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  • 1
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    Celestial mechanics and dynamical astronomy 78 (2000), S. 167-195 
    ISSN: 1572-9478
    Keywords: chaos ; numerical tools ; Nekhoroshev ; Chirikov
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract It is already known (Froeschlé, Lega and Gonczi, 1997) that the Fast Lyapunov Indicator (FLI), that is the computation on a relatively short time of the largest Lyapunov indicator, allows to discriminate between ordered and weak chaotic motion. We have found that, under certain conditions, the FLI also discriminates between resonant and non-resonant orbits, not only for two-dimensional symplectic mappings but also for higher dimensional ones. Using this indicator, we present an example of the Arnold web detection for four and six-dimensional symplectic maps. We show that this method allows to detect the global transition of the system from an exponentially stable Nekhoroshev’s like regime to the diffusive Chirikov’s one.
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  • 2
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    Celestial mechanics and dynamical astronomy 78 (2000), S. 197-210 
    ISSN: 1572-9478
    Keywords: chaos ; KAM tori ; cantori ; asymptotic curves
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We find the form of cantori surrounding an island of stable motion in the standard map for various values of the nonlinearity parameter K near the value K = 5 (much larger than the critical value K cr = 0.971635...). The asymptotic curves of unstable periodic orbits inside the cantorus cross it after a certain time and then escape to the large chaotic sea. For K = 5 the crossing time (in appropriate units) is t = 1 and the escape time is t = 2. For K = 4.998 the crossing time is t = 7 and the escape time t = 23000. This delay of escape is due to the existence of higher order cantori, with very small gaps. We found that, as K increases the noble torus [2,4,1,1,..] is destroyed before the destruction of the higher order tori [2,4,1,1,1,1,2,1,...] and [2,4,1,1,1,1,3,1,...]. Thus the torus with the simplest noble number is not the last KAM curve to be destroyed. Then we find that nearby orbits deviate considerably, but the average times spent near various resonance before escape are very similar.
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  • 3
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    Celestial mechanics and dynamical astronomy 74 (1999), S. 59-67 
    ISSN: 1572-9478
    Keywords: planetary systems ; Liapunov exponents ; chaos ; symplectic integration
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Equations are presented for the computation of tangent maps for use in nearly Keplerian motion, approximated by use of a symplectic leapfrog map. The resulting algorithms constitute more accurate and efficient methods to obtain the Liapunov exponents and the state transition matrix, and can be used to study chaos in planetary motions, as well as in orbit determination procedures from observations. Applications include planetary systems, satellite motions and hierarchical, nearly Keplerian systems in general.
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  • 4
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    Celestial mechanics and dynamical astronomy 74 (1999), S. 111-146 
    ISSN: 1572-9478
    Keywords: Mimas–Tethys system ; chaos ; secondary resonances ; tides ; capture probability
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We have investigated the role of the 200 yr period discovered by Vienne and Duriez (1992) on the tidal evolution of the Mimas–Tethys system through the 2:4 ii′ present resonance. Three terms are found to generate this period. We present a perturbed‐pendulum model in which these terms bring about a perturbation to the ideal ii′ resonance pendulum, which is in a direct ratio to the eccentricity e′ of Tethys. Although e′ is now very small, it is shown that this quantity could have been much greater in the past. We also show, thanks to this model, that these terms may have brought about a stochastic layer of noticeable width at the time of capture in the ii′ resonance, with the consequence that the possible values of the inclination i of Mimas before capture range from 0.4° to 0.6° (these uncertainties arise from the present uncertainties on e′). The role of each one of the three terms is examined in the appearance of chaos. A capture into the 1/1 secondary resonance (between the libration period of the primary ii′ resonance and the period of about 200 yr) is found possible. It means that the system could have experienced several captures in the primary resonance, instead of a single one, and that i could have been, with this assumption, much lower than 0.4°. A probability of capture into this secondary resonance as a function of the eccentricity of Tethys on encounter is derived, using Malhotra's method (Malhotra, 1990). Allan's values of i = 0.42° and e′ ≈ 0 (Allan, 1969) are therefore called into question, and taking e′ ≠ 0 is shown to be absolutely necessary if we want to understand the phenomena at work in the Mimas–Tethys system.
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  • 5
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    Celestial mechanics and dynamical astronomy 76 (2000), S. 23-34 
    ISSN: 1572-9478
    Keywords: one dimensional three-body problem ; triple collision ; chaos
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We consider the motions of particles in the one-dimensional Newtonian three-body problem as a function of initial values. Using a mapping of orbits to symbol sequences we locate the initial values leading to triple collisions. These turn out to form curves which give clear structure to the region in which the motions depend sensitively on initial conditions. In addition to finding the triple collision orbits we also locate orbits which end up to a triple collision in both directions of time, that is, orbits which are finite both in space and time.
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  • 6
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    Celestial mechanics and dynamical astronomy 76 (2000), S. 187-214 
    ISSN: 1572-9478
    Keywords: three-body problem ; triple collision ; binary collision ; escape ; chaos
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Dominant factors for escape after the first triple-encounter are searched for in the three-body problem with zero initial velocities and equal masses. By a global numerical survey on the whole initial-value space, it is found that not only a triple-collision orbit but also a particular family of binary-collision orbits exist in the set of escape orbits. This observation is justified from various viewpoints. Binary-collision orbits experiencing close triple-encounter turn out to be close to isosceles orbits after the encounter and hence lead to escape. Except for a few cases, binary-collision orbits of near-isosceles slingshot also escape.
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  • 7
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    Celestial mechanics and dynamical astronomy 78 (2000), S. 17-46 
    ISSN: 1572-9478
    Keywords: asteroids ; proper elements ; chaos ; families
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract For the orbits with low to moderate inclination and eccentricity, in the asteroid main belt, the analytically computed proper elements are accurate to a level very close to the best result achievable by any analytical theory. This fundamental limitation results from the infinite web of resonances and because of the occurrence of chaotic motions. Still, there are some regions of the belt in which these proper elements are of degraded accuracy, thus preventing a reliable definition of asteroid families and detailed studies of the dynamical structure. We have used a different method to compute asteroid proper elements, following the approach introduced in the LONGSTOP project to describe the secular dynamics of the major outer planets. By applying purely numerical techniques, we produced so-called ‘synthetic’ proper elements for a catalog of 10,256 asteroids with osculating semimajor axes between 2.5 and 4.0 AU. The procedure consisted of simultaneous integration of asteroid and planetary orbits for 2 Myr, with online filtering of the short-periodic perturbations. The output of the integration was spectrally resolved, and the principal harmonics (proper values) extracted from the time series. For each asteroid we have also tested the accuracy and stability in time of the proper elements, and estimated the maximum Lyapunov Characteristic Exponent to monitor the chaotic behaviors. This provided information on the reliability of the data for each orbit, in particular allowing to select 1,852 cases for an extended integration (10 Myr) of the orbits showing instability. The results indicate that for more than half of the cases the proper elements have a time stability improved by more than a factor 3 with respect to the elements computed by the previous analytical theory. But of course there are also unstable cases for which the proper elements are less accurate and reliable, the extreme examples being 23 orbits exhibiting hyperbolic escape from the solar system. This form of escape from the asteroid belt could be responsible for a significant mass loss over the age of the solar system.
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  • 8
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    Celestial mechanics and dynamical astronomy 64 (1996), S. 93-105 
    ISSN: 1572-9478
    Keywords: asteroids ; resonance ; chaos ; Kirkwood gaps
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The utilization of chaotic dynamics approaches allowed the identification of many modes of motion in resonant asteroidal dynamics. As these dynamical systems are not integrable, the motion modes are not separated and one orbit may transit from one mode to another. In some cases, as in the \31 resonance, these transitions may lead, in a relatively short time scale, to eccentricities so high that the asteroid may approach the Sun and be destroyed. In the \21 and \32 resonances these transitions are much slower and only indirect estimations of the time which is needed for a generic asteroid to leave the resonance are possible. It may reach hundreds of million years in the more robust regions of the \21 resonance and a time of the order of billions of years in those of the \32 resonance. These values are consistent with the observed depletion of the \21 resonance (only a few asteroids known while almost 60 asteroids are known in the \32 resonance).
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  • 9
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    Celestial mechanics and dynamical astronomy 61 (1995), S. 287-313 
    ISSN: 1572-9478
    Keywords: Two-body problem ; radiation pressure ; horseshoes ; chaos ; three-body problem
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We study a perturbed Newtonian two-body problem, in which the perturbation is due to a force field of constant magnitude but rotating direction. By considering this system as a perturbation of the non-rotating case a Melnikov-type analysis allows us to show the existence of horseshoes in the level sets of the Hamiltonian and the subsequent sensitive dependence on initial conditions and non-integrability. We discuss the consequences of these results for a particular planar restricted three-body problem.
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  • 10
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    Celestial mechanics and dynamical astronomy 70 (1998), S. 181-200 
    ISSN: 1572-9478
    Keywords: chaos ; dynamics ; comets ; NEAs ; Lyapunov exponent
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The dynamics of two families of minor inner solar system bodies that suffer frequent close encounters with the planets is analyzed. These families are: Jupiter family comets (JF comets) and Near Earth Asteroids (NEAs). The motion of these objects has been considered to be chaotic in a short time scale,and the close encounters are supposed to be the cause of the fast chaos. For a better understanding of the chaotic behavior we have computed Lyapunov Characteristic Exponents (LCEs) for all the observed members of both populations. LCEs are a quantitative measure of the exponential divergence of initially close orbits. We have observed that most members of the two families show a concentration of Lyapunov times (inverse of LCE) around 50–100yr. The concentration is more pronounced for JF comets than for NEAs, among which a lesser spread is observed for those that actually cross the Earth's orbit (mean perihelion distance q 〈 1.05 AU). It is also observed that a general correspondence exists between Lyapunov times and the time between consecutive encounters. A simple model is introduced to describe the basic characteristics of the dynamical evolution. This model considers an impulsive approach, where the particles evolve unperturbedly between encounters and suffer ‘kicks’ in semimajor axis at the encounters. It also reproduces successfully the short Lyapunov times observed in the numerical integrations and is able to estimate the dynamical lifetimes of comets during a stay in the Jupiter family in correspondence with previous estimates. It has been demonstrated with the model that the encounters with the largest effect on the exponential growth of the distance between initially nearby orbits are neither the infrequent deep encounters, nor the frequent and far ones; instead, the intermediate approaches have the most relevant contribution to the error growth. Such encounters are at a distance a few times the radius of the Hill's sphere of the planet (e.g. 3). An even simpler model allows us to get analytical estimates of the Lyapunov times in good agreement with the values coming from the model above and the numerical integrations. The predictability of the medium‐term evolution and the hazard posed to the Earth by those objects are analysed in the Discussion section.
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  • 11
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    The European physical journal 321 (1985), S. 403-409 
    ISSN: 1434-601X
    Keywords: 21.10.Ky ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The quadrupole moments of the neutron isomers in140,142Sm were determined by measuring the quadrupole interaction of Sm in Gd using single crystals. The moment for the 10+ isomer in140Sm was determined to be ¦Q¦=167(48) fm2 and for the 7− isomer in142Sm ¦Q¦=112(27) fm2. The quadrupole moments are a measure for a deformation which turned out to be very similar to the deformation found for corresponding proton isomers in Gd isotones.
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  • 12
    ISSN: 1434-601X
    Keywords: 21.10.Tg ; 21.60.−n ; 25.20.Lj ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The115In(γ, γ′) reaction was measured at the S-DALINAC using bremsstrahlung with endpoint energiesE 0=3.1, 4.6 and 5.2 MeV. In the excitation energy range of 1–5 MeV in total 32 transitions were observed, 18 of which were hithertoo unknown. The results are compared to two quasiparticle-phonon model calculations, one with a model space of ‘quasiparticle⊗phonon’ and one extended by ‘quasiparticle⊗two-phonon’ configurations. A substantial improvement is achieved in the description of low-lying115In states by the consideration of the more complex configurations. The calculations quantitatively account for the summed115In(γ, γ′) integrated cross sections and show a comparable amount of fragmentation of the individual transition strengths. The model interpretation of the microscopic structure of the experimentally observed transitions is discussed.
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  • 13
    ISSN: 1434-601X
    Keywords: 27.60.+j ; 25.70.Gh
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The level scheme of147Tb has been extended to 116 levels and 198 transitions in two experiments with the OSIRIS Compton suppressed detector array at the HMI Berlin with the reactions122Sn(31P, 6n)147Tb at 160 MeV and120Sn(31P, 4n)147Tb at 152 MeV. Evidence for a new high spin isomer atE=7664.1 keV with a life-time of the order of 2 ns has been found.
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  • 14
    ISSN: 1434-601X
    Keywords: 23.20.Lv ; 23.20.En ; 27.60.+j
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    Topics: Physics
    Notes: Abstract High spin states are populated in102Ag using the reaction16O+89Y with projectile energies in the energy range 60–80 MeV. Gamma multipolarities are inferred from DCO ratios and coincidence relationships are established among the gamma rays assigned to102Ag. A comprehensive level scheme is constructed with four band systems, two of positive parity and the other two of negative parity. The present study extended spins upto 19− in the main negative parity band. A new band is populated in the present work and is similar to the one observed in106Ag.
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  • 15
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    The European physical journal 351 (1995), S. 357-358 
    ISSN: 1434-601X
    Keywords: 27.60.+j ; 23.20.Lv
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    Topics: Physics
    Notes: Abstract Evidence for the 2+ level in102Sr is obtained from theβ-decay of102Rb, mass separated at the ISOLDE facility. The energy of 126 keV and the collectivity of the 2+→0+ transition indicate that102Sr is a strongly deformed rigid rotor. In addition, a sizeable lifetime is measured for the 94 keV transition in102Y.
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  • 16
    ISSN: 1434-601X
    Keywords: 23.20.Lv ; 27.60.+j
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    Topics: Physics
    Notes: Abstract From new measurements, a half-live of 4.2±0.3 s has been clearly established in127Pr. This value confirms our first result [4] and rules out other data [5]. The127Pr activity was produced by bombarding92Mo or94Mo targets with 210 MeV40Ca beams. The mass identification has been made using an ion-guide coupled with an on-line isotope separator. The partial level scheme proposed for127Ce has been deduced from β-gated γ spectra and Xγ- and γγ-coincidences. A new band structure based on a 1/2+ state is established.
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  • 17
    ISSN: 1434-601X
    Keywords: 27.60.+j ; 23.20. Lv ; 21.60. Ev
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    Topics: Physics
    Notes: Abstract The level structure of104Ag has been studied through the103Rh (α, 3nγ) reaction at Eα=40 and 45 MeV. The principal features of the proposed level scheme are in agreement with those obtained earlier through heavy ion reaction. Two quasiparttcle-plus-rotor model calculation has been performed, and the results are compared with experimental data.
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  • 18
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    The European physical journal 351 (1995), S. 13-18 
    ISSN: 1434-601X
    Keywords: 21.60.EV ; 23.20.Ck ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The half-lives of seven levels in105Mo have been determined with high precision at the fission-product separator Josef. Theβ-γ-γ triple coincidence method with plastic and BaF2 scintillators was used for a determination of the time between theβ q feeding of a level of interest and itsγ depopulation. A value ofβ q =0.38 (1) for the deformation parameter has been deduced from the half-lives of the first and second excited states. The results of Particle-Rotor model-calculations with the Nilsson parametersκ=0.084 andμ=0.28 support the assignment of the Nilsson orbital [532] 5/2− to the ground state of105Mo.
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  • 19
    ISSN: 1434-601X
    Keywords: 23.20.Lv ; 27.60.+j ; 21.60.Cs
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    Topics: Physics
    Notes: Abstract An extended level scheme of109Sn is presented showing high-spin states up to Ex≈ 8 MeV and spins up toJπ=(41/2+). Their decay to the 5/2+ ground state has been observed identifying a 12.8 keV 7/2+ → 5/2+ transition. A half-life of T1/2=7(1) ns has been measured for the 17/2+ state atE x =2114 keV. The experimental data are compared with the predictions of shell-model calculations.
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  • 20
    ISSN: 1434-601X
    Keywords: 21.10.Re ; 23.20.Lv ; 27.60.+j
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    Topics: Physics
    Notes: Abstract High spin states of117Xe have been investigated by means of in-beam γ-ray spectroscopy using the reaction92Mo(28Si, 2pn) at beam energies of 100 to 120 MeV. The previously known νh11/2 bands are confirmed and the νg7/2 favored-signature band is extended up to 47/2+, in which two band crossings are observed at ħω=0.33 and 0.44 MeV, respectively. Two new positive-parity bands have been established, one of which is most likely the νg7/2 unfavored-signature band. A new transition cascade with irregular level spacings is also observed.
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  • 21
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    The European physical journal 352 (1995), S. 247-255 
    ISSN: 1434-601X
    Keywords: 21.10.Hw ; 27.60.+j ; 23.20.Lv
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    Topics: Physics
    Notes: Abstract High spin states up toJ=14 and excitation energy up toE *=3076 keV have been observed in the odd-odd nucleus100Tc with the reaction96Zr(7Li, 3n), at bombarding energies between 21 and 31 MeV, by in-beam γ spectroscopy and conversion-electron measurements. A ΔJ=1 negative parity band similar to that observed in theN=57 isotone102Rh, and based on the 8−, 708 keV state has been identified. The observed band can be interpreted in terms of collective core excitations based on a two-quasiparticle state of(πg9/2 ⊗ νh11/2) configuration. Comparison with IBFM-2 calculations have been performed.
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  • 22
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    The European physical journal 352 (1995), S. 293-301 
    ISSN: 1434-601X
    Keywords: 27.60.+j ; 23.20.Lv
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    Topics: Physics
    Notes: Abstract The low-energy level scheme of theN=63 nucleus101Sr has been obtained from a β-decay study of101Rb. The ν[532]5/2 and ν[411]3/2 orbitals are well established as the ground state and a band head at 271.2keV, respectively. The general properties of the level scheme indicate a quadrupole deformation ofβ ≃ 0.4, confirming the unique feature of saturation of deformation inN ≥ 60 Sr isotopes. The energies of theK=3/2 intraband transitions in the odd-neutron neighbours99Sr61 and101Sr63 are very similar. More generally, the identical bands at low spin in98–101Sr nuclei are correlated with the mass-independent moments of inertia in this region.
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  • 23
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    The European physical journal 321 (1985), S. 593-598 
    ISSN: 1434-601X
    Keywords: 25.85.Ec ; 21.10.Ky ; 27.60.+j
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    Topics: Physics
    Notes: Abstract Theg factors of the first excited 2+ levels in the neutron-rich nuclei102Mo and104Mo have been studied through the measurement of the perturbed angular correlations for theγ-γ cascades between the 0 2 + -2 1 + -0 1 + level sequences. The results of g=0.42±0.07 for102Mo and ofg= −0.11 +0.12 for104Mo agree with the prediction of the vibrational-rotational model. In terms of IBA, with the assumption ofN π=3 for the Mo isotopes which takes into consideration a two particle, two-hole excitation across the Z=40 subshell, the proton-bosong factor is deduced to beg π=1.00±0.23. It is shown that this value provides evidence for subshell effects in100Zr.
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  • 24
    ISSN: 1434-601X
    Keywords: 27.60.+j ; 25.70.Gh
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    Topics: Physics
    Notes: Abstract The level scheme of148Tb has been extended to an excitation energyE x =14.0 MeV and a spinI≈ 38ħ in two experiments with the OSIRIS Comptom suppressed detector array at the HMI Berlin using the reactions122Sn(31P,5n)148Tb at 160 MeV and120Sn(31P,3n)148Tb at 152 MeV.
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  • 25
    ISSN: 1434-601X
    Keywords: 23.20.Lv ; 27.60.+j
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    Topics: Physics
    Notes: Abstract High spin levels in119Te have been populated following the96Zr (30Si, α 3n)119Te reaction at a beam energy of 135 MeV. The subsequentγ-ray deexcitation was studied usingγ-ray spectroscopic methods. New levels and several spin and parity assignments up toJ π=55/2− were established. The decay scheme at high-spin exhibits single-particle characteristics associated with the fully aligned ν(h11/2)3 π(g7/2)2 configuration for the 39/2− level, while the 55/2− level could be interpreted as fully aligned π(d5/2)2 ν h 11 2/5 g 7 2/−2 ) configuration.
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  • 26
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    The European physical journal 352 (1995), S. 373-390 
    ISSN: 1434-601X
    Keywords: 21.10.Sf ; 21.60.Cs ; 23.20.-g ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The neutron deficient nuclei98Ag,104Sn withT z =2 and103In,105Sn (T z=5/2) were studied in-beam following the reaction of 250 MeV58Ni+50Cr. Neutron and charged particle (p, α) gatedγγ-coincidence spectra were used to identify these nuclei, which are populated with yields between 0.05% and 2% of the total residue cross section, and to determine their level schemes. In a comprehensive shell model study various approaches for the residual interaction were used to describe these newly and several previously studied neutron deficient nuclei. As a result predictions for the neutron single particle energies for100Sn are obtained and used to discuss the next generation of experiments.
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  • 27
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    The European physical journal 352 (1995), S. 391-395 
    ISSN: 1434-601X
    Keywords: 21.10.Re ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The band structures of121, 123I nuclei have been studied using a version of the particle-rotor-model in which the experimental excitation energies of the neighbouring (A-1) cores can be fed directly as input parameters. The calculations have been carried out with axially symmetric Nilsson potential with both prolate and oblate deformations. The parameters of the model have been chosen from earlier theoretical work and experimental odd-even mass differences. Only the Coriolis attenuation factor has been treated as adjustable parameter. The theoretical band structures are in very good agreement with the available experimental data.
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  • 28
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    Optical review 5 (1998), S. 280-284 
    ISSN: 1349-9432
    Keywords: semiconductor laser ; optical feedback ; chaos ; relaxation oscillation ; linear stability analysis
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    Topics: Physics
    Notes: Abstract The stability enhancement of laser output power for the change of external cavity position in semiconductor lasers with optical feedback is observed by experiment. The relaxation oscillation frequency which plays an important role in the dynamics of the nonlinear system is also investigated as a function of the external cavity length. The period of the stability enhancement along the position of the external cavity is exactly coincident with the length corresponding to the relaxation oscillation frequency of the solitary laser. The experimental results are compared with theoretical and excellent coincidence between the two is found.
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  • 29
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    Optical review 6 (1999), S. 359-364 
    ISSN: 1349-9432
    Keywords: semiconductor laser ; photorefractive optical feedback ; instability ; chaos
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    Topics: Physics
    Notes: Abstract The dynamics of semiconductor lasers with photorefractive phase conjugate optical feedback are experimentally studied. Photorefractive fringes considered here are rather static compared with time fluctuations of laser output power. Therefore, it is expected that a semiconductor laser with photorefractive feedback shows similar dynamics to those with conventional optical feedback. We examine relaxation oscillation and external cavity modes of laser output power in the presence of photorefractive phase conjugate feedback. It is proved that the dynamics of photorefractive phase conjugate feedback are fundamentally the same as those of conventional optical feedback.
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    ISSN: 1349-9432
    Keywords: semiconductor laser ; optical feedback ; low frequency fluctuation ; chaos
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    Notes: Abstract The properties of low-frequency fluctuations in semiconductor lasers with optical feedback from a long external cavity are experimentally studied. Frequency-locking of the laser light output to the injection current modulation is observed when the modulation frequency approaches the external cavity mode. The modulation frequency for the successful frequency-locking is always less than the external cavity mode frequency and the locking domains as a function of the modulation amplitude is asymmetric with respect to the frequency detuning.
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    Pure and applied geophysics 147 (1996), S. 729-744 
    ISSN: 1420-9136
    Keywords: Volcanic tremor ; intermittency ; chaos
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    Topics: Geosciences , Physics
    Notes: Abstract Harmonic tremor is widely studied and modelled in a very narrow frequency band (1–5 Hz) which represents the eigenfrequencies of a resonator assumed as the source of the phenomenon. Minimal effort was dedicated towards understanding its behaviour in larger temporal scales. Here we characterise the dynamic behaviour of volcanic tremor while evaluating the complete spectrum of the generalised dimension of the phase space. The starting time series constitutes the tremor amplitude picked every 10 minutes. The choice of this lag time is made on the basis of a qualitative analysis of the properties of the tremor. The results show intermittent behaviour of the dynamics which requires an 8-dimensional map to be completely described. An interesting result is that the maximum clustering of point density in phase space occurs in a monodimensional space which implies a periodicity sometimes observed experimentally. An appropriate predictive model needs more constraints on the nature of the eight variables involved in the process.
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    Journal of statistical physics 39 (1985), S. 477-491 
    ISSN: 1572-9613
    Keywords: Solar activity ; magnetic cycles ; dynamos ; chaos
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    Notes: Abstract Slowly rotating main-sequence stars with deep convective zones have activity cycles like the sun's. The solar cycle is aperiodic and modulated to give intervals of reduced activity. A simple sixth-order system, obtained by truncating the dynamo equations, has solutions that mimic this behavior. The transition to chaos is analyzed and the astrophysical significance of these results is discussed.
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    Journal of statistical physics 43 (1986), S. 479-488 
    ISSN: 1572-9613
    Keywords: Homoclinic orbit ; Heteroclinic orbit ; bifurcations ; chaos ; Lorenz equations
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    Notes: Abstract The local bifurcation structure of a heteroclinic bifurcation which has been observed in the Lorenz equations is analyzed. The existence of a particular heteroclinic loop at one point in a two-dimensional parameter space (a “T point”) implies the existence of a line of heteroclinic loops and a logarithmic spiral of homoclinic orbits, as well as countably many other topologically more complicatedT points in a small neighborhood in parameter space.
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    Journal of statistical physics 46 (1987), S. 789-794 
    ISSN: 1572-9613
    Keywords: Cellular automata ; Kauffman model ; chaos ; phase transition ; percolation
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    Notes: Abstract The phase transition between frozen and chaotic behavior in Kauffman's cellular automata on a nearest neighbor square lattice does not agree with the percolation threshold of the forcing functions.
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    Journal of statistical physics 53 (1988), S. 1299-1314 
    ISSN: 1572-9613
    Keywords: Lyapunov ; scaling ; chaos ; nonlinear dynamics ; billiard ; gravity ; random matrix
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    Notes: Abstract We consider the motion of a point particle (billiard) in a uniform gravitational field constrained to move in a symmetric wedge-shaped region. The billiard is reflected at the wedge boundary. The phase space of the system naturally divides itself into two regions in which the tangent maps are respectively parabolic and hyperbolic. It is known that the system is integrable for two values of the wedge half-angleθ 1 andθ 2 and chaotic forθ 1〈θ〈θ 2. We study the system at three levels of approximation: first, where the deterministic dynamics is replaced by a random evolution; second, where, in addition, the tangent map in each region is, replaced by its average; and third, where the tangent map is replaced by a single global average. We show that at all three levels the Lyapunov exponent exhibits power law behavior nearθ 1 andθ 2 with exponents 1/2 and 1, respectively. We indicate the origin of the exponent 1, which has not been observed in unaccelerated billiards.
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    Journal of statistical physics 54 (1989), S. 893-913 
    ISSN: 1572-9613
    Keywords: p-adic numbers ; dynamical systems ; chaos ; quasiperiodicity
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    Topics: Physics
    Notes: Abstract The quadratic map overp-adic numbers is studied in some detail. We prove that near almost all indifferent fixed points it is topologically conjugate to a quasiperiodic linear map. We also establish the existence of chaotic behavior and describe it using symbolic dynamics.
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    Journal of statistical physics 54 (1989), S. 925-948 
    ISSN: 1572-9613
    Keywords: Symmetry breaking ; chaos ; band splitting ; crisis ; piecewise linear map
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    Notes: Abstract A new type of crisis is shown to exist in a broad class of systems (including the Lorenz model) which leads to an anomalous band splitting or to a symmetry-breaking bifurcation of the strange attractor, depending on the actual values of the control parameters. A piecewise linear model is used to understand the mechanism of this crisis and to obtain exact results.
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    Journal of statistical physics 81 (1995), S. 761-775 
    ISSN: 1572-9613
    Keywords: Logistic map ; diffusion ; Fisher equation ; chaos ; oscillations
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    Notes: Abstract The dynamics of a biological population governed by a modified Fisher equation is studied by means of Monte Carlo simulations. Reproduction of the population occurs at discrete times, while transport caused by diffusion and conduction takes place on shorter time scales. The discrete reproduction, modeled with a set of coupled logistic maps, exhibits phenomena which are not evident in the usual continuum version of the Fisher equation. Several mechanisms for biennial oscillations of the total population are investigated. One of these shows an ordered coupling between random diffusive motion and the chaotic attractor of the logistic map.
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  • 39
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    Journal of statistical physics 88 (1997), S. 807-824 
    ISSN: 1572-9613
    Keywords: Billiards ; Kolmogorov–Sinai entropy ; Lyapunov exponents ; ergodic theory ; chaos ; numerical experiments
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    Notes: Abstract We perform new experiments on the Kolmogorov–Sinai entropy, Lyapunov exponents, and the mean free time in billiards. We study their dependence on the geometry of the scatterers made up of two interpenetrating square lattices, each one with circular scatterers with different radius. We find, in particular, that the above quantities are continuous functions of the ratio of the scatterer radius. However, it seems that their derivative is discontinuous around the radius ratio which separates the diffusive and nondiffusive types of geometries.
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    Journal of statistical physics 93 (1998), S. 833-842 
    ISSN: 1572-9613
    Keywords: Shell models ; turbulence ; chaos ; Lyapunov exponent ; conserved quantities ; shell maps
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    Notes: Abstract We study the chaotic behavior of the GOY shell model by measuring the variation of the maximal Lyapunov exponent with the parameter ε which determines the nature of the second invariant (the generalized “helicity” invariant). After a Hopf bifurcation, we observe a critical point at ε c ∼0.38704 above which the maximal Lyapunov exponent grows nearly linearly. For high values of ε the evolution becomes regular again, which can be explained by a simple analytic argument. A model with few shells shows two transitions. To simplify the model substantially we introduce a shell map which exhibits similar properties as the GOY model.
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    Journal of statistical physics 95 (1999), S. 867-902 
    ISSN: 1572-9613
    Keywords: kinetics of phase transitions ; domain coarsening ; asymptotic behavior ; self-similarity ; stability ; chaos
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    Notes: Abstract The classical Lifshitz–Slyozov–Wagner theory of domain coarsening predicts asymptotically self-similar behavior for the size distribution of a dilute system of particles that evolve by diffusional mass transfer with a common mean field. Here we consider the long-time behavior of measure-valued solutions for systems in which particle size is uniformly bounded, i.e., for initial measures of compact support. We prove that the long-time behavior of the size distribution depends sensitively on the initial distribution of the largest particles in the system. Convergence to the classically predicted smooth similarity solution is impossible if the initial distribution function is comparable to any finite power of distance to the end of the support. We give a necessary criterion for convergence to other self-similar solutions, and conditional stability theorems for some such solutions. For a dense set of initial data, convergence to any self-similar solution is impossible.
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    Journal of statistical physics 40 (1985), S. 371-395 
    ISSN: 1572-9613
    Keywords: Dynamical systems ; nonlinear dynamics ; chaos ; turbulence ; intermittent turbulence ; intermittency ; noise ; external noise ; fluctuations ; external fluctuations ; Ginzburg-Landau equation ; amplitude equation ; spatially growing waves ; convective instability ; spatial instability ; secondary instability ; noise-sustained structure ; noise amplification ; spatial noise amplification ; pattern formation
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    Notes: Abstract The time-dependent generalized Ginzburg-Landau equation is an equation that is related to many physical systems. Solutions of this equation in the presence of low-level external noise are studied. Numerical solutions of this equation in thestationary frame of reference and with anonzero group velocity that is greater than a critical velocity exhibit a selective spatial amplification of noise resulting in spatially growing waves. These waves in turn result in the formation of a dynamic structure. It is found that themicroscopic noise plays an important role in themacroscopic dynamics of the system. For certain parameter values the system exhibits intermittent turbulent behavior in which the random nature of the external noise plays a crucial role. A mechanism which may be responsible for the intermittent turbulence occurring in some fluid systems is suggested.
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    Journal of statistical physics 43 (1986), S. 369-390 
    ISSN: 1572-9613
    Keywords: Nonlinear dynamics ; circle map ; period doubling bifurcations ; chaos ; invariant measures ; average Lyapunov exponents ; path integrals
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    Topics: Physics
    Notes: Abstract The circle map provides a generic model for the response of damped, nonlinear oscillators to periodic perturbations. As the parameters are varied this dynamical system exhibits transitions from regular, ordered behavior to chaos. In this paper the regular and irregular behavior of the circle map are examined for a broad range of nonlinearities and frequencies which span not only the regular and transition regimes, which have been studied extensively, but also the strongly nonlinear, chaotic regime. We discuss the bistable behavior (split bifurcations) associated with maps with multiple extrema that gives rise to two disjoint attractors which can be periodic or chaotic and to the low order periodic orbits emerging from chaos via tangent bifurcations. To describe the chaotic behavior we use a statistical description based on a path integral formulation of classical dynamics. This path integral method provides a convenient means of calculating statistical properties of the nonlinear dynamics, such as the invariant measure of the average Lyapunov exponent, which in many cases reduce to analytic expressions or to numerical calculations which can be completed in a fraction of the time required to explicitly iterate the map.
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    Journal of statistical physics 48 (1987), S. 151-199 
    ISSN: 1572-9613
    Keywords: Homoclinic tangency ; bifurcation theory ; periodic attractors ; chaos ; hyperbolic repellor ; symbolic dynamics ; chemical thermokinetics ; cool flame-ignition oscillations
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    Notes: Abstract Nonlinear autonomous dynamical systems with ahomoclinic tangency to a periodic orbit are investigated. We study the bifurcation sequences of the mixed-mode oscillations generated by the homoclinicity, which are shown to belong to two different types, depending on the nature of the Liapunov numbers of the basic periodic orbit. A detailed numerical analysis is carried out to show how the existence of a tangent homoclinic orbit allows us to understand in a quantitative way a particular and regular sequence of cool flame-ignition oscillations observed in a thermokinetic model of hydrocarbon oxidation. Chaotic cool flame oscillations are also observed in the same model. When the control parameter crosses a critical value, this chaotic set of trajectories becomes globally unstable and forms a Cantor-like hyperbolic repellor, and the ignition mechanism generates ahomoclinic tangency to the Cantor set of trajectories. The complex bifurcation diagram may be globally reconstructed from a one-dimensional dynamical system, thanks to the strong contractivity of thermokinetics. It is found that a symbolic dynamics with three symbols is necessary to classify the periodic windows of the complex bifurcation sequence observed numerically in this system.
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    Journal of statistical physics 48 (1987), S. 959-975 
    ISSN: 1572-9613
    Keywords: Belousov-Zhabotinsky system ; chemical oscillations ; dissipative structures ; diffusion instabilities ; chaos
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    Notes: Abstract A mechanism and a model of a ferroin-catalyzed oscillating chemical system are descrined. This reaction presents an excellent example of a far-from-equilibrium system that forms spatial and temporal dissipative structures. The model shows that while the well-stirred system has a unique and stable stationary state, the same reagent spread in a thin layer may form complex spatiotemporal paterns. Stationary periodic patterns of both small and large amplitude, standing waves, and inhomogeneous chaotic oscillations are found in the model.
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    Journal of statistical physics 48 (1987), S. 977-990 
    ISSN: 1572-9613
    Keywords: Nonlinear dynamics ; chaos ; crisis ; Belousov-Zhabotinskii reaction
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    Notes: Abstract An abrupt transition that has the character of aninterior crisis was observed in an experiment on the Belousov-Zhabotinskii reaction as a control parameter was varied (a crisis is a qualitative change in the dynamics of a system observed when an attractor collides with the stable manifold of a fixed point). The interpretation of the observed behavior as a crisis is corroborated by a numerical analysis of a seven-variable model of the reaction. The waveforms, attractors, and maps obtained in the simulation are remarkably similar to those obtained in the laboratory experiment. The simulation indicates that the crisis is a consequence of a multivalued first return map.
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    Journal of statistical physics 48 (1987), S. 1269-1282 
    ISSN: 1572-9613
    Keywords: Mixmaster model ; ergodic theory ; chaos ; Einstein equations ; cosmological singularity ; Kaluza-Klein cosmology
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    Notes: Abstract The topological dynamics of the mixmaster models in space-time dimension d+1 are investigated. We use a new parametrization to reduce the mixmaster map to a translation combined with an appropriate isometry or a dilating inversion. For d⩽9, we show that the mixmaster map is ergodic and topologically mixing. For d⩾10, the mixmaster map reduces to the identity after a finite number of iterations, except for a set of initial data with zero Lebesgue measure.
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    Journal of statistical physics 49 (1987), S. 511-550 
    ISSN: 1572-9613
    Keywords: Ergodicity ; time-dependent Hamiltonian ; decay of correlations ; adiabatic invariant ; billiard ; chaos
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    Notes: Abstract For a “slowly” time-dependent Hamiltonian system exhibiting chaotic motion that ergodically covers the energy surface, the phase space volume enclosed inside this surface is an adiabatic invariant. In this paper we examine, both numerically and theoretically, how the error in this “ergodic adiabatic invariant” scales with the slowness of the time variation of the Hamiltonian. It is found that under certain circumstances, the error is diffusive and scales likeT −1/2, whereT is the characteristic time over which the Hamiltonian changes. On the other hand, for other cases (where motion in the Hamiltonian has a long-time 1/t tail in a certain correlation function), the error scales like [T −1 ln(T)]1/2. Both of these scalings are verified by numerical experiments. In the situation where invariant tori exist amid chaos, the motion may not be fully ergodic on the entire energy surface. The ergodic adiabatic invariant may still be useful in this case and the circumstances under which this is so are investigated numerically (in particular, the islands have to be small enough).
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    Journal of statistical physics 78 (1995), S. 1571-1589 
    ISSN: 1572-9613
    Keywords: Boltzmann ; ergodicity ; irreversibility ; Ruelle principle ; SRB measures ; chaos ; nonequilibrium
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    Notes: Abstract The contents of a not too well-known paper by Boltzmann are critically examined. The etymology of the word ergodic and its implications are discussed. A connection with the modern theory of Ruelle is attempted.
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    Journal of statistical physics 80 (1995), S. 481-485 
    ISSN: 1572-9613
    Keywords: Genericity ; chaos ; topological entropy
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    Notes: Abstract We prove the existence of an open and dense subset of mapsfεDiff ω ∞ (S2) which have positive topological entropy. It follows that these maps have infinitely many hyperbolic periodic points and an exponential growth rate of hyperbolic periodic points. The proof is an application of Pixton's theorem
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    Journal of statistical physics 82 (1996), S. 1099-1112 
    ISSN: 1572-9613
    Keywords: Ising model with long-range interactions ; Sierpiński-gasket lattice ; correlation functions ; chaos
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    Notes: Abstract A class of multispin correlation functions of an Ising model with ferromagnetic nearest neighbor interactionsK and constant (distance-independent) long-range interactionsQ 1=Q,l=1,2,..., on the Sierpiński-gasket lattice is considered. Using an exact method for calculating thermodynamic functions of hierarchically constructed Ising systems, it is shown that, for a set of values ofQ and for almost all values ofK, someM k-spin correlation functions, whereM k=3 k +3 withk=1,2,...,n andn=1,2,... being the order of lattice construction, change chaotically asn, k, and therebyM k increase to infinity. Accordingly, in the thermodynamic limit, these correlation functions prove to be nonanalytic for appropriate values ofQ andK. SinceM k-point correlation functions withk being finite, i.e., correlation functions involving finite numbers of spins, remain analytic asn tends to infinity, there is a smooth crossover between analytic properties of correlation functions of the two types.
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    Journal of statistical physics 85 (1996), S. 25-40 
    ISSN: 1572-9613
    Keywords: Glivenko-Cantelli theorem ; fractal ; almost sure convergence ; moment estimators ; least square estimators ; dynamical systems ; chaos
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    Notes: Abstract The Grassberger-Procaccia (GP) empirical spatial correlation integral, which plays an important role in dimension estimation, is the proportion of pairs of points in a segment of an orbit of lengthn, of a dynamical system defined on a metric space, which are no more than a distancer apart. It is used as an estimator of the GP spatial correlation integral, which is the probability that two points sampled independently from an invariant measure of the system are no more than a distancer apart. It has recently been proven, for the case of an ergodic dynamical system defined on a separable metric spaceythat the GP empirical correlation integral converges a.s. to the GP correlation integral at continuity points of the latter asn→∞. It is shown here that for ergodic systems defined on ℜd with the “max” metric the convergence is uniform inr. Further, a simplified proof based on weak convergence arguments of the result in separable spaces is given. Finally, the Glivenko-Cantelli theorem is used to obtain ergodic theorems for both the moment estimators and least square estimators of correlation dimension.
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    Journal of statistical physics 87 (1997), S. 1253-1271 
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    Keywords: Lorentz lattice gases ; chaos ; thermodynamic formalism ; random walks ; localization transition
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    Notes: Abstract The thermodynamic formalism expresses chaotic properties of dynamical systems in terms of the Ruelle pressure ψ(β). The inverse-temperature-like variable β allows one to scan the structure of the probability distributin in the dynamic phase space. This formalism is applied here to a lorentz lattice gas. where a particle moving on a lattice of sizeL d collides with fixed scatterers placed at random locations. Here we give rigorous arguments that the Ruelle pressure in the limit of infinite systems has two branches joining with a slope discontinuity at β=1. The low- and high-β branches correspond to localization of trajectories on respectively the “most chaotic” (highest density) region and the “most deterministic” (lowest density) region, i.e. ψ(β) is completely controlled by rare fluctuations in the distribution of scatterers on the lattice. and it dose not carry and information on the global structure of the static disorder. As β approaches unity from either side, a localization-delocalization transition leads to a state where trajectories are extended and carry information on transprot properties. At finiteL the narrow region around β=1 where the trajectories are extended scales as (InL)−2. where α depends on the sign of 1−β, ifd〉1, and as (L InL)−1 ifd=1. This result appears to be general for diffusive systems with static disorder, such as random walks in random environments or for the continuous Lorentz gas. Other models of random walks on disordered lattices, showing the same phenomenon, are discussed.
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    Journal of statistical physics 92 (1998), S. 909-972 
    ISSN: 1572-9613
    Keywords: Perturbation theory ; Hamiltonian dynamics ; wave–particle interaction: transport properties ; chaos ; plasma turbulence
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    Notes: Abstract The dynamics defined by the Hamiltonian $$H = p^2 /2 + A\sum\nolimits_{m = - M}^M {\cos (q - mt + \varphi m)}$$ , where the φ m are fixed random phases, is investigated for large values of A, and for $$M \gg A^{2/3}$$ . For a given P * and for $$\Delta \upsilon \geqslant A^{2/3}$$ , this Hamiltonian is transformed through a rigorous perturbative treatment into a Hamiltonian where the sum of all the nonresonant terms, having a Q dependence of the kind cos(kQ − nt + φ m) with $$|n/k - P^ * | 〉 \Delta \upsilon$$ , is a random variable whose r.m.s. with respect to the φ m is exponentially small in the parameter $$\varepsilon = A/\Delta \upsilon ^{3/2}$$ . Using this result, a rationale is provided showing that the statistical properties of the dynamics defined by H, and of the reduced dynamics including at each time t only the terms in H such that $$|m - p(t)| \leqslant \alpha A^{2/3}$$ , can be made arbitrarily close by increasing α. For practical purposes α close to 5 is enough, as confirmed numerically. The reduced dynamics being nondeterministic, it is thus analytically shown, without using the random-phase approximation, that the statistical properties of a chaotic Hamiltonian dynamics can be made arbitrarily close to that of a stochastic dynamics. An appropriate rescaling of momentum and time shows that the statistical properties of the dynamics defined by H can be considered as independent of A, on a finite time interval, for A large. The way these results could generalize to a wider class of Hamiltonians is indicated.
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    Il nuovo cimento della Società Italiana di Fisica 18 (1996), S. 765-770 
    ISSN: 0392-6737
    Keywords: Solitons ; chaos ; Solitons ; BGK modes
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    Notes: Summary A new dromion solution is obtained for a (2+1)-dimensional integrable model: the Davey-Stewartson equation. Some interesting questions which emerge in the procedure of getting the solution are also discussed.
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  • 56
    ISSN: 1349-9432
    Keywords: semiconductor laser ; optical feedback ; chaos ; relaxation oscillation ; coherence collapse
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    Notes: Abstract The dynamic characteristics of a semiconductor laser with optical feedback are strongly dependent on the injection current and the reflectivity and position of the external feedback reflector. We investigated the relaxation oscillation enhancement and coherence collapse state of the laser oscillation based on the laser rate equations. It is well known that laser output power jumps with increase of the injection current due to external mode transition. But here for the first we time demonstrate the existence of a chaotic scenario within successive laser power jumps. The results calculated by numerical simulations based on the rate equations are compared with those of the experiments and good coincidence between them is found.
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    Acta mechanica solida Sinica 10 (1997), S. 316-321 
    ISSN: 0894-9166
    Keywords: continuous dynamical system ; chaos ; parametric open-plus-closed-loop control ; the Lorenz model
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract This paper presents a parametric open-plus-closed-loop control approach to controlling chaos in continuous dynamical systems. As an example, chaos in the Lorenz model is controlled to demonstrate its application. Finally, the relations between the parametric open-plus-closed-loop control and the former control methods, such as the open-plus-closed-loop control and the parametric entrainment control, are discussed.
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    Acta mechanica solida Sinica 10 (1997), S. 262-275 
    ISSN: 0894-9166
    Keywords: global bifurcation ; chaos ; nonlinear vibration ; basin ; fractal
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract The global bifurcation and chaos are investigated in this paper for a van der Pol-Duffing-Mathieu system with a single-well potential oscillator by means of nonlinear dynamics. The autonomous system corresponding to the system under discussion is analytically studied to draw all global bifurcation diagrams in every parameter space. These diagrams are called basic bifurcation ones. Then fixing parameter in every space and taking the parametrically excited amplitude as a bifurcation parameter, we can observe how to evolve from a basic bifurcation diagram to a chaos pattern in terms of numerical methods. The results are sufficient to show that the system has distinct dynamic behavior. Finally, the properties of the basins of attraction are observed and the appearance of fractal basin boundaries heralding the onset of a loss of structural integrity is noted in order to consider how to control the extent and the rate of the erosion in the next paper.
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  • 59
    ISSN: 1090-6487
    Keywords: 23.40.−s ; 27.60.+j ; 27.40.+z
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    Notes: Abstract The lifetimes of a negative muon in the isotopes 132Xe and 40Ar in the solid phase are measured. The lifetime of μ − in the 1s state of the isotope 132Xe is τ(132Xe)=101.7±1.7 ns, which corresponds to a total nuclear capture rate Λc(132Xe)=9.4±0.2 μs−1. The lifetime of μ − in the isotope 40Ar, viz., τ (40Ar)=568±6 ns, corresponding to a capture rate Λc(40Ar)=1.31±0.01 μs−1, is obtained to several times better accuracy as compared to previously published results.
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    JETP letters 71 (2000), S. 4-7 
    ISSN: 1090-6487
    Keywords: 21.10.Gv ; 21.10.Re ; 21.60.Fw ; 23.20.Lv ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The quasiclassically exact solution for the second inertial parameter ℬ is found in a self-consistent way. It is shown that superdeformation and nonuniform pairing arising from the rotation-induced pair density significantly reduce this parameter. The new signature for the transition from pairing to normal phase is suggested in terms of the variation ℬ/A versus spin. Experimental data indicate the existence of such a transition in the three SD mass regions.
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  • 61
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    JETP letters 68 (1998), S. 1-6 
    ISSN: 1090-6487
    Keywords: 23.40.Bw ; 27.50.+e ; 27.60.+j
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    Topics: Physics
    Notes: Abstract A comparison is made of the probability of the process of two-neutrino double β decay for 82Se and 96Zr in direct (counter) and geochemical experiments. The experimental data for 130Te are analyzed. It is shown that this probability is systematically lower in geochemical experiments, which characterize the probability of 2 β(2 v) decay 109 yr ago. It is proposed that this could be due to a change in the weak-interaction constant with time. It is proposed that a series of new, precise measurements be performed with the aid of counters and geochemical experiments.
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  • 62
    ISSN: 1090-6487
    Keywords: 25.30.Mr ; 27.50.+e ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The lifetime of a negative muon in the 1S state in the isotopes 84Kr and 136Xe was measured. The values obtained, τ(84Kr)=139.2±2.9 ns and τ(136Xe)=111.0±4.6 ns, correspond to total nuclear capture rates Λc(84Kr)=6.75±0.15 μs−1 and Λ c(136Xe)=8.6±0.4 μs−1. Theoretical calculations of the rate of nuclear capture of a negative muon are performed for the Kr isotopes. The experimental results are compared with the theoretical calculations.
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  • 63
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    JETP letters 67 (1998), S. 453-458 
    ISSN: 1090-6487
    Keywords: 12.10.Dm ; 14.60.Lm ; 14.60.Pq ; 13.10+q ; 27.60.+j
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    Topics: Physics
    Notes: Abstract A discussion is given on the prospects for making a precise determination of the value of sin2θ W (θW is the Weinberg angle) and for improving the sensitivity of the search for the antineutrino magnetic moment to ≈1.5×10−11μB and for the $$\tilde v_e \leftrightarrow \tilde v_x $$ mixing parameter to sin22θ ≈10−2 by measuring in a single experiment the cross sections for $$\tilde v_e e$$ scattering for the reaction $$\tilde v_e p \to e^ + n$$ . Such an experiment with ∼100 000 events/yr detected for each reaction can be carried out, for example, using the BOREXINO detector and an approximately 10 MCi 90Sr source.
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  • 64
    ISSN: 1090-6487
    Keywords: 25.45.−z ; 27.60.+j ; 27.80.+w
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    Topics: Physics
    Notes: Abstract Yields of protons emitted in the D+D reaction in Pd, Au/Pd/PdO, Ti, and Au foils are measured by a d E-E counter telescope for bombarding energies between 2.5 and 10 keV. The experimental yields are compared with those predicted from a parametrization of the cross section and stopping power at higher energies. It is found that for Ti and Au target the enhancement of the D(d,p)T reaction is similar to that observed with a deuterium gas target (several tens of eV). The dependence of the yields on the bombarding energy corresponds well to the screening potential parameters U s=250±15 eV for Pd and 601 ±23 eV for Au/Pd/PdO. Possible models of the enhancement obtained are discussed.
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  • 65
    ISSN: 1090-6487
    Keywords: 23.40.−s ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The lifetime of negative muons in the 129Xe 1s state was measured. The muon capture rate in 129Xe is compared with that in the 132, 136Xe isotopes. The capture rate was found to depend on the mass number of the cited isotopes. The experimental results are compared with the results of calculations by the semiempirical Goulard-Primakoff formula.
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  • 66
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    European biophysics journal 17 (1989), S. 273-280 
    ISSN: 1432-1017
    Keywords: Ventricular cardiocytes ; nonlinear dynamics ; chaos ; devil's staircase
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    Topics: Biology , Physics
    Notes: Abstract We measured the non-linear dynamics of cardiac action potentials by varying the stimulation frequency from 2 to 20 Hz and obtained the following results: (i) When the fast Na+ current initiated the action potentials (‘fast action potentials’) periodicity was maintained, i.e. the pattern of action potentials repeated after a finite number of stimuli. Chaotic sequences were absent. The transition from one sequence to the next occurred as a devil's staircase. (ii) When, however, the slow Ca2+ current initiated the action potentials (‘slow action potentials’), we observed chaos, i.e. fully irregular behaviour, as well as bifurcations. (iii) Our results confirm the supposition that the global dynamics of cardiac cells can be well described by simple one-dimensional maps which predict these two kinds of behaviour.
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  • 67
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    Acta mechanica Sinica 12 (1996), S. 1-14 
    ISSN: 1614-3116
    Keywords: ellipticity ; hydrodynamic instabilities ; chaos ; phase transition
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract Ellipticity as the underlying mechanism for instabilities of physical systems is highlighted in the study of model nonlinear evolution equations with dissipation and the study of phase transition in Van der Waals fluid. Interesting results include spiky solutions, chaotic behavior in the context of partial differential equations, as well as the nucleation process due to ellipticity in phase transition.
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  • 68
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    Acta mechanica Sinica 11 (1995), S. 357-372 
    ISSN: 1614-3116
    Keywords: semi-analytical and semi-numerical method ; global bifurcations ; chaos ; van del Pol-Duffing-Mathieu system
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract Semi-analytical and semi-numerical method is used to investigate the global bifurcations and chaos in the nonlinear system of a Van der Pol-Duffing-Mathieu oscillator. Semi-analytical and semi-numerical method means that the autonomous system, called Van der Pol-Duffing system, is analytically studied to draw all global bifurcations diagrams in parameter space. These diagrams are called basic bifurcation diagrams. Then fixing parameter in every space and taking parametrically excited amplitude as a bifurcation parameter, we can observe the evolution from a basic bifurcation diagram to chaotic pattern by numerical methods.
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  • 69
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    Acta mechanica Sinica 13 (1997), S. 106-112 
    ISSN: 1614-3116
    Keywords: faraday experiment ; chaos ; resonant interaction
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract Free surface waves in a cylinder of liquid under vertical excitation with slowly modulated amplitude are investigated in the current paper. It is shown by both theoretical analysis and numerical simulation that chaos may occur even for a single mode with modulation which can be used to explain Gollub and Meyer's experiment. The implied resonant mechanism accounting for this phenomenon is further elucidated.
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  • 70
    ISSN: 1614-3116
    Keywords: thermal convection flow ; transition ; chaos ; electron beam fluorescence technique
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract Chaotic phenomena in the wake of thermal convection flow fields above a heating flat plate were investigated experimentally. A newly developed electron beam fluorescence technique (EBF) was used to simultaneously measure density fluctuation at 7 points in a cross section above the plate. Correlation dimensions, intermittence coefficients, Fourier spectrum have been obtained for different Grashof numbers. Spatial distribution of correlation dimensions are presented. The experimental result shows that there is a certain relationship between the density fluctuation and theGr number. And time-spacial characteristic of chaos evolution is also given.
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  • 71
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    Applied mathematics and mechanics 19 (1998), S. 625-635 
    ISSN: 1573-2754
    Keywords: shallow arch ; internal resonance ; steady state motion ; bifurcation ; chaos
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Mathematics , Physics
    Notes: Abstract The bifurcation dynamics of shallow arch which possesses initial deflection under periodic excitation for the case of 1∶2 internal resonance is studied in this paper. The whole parametric plane is divided into several different regions according to the types of motions; then the distribution of steady state motions of shallow arch on the plane of physical parameters is obtained. Combining with numerical method, the dynamics of the system in different regions, especially in the Hopf bifurcation region, is studied in detail. The rule of the mode interaction and the route to chaos of the system is also analysed at the end.
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  • 72
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    Applied mathematics and mechanics 20 (1999), S. 830-836 
    ISSN: 1573-2754
    Keywords: chaos ; Melnikov method ; Poincaré map ; phase portrait ; time-displacement diagram ; O343.5
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Mathematics , Physics
    Notes: Abstract In this paper, the system of the forced vibration $$\ddot T - \lambda _1 T + \lambda _2 T^2 + \lambda _3 T^3 = \varepsilon \left( {g\cos \omega t - \varepsilon '\dot T} \right)$$ is discussed, which contains square and cubic items. The critical condition that the system enters chaotic states is given by the Melnikov method. By Poincaré map, phase portrait and time-displacement history diagram, whether the chaos occurs is determined.
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  • 73
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    Studia geophysica et geodaetica 42 (1998), S. 335-342 
    ISSN: 1573-1626
    Keywords: fast dynamo ; rotating convection ; chaos ; MHD
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    Topics: Architecture, Civil Engineering, Surveying , Geosciences , Physics
    Notes: Abstract As a step towards a physically realistic model of a fast dynamo, we study numerically a kinematic dynamo driven by convection in a rapidly rotating cylindrical annulus. Convection maintains the quasi-geostrophic balance whilst developing more complicated time-dependence as the Rayleigh number is increased. We incorporate the effects of Ekman suction and investigate dynamo action resulting from a chaotic flow obtained in this manner. We examine the growth rate as a function of magnetic Prandtl number Pm, which is proportional to the magnetic Reynolds number. Even for the largest value of Pm considered, a clearly identifiable asymptotic behaviour is not established. Nevertheless the available evidence strongly suggests a fast dynamo process.
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  • 74
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    Applied mathematics and mechanics 19 (1998), S. 67-73 
    ISSN: 1573-2754
    Keywords: Reyleigh number ; Lorenz system ; chaos
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Mathematics , Physics
    Notes: Abstract Controlling chaos in the Lorenz system with a controllable Rayleigh number is investigated by the state space exact linearization method. Based on proving the exact linearizability, the nonlinear feedback is utilized to design the transformation changing the original chaotic system into a linear controllable one so that the control is realized. Numerical examples of control are presented.
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  • 75
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    Applied mathematics and mechanics 21 (2000), S. 1008-1015 
    ISSN: 1573-2754
    Keywords: subharmonic bifurcation ; heteroclinic orbit ; chaos ; Melnikov function ; O34
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Mathematics , Physics
    Notes: Abstract The dynamics behaviour of tension bar with periodic tension velocity was presented. Melnikov method was used to study the dynamic system. The results show that material nonlinear may result in anomalous dynamics response. The subharmonic bifurcation and chaos may occur in the determined system when the tension velocity exceeds the critical value.
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  • 76
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    Applied mathematics and mechanics 20 (1999), S. 360-364 
    ISSN: 1573-2754
    Keywords: buckled plate ; chaos ; Poincaré section
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    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Mathematics , Physics
    Notes: Abstract The primary aim of this paper is to study the chaotic motion of a large deflection plate. Considered here is a buckled plate, which is simply supported and subjected to a lateral harmonic excitation. At first, the partial differential equation governing the transverse vibration of the plate is derived. Then, by means of the Galerkin approach, the partial differential equation is simplified into a set of two ordinary differential equations. It is proved that the double mode model is identical with the single mode model. The Melnikov method is used to give the approximate excitation thresholds for the occurrence of the chaotic vibration. Finally numerical computation is carried out.
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  • 77
    ISSN: 1573-6873
    Keywords: electroreceptor ; catfish ; chaos ; unstable orbit ; periodic orbit ; sensory oscillator ; noise ; random process
    Source: Springer Online Journal Archives 1860-2000
    Topics: Computer Science , Medicine , Physics
    Notes: Abstract We report the results of a search for evidence of periodic unstableorbits in the electroreceptors of the catfish. The function of thesereceptor organs is to sense weak external electric fields. Inaddition, they respond to the ambient temperature and to the ioniccomposition of the water. These quantities are encoded by receptorsthat make use of an internal oscillator operating at the level of themembrane potential. If such oscillators have three or more degreesof freedom, and at least one of which also exhibits a nonlinearity,they are potentially capable of chaotic dynamics. By detecting theexistence of stable and unstable periodic orbits, we demonstratebifurcations between noisy stable and chaotic behavior using theambient temperature as a parameter. We suggest that the techniquedeveloped herein be regarded as an additional tool for the analysisof data in sensory biology and thus can be potentially useful instudies of functional responses to external stimuli. We speculatethat the appearance of unstable orbits may be indicative of a stateof heightened sensory awareness by the animal.
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    Journal of seismology 2 (1998), S. 159-171 
    ISSN: 1573-157X
    Keywords: chaos ; dynamical systems ; Hurst exponent ; stochasticprocess ; time series
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    Topics: Geosciences , Physics
    Notes: Abstract A procedure is presented for the analysis of complex stationary time series for which the Fourier power spectra reveals broadband noise or broadened pulses. We first determine the Hurst exponent from which we may know whether the time series under study is mainly random or if the data points present correlations. If the data are correlated, a chaotic analysis will reveal whether they may be interpreted as a low dimensional nonlinear system (defined by a low correlation dimension and a finite and positive Kolmogorov entropy and largest positive Lyapunov exponent) or as a stochastic process. We have studied three kind of temporal series: inter-event time series of infrasonic pulses recorded at Stromboli volcano, and, S-coda waves and microseisms, that have been recorded at the eastern Pyrenees. Results show that microseisms and Coda waves can be modeled as a low dimensional deterministic system, Correlation dimensions 2.3, 3.2, respectively. At the contrary infrasonic has resulted stochastic. This chaotic character can be attributed to the medium properties. Coda waves with scattering through a fractal distribution of scatters or to multiple reflection inside resonators (for example sedimentary basins) and microseisms as a propagation of wave guide of variable cross section which have the same temporal characteristics as a nonlinear forced oscillator.
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    Journal of seismology 3 (1999), S. 393-408 
    ISSN: 1573-157X
    Keywords: cepstrum ; chaos ; correlation dimension ; nonlinear oscillators
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    Topics: Geosciences , Physics
    Notes: Abstract The discussion about the source of low frequency events generally wrecorded on active volcanoes is still open and needs deeper understanding of the phenomena involved in their generation. Most of the models view such a phenomenon as a source effect (oscillation of volcanic fluids in conduits or cracks), although a different explanation as a path or site effect exists. In the present paper we analysed 26 seismic signals recorded at Vulcano and 60 at Stromboli in order to put some constraints on the functional shape of the recorded signals. They evidence all the characteristics of the low frequency events. The spectral analysis reveals sharp peaks in the range 0.5–4 Hz, while the cepstra suggest that the signals are composed by a two-sine kind function. This suggestion is confirmed by the two-dimensional projections of the reconstructed phase space. The correlation dimension of the attractor is very close to 3 for both the volcanoes confirming the existence of a toroidal structure in the phase space. This implies that we can suggest as a model for the low frequency events source a physical mechanism very similar to a Duffing oscillator or any other quasiperiodic one. In particular in the cases of the analysed volcanoes we recognise two independent oscillations.
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  • 80
    ISSN: 1435-1528
    Keywords: Periodically forced spheroids ; chaos ; particle separation
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    Topics: Chemistry and Pharmacology , Physics
    Notes: Abstract In this paper, we consider the technologically important problem of periodically forced spheroids in simple shear flow and demonstrate the existence of chaotic parametric regimes. The approach used by Strand (1989) (for the Strong Brownian limit) is inappropriate in the chaotic regimes corresponding to the weak Brownian limit. Our results also indicate a strong dependence of the solutions obtained on the aspect ratio of the spheroids. This strong dependence on the aspect ratio may be utilized to separate particles from a suspension of particles having different shapes but similar sizes.
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    The European physical journal 326 (1987), S. 107-119 
    ISSN: 1434-601X
    Keywords: 23.90.+w ; 27.60.+j
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    Topics: Physics
    Notes: Abstract Proton radioactivities with decay energies of (0.98±0.08) MeV and (0.83±0.08) MeV were produced by the fusion reactions58Ni+58Ni→116Ba ⋆ and58Ni+54Fe→112Xe ⋆, and their halflives were measured to be (33±7) μs and (109±17) μs, respectively. The intensities of the lines correspond to production cross sections of about 30 μb and 40 μb. The two activities are assigned to the direct proton decay of113Cs and109I. The measured halflives are compared with values calculated ford 5/2 andg 7/2 groundstates of109I and113Cs and spectroscopic factors are deduced for the decays. An extensive search for the proton decay of105Sb, produced in the reaction50Cr(58Ni,p2 n)105Sb, had a negative result, excluding decay energies between 0.5 MeV and 1.5 MeV for halflives between 10 ns and 5 s.
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  • 82
    ISSN: 1434-601X
    Keywords: 35.10.Di ; 21.10.Ft ; 21.10.Ky ; 27.60.+j
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    Topics: Physics
    Notes: Abstract With high resolution collinear fast beam laser spectroscopy in the 451 nm-line of Indium nuclear moments and the change in the mean square radii of the nuclear charge distribution of105,106 In have been determined.
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  • 83
    ISSN: 1434-601X
    Keywords: 21.10.Dr ; 21.60.Cs ; 27.60.+j
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    Notes: Abstract Using a148Gd radioactive target and the (p,d), (d,t), and (3He,α) single neutron pick-up reactions we have measured the147Gd mass excess as — 75,366(4) keV, which differs by 139(24) keV from the adopted value of the 1983 mass table. From this result, and from recently reported first transfer-reaction mass determinations for145Eu and146Eu, we have recalculated the masses of nuclei above146Gd from a previous shell model analysis of high-spin states.
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  • 84
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    Keywords: 35.10.Di ; 21.10.Ft ; 21.10.Ky ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The hyperfine structure splittings (hfs) and isotope shifts (IS) in the atomic transitions 5s 2 5p 2 1 S 0 → 5s 2 5p6s 1,3 P 1 have been measured for the radioactive isotopes108−111Sn and all stable ones. The tin isotopes were prepared as fast atomic beams for collinear laser spectroscopy at the GSI online mass separator following a fusion reaction. Nuclear spins, magnetic dipole, electric quadrupole moments and changes in mean square charge radii have been determined. In109Sn the spinI=5/2 was measured for the nuclear ground state (T 1/2=18 min) in contradiction to the literature value. The mean square charge radii show a parabolic behaviour with a maximum at N=66. This is interpreted by collective effects, which are considerably stronger than accounted for by theB(E2)-values.
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  • 85
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    Keywords: 23.40.Hc ; 21.10.Dr ; 21.10.Pc ; 27.60.+j ; 29.30.Kv
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    Topics: Physics
    Notes: Abstract With the use of the58Ni+50Cr fusion-evaporation reaction and chemically selective on-line mass separation, the EC/β + decay of104Sn was studied byγ-ray and conversionelectron spectroscopy. In the course of these studies, a new 15.7-s isomeric state of104In was observed. Reinvestigation of theβ-decays of the two heavier even isotopes of tin, produced in the58Ni+58Ni reaction and mass separated without chemical discrimination, brought new information on the decay of106Sn and108Sn. The QEC values of104Sn,106Sn and108Sn were determined to be 4550 −250 +300 keV, 3200±100 keV and 〈 2270 keV, respectively. In the data analysis, the emphasis is put on the identification of the 0+ → 1+ Gamow-Tellerβ transitions and determination of their strengths. For104−110Sn, the total Gamow-Teller strengths are measured to be 20% to 30% of that predicted by the single-particle shell model with the inclusion of pairing correlations and core polarization. Predictions of the decay properties of the as yet unobserved102Sn and100Sn are made.
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    The European physical journal 330 (1988), S. 221-222 
    ISSN: 1434-601X
    Keywords: 21.10.Re ; 23.20.Lv ; 27.60.+j
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    Topics: Physics
    Notes: Abstract High spin states of126Xe have been populated by means of the116Cd(13C, 3n) reaction using the OSIRIS-12 detector system. A level scheme consisting of 13 bands has been established. More than 40 new levels were observed and several spin and parity assignments could be made. Experimental Routhians and alignments of selected bands are presented.
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    The European physical journal 330 (1988), S. 365-369 
    ISSN: 1434-601X
    Keywords: 21.60.Fw ; 23.20.Lv ; 27.60.+j
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    Topics: Physics
    Notes: Abstract Unique-parity states of97Y are studied in the framework of the interacting boson-fermion model (IBFM). Spin assignments for the levels of the unique-parity yrast band are proposed on the basis of nuclear systematics and the IBFM band pattern associated with coupling of a particle-type quasiparticle (g9/2) to the SU(5) core38 96Sr58. The good fit of the experimental data with the IBFM calculations confirms the single particle character of this immediate neighbour of the doubly sub-magic nucleus96Zr.
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    The European physical journal 331 (1988), S. 21-27 
    ISSN: 1434-601X
    Keywords: 29.30.Fq ; 27.60.+j ; 35.10.Bg
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    Topics: Physics
    Notes: Abstract The β+ spectra of neutron-deficient nuclei with mass numbers 103 and 104 have been measured, using a semiconductor beta spectrometer. The nuclei were produced by on-line mass separation of reaction products formed by bombarding an enriched Mo target with Ne ions. Values for QEC have been deduced. The decay energies are in agreement with systematics. The decay of104In shows remarkably strong feeding to levels above 5 MeV. In addition, QEC values for103Cd,103Ag,104Ag and104mAg have been determined.
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    The European physical journal 332 (1989), S. 103-104 
    ISSN: 1434-601X
    Keywords: 21.10.−k ; 27.60.+j ; 23.20.Ck
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    Topics: Physics
    Notes: Abstract The ratio of the B(E2) values for the 0 1 + → 2 1 + transitions in138Ce and142Ce was measured by Coulomb excitation with α-particles. From the known value of the transition probability in142Ce it results: B(E2,138Ce, 0 1 + → 2 1 + =0.45 +/−0.03 e2 b 2
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    The European physical journal 322 (1985), S. 331-332 
    ISSN: 1434-601X
    Keywords: 23.40.−S ; 23.20.−g ; 27.60.+j
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    Topics: Physics
    Notes: Abstract The beta decay of the 2+ 92m Nb was reinvestigated via93Nb(γ, n) reaction. The feeding of the 2+ 2,067 keV level of92Zr was determined measuring the intensity of the 1,132 keV gamma-ray transition.
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    The European physical journal 332 (1989), S. 275-284 
    ISSN: 1434-601X
    Keywords: 23.40.Hc ; 21.10.Dr ; 27.60.+j ; 29.30.Kv
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Neutron-deficient isotopes of cadmium were produced in thep(600 MeV)+natSn spallation reaction. The ISOLDE facility provided mass-separated beams of these isotopes. The production yield was 103 to 104 atoms/s for100Cd and roughly two orders of magnitude less for98Cd. The properties of the100Cd→100Ag decay were studied in detail by X-ray,γ-ray and conversion electron spectroscopy. Forty nineγ-transitions were assigned to this decay, and all but five of them were placed in the decay scheme. The half-life was determined to be 49.1±0.5 s. TheQ EC value of 3890±70 keV was deduced from a comparison of experimental and theoreticalβ +/(EC+β + probability ratios. Seven 0+→1+ Gamow-Teller transitions with log ft values between 3.5 and 4.9 were identified. The total (summed) strength is about five times smaller than predicted by the shell model for the transformation of ag 9/2 proton into ag 7/2 neutron. The quenching of the Gamow-Teller strength and other questions of nuclear structure are discussed for the100Cd decay. The properties of98Cd are inferred by extrapolation of104,102,100Cd data, and some preliminary experimental results on98Cd decay are presented.
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  • 92
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    The European physical journal 333 (1989), S. 1-4 
    ISSN: 1434-601X
    Keywords: 21.10.Pc ; 21.60.Fw ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The structure of the low-lying states with negative parity of 37 93 Rb56 has been studied in the framework of the Interacting Boson-Fermion Model (IBFM) using the even-even neighbour 38 94 Sr56 as a core. A good description of the properties of the levels has been obtained. A sensitive test of the quality of the theoretical studies is the decay pattern of the second excited state at 267 keV with a half-life of 2.0(2) ns. The calculations givet 1/2=2.26 ns and they predict the existence of a 13 keV transition into the first excited state, the existence of which has been confirmed afterwards by experiments.
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  • 93
    ISSN: 1434-601X
    Keywords: 23.40.Hc ; 21.60.Cs ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Two-particle excitations in the two-proton nucleus148Dy populated inβ-decay of 10-s 148Ho(6−) were investigated throughγ-ray measurements following on-line mass separation. Theπh 11/2s1/2 two-proton doublet and the (vh 9/2 s 1 2/−1 )5− neutron particle hole configuration are firmly identified, and theπh 11/2 d 5 2/−1 and πh11/2D3/2 multiplets are also observed. The results suggest dominantπh 11/2vs 1 2/−1 character for the148Ho 6−-isomer.
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  • 94
    ISSN: 1434-601X
    Keywords: 21.10-k ; 23.20-Lv ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Residual activities produced via35Cl or32S beams in thin112Sn and106Cd targets have been studied by γ-ray and X-ray spectroscopy techniques behind a He-jet system. Mass identification of the products has been performed by coupling the He-jet to the medium current ion source of an isotope separator. Neutron-deficient nuclei with 137≦A≦144 have been identified. Decay schemes of several new isotopes as138Eu (12s),141Gd (22s),143Tb (12s and 〈17s),144Dy (9s) and possibly140Gd (11s) have been derived. New informations have also been provided for137Sm (45s),139Eu (24s) and144Tb (5s). Data have been presented through systematics. The shapes of these nuclei and their trends versusN andZ have been analysed.
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  • 95
    ISSN: 1434-601X
    Keywords: 21.10.Ft ; 21.10.Ky ; 27.50. +e ; 27.60.+j ; 35.10.Fk ; 35.80. +s ; 25.55.−e
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The isotope shifts and hyperfine splittings for 11 strontium isotopes (A=80–90) and two isomers for the optical transition λ=293.2 nm were measured. The magnetic dipole and electric quadrupole moments and the changes of the mean square charge radii are derived. The results are discussed with respect to the increasing nuclear deformation and the anomalous coupling scheme of light Sr nuclei.
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  • 96
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    The European physical journal 327 (1987), S. 119-126 
    ISSN: 1434-601X
    Keywords: 25.85.Ec ; 23.20.En ; 23.20.Gq ; 23.20.Lv ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Theβ − decay of the longer-lived isomer in100Nb has been studied at the fission-product separator JOSEF. Measurements ofγ-ray singles spectra, ofγ-γ coincidences and ofγ-γ angular correlations have been performed. A value oft 1/2=2.99(11)s has been determined for the isomer which probably hasI π=4+ or 5+. A scheme of the levels of100Mo which are populated in the decay of this isomer has been established. Information on the spins of several states of100Mo has been obtained. Thus,I=0 levels have been identified at 1,505, 2,038 and 2,087 keV. The mixing ratios have been determined for the 22 +→21 + and 23 +→21 + transitions. The results provide evidence for a vibrational structure of100Mo with separate bands based on the ground state and on the first excited 0+ level.
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  • 97
    ISSN: 1434-601X
    Keywords: 23.40.Hc ; 21.10.Dr ; 21.10.Pc ; 27.60.+j ; 29.30.Kv
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Neutron-rich isotopes of palladium were produced via the fission of238U by 20 MeV protons. These isotopes were selected using the ion guide-fed on-line mass-separator facility IGISOL at Jyväskylä. Their decays were studied byβ-ray,γ-ray and conversion-electron spectroscopy. For114Pd and116Pd, the decay schemes established previously were confirmed; additionally multipolarities were determined for a few transitions. In the case of118Pd, only an approximate half-life was known from a previous radiochemical experiment. In the present study, 15 gamma transitions were observed, most of which were placed in a decay scheme. The half-life and the decay energy were found to beT 1/2=1.9±0.1 s andQ β=4.0±0.2 MeV. The decay schemes of114Pd,116Pd and118Pd include — respectively — two, two and four 0+→1+ Gamow-Teller beta transitions with logft values between 4.1 and 5.1. The strength of these transitions is discussed in terms of the extreme single particle shell model with pairing and the spherical proton-neutron quasiparticle random phase approximation. The possible role of deformation is considered using a shell correction method. Predictions for the decay properties of the as yet unobserved120Pd are given.
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  • 98
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    The European physical journal 334 (1989), S. 163-175 
    ISSN: 1434-601X
    Keywords: 23.20.CK ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A new and transparent method for the analysis of recoil distance Doppler shift data is presented, which we call thedifferentialdecay curve method (DDCM). The DDCM can be used for singles as well as for coincidence plunger data and systematic errors can be discovered with it much easier than in the conventional analysis. In addition we propose a modification of the normal plunger which we call the differential plunger. With the differential plunger in principle it is possible to determine lifetimes from quantities measured at only one target to stopper distance. The DDCM was tested with lifetime data for120Xe and128Ba.
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  • 99
    ISSN: 1434-601X
    Keywords: 21.10. Jx ; 25.70. De ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The (14C,16O) reaction on Cd isotopes has been investigated at an energy of 60 MeV. Relative spectroscopic strengths to the ground states are found to decrease nearN=60.
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  • 100
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    The European physical journal 323 (1986), S. 179-184 
    ISSN: 1434-601X
    Keywords: 21.60.Cs, Ev, Fw ; 25.55.Fm ; 27.60.+j
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The available experimental data on the (3He,n) reaction between the ground states of even-even nuclei and lowest 1/2− levels of odd-A nuclei in theA ≈ 100 region are analyzed in a systematic way by the DWBA. The deduced relative intensities of these two-proton transfers, and their uncertainties, are compared to the predictions of various nuclear models. In particular, the influence of the finite dimension of the configuration space available to the transferred protons, and of the blocking effect of a 2p 1/2− proton, are examined.
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