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BOOK OF ABSTRACTS
6th Workshop on Current Problems in Physics:
Zielona Góra - Lviv
23 - 25 September 2013, Zielona Góra, Poland
2
The Workshop on Current Problems in Physics
2013 (WCPP'13) is already the sixth in a series of
meetings which represent annual forum for the
Polish and Ukrainian physicists community to
present their latest scientific results. Usually, the
meetings are attended by representatives of other
countries, too. An important feature of the
conference is the possibility for young scientists
to present their research results and interact
with the more experienced colleagues from other
countries. The Workshop will be held in Zielona
Góra from 23 to 25 September 2013.
The conference is organized under the auspices of
His Magnificence Rector of the University of
Zielona Góra, professor Tadeusz Kuczyński.
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Conference programme
Monday 23.09.2013
Arrival of participants
Tuesday 24.09.2013
9:00-9:10 Opening ceremony
Session I – Chairman: G. Melikidze
special session on integrable systems to celebrate
professor Stanislaw Kasperczuk 70th birthday
9:10-09:30 S. Kasperczuk
09:30-10:00 M. Błaszak
10:00-10:20 A. Maciejewski
10:20-10:40 M. Przybylska
10:40-10:50 Coffee Break
10:50-11:10 P. Rozmej
11:10-11:20 W. Szumiński
Session II – Chairman: V.M. Tkachuk
selected aspects of classical and quantum theory
11:20-11:40 A. Duviryak
11:40-12:00 S. Kondej
12:00-12:20 P. Jachimowicz
12:20-12:40 M. Stetsko
12:40:13:00 A. Kuzmak
13:00-14:00 Lunch
Session III – Chairman: W. Leoński
quantum optics, quantum correlations, quantum information
14:00-14:30 R. Tanaś
14:30-14:50 V. Cao Long
14:50-15:10 A. Kowalewska-Kudłaszyk
15:10-15:30 J. K. Kalaga
15:30-15:45 T. D. Nguyen
15:45-16:00 Coffee Break
Session IV – Chairman: K. Urbanowski symmetry, fundamental interactions, cosmology
16:00-16:30 V. M. Tkachuk
16:30-16:50 Yu. Yaremko
16:50-17:20 A. Szary
17:20-17:40 K. Raczyńska
19:00_____ dinner under Braniborska tower observatory
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Wednesday 25.09.2013
Session I – Chairman: K.W. Wojciechowski
medical applications
9:00-9:20 J. Piskorski
9:20-9:40 S. Żurek
9:40-10:10 G. Garbacz
Session II – Chairman: J. Piskorski
nanotechnology, nanomedicine
10:10-10:25 B. Zapotoczny
10:25-10:40 A. Timoszyk
10:40-10:55 A. Defort
10:55-11:10 J. Mleczko
11:10-11:25 Coffee Break
Session III – Chairman: A. Drzewiński
metamaterials, mechanical properties
11:25-11:55 K.W. Wojciechowski
11:55-12:15 J. Narojczyk
Session IV – Chairman: V. Cao Long spectroscopy, luminescence, materials
12:15-12:45 N. Guskos
12:45-13:05 A. Rovenchak
13:05:13:20 G. Panochko
13:20-14:20 Lunch
Session V – Chairman: V. Cao Long
statistical physics methods, models
14:20-14:35 T. Masłowski
14:35-14:50 M. Zubaszewska
14:50-15:05 A. Durajski
15:05-15:25 M. Jarosik
15:25-15:45 Coffee Break
15:45-16:00 B. Brzostowski
16:00-16:15 M. Wojciechowski
16:15-16:30 D. Woźniak
5
ABSTRACTS
6
Classical and quantum Stackel systems
M. Błaszak
Faculty of Physics, A. Mickiewicz University,
Umultowska 85, 61-614 Poznań, Poland
In the talk is presented a theory of separability for a class of Liouville integrable
hamiltonian systems with all constants of motion quadratic in momenta. Then, the so
called minimal quantization procedure is applied and is analyzed the problem of quantum
separability of such constructed quantum systems.
7
Chain-model approximations for the Cr8
molecular magnet. DFT approach.
B. Brzostowski1, M. Wojciechowski
1, D. M. Tomecka
2,
G. Kamieniarz2, V. Bellini
3,4, F. Troiani
3, F. Manghi
3,
M. Affronte3
1 Institute of Physics, University of Zielona Góra,
65-516 Zielona Góra, Poland;
2 Faculty of Physics, A. Mickiewicz University,
61-614 Poznań, Poland;
3 CNR-INFM-National Research Center on nanoStructures
and bioSystems at Surfaces (S3),
Via Campi 213/A, 41100 Modena, Italy;
4 Istituto di Struttura della Materia (ISM) - Consiglio Nazionale delle Ricerche (CNR),
I-34149, Trieste, Italy;
We present a density functional theory (DFT) study of the electronic and magnetic
properties of the Cr8 molecular ring. The all-electron linearized augmented plane wave
method (LAPW) implemented in the Wien2k package and pseudopotential method
implemented in Siesta package are used to calculate the electronic states, exchange
coupling parameters of an infinite chain model system of Cr88. We demonstrate how, under
opportune modifications to the ring cycle structure, different one-dimensional chain models
can be devised, with the capability of mimicking with good approximation the electronic
and magnetic properties of the original Cr8 molecule. Such models offer an unique
opportunity, in virtue of the reduced computational effort, to carry out extensive
investigations of a whole set of molecules belonging to the Cr-based molecular rings
family.
8
Application of functionalized iron oxide
nanoparticles to determine catecholamines
A. Defort, J. Nowak-Jary, J. J. Kozioł
Faculty of Biological Sciences, University of Zielona Góra,
ul. Szafrana 1, 65-516 Zielona Góra, Poland
Magnetic iron oxide nanoparticles provide attractive possibilities in biomedical
application such cell labeling and separation, target drug delivery and biosensor [1,2].
These applications require magnetic nanoparticles to be well-dispersed in liquid media,
chemically stable and uniform in size. Due to the magnetic dipolar attraction, unmodified
magnetite nanoparticles incline to aggregate into clusters and inhibit the advantage of the
specific properties by single-domain. The aggregation associated with magnetite
nanoparticles can be avoided by creating an electrostatic double layer using a surfactant
steric stabilizer or silica coating [3]. In this presentation magnetic nanoparticles (Fe3O4)
are prepared by co-precipitation method and modify by silica using Stöber process [4].
The applications of arylboronic acids as catecholamine sensors are broad, because they
are small and exible molecules. They can form fast and reversible cyclic esters with
compounds containing diol moieties in aqueous media. Arylboronic acids potentially
offer non-invasive continuous blood glucose monitoring, in some cases without the need
for reference measurements. The information can be provided by attachment of the
boronic acid moiety (for example Alizarine S) to a proper reporting unit, which undergoes
a significant change in fluorescence emission [5]. This presentation will focus on the
synthesis of magnetic iron oxide nanoparticles of arylboronic acids and their important
properties which eventually will make them suitable as key elements in future non-
invasive continuous catecholamine sensors such an epinephrine, norepinephrine or sialic
acid [6].
References
[1] J. Chen, Y. Miao, N. He, X. Wu, S. Li, Biotechnology Advances 22 (2004) 505.
[2] J. Lee, Y. Lee, J.K. Youn, Biocatalysts. Small 4 143.
[3] Z. Lu, G. Wang, J. Zhuang, W. Yang, Colloids and Surfaces A: Physicochem. Eng.
Aspects (2006) 140.
[4] Z.Y. Lu, et al., Colloids and Surfaces A: Physicochem. Eng. Aspects 317 (2008) 450.
[5] G. Springsteen, B. Wang, Tetrahedron 58 (2002) 5291.
[6] M. Perry, Q. Li, R.T. Kennedy, Analytica Chimica Acta 653 (2009) 1.
9
The high-pressure superconductivity in hydrogen-
rich compounds
A. Durajski
Institute of Physics, Częstochowa University of Technology,
Ave. Armii Krajowej 19, 42-200 Częstochowa, Poland
Solid molecular hydrogen and the possibility of its metallization has fascinated condensed
matter researchers since the prediction of the pressure required for metallization was
proposed by Wigner and Huntington in 1935 [1],[2]. The possibility of forming metallic
hydrogen using hydrogenated materials was subsequently studied and discussed [3]. The
recent ab initio calculations suggest that the superconducting state in metallic hydrogen-
rich compounds under the pressure has the critical temperatures much higher than the
boiling point of liquid nitrogen. For this reason, the relevant thermodynamic parameters of
the superconducting state in SiH4, Si2H6, SiH4(H2)2, GeH4, GaH4(H2)2 and CaH6, have been
determined within the framework of the Eliashberg theory. It has been shown that for a
wide range of the Coulomb pseudopotential the values of the ratio of the energy
gap to the critical temperature ( ), the ratio of the specific heat jump to the
heat in the normal state ( ) and the ratio connected with the
thermodynamic critical field ( ) significantly exceed the values predicted
by the BCS theory [4], [5]. This fact is connected with strong coupling electron-phonon
interaction and the retardation effects existing in the analyzed systems.
References
[1] E. Wigner, H.B. Huntington, J. Chem. Phys. 3, 764 (1935).
[2] N. W. Ashcroft, Phys. Rev. Lett, 21, 1748 (1968).
[3] N. W. Ashcroft, Phys. Rev. Lett, 92, 187002 (2004).
[4] R. Szczęśniak, A.P. Durajski, Solid State Conunun. 153, 26 (2013).
[5] R. Szczęśniak, A.P. Durajski, J. Phys. Chem. Solids 74, 641 (2013).
10
Dificulties in prediction of the oral drug delivery -
about differences between theory and reality form
pharmaceutical point of view.
G. Garbacz1, W. Weitschies
2
1 Physiolution GmbH,
Walther Rathenau Strasse 49 a, 17489 Greifswald, Germany
2 Center of Drug Absorption and Transport,
Felix-Hausdorff-Strasse 3, 17487 Greifswald, Germany
A reliable estimation of drug delivery behavior is a prerequisite for rational and efficient
development of dosage forms. It is frequently believed that this challenging goal may be
achieved using standard test methods as well as different mathematical models describing
the drug delivery processes. Unfortunately, the clinical data often demonstrate insufficient
predictive power of the available models. The main reasons thereof are the lack of the good
understanding of the gastro-intestinal (GI) physiology as well as the variability on the
conditions on the drug absorption site. Interestingly, both factors cannot be realistically
simulated using compendial test equipment for dissolution testing. We will briefly
introduce the selected aspects of the human GI physiology, evolution and goals of
dissolution testing as well as the development and use of test devices that are intended to
simulate the GI conditions. The data will be discussed in the light of the test results and
experiences obtained with the new dissolution stress test device that simulates physic-
chemical and mechanical conditions of the GI passage of dosage forms developed by our
group.
11
Magnetic resonance study of co-modified (Co,N)-TiO2
N. Guskos1,2
, S. Glenis1, G. Zolnierkiwicz
2, A. Guskos
2, J. Typek
2, P.
Berczynski2, D. Dolat
3, B. Grzmil
3, B. Ohtani
4 and A.W. Morawski
3
1Department of Solid State Physics, University of Athens, Panepistimioupolis,
GR-157 84 Athens, Greece
2Department of Physics, West Pomeranian University of Technology,
Al. Piastow 48, 70-311 Szczecin, Poland
3Department of Chemical and Environmental Engineering,
West Pomeranian University of Technology,
Al. Piastow 17, 70-310 Szczecin, Poland
4Catalysis Research Center, Hokkaido University, Sapporo 001-0021 Japan
The nCo,N-TiO2 (n=1, 5 and 10 wt.%) nanocomposites have been prepared by comodification of commercial
amorphous titanium dioxide via impregnation followed by calcination at 800°C in ammonia atmosphere. The
photocatalytic properties strongly depend on concentration of cobalt ions of the obtained samples. The magnetic
properties of (Co,N)-TiO2 nanocomposites have been investigated by FMR/EPR spectroscopy in 4-290 K range
(Fig. 1). The intense FMR spectra of cobalt nanoparticle agglomerates were dominant in the whole temperature
range for all samples. In addition, intense EPR spectra of trivalent titanium ions were recorded for sample with
n=1% (Fig.1) while for other two samples two orders of magnitude smaller intensities of spectra were
registered. Above a certain treshhold concentration of Ti3+
a drastic deterioration of the photocatalytic properties
is observed, and sample with n = 1% is the worst in this respect.
0 2000 4000 6000 8000
-80000
-60000
-40000
-20000
0
20000
40000
60000
d"/
dH
[A
rb. u
nits]
Magnetic field H [G]
T=4 K
T=290 K
T=10 KTi3+
Fig. Temperature dependence of the FMR/EPR Spectra of (1%Co,N)-TiO2.
12
Pairing mechanism for the high-Tc
superconductivity: symmetries and
thermodynamic properties
M. Jarosik, R. Szczęśniak
Institute of Physics, Częstochowa University of Technology,
Ave. Armii Krajowej 19, 42-200 Częstochowa, Poland
The pairing mechanism for the high-Tc superconductors based on the electron-phonon
(EPH) and electron-electron-phonon (EEPH) interactions has been presented. On the fold
mean-field level, it has been proven, that the obtained s-wave model supplements the
predictions based on the BCS van Hove scenario. In particular: (i) For strong EEPH
coupling and T < Tc the energy gap () is very weak temperature dependent; up to the
critical temperature extends into the anomalous normal state to the Nemst temperature.
(ii) The model explains well the experimental dependence of the ratio R 2(0)/kTc on
doping for the reported superconductors In the terms of the few fundamental parameters.
In the presented paper, the properties of the d-wave superconducting state in the two-
dimensional system have been also studied. The obtained results, like for s-wave, have
shown the energy gap amplitude crossover from the BCS to non-BCS behaviour, as the
value of the EEPH potential increases. However, for T > Tc the energy gap amplitude
extends into the anomalous normal state to the pseudogap temperature. Finally, it has been
presented that the anisotropic model explains the dependence of the ratio R on doping for
the considered superconductors.
13
Quantum chaos of nonlinear oscillator system
and Kullback - Leibler quantum divergence
J. K. Kalaga1, A. Kowalewska-Kudłaszyk
2,
W. Leoński1, V. Cao Long
1
1Quantum Optics and Engineering Division, Institute of Physics,
University of Zielona Góra,
Prof. Z. Szafrana 4a, 65-516 Zielona Góra, Poland
2Faculty of Physics, A. Mickiewcz University,
Umultowska 85, 61-614 Poznań, Poland
We discuss a system containing nonlinear Kerr-like oscillator, driven by a series of ultra
short external pulses. Using Kullback - Leibler quantum divergence K[q|] we define linear
and nonlinear quantum divergences. We analyze behavior of these divergences for various
values of the parameters determining character of system's dynamics and show that they
can be applied as witnesses of quantum-chaotic evolution of the system. We show that the
nonlinear divergence is more sensitive for the quantum-chaotic behavior than its linear
counterpart.
14
Double line interaction
Sylwia Kondej
Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65246 Zielona Góra, Poland
The talk is addressed to the problem of, so called, leaky quantum wires which can be
modelled by delta potential supported by two parallel straight lines. We discuss spectral
properties of such a system, for example, we formulate conditions guaranteeing existence
of discrete eigenvalues. Furthermore, we show that for a certain class of systems with
a mirror symmetry the embedded eigenvalues phenomena holds.
The talk is based on a common work with David Krejčiřík
15
Kerr coupler operating on Werner-like states ―
entanglement creation and evolution
A. Kowalewska-Kudłaszyk1, W. Leoński
2
1 Faculty of Physics, A. Mickiewcz University,
Umultowska 85, 61-614 Poznań, Poland
2 Quantum Optics and Engineering Division, Institute of Physics,
University of Zielona Góra,
Prof. Z. Szafrana 4a, 65-516 Zielona Góra, Poland
We consider a problem of creation of pure entangled states in two-qubit space from initial
Werner or Werner-like state by Nonlinear Quantum Scissors (NQS). NQS systems are
based on Kerr-like oscillators and can operate in optical domain, but there are also
examples of Kerr-like Hamiltonians used in condensed matter systems. NQS are able,
under some assumptions, to restrict substantially the number of states involved in the
dynamics and therefore are called quantum scissors.
Such state reduction can lead to generation of maximally, or almost maximally entangled
states. It was already shown that for two Kerr-like oscillators the system with various types
of interactions (linear, nonlinear and parametric) behave like two-qubit, qutrit-qubit or two-
qutrit system. It was also shown that we are able to generate entangled states from initial
number states within Kerr-couplers.
At present we would like to show that there is also a possibility of creating pure entangled
states even though the system is initially in incoherent combination of a completely mixed
state and a maximally entangled pure state (Werner or Werner-like states). We consider the
influence of various types of damping processes on entanglement creation. The analytical
conditions for obtaining different types of entanglement decay: asymptotic or decay in
finite time and its possible revival after a significantly long time period, are presented.
16
Preparation of quantum states of two spins-
in the Schmidt decomposition
A. R. Kuzmak
Department for Theoretical Physics, Ivan Franko National University of Lviv,
12 Drahomanov St., Lviv, UA-79005, Ukraine
We consider a system of two spins and their interaction is represented by isotropic
Heisenberg Hamiltonian. Our aim is to create arbitrary quantum state of two spins having
started with | state. We can easily prepare this state because it is an eigenvector of the
system of two spins which is located in the magnetic field directed along the z-axis. The
method which we suggest consist of two steps. At the first step, using the evolution
operator with isotropic Heisenberg Hamiltonian we obtain the state which depends on time
of evolution. At the second step, the spins are driven individually by magnetic pulse fields.
Finally, we obtain arbitrary state of two qubits which can be easily represented in the
Schmidt decomposition. This state is defined by time of evolution and parameters which
are determined strength and direction of magnetic fields.
We propose to realize this method on the physical system of atoms which have a nuclear
spin I of 1/2 and one valence electron. Therefore, these systems can be considered as a two-
qubit systems. Factorized initial state | state can be easily prepared for these systems
[1]. We consider the system of 31
P donor in silicon because it is system with high degree of
quantum coherence, and states of this system are measured with high fidelity [1].
References
[1] J.J. Pla et al., Nature 496 (2013) 334.
17
EIT in Lambda configuration: multilevel model
and model with structured continua
V. Cao Long, W. Leoński
Quantum Optics and Engineering Division, Institute of Physics,
University of Zielona Góra,
Prof. Z. Szafrana 4a, 65-516 Zielona Góra, Poland
We present some new results concerning so-called electromagnetically induced
transparency (EIT) [1] in Lambda scheme. We discuss two different models. One of them
involves discrete levels [2,3] , whereas the second one contains structured continua [4].
Applying multilevel model, we reconstruct multi-peak spectra registered by Warsaw Group
in a sample of cold 85Rb atoms trapped in MOT. Moreover, we show that the nature of the
spectra exhibiting several transparency windows can be explained on a basis of the second
model, that with several autoionizing states, or equivalently, with Fano structured continua.
References
[1] K. Kowalski, V. Cao Long, K. Dinh Xuan, M. Głódź, B. Nguyen Huy, J. Szonert,
Comp. Meth. Sci. Technol. Special Issue 2 (2010) 131.
[2] K. Kowalski, V. Cao Long, H. Nguyen Viet, S. Gateva, M. Głódź, J. Szonert,
J. Non-Cryst. Solids 355 (2009) 1295.
[3] A. Żaba, V. Cao Long, M. Głódź, E. Paul-Kwiek, K. Kowalski, J. Szonert, D. Woźniak
and S. Gateva Ukr. J. Phys. 14 (2013) 138.
[4] T. Bui Dinh, W. Leoński, V. Cao Long and J. Peřina Jr. Optica Applicata (2013) in print.
18
Necessary conditions for integrability of algebraic
Hamiltonian systems
A.J. Maciejewski
Institute of Astronomy, University of Zielona Góra, Poland
Necessary conditions for integrability of algebraic Hamiltonian systems Abstract: Systems
with Hamiltonian functions algebraic in coordinates and momenta are considered. For such
systems the right hand sides of Hamilton equations typically are not single valued. This is
why the Ziglin or the Morales-Ramis theory cannot be applied directly to study their
integrability. The main idea is following. One can extend the phase space of the system in
such a way that the extended system is meromorphic and Hamiltonian with respect to a
certain degenerated Poisson structure. Although the proposed construction is not unique it
allows to obtain necessary conditions for the integrability in the framework of differential
Galois theory. Applying this approach necessary conditions for integrability of algebraic
homogeneous potentials of rational homogeneity degree are obtained.
19
Magnetic nanoparticles and antigen-antibody
reactions; can magnetic nanoparticles modify
antigen-gen-antibody reaction
J. Mleczko
Institute of Genetics and Microbiology, Uniwersity of Wrocław,
ul. Przybyszewskiego 63/7, 51-148 Wrocław
Magnetic nanoparticles in water solution under external magnetic field modify/change the
local (near their surface) value of pH and temperature and do not necessarily influence on
their value in a bulk solution. Antigen-antibody reactions constitue important group of
biological/biochemical reactions in human/animal organisms and commonly are used in
biomedical tests. Efficiency of antigen antibody reactions significantly depend on pH and
temperature. The magnetic nanoparticles exhibit very low toxicity and because of their
pliability on control by magnetic field they are becoming useful for experimental and
biomedical applications. Magnetic nanopartices could open up possibility of local lowering
or increasing (controlling) of dynamics and efficiency of antigen-antibody reactions in
human body.
20
Partial auxeticity of soft polydisperse dimers at
zero temperature.
J. W. Narojczyk, K. W. Wojciechowski, M. Kowalik
Institute of Molecular Physics Polish Academy of Sciences,
Mariana Smoluchowskiego 17, 60-179 Poznań, Poland
Influence of atomic size polydispersity on Poisson's ratio [1] of cubic systems consisted of
di-atomic molecules (dimers) is studied by computer simulation. The simulations,
performed in the NV T ensemble, are restricted to the static case, i.e. to the zero temperature
(T = 0K). The positions of the dimer centres of mass and their orientations are aperiodic but
the constituting atoms form the (perfect or slightly distorted in the polydisperse case) f.c.c.
lattice. Such a phase, called the degenerate crystal (DC) [2], is illustrated in Figure 1.
a) b)
Figure 1: Example of microscopic structure of DC polydisperse dimer system. The structure
shown consists of 432 dimers and has the polydispersity parameter δ equal to 3%. In (a) the
atoms are drawn in the shades of gray, indicating their size relative to other atoms. The
darker the color, the larger the atomic diameter. The gray cube indicates the periodic box.
In (b) dimer center positions and orientations for the structure in (a) are represented by
points and line segments connecting the atomic centers.
Size polydispersity concerns all atoms in the model. Interactions are short-ranged -
restricted to nearest-neighbouring atoms, i.e. those sharing a common wall of their Voronoi
polyhedra. The atoms interact with soft, repulsive n-inverse-power potential.
Poisson's ratio is the negative ratio of the relative change in the transverse dimension to the
relative change in the longitudinal dimension when infinitesimal change of the longitudinal
stress is applied [1]. For most commonly used materials, the Poisson's ratio is positive. This
means that when stretched (compressed) longitudinally, such a material will shrink
(expand) in transverse dimensions. There are materials however, which behave contrary.
They expand (shrink) transversely when stretched (compressed) longitudinally. They are
called auxetics and for such unusual materials the Poisson's ratio is negative. In the case of
anisotropic materials, Poisson's ratio (ναβ) may depend on both the longitudinal (α) and
transversal (β) direction. It is known that, in general, the disorder of crystalline lattice leads
to the increase of average Poisson's ratio, both in the case of isotropic [3-6] and anisotropic
[7-9] systems. However, in the case of cubic systems a direction exists (β = [1 0]) for
which, polydispersity has the opposite effect, when the sample is deformed in α = [110]. In
this case it has been found, that increasing polydispersity leads to a decrease of the
Poisson's ratio [8, 9], down to negative values. For unconstrained, polydisperse cubic
21
system (f.c.c. spheres), the decrease was insignificant [8], and negligible in the limit of hard
interactions. Negative Poisson's ratio was observed for a range of soft interactions. For
f.c.c. dimers, the increasing polydispersity decreases significantly, down to -0.8,
in the range of hard interactions [9]. Various models of dimers were studied [10] and the
observed effect was found to be robust with respect to model details. Hence, this effect can
be of interest from practical applications perspective.
Acknowledgments
Part of the simulations was performed at Pozna_n Supercomputing and Networking Center (PCSS).
References
[1] L. D. Landau and E. M. Lifshitz, Theory of Elasticity, Pergamon Press, London, 1986.
[2] K. W. Wojciechowski, D. Frenkel and A. C. Brańka, Non-periodic solid phase in a two
dimensional hard-dimer system, Physical Review Letters, 66:3168-3171, 1991.
[3] K. W. Wojciechowski and J. Narojczyk, Inuence of disorder on the Poisson's ratio of
static solids in two dimensions, Reviews on Advanced Materials Science, 12:120-126,
2006.
[4] J. W. Narojczyk and K. W. Wojciechowski, Computer simulation of the Poisson's ratio
of soft polydisperse discs at zero temperature, Materials Science (Poland), 24:921-927,
2006.
[5] J. W. Narojczyk and K. W. Wojciechowski, Elastic properties of two-dimensional soft
discs of various diameters at zero temperature, Journal of Non-Crystalline Solids,
352:4292-4298, 2006.
[6] J. W. Narojczyk and K. W. Wojciechowski, Elasticity of periodic and aperiodic
structures of polydisperse dimers in two dimensions at zero temperature, Physica Status
Solids (b), 245:2463-2468, 2008.
[7] J. W. Narojczyk, A. Alderson, A.R. Imre, F. Scarpa, and K. W. Wojciechowski,
Negative Poisson's ratio behavior in the planar model of asymmetric trimers at zero
temperature, Journal of Non-Crystalline Solids, 354:4242-4248, 2008.
[8] J. W. Narojczyk and K. W. Wojciechowski, Elastic properties of the fcc crystals of soft
spheres with size dispersion at zero temperature, Physica Status Solidi (b), 245:606-613,
2008.
[9] J. W. Narojczyk and K. W. Wojciechowski, Elastic properties of degenerate f.c.c.
crystal of polydisperse soft dimers at zero temperature, Journal of Non-Crystalline
Solids, 356:2026-2032, 2010.
[10] J. W. Narojczyk, K. W. Wojciechowski and M. Kowalik, Partially auxetic properties
of polydisperse soft dimer systems at zero temperature, Journal of Chemical Physics,
submitted.
22
Maximally entangled states generation in kicked
Kerr-like coupler models
T. D. Nguyen, W. Leoński, V. Cao Long,
Quantum Optics and Engineering Division, Institute of Physics,
University of Zielona Góra,
Prof. Z. Szafrana 4a, 65-516 Zielona Góra, Poland
We discuss a system involving Kerr-like nonlinear coupler [1] excited by a series of ultra-
short external coherent pulses. We show that despite the simplicity of the model, it can
behave in non-trivial way. In particular, we discuss and compare two cases of kicked
nonlinear coupler's model (with and without crosscoupling), showing that the quantum
evolution of the system remains closed within a two-qubit Hilbert space. Hence, the system
can be treated as nonlinear quantum scissors [2]. Moreover, maximally entangled Bell
states can be generated during the system's evolution similarly as in [3]. We show that
despite the presence of damping processes, some amount of entanglement can survive in
the system.
References
[1] N. Korolkova, J. Peřina, Quantum statistics and dynamics of Kerr nonlinear couplers,
Opt. Commun. 136, 135-149 (1997).
[2] W. Leoński, A. Kowalewska-Kudłaszyk, Quantum Scissors-Finite- Dimensional States
Engineering, Progr. Opt. 56, 131-185 (2011).
[3] A. Miranowicz, W. Leoński, Two-mode optical state truncation and generation of maximally
entangled states in pumped nonlinear couplers, J. Phys. B: At. Mol. Opt. Phys. 39, 1683-1700
(2006).
23
Parameters of scalar field dark energy in the light
of Planck 2013 results
B. Novosyadlyj, O. Sergijenko
Astronomical Observatory of Ivan Franko National University of Lviv, Ukraine
The Planck 2013 results [1] together with data on baryon acoustic oscillations (BAO) [2-4]
and distance moduli of SNe Ia [5,6] are used for determination of best-fit parameters and
their confidential ranges for cosmological model with cold dark matter and scalar field dark
energy. The scalar field (xi) defined by the canonical Lagrangian
and generalized linear barotropic equation of state pde = 2
qde+C = wdeqde presents the
dynamical quintessence or phantom dark energy depending on the current value of equation
of state parameter wde and its value in the early or future Universe. The best-fit values of
scalar field dark energy parameters and their confidential ranges, obtained using Markov
chain Monte Carlo method and data [1-6], give the possibility to state that the dark energy
is phantom at confidential level > 1. The confidential level of existence of dark energy of
any type is very high: > 10.
References
[1] Planck collaboration, arXiv:1303.5075.
[2] F. Beutler, C. Blake, M. Colless et al., MNRAS 416 (2011) 3017 .
[3] N. Padmanabhan N., X. Xu, D..J. Eisenstein et al., MNRAS 427 (20120) 2132.
[4] L. Anderson, E. Aubourg, S. Bailey et al., MNRAS 427 (2012) 3435.
[5] M. Sullivan, J. Guy, A. Conley et al., Astrophys. ,/. 737 (2011) 102.
[6] X. Suzuki, D. Rubin, C. Lidman. et al., Astrophys. ,/. 746 ( 2012) 85.
24
Investigation of the local structure of boron
andlithium in some borate compunds by MAS
NMR spectroscopy
B. V. Padlyak1,2
, N. A. Sergeev3, M. Olszewski
3
1Division of Spectroscopy of Functional Materials,
Institute of Physics, University of Zielona Góra,
Szafrana Str. 4a, 65-516 Zielona Góra, Poland
2 2Sector of Spectroscopy, Institute of Physical Optics,
Dragomanova Str. 23, 79-005 Lviv, Ukraine
3 Institute of Physics, University of Szczecin,
Wielkopolska Str. 15, 70-451 Szczecin, Poland
The magic angle spinning nuclear magnetic resonance (MAS NMR) spectra of the 11
B, and 7Li isotopes in a series of un-doped glassy and crystalline borate compounds with Li2B4O7,
LiB3O5, LiCaBO3, LiKB4O7 and SrB4O7 chemical compositions were investigated and
analysed. Investigated borate glasses of high optical quality and chemical purity were
obtained from corresponding polycrystalline compounds using standard glass synthesis
according to [1]. The borate single crystals were obtained by Czochralski method. The main
structural units (BO3, BO4, and LiO4 atomic groups) and their proportions in the Li2B4O7,
LiB3O5, LiCaBO3, LiKB4O7 and SrB4O7 glasses and crystals have been established based
on the comparative analysis of the 11
B and 7Li MAS NMR experimental spectra in them.
The obtained results of MAS NMR spectroscopy show good correlation with X-ray
diffraction data for local structure of the cationic sites in borate glasses and crystals with
same chemical compositions [1].
References
[1] B.V. Padlyak, S.I. Mudry, Y.O. Kulyk, A. Drzewiecki, V.T. Adamiv, Y.V. Burak, I.M. Teslyuk,
Mater. Sci.-Poland 30 (2012) 264.
25
The 3He impurity states in 4He
I. Vakarchuk1, G. Panochko
2
1 Department for Theoretical Physics, Ivan Franko National University of Lviv, Ukraine
2 College of Natural Sciences, Ivan Franko National University of Lviv, Ukraine
We consider a set of spinless Bose-particles of mass m with coordinates r1, ... , rN and an
impurity atom of mass M with coordinate r. For the system of “liquid helium + impurity 3He” full- and one-particle density matrices for all temperatures by means of the method of
collective variables in the approximation of pair correlations are found. The contribution to
the full density matrix that takes into account the effect of impurities on the state of the
system at finite temperatures is calculated. At low temperatures this contribution is
considered as a correction to the ground-state energy of the system. The input data for the
numerical calculations are the Fourier coefficients of the two-particle interaction potential
between liquid and impurity which are written via the structure factor S(k) of liquid 4He
obtained from X-rays scattering measurements. The estimation of the effective mass of the
impurity is made.
26
Heart Rate Asymmetry - mathematical,
physiological and medical aspects
J. Piskorski
Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland
Heart rate asymmetry (HRA) is a newly discovered phenomenon by which the behavior of
decelerations and accelerations of heart rate is different. The variance based HRA states
that the contribution of decelerations to short-term heart rate variability is greater than that
of accelerations, and that the contribution of accelerations to long-term and total variability
is greater than that of decelerations. The structure based HRA states that the runs of
accelerations are longer than those of decelerations. Both types are closely related and turn
out to be physiologically and medically important.
27
The inhomogeneous Suslov problem
M. Przybylska1, L.C. Garcia-Naranjo
2,
A.J. Maciejewski3, J.C. Marrero
4
1 Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland 2
3 Institute of Astronomy, University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland 4
We consider the Suslov problem of nonholonomic rigid body motion with inhomogeneous
constraints. We show that if the direction along which the Suslov constraint is enforced is
perpendicular to a principal axis of inertia of the body, then the reduced equations are
integrable and possess an invariant measure. Interestingly, the first integral that permits
integration is transcendental and the density of the invariant measure depends on the
angular velocities. Moreover, in this case, using the so-called alpha-method of Painleve one
can identify when all solutions of the system are single-valued and find their explicit form.
28
Unstable states and cosmology
K. Raczyńska
University of Zielona Góra, Institute of Physics,
ul. Prof. Z. Szafrana 4a, 65-516 Zielona Góra, Poland.
It is known that space regions with unstable false vacuum may originate during the process
of the creation of the Universe [1]. Some of them can survive up to times when their
survival probability has a non-exponential (an inverse power-like) form [2]. The energy of
these false vacuum states at asymptotically late times, (much latter than the transition time,
when contributions to the survival probability of its exponential and non-exponential parts
are comparable), was analyzed in [3]. We analyze properties of the energy of the unstable
false vacuum states at transition time regions in a given model of the unstable state. We
show that at this time region large and rapid fluctuations of this energy occur.
References
[1] S. Coleman, Phys. Rev. D 15, 2929 (1977); C.G. Callan and S. Coleman, Phys. Rev. D,
16, 1762 (1977).
[2] L. M. Krauss, J. Dent, Phys. Rev. Lett., 100, 171301 (2008).
[3] K. Urbanowski, Phys. Rev. Lett., 107, 209001 (2011).
29
Enumeration of plane partitions with a restricted
number of parts
A. Rovenchak
Department of Theoretical Physics, Ivan Franko National University of Lviv,
12 Drahomanov Str., Lviv, UA-79005, Ukraine
The quantum-statistical approach is used to estimate the number of restricted plane
partitions of an integer n with the number of parts not exceeding some finite N. The analogy
between this number- theoretical problem and the enumeration of microstates of the ideal
two-dimensional Bose-gas is used. The conjectured expression for the number of restricted
plane partitions shows a good agreement between calculated and exact values for
n = 10 20.
30
New nonlinear equations in the shallow water
wave problem
A. Karczewska1, P. Rozmej
2, Ł. Rutkowski
2
1 Faculty of Mathematics, Computer Science and Ekonometrics,
University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland
2Faculty of Physics and Astronomy, University of Zielona Góra,
ul. Szafrana 4a, 65-246 Zielona Góra, Poland
The classical problem of irrotational long waves on the shallow water is reconsidered. The
model of ideal fluid moving under the influence of gravity is used with an appropriate
perturbation approach allowing consistent treatment of small parameters. Additionally to
two standard parameters which control amplitude of waves and shallowness of the system,
respectively, the third one, governing the amplitude of the bottom topography is introduced.
Under the assumption that the bottom does not vary rapidly with the horizontal coordinates
the new nonlinear equations describing shallow water waves are derived. Several different
forms of equations have been obtained for different orders in three small parameters. For
the flat bottom KdV equations of different orders, depending of the order of perturbation
are recovered. Some particular examples of numerical solutions to those equations are
presented, as well.
31
Dirac oscillator and nonrelativistic Snyder-de
Sitter algebra
N.M. Stetsko
Department of Theoretical Physics, Ivan Franko National University of Lviv,
12 Drahomanov Str., Lviv, UA-79005, Ukraine
Three dimensional Dirac oscillator was considered in deformed space obeyed to deformed
commutation relations known as Snyder-de Sitter algebra. Snyder-de Sitter commutation
relations give rise to appearance minimal uncertainty in position as well as in momentum.
To derive energy spectrum and wavefunctions of the Dirac oscillator supersymmetric
quantum mechanics and shape invariance technique was applied.
32
Non-dipolar magnetic field at the polar cap of
neutron stars: Two Modes of Inner Acceleration
Region
A. Szary
Institute of Astronomy, University of Zielona Góra,
65-516 Zielona Góra, Poland
The analysis of X-ray observations suggest an ultrastrong surface magnetic field at the
polar cap of pulsars. On the other hand, the temperature of the hot spots is about a few
million Kelvins. Based on these two facts we use the Partially Screened Gap (PSG) model
to describe the Inner Acceleration Region (IAR). The PSG model assumes that the
temperature of the actual polar cap is equal to the so-called critical value, i.e. the
temperature at which the outflow of thermal ions from the surface screens the gap
completely.
We have found that, depending on the conditions above the polar cap, the generation of
high energetic photons in IAR can be caused either by Curvature Radiation (CR) or by
Inverse Compton Scattering (ICS). Completely different properties of both processes result
in two different scenarios of breaking the acceleration gap: the so-called PSG-off mode for
the gap dominated by CR and the PSG-on mode for the gap dominated by ICS. The
existence of two different mechanisms of gap breakdown naturally explains the mode-
changing phenomenon. Different characteristics of plasma generated in the acceleration
region for both processes also explain the pulse nulling phenomenon.
33
Constrained N-body problems
W. Szumiński
Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland
We consider a problem of mass points interacting gravitationally whose motion is subjected
to certain holonomic constraints. The motion of points is restricted to certain curves and
surfaces or hyper-surfaces. We illustrate the complicated behaviour of trajectories of these
systems using Poincaré cross sections. For some models we prove their non-integrability
analyzing properties of the differential Galois group of variational equations along certain
particular solutions of considered systems. Also some integrable cases are identified.
34
Quantum correlations in a two-atom system
R. Tanaś
Nonlinear Optics Division, Faculty of Physics, Adam Mickiewicz University,
Umultowska 85, 61-614 Poznań, Poland
Quantum correlations in systems composed of several subsystems are presently the subject
of intensive studies because of their crucial role in quantum information processing. It is
important to have reliable measures of quantum correlations to distinguish them from
classical correlations. Recently, various measures of quantum correlations have been
introduced and tested. Probably the most popular of them is quantum entanglement, but
there are other measures, such as quantum discord, geometric quantum discord,
measurement induced disturbance and others. We will shortly discuss some of them. The
simplest multipartite system is a bipartite system composed of two qubits, or two two-level
atoms. In case of two-level atoms interacting with the reservoir of electromagnetic field
modes in the vacuum, the evolution of the system can be described by the well known
Lehmberg-Agarwal master equation. The collective evolution of the two-atom system
depends on two collective parameters: collective damping and dipole-dipole interaction,
which both depend on the interatomic distance. Such a system is a good testing ground for
studying evolution of quantum correlations. Nice feature of the system is the fact that, if the
spontaneous emission is the only relaxation process and the system is not driven, the so
called X-form of the density matrix is preserved during the evolution. Examples of time
evolution of various measures of quantum correlations in the two-atom system for different
initial states of the system will be given to illustrate the similarities and differences between
the most popular measures of quantum correlations.
35
Optical properties of gold nanoparticles
A. Timoszyk, A. Mirończyk and J. J. Kozioł
Faculty of Biological Sciences, University of Zielona Góra,
ul. Szafrana 1, 65-516 Zielona Góra, Poland
Gold nanoparticles (GNPs) have been considered as an important area of research due to
their unique properties and their biomedical science including drug delivery, photothermal
therapy, chemical sensing, tissue/tumor imaging and immune-chromatographic
identification of pathogens [1-3]. Due to the recent increasing green chemistry, synthesis of
GNPs must be a nontoxic and environmentally friendly. Biological methods of GNPs
synthesis using plant extract or microorganisms have offered a reliable eco-friendly
alternative to chemical and physical methods [4]. Metal nanoparticles have unique physical
and chemical properties, which are strongly affected by particle size, size distribution,
shape and particle-to-particle interaction [5, 6]. When exited with an electromagnetic field,
GNPs produce an intense absorption attributed to the collective oscillation of electrons on
the particle surface, termed a plasmon resonance [7, 8]. The resonant frequency is high
dependent on particle size, shape and environment. For instance, the sphere geometry of
GNPs allows for control of optical properties in a highly predictive manner, making them a
new class of materials that are capable of tailoring radiation throughout the visible and
infrared wavelength regimes [9]. Because of the mentioned factors above the GNPs could
be characterized by UV-visible spectroscopy, fluorescence spectroscopy, Scanning Electron
Microscopy (SEM) and Different Light Scattering (DLS).
References
[1] L. Du, H. Jiang, X. Liu, E. Wang, Electrochem. Commmun. 9 (2007) 1165.
[2] X. Zhang, S. Yan, R.D. Tyagi, R.Y. Surampalli, Chemosphere 82 (2011) 489.
[3] C.G. Kumar, S.K. Mamidyala, Colloid Surf. B: Biointerfaces 84 (2011) 462.
[4] A.K. Suresh, D.A. Pelletier, W. Wang, M.L. Broich, J-W. Moon, B. Gu, D.P. Allison, D.C. Joy,
T.J. Phelps, M.J. Doktycz, Acta Biomater. 7(5) (2011) 2148.
[5] R. Sardar, A.M. Funston, P. Mulvaney, R.W. Murray, Langmuir 25(24) (2009) 13840.
[6] A. Sànchez-Iglesias, I. Pastoriza-Santos, J. Pérez-Juste, B. Rodríguez- González, F. Javier García
de Abajo, L.M. Liz-Marzán, Advanced Materials 18 (2006) 2529.
[7] T. Ahmad, I.A. Wani, J. Ahmed, O.A. Al-Hartomy, Appl. Nanosci.
DOI 10.1007/s13204-013-0224-y.
[8] W. Rechberger, A. Hohenau, A. Leitner, J.R. Krenn, B. Lamprecht, F.R. Aussenegg,
Optics Commun. 220 (2003) 137.
[9] G. Schatz, K. Shuford, Nanoscape 2(1) (2005) 27
36
Effect of the generalized uncertainty principle on
Galilean and Lorentz transformations
V. M. Tkachuk
Department for Theoretical Physics, Ivan Franko National University of Lviv,
12 Drahomanov St., Lviv, UA-79005, Ukraine
Generalized Uncertainty Principle (GUP) was obtained in string theory and quantum
gravity and suggested the existence of a fundamental minimal length which, as was
established, can be obtained within the deformed Heisenberg algebra. We use the deformed
commutation relations or in classical case (studied in this paper) the deformed Poisson
brackets, which are invariant with respect to the translation in configurational space. We
have found the transformations relating coordinates and times of moving and rest frames of
reference in the space with GUP in the first order over parameter of deformation. For the
non- rclativistic case we find the deformed Galilean transformation which is similar to the
Lorentz one written for Euclidean space with signature (1,1,1,1). The role of the speed of
light here plays some velocity u related to the parameter of deformation, which as we
estimate is many order of magnitude large then the speed of light u 1.2 1022
c.
The coordinates of the rest and moving frames of reference for a relativistic particle in the
space with GUP satisfy the Lorentz transformation with some effective speed of light. We
estimate that the relative deviation of this effective speed of light from c
is ( — e)/c 3.5 10-45
. Finally, note that the influence of GUP on the motion of
particle and the Lorentz transformation in the first order over the parameter of deformation
is hidden in 1/c2 relativistic effects.
37
Two-dimensional models of auxetic foams
K. W. Wojciechowski
Institute of Molecular Physics, Polish Academy of Sciences,
M. Smoluchowskiego 17/19, 60-179 Poznań, Poland
Poisson’s ratio is defined as the negative ratio of the relative change in the transverse
dimension to the relative change in the longitudinal dimension when infinitesimal change
of the longitudinal stress is applied with other components kept fixed [1]. Foams of
negative Poisson’s ratio have been first manufactured by Lakes in 1987 [2]. Materials
exhibiting negative Poisson’s ratio were coined auxetics by Evans [3].
In this lecture, results of computer simulation studies of two simple models of auxetic
foams in two dimensions [4] will be discussed.
Acknowledgments
Part of the simulations was performed at Poznań Supercomputing and Networking Center (PCSS).
References
[1] L. D. Landau and E. M. Lifshitz, Theory of Elasticity, Pergamon Press, London, 1986.
[2] R. S. Lakes, Science 235, 1038 (1987).
[3] K. E. Evans, Endeavour 15, 170 (1991).
[4] A. A. Poźniak, J. Smardzewski, and K. W. Wojciechowski, Smart Materials and
Structures 22, art. 084009 (2013).
38
Theoretical study of magnetic properties of
compounds containing transitional metals
M. Wojciechowski1, B. Brzostowski
1, G. Kamieniarz
2,
A. Bieńko3, J. Mroziński
3
1Institute of Physics, University of Zielona Góra,
ul. Prof. Szafrana 4a, 65-516 Zielona Góra
2Faculty of Physics, A. Mickiewicz University,
ul. Umultowska 85, 61-614 Poznań
3Faculty of Chemistry, University of Wrocław,
ul. F. Joliot-Curie 14, 50-383 Wrocław
Theoretical study of magnetic properties of compounds containing transitional metals
Based on first principles density functional theory (DFT) calculations, we present study of
magnetic compounds. These compounds are (mostly) pentamers containing such
transitional metals as iron, nickel, chromium and copper. Preliminary results for Cu3Cr2 and
Fe2Ni3 structures are presented and discussed. These include spin density maps and energy
values. The 'vanishing' of magnetic moment due to charge transfer between metallic ions is
observed. These results are qualitatively in agreement with empirical results. However full
quantitative explanation of the process requires further study. The computational problems
that arise in the research are also discussed, primarily long computational times which
result from large amount of atoms comprising the structure and methods to overcome them
are presented.
39
Relativistic effects in Penning trap
Yu. Yaremko1, M. Przybylska
2, A.J. Maciejewski
3
1Department for Theoretical Physics, Ivan Franko National University of Lviv,
12 Drahomanov St., Lviv, UA-79005, Ukraine
2 Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland
3 Institute of Astronomy, University of Zielona Góra,
65-516 Zielona Góra, Poland
We are interested in the motion of a classical charge within a processing chamber of a
Penning trap. We examine the relativistic Lagrangian and Hamiltonian dynamics and show
that the radial and axial motions are coupled to each other whenever the special relativity is
taken into account. We demonstrate that for wz ≠ 0 the Hamiltonian system is not integrable
in the Liouville sense in the class of functions meromorphic in coordinates and momenta.
The nonintegrability proof is based on analysis of differential Galois group of variational
equations along a certain particular solution. Also some Poincare sections illustrating
dynamics for physically important values of parameters are shown. In a specific case of
oscillations along the axis of symmetry of quadruple potential the equations of motion are
solved. The solution is expressed in terms of Jacobi elliptic functions. The approximation of
high-energy radial oscillating mode and low-energy axial oscillating mode is analyzed. The
observable relativistic effects such as radiation friction and relativistic cyclotron resonance
are considered.
40
Synthesis of superparamagnetic iron oxide
nanoparticles (SPIONs) in mesoporous silica
materials
B. Zapotoczny1, M.R. Dudek
1, J.J. Kozioł
2, N. Guskos
3,4.
1 Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65-069 Zielona Góra, Poland
2 Faculty of Biological Sciences, University of Zielona Góra,
ul. Szafrana 1, 65-516 Zielona Góra, Poland
3 Department of Solid State Physics, University of Athens,
Panepistimiopolis 15 784, Greece
4 Institute of Physics, West Pomeranian University of Technology,
Al. Piastów 17, 70-310 Szczecin, Poland
Mesoporous silica materials are promising for drug delivery, e.g. [1-3]. Their high surface
areas, tunable pore sizes and volumes give opportunity to carry chemicals, including drugs.
Moreover, high chemical and mechanical stability of silica makes this material perfect as a
template for synthesis inside the pores.
The method of the synthesis of superparamagnetic iron oxide nanoparticles (SPIONS)
directly inside the pores of porous silica will be presented. It is a modification of the
Massart method [4]. According to the diameter of pores, different size of iron oxide
nanoparticles was obtained. The synthesized material has good magnetic properties
(saturation magnetizations 0,7 - 17 emu/g, where the highest saturation magnetizations for
pure iron oxides exhibit magnetite and maghemite: 90–95 emu/g and 60–80 emu/g,
respectively) [5]). Estimated size of gained SPIONs diameter varies from 0.5 to 6 nm.
Samples exhibit superparamagnetic properties in a wide temperature range, both at room
temperature and at 2K.
Porous silica with magnetic nanoparticles have also other advantages. One of them is that
magnetic silica can be controlled by external magnets; another that it can generate magnetic
hyperthermia. Both advantages can be used in drug delivery systems. The recent results on
the use of fabricated magnetic silica as drug delivery nanocapsules will also be mentioned.
Acknowledgements:
The author (B.Z.) is a scholar within Sub-measure 8.2.2 Regional Innovation Strategies, Measure 8.2 Transfer of
knowledge, Priority VIII Regional human resources for the economy Human Capital Operational Programme co-
financed by European Social Fund and state budget.
References
[1] A.B.D. Nandiyanto, S. Kim, F. Iskandar, K. Okuyama Synthesis of spherical mesoporous silica
nanoparticles with nanometer-size controllable pores and outer diameters, Microporous and
Mesoporous Materials 120 (2009) 447–453.
[2] M. Vallet-Regı, F. Balas, M. Colilla, M. Manzano Bioceramics and pharmaceuticals: A
remarkable synergy, Solid State Sciences 9 (2007) 768-776.
[3] A.B.D. Nandiyanto, K. Okuyama Progress in developing spray-drying methods for the production
of controlled morphology particles: From the nanometer to submicrometer size ranges, Advanced
Powder Technology 22 (2011) 1–19.
[4] R. Massart, IEEE T. Magn. 17 (1981) 1247.
[5] B.D. Cullity, C. Graham, Introduction to Magnetic Materials, J. Wiley & Sons, New York, 2008.
41
Critical Casimir forces along the iso-fields
M. Zubaszewska1, A. Maciołek
2,3,4, A. Drzewiński
1
1 Institute of Physics, University of Zielona Góra,
ul. Szafrana 4a, 65-516 Zielona Góra, Poland
2 Max-Planck-Institut für Intelligente Systeme,
Heisenbergstr. 3, D-70569 Stuttgart, Germany
3 IV Institut für Theoretische Physik, Universität Stuttgart,
Pfaffenwaldring 57, D-70569 Stuttgart, German0079
4 Institute of Physical Chemistry, Polish Academy of Sciences,
Kasprzaka 44/52, PL-01-224 Warsaw, Poland
The present study are related to recent experiments showing that plasma membranes are
near a critical point in the two-dimensional Ising class. Using the numerical density-matrix
renormalization-group technique and the Derjaguin approximation we determine the critical
Casimir force and its potential for two discs. To verify our numerical results we analytically
derive the asymptotic decay law.
The most interesting result of our calculation is a signicant increase in the value of the
critical Casimir force along the iso-elds which lie between the bulk coexistence and and the
capillary condensation line. It may have an important consequences for lipid membranes
with protein inclusions, because most probably the concentration of components of the
membrane is not exactly at its critical value.
Acknowledgements:
The author (M.Z.) is a scholar within Sub-measure 8.2.2 Regional Innovation Strategies, Measure 8.2 Transfer of
knowledge, Priority VIII Regional human resources for the economy Human Capital Operational Programme co-
financed by European Social Fund and state budget. Numerical calculations were performed in WCSS Wrocław
(Poland, grant 82).
42
A characteristic structures in entropy surfaces of
cardiovascular time series estimated by the Norm
Component Matrix Algorithm
S. Żurek
Institute of Physics, University of Zielona Góra, ul. Szafrana 4a, 65-516
Zielona Góra, Poland
Sample entropy (SampEn) is a popular complexity measure in HRV analysis. SampEn is
estimated by fixing the values of the embedding dimension "m" and distance threshold "r"
and traditionally SampEn is calculated with m = 2 and r = 0.2 times the standard deviation
of the series. Attempts to extend the estimates to different (m,r) pairs are hampered by the
high computational burden of the traditional algorithm. However, recently an extremely fast
Norm Component Matrix (NCM) algorithm was proposed for SampEn calculation [1]
which allows analyzing whole ranges of (m,r) values leading to entropy surfaces. This short
lecture presents the first attempts to calculate these surfaces by NCM and discusses their
properties for both synthetic and physiological time series.
References
[1] S. Żurek, P. Guzik, S. Pawlak, M. Kośmider, J. Piskorski, Physica A, 391 (2012) 6601