共查询到20条相似文献,搜索用时 78 毫秒
1.
Hiroshi Koibuchi 《Journal of statistical physics》2007,127(3):457-470
A first-order transition is numerically found in a spherical surface model with skeletons, which are linked to each other
at junctions. The shape of the triangulated surfaces is maintained by skeletons, which have a one-dimensional bending elasticity
characterized by the bending rigidity b, and the surfaces have no two-dimensional bending elasticity except at the junctions. The surfaces swell and become spherical
at large b and collapse and crumple at small b. These two phases are separated from each other by the first-order transition. Although both of the surfaces and the skeleton
are allowed to self-intersect and, hence, phantom, our results indicate a possible phase transition in biological or artificial
membranes whose shape is maintained by cytoskeletons. 相似文献
2.
C. Monthus T. Garel 《The European Physical Journal B - Condensed Matter and Complex Systems》2006,53(1):39-45
The directed polymer in a 1+3 dimensional
random medium is known to present a disorder-induced phase
transition. For a polymer of length L, the high temperature
phase is characterized by a diffusive behavior for the end-point
displacement R2 ∼L and by free-energy fluctuations of order
ΔF(L) ∼O(1). The low-temperature phase is characterized by
an anomalous wandering exponent R2/L ∼Lω and
by free-energy fluctuations of order ΔF(L) ∼Lω
where ω∼0.18. In this paper, we first study the scaling
behavior of various properties to localize the critical temperature
Tc. Our results concerning R2/L and ΔF(L) point towards
0.76 < Tc ≤T2=0.79, so our conclusion is that Tc is equal
or very close to the upper bound T2 derived by Derrida and
coworkers (T2 corresponds to the temperature above which the ratio
remains finite as L ↦
∞). We then present histograms for the free-energy, energy and
entropy over disorder samples. For T ≫Tc, the free-energy
distribution is found to be Gaussian. For T ≪Tc, the free-energy
distribution coincides with the ground state energy distribution, in
agreement with the zero-temperature fixed point picture. Moreover the
entropy fluctuations are of order ΔS ∼L1/2 and follow a
Gaussian distribution, in agreement with the droplet predictions,
where the free-energy term ΔF ∼Lω is a near
cancellation of energy and entropy contributions of order L1/2. 相似文献
3.
Ya.I. Azimov 《The European Physical Journal A - Hadrons and Nuclei》2003,16(2):209-219
Isospin-violating mixing of ρ- and ω-mesons is reconsidered in terms of propagators. Its influence on various pairs of (ρ,ω)-decays
to the same final states is demonstrated. Some of them, (ρ,ω)↦π+π- and (ρ,ω)↦πγ, have been earlier discussed in the literature, others (e.g., (ρ,ω)↦ηγ and (ρ,ω)↦e
+
e
-) are new in this context. Changes in partial widths for all the decay pairs are shown to be correlated. The set of present
experimental data, though yet inconclusive, provides some limits for the direct (ρω)-coupling and indirectly supports enhancement
of ρ↦πγ in comparison with ρ±↦π±γ, though not so large as in some previous estimates.
Received: 16 September 2002 / Accepted: 23 September 2002 / Published online: 4 February 2003
RID="a"
ID="a"e-mail: azimov@pa1400.spb.edu
Communicated by V.V. Anisovich 相似文献
4.
H. Müller 《The European Physical Journal A - Hadrons and Nuclei》2001,11(1):113-119
We investigate the reaction pp↦da
0
+ at COSY and SIS energies together with accompanying background reactions and inclusive particle yields. The a
0
+ is considered as a usual u
quark model state with two decay channels a
0
+↦K
+
and a
0
+↦π+η. Calculated cross-sections for a
0
+ production as well as for the corresponding non-resonant channels pp↦dK
+
and pp↦dπ+η are compared. Especially, in case of the final channel dπ+η, high statistics measurements are necessary to extract the a
0
+ signal from the high non-resonant background.
Received: 20 December 2000 / Accepted: 7 May 2001 相似文献
5.
Sayipjamal Dulat Bing-Song Zou 《The European Physical Journal A - Hadrons and Nuclei》2005,26(1):125-134
With accumulation of high statistics data at BES and CLEO-c, many new interesting channels can get enough statistics for partial-wave
analysis (PWA). Among them, ψ↦γpˉ,γΛˉ,γΣˉ,γΞˉ channels provide a good place for studying baryon-antibaryon interactions; the double radiative decays ψ↦γγV with V ≡ ρ,ω,φ have a potential to provide information on the flavor content of any meson resonances (R) with positive charge parity
(C = +) and mass above 1 GeV through ψ↦γR↦γγV; ψ(2s)↦γχc0,1,2 with χc0,1,2↦Kˉπ+π- and 2π+2π- decays are good processes to study χcJ charmonium decays. Using the covariant tensor formalism, here we provide theoretical PWA formulae for these channels. 相似文献
6.
F. Liu W. Wang W. Zheng Y. Wang 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,42(3):435-440
In this study, spatially resolved measurements of the
emission intensity of OH (A2Σ↦X2Π, 0-0) and the
vibrational temperature of N2 (C) have been performed during a positive
pulsed streamer discharge with a wire-plate electrode configuration at
atmospheric pressure. The effects of pulse peak voltage, pulse repetition
rate and the added O2 flow rate on the spatial distributions of the
emission intensity of OH (A2Σ↦X2Π, 0-0) and the
vibrational temperatures of N2 (C) perpendicular to the wire in the
direction towards the plate (in the radial direction) are investigated. It
has been found that the emission intensity of OH (A2Σ↦X2Π, 0-0) increases with increasing pulse peak voltage and pulse
repetition rate and decreases with increasing the distance from the wire
electrode. When the different oxygen flows are added in N2 and H2O
mixture gas, the emission intensity of OH (A2Σ↦X2Π, 0-0) decreases with increasing the flow rate of oxygen. The
vibrational temperature of N2 (C) is nearly independent of pulsed peak
voltage and pulsed repetition rate, but increases with increasing the added
O2 flow rate and keeps almost constant in the radial direction under
the present experimental conditions. This measurement plays a crucial role
in understanding the discharge characters of pulsed streamer discharge and
establishing the molecule reaction dynamics model of pulsed streamer
discharge. 相似文献
7.
The reaction γd↦π+nn is calculated up to order χ5/2 in chiral perturbation theory, where χ denotes the ratio of the pion to the nucleon mass. Special emphasis is put on the
role of nucleon recoil corrections that are the source of contributions with fractional power in χ. Using the known near-threshold
production amplitude for γp↦π+n as the only input, the total cross-section for γd↦π+nn is described very well. A conservative estimate suggests that the theoretical uncertainty for the transition operator amounts
to 3% for the computed amplitude near threshold. 相似文献
8.
C.M. Marian F. Schneider M. Kleinschmidt J. Tatchen 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,20(3):357-367
Electronic spectra of uracil in its diketo (lactam) form and five enol (lactim) tautomeric forms have been investigated by
means of combined density functional and configuration interaction methods. We have simulated the effects of hydrogen bonding
with a protic solvent by recomputing the spectrum of uracil in the presence of two, four, or six water molecules. Geometries
of the electronic ground state and several low-lying excited states have been optimized. Spin-orbit coupling has been determined
for correlated wavefunctions employing a non-empirical spin-orbit mean-field approach. In accord with experiment, we find
the diketo tautomer to be the most stable one. The calculations confirm that the first absorption band arises from the 1( π↦π*) S
0↦S
2 excitation. The experimentally observed vibrational structure in this band originates from a breathing mode of the six ring.
Complexation with water molecules is seen to cause a significant blue shift of n↦π* excitations while leaving π↦π* excitations nearly uninfluenced. Computed radiative lifetimes are presented for the experimentally known weak phosphorescence
from the π↦π* excited T1 state. Among the uracil lactim tautomers, one is particularly interesting from a spectroscopic point of view. In this tautomer,
the π↦π* excitation gives rise to the S1 state.
Received 18 February 2002 / Received in final form 5 June 2002 Published online 13 September 2002 相似文献
9.
Koibuchi H 《The European physical journal. E, Soft matter》2008,26(3):301-308
We study the phase structure of a surface model by using the canonical Monte Carlo simulation technique on triangulated, fixed connectivity, and spherical surfaces with many fine holes. The size of a hole is assumed to be of the order of lattice spacing (or bond length) and hence can be negligible compared to the surface size in the thermodynamic limit. We observe in the numerical data that the model undergoes a first-order collapsing transition between the smooth phase and the collapsed phase. Moreover the Hasudorff dimension H remains in the physical bound, i.e., H < 3 not only in the smooth phase but also in the collapsed phase at the transition point. The second observation is that the collapsing transition is accompanied by a continuous transition of surface fluctuations. This second result distinguishes the model in this paper and the previous one with many holes, whose size is of the order of the surface size, because the previous surface model with large-sized holes has only the collapsing transition and no transition of surface fluctuations. 相似文献
10.
11.
L. Frunza A. Schönhals H. Kosslick S. Frunza 《The European physical journal. E, Soft matter》2008,26(4):379-386
A series of AlMCM-41 molecular sieves was prepared with constant composition (Si/Al = 14.7) and presumably same pore structure
but different pore diameters (from 2.3 to 4.6 nm). The pore size distribution is narrow for each sample. The rotational fluctuations
of water molecules confined inside the pores were investigated applying broadband dielectric spectroscopy (10−2–107 Hz) over a large temperature interval (213–333K). A relaxation process, slower than that expected for bulk water, was observed
which is assigned to water molecules forming a surface layer on the pore walls. The estimated relaxation time has an unusual
non-monotonic temperature dependence, which is rationalized and modeled assuming two competing processes: rotational fluctuations
of constrained water molecules and defect formation (Ryabov model). This paper focuses on the defects and notably the influence
of the hydroxyl groups of the pore walls. The Ryabov model is fitted to the data and characteristic parameters are obtained.
Their dependence on pore diameter is considered for the first time. The found results are compared with those obtained for
other types of molecular sieves and related materials. 相似文献
12.
H. Koibuchi 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,59(1):55-62
Nambu-Goto model is investigated by using the canonical Monte Carlo simulation technique on dynamically triangulated surfaces
of spherical topology. We find that the model has four distinct phases; crumpled, branched-polymer, linear, and tubular. The
linear phase and the tubular phase appear to be separated by a first-order transition. It is also found that there is no long-range
two-dimensional order in the model. In fact, no smooth surface can be seen in the whole region of the curvature modulus α,
which is the coefficient of the deficit angle term in the Hamiltonian. The bending energy, which is not included in the Hamiltonian,
remains large even at sufficiently large α in the tubular phase. On the other hand, the surface is spontaneously compactified
into a one-dimensional smooth curve in the linear phase; one of the two degrees of freedom shrinks, and the other degree of
freedom remains along the curve. Moreover, we find that the rotational symmetry of the model is spontaneously broken in the
tubular phase just as in the same model on the fixed connectivity surfaces. 相似文献
13.
We introduce a solid-on-solid growth process which evolves by random deposition of dimers, surface diffusion, and evaporation
of monomers from the edges of plateaus. It is shown that the model exhibits a robust transition from a smooth to a rough phase.
The roughening transition is driven by an absorbing phase transition at the bottom layer of the interface, which displays
the same type of critical behavior as the pair contact process with diffusion 2A↦3A, 2A↦.
Received 14 October 2002 Published online 14 February 2003
RID="a"
ID="a"e-mail: Haye.Hinrichsen@physik.uni-wuppertal.de 相似文献
14.
E. Heinsalu M. Patriarca F. Marchesoni 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,69(1):19-22
We study the effects of the confining conditions on the
occurrence of stochastic resonance (SR) in continuous bistable
systems. We model such systems by means of double-well potentials
that diverge like |x|q for |x|↦∞. For super-harmonic
(hard) potentials with q > 2 the SR peak sharpens with increasing q, whereas for sub-harmonic (soft) potentials, q < 2, it
gets
suppressed. 相似文献
15.
I. Endo H. Koibuchi 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,66(4):467-475
We numerically study the phase structure of two types of triangulated spherical surface models, which includes an in-plane
shear energy in the Hamiltonian, and we found that the phase structure of the models is considerably influenced by the presence
of the in-plane shear elasticity. The models undergo a first-order collapsing transition and a first-order (or second-order)
transition of surface fluctuations; the latter transition was reported to be of second-order in the first model without the
in-plane shear energy. This leads us to conclude that the in-plane elasticity strengthens the transition of surface fluctuations.
We also found that the in-plane elasticity decreases the variety of phases in the second model without the in-plane energy.
The Hamiltonian of the first model is given by a linear combination of the Gaussian bond potential, a one-dimensional bending
energy, and the in-plane shear energy. The second model is obtained from the first model by replacing the Gaussian bond potential
with the Nambu-Goto potential, which is defined by the summation over the area of triangles. 相似文献
16.
P. Richmond 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,20(4):523-526
A simple agent model is introduced by analogy with the mean field approach to the Ising model for a magnetic system. Our model
is characterised by a generalised Langevin equation = F
ϕ + G
ϕ
t
where
t
is the usual Gaussian white noise, i.e.:
t
t
′
= 2Dδ
t-t
′
and
t
= 0. Both the associated Fokker Planck equation and the long time probability distribution function can be obtained analytically.
A steady state solution may be expressed as P
ϕ =
exp{ - Ψϕ - ln G(ϕ)} where Ψϕ = -
F/
G
dϕ and Z is a normalization factor. This is explored for the simple case where F
ϕ = Jϕ + bϕ2 - cϕ3 and fluctuations characterised by the amplitude G
ϕ = ϕ + ɛ when it readily yields for ϕ≫ɛ, a distribution function with power law tails, viz: P
ϕ =
exp{2bϕ-cϕ2
/D}. The parameter c ensures convergence of the distribution function for large values of ϕ. It might be loosely associated with the activity
of so-called value traders. The parameter J may be associated with the activity of noise traders. Output for the associated time series show all the characteristics
of familiar financial time series providing J < 0 and D≈ | J|.
Received 25 July 2000 相似文献
17.
S.-U. Haq S. Mahmood M. A. Kalyar M. Rafiq R. Ali M. A. Baig 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,44(3):439-447
We present experimentally measured absolute values of the photoionization
cross sections from the 5s5p 1P1 and 5s5p 3P1 excited
states of strontium at the first ionization threshold as 11.4±1.8 Mb
and 10.7±1.7 Mb respectively using saturated absorption technique
along with a thermionic diode ion detector in conjunction with a Nd:YAG
pumped dye laser system. These threshold photoionization cross sections
values have been utilized to determine the oscillator strengths of the
5s5p 1P1↦5snd 1D2 and 5s5p 3P1↦5snd 3D2 Rydberg transitions. The oscillator strength densities in the
continuum corresponding to the 5s5p 3P1 excited state have also
been determined by measuring the photoionization cross sections at five
ionizing wavelengths above the first ionization threshold. Smooth merging of
the discrete f-values into the oscillator strength densities has been
observed for the 5s5p 3P1↦5snd 3D2 series across the
ionization threshold. 相似文献
18.
Y. Yan J. Y. Zhang T. Cui Y. Li Y. M. Ma J. Gong Z. G. Zong G. T. Zou 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,61(4):397-403
The lattice dynamics of lithium nitride (Li3N) under high pressure are extensively investigated to probe its phase transformations by using the pseudopotential plane-wave
method within the density functional theory. A new second order α↦α′-Li3N phase transition is identified for the first time. The newly proposed α′-phase possesses a hexagonal symmetry with four ions in the unit cell having a space group of P-3m1. Further enthalpy and
phonon calculations support the existence of this phase, which stabilizes in a narrow pressure range of 2.8 – 3.6 GPa at zero
temperature. Upon further compression, transitions to denser packed phases of β-and γ-Li3N are typical first order. The analysis of the electronic densities of states suggests that all the high pressure modifications
of Li3N are insulators and, interestingly, the typical behavior of compression is to broaden the band gap. 相似文献
19.
V.Yu. Grishina L.A. Kondratyuk E.L. Bratkovskaya M. Büscher W. Cassing 《The European Physical Journal A - Hadrons and Nuclei》2000,9(2):277-285
We investigate the reactions πN↦a
0
N and pp↦da
0
+ near threshold and at medium energies. An effective Lagragian approach and the Regge pole model are applied to analyze different
contributions to the cross-section of the reaction πN↦a
0
N. These results are used to calculate the differential and total cross-sections of the reaction pp↦da
0
+ within the framework of the two-step model in which two nucleons produce an a0-meson via π-meson exchange and fuse to a deuteron. The necessity of new measurements on a0 production and branching fractions (of its decay to the K
and πη channels) is emphasized for clarifying the a0 structure. Detailed predictions for the reaction pp→da
0
+ are presented for the energy regime of the proton synchrotron COSY-Jülich.
Received: 4 August 2000 / Accepted: 17 September 2000 相似文献
20.
A. Ghoshal P. Mandal 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,44(2):327-335
e+ + H(ns) ↦e+ + H(n′s) transitions for arbitrary n and
n′ have been studied using the distorted-wave formalism in the
momentum space [Ghoshal and Mandal, Phys. Rev. A 72, 032714 (2005)]. The distorted-wave
scattering amplitudes have been written in a simple closed analytical form. A detailed
study has been made on differential and total cross sections in the energy range 20–300 eV.
Resonance-like behaviour of the
differential cross section has been observed in the the region of lower scattering angles
for high Rydberg transitions. To the best of our knowledge the distorted-wave results for
differential and total cross sections for such arbitrary transitions are reported for the
first time in the literature. 相似文献