The quasi-magnetic-hysteresis behavior of polydisperse ferrofluids with small coupling constant

2012 ◽  
Vol 407 (24) ◽  
pp. 4638-4642 ◽  
Author(s):  
Jian Li ◽  
Yueqiang Lin ◽  
Xiaodong Liu ◽  
Lihua Lin ◽  
Qingmei Zhang ◽  
...  

2002 ◽  
Vol 12 (9) ◽  
pp. 355-355
Author(s):  
J. L. Musfeldt ◽  
A. B. Sushkov ◽  
J. Jegoudez ◽  
A. Revcolevschi ◽  
P. Millet ◽  
...  

Optical spectroscopy is a sensitive probe of charge, spin, and lattice degrees of freedom. In this talk, I will detail our magneto-optical work on alpha'-NaV2O5, a prototypical ladder material, as well as the new Na2V3O7 nanotubes. Using changes in electronic structure with temperature and applied magnetic field, we have mapped out the H-T phase diagram of alpha'-NaV2O5. We find a temperature independent phase boundary at 27 T which persists above Tc (34 K), a kink in Tc(H) near 27 T, and H$\wedge $2 behavior of Tc(H) in the high field phase with an unusually small coupling constant. The energy scale of Tc and the newly discovered phase boundary at Hc (27 T) are identical. Confinement effects are investigated in the related nanotubes. Results include a larger gap than in analogous bulk materials as well as a low-energy rattling mode, which corresponds to the motion of Na+ ions inside the nanotube.



2009 ◽  
Vol 2009 ◽  
pp. 1-52 ◽  
Author(s):  
J.-M. Barbaroux ◽  
J.-C. Guillot

We consider a Hamiltonian with cutoffs describing the weak decay of spin 1 massive bosons into the full family of leptons. The Hamiltonian is a self-adjoint operator in an appropriate Fock space with a unique ground state. We prove a Mourre estimate and a limiting absorption principle above the ground state energy and below the first threshold for a sufficiently small coupling constant. As a corollary, we prove the absence of eigenvalues and absolute continuity of the energy spectrum in the same spectral interval.



2017 ◽  
Vol 32 (37) ◽  
pp. 1750198 ◽  
Author(s):  
A. V. Kovtun ◽  
E. Ya. Nugaev

We discuss stability of Q-balls interacting with fermions in theory with small coupling constant [Formula: see text]. We argue that for configurations with large global U(1)-charge [Formula: see text], the problem of classical stability becomes more subtle. For example, in model with flat direction there is maximal value of charge for stable solutions with [Formula: see text]. This result may be crucial for the self-consistent consideration of Q-ball evaporation into the fermions. We study the origin of additional instability and discuss possible ways to avoid it.



1992 ◽  
Vol 47 (12) ◽  
pp. 1681-1686 ◽  
Author(s):  
Peter Baran ◽  
Arnd Böttcher ◽  
Horst Elias ◽  
Wolfgang Haase ◽  
Martina Hüber ◽  
...  

The reaction of the tetrahydrosalen ligand H2L = N,N′-bis(2-hydroxy-3-t-butyl-5-methylbenzyl)- 1,2-diaminoethane with iron(III) chloride in the presence of sodium methoxide affords a neutral complex of the composition [FeL(OMe)]. Single crystal X-ray analysis of this complex shows dinuclear units, [FeL(OMe)]2 = 1, with two methoxide bridges. Complex 1 crystallizes in the monoclinic space group C 2/c with a = 31.67(1)Å, b = 12.544(4)Å, c = 14.135(5)Å and β = 101.33(1)°. The two edge-sharing FeO4N2-octahedra are distorted and connected by a center of inversion. The iron(III) centers are separated by 3.203 Å and weakly antiferromagnetically coupled (J = —5.7 cm-1), which follows from temperature-dependent magnetic susceptibility measurements in the range 4.2 to 280 K. The effective magnetic moment per iron(III) is µeff = 5.24 μΒ at 280 K. The observed small coupling constant J fits well into the magnetostructural relationship suggested recently by Gorun and Lippard (Inorg. Chem. 30,1625 (1991)).



1998 ◽  
Vol 13 (31) ◽  
pp. 2481-2493 ◽  
Author(s):  
I. YA. AREF'EVA ◽  
A. S. KOSHELEV ◽  
P. B. MEDVEDEV

Classical dynamics in SU(2) matrix theory is investigated. A classical chaos–order transition is found. For small enough angular momentum (even for small coupling constant), the system exhibits a chaotic behavior, for large enough angular momentum, the system is regular.



Author(s):  
Fumio Hiroshima ◽  
Susumu Osawa

The asymptotic behavior of the effective mass meff(Λ) of the so-called Nelson model in quantum field theory is considered, where Λ is an ultraviolet cutoff parameter of the model. Let m be the bare mass of the model. It is shown that for sufficiently small coupling constant α of the model, meff(Λ)/m can be expanded as meff(Λ)/m=1+∑n=1∞an(Λ)α2n. A physical folklore is that an(Λ)=O(logΛ(n-1)) as Λ→∞. It is rigorously shown that 0<limΛ→∞a1(Λ)<C,  C1≤limΛ→∞a2(Λ)/log⁡Λ≤C2 with some constants C, C1, and C2.





1990 ◽  
Vol 45 (3) ◽  
pp. 290-298 ◽  
Author(s):  
Jürgen Allwohn ◽  
Ralf Hunold ◽  
Monika Pilz ◽  
Rolf-Günter Müller ◽  
Werner Massa ◽  
...  

Strong C—Sn hyperconjugation in C-stannylmethyleneborane 3 is indicated by (1) a small B—sp2C—Sn bond angle (105.6°), (2) a long sp2C—Sn bond (216 pm), (3) a very short B=C double bond (131 pm), (4) a very small coupling constant 1J(119Sn-13C) = 125 Hz for the sp2C—Sn bond and (5) shielding of the boron atom of the B=C double bond by 20 ppm as compared to methyleneboranes without strong hyperconjugation. The boron atoms of the B=C double bond of 3 and related methyleneboranes act as π-donor and σ-acceptor, the substituents X at the carbon atom of the B=C double bond as π-acceptors and, through their C—X σ-bonds, as σ-donors. The partly bridged methyleneborane 3 closes the gap between unbridged and bridged methyleneboranes. Relationships to non-classical carbocations are pointed out.



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