March 2003 Published online 15 April 2003 相似文献
20.
D. Schwarzhans D. Zimmermann 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,22(2):193-198
The absorption spectrum of NaAr has been investigated with high resolution using a supersonic beam of molecules and a tunable
dye laser. About 3 300 absorption lines due to the transition A
2
Π ←
X and B
2
Σ ←
X have been observed. In addition, we observed the spectral distribution of the fluorescence for a particular absorption line.
From all experimental data the X
2
Σ
+
interaction potential has been deduced in a fully quantum-mechanical method of approach. The potential is given in terms
of an analytical Hartree-Fock-Dispersion function. For the equilibrium parameters of the X state we get R
e
= 5.01(1) ? and D
e
= 41.6(2)
cm
-1
.
Received 28 August 2002 / Received in final form 15 October 2002 Published online 17 December 2002
RID="a"
ID="a"Now at Knick Elektronische Messger?te, Beuckestr. 22, 14163 Berlin, Germany.
RID="b"
ID="b"e-mail: dz@kalium.physik.tu-berlin.de 相似文献