Analysis of parahydrogen polarized spin system in low magnetic fields

2014 ◽  
Vol 16 (29) ◽  
pp. 15411-15421 ◽  
Author(s):  
P. Türschmann ◽  
J. Colell ◽  
T. Theis ◽  
B. Blümich ◽  
S. Appelt

Parahydrogen polarized spin systems allow for structure determination even in low magnetic fields of a few millitesla and enable efficient polarization transfer to rare heteronuclei.

1991 ◽  
Vol 05 (29) ◽  
pp. 1919-1924 ◽  
Author(s):  
M.J. TAHMASEBI ◽  
Y. SOBOUTI

A spin system in a time variable magnetic field is considered. For certain fields there exists a frame in which the Hamiltonian becomes static. The criterion for such fields is derived. The unitary transformation that accomplishes this task is obtained and the underlying Schrodinger equation is solved exactly.


2021 ◽  
Vol 185 (2) ◽  
Author(s):  
Shuai Shao ◽  
Yuxin Sun

AbstractWe study the connection between the correlation decay property (more precisely, strong spatial mixing) and the zero-freeness of the partition function of 2-spin systems on graphs of bounded degree. We show that for 2-spin systems on an entire family of graphs of a given bounded degree, the contraction property that ensures correlation decay exists for certain real parameters implies the zero-freeness of the partition function and the existence of correlation decay for some corresponding complex neighborhoods. Based on this connection, we are able to extend any real parameter of which the 2-spin system on graphs of bounded degree exhibits correlation decay to its complex neighborhood where the partition function is zero-free and correlation decay still exists. We give new zero-free regions in which the edge interaction parameters and the uniform external field are all complex-valued, and we show the existence of correlation decay for such complex regions. As a consequence, we obtain approximation algorithms for computing the partition function of 2-spin systems on graphs of bounded degree for these complex parameter settings.


2020 ◽  
Vol 34 (13) ◽  
pp. 2050129
Author(s):  
Erhan Albayrak

The A, B and C atoms with spin-1/2, spin-3/2 and spin-5/2 are joined together sequentially on the Bethe lattice in the form of ABCABC[Formula: see text] to simulate a molecule as a triple mixed-spin system. The spins are assumed to be interacting with only their nearest-neighbors via bilinear exchange interaction parameter in addition to crystal and external magnetic fields. The order-parameters are obtained in terms of exact recursion relations, then from the study of their thermal variations, the phase diagrams are calculated on the possible planes of our system. It is found that the model gives only second-order phase transitions in addition to the compensation temperatures.


2006 ◽  
Vol 51 ◽  
pp. 557-560 ◽  
Author(s):  
H Mitamura ◽  
S Mitsuda ◽  
S Kanetsuki ◽  
H A Katori ◽  
T Sakakibara ◽  
...  

2002 ◽  
Vol 16 (20n22) ◽  
pp. 3369-3372
Author(s):  
B. WOLF ◽  
S. ZHERLITSYN ◽  
S. SCHMIDT ◽  
B. LÜTHI ◽  
M. LANG

Low-dimensional spin systems reveal new and unexpected physical phenomena such as distinct plateaus in the magnetization as a function of magnetic field. In this paper we present ultrasonic measurements for the quasi-two-dimensional spin system SrCu2(BO3)2 in magnetic fields up to 50 T. From this technique we obtained detailed information about the spin state, the magnetic excitations and their interaction with phonons. The dimerized quantum-spin system SrCu2(BO3)2 exhibits plateaus in the magnetization and shows surprisingly strong magneto-elastic effects as a function of temperature and magnetic field. The pronounced elastic anomalies indicate a resonant interaction between the sound wave and the magnetic excitations.


2006 ◽  
Vol 181 (1) ◽  
pp. 126-134 ◽  
Author(s):  
Jorge L. Neves ◽  
Björn Heitmann ◽  
Timo O. Reiss ◽  
Heloiza H.R. Schor ◽  
Navin Khaneja ◽  
...  

2011 ◽  
Vol T143 ◽  
pp. 014005 ◽  
Author(s):  
Yu V Bezvershenko ◽  
P I Holod ◽  
A Messina

2017 ◽  
Vol 14 (10) ◽  
pp. 1750136 ◽  
Author(s):  
Akbota Myrzakul ◽  
Ratbay Myrzakulov

In this paper, we study integrable multilayer spin systems, namely, the multilayer M-LIII equation. We investigate their relation with the geometric flows of interacting curves and surfaces in some space [Formula: see text]. Then we present their Lakshmanan equivalent counterparts. We show that these equivalent counterparts are, in fact, the vector nonlinear Schrödinger equation (NLSE). It is well known that the vector NLSE is equivalent to the [Formula: see text]-spin system. Also, we have presented the transformations which give the relation between solutions of the [Formula: see text]-spin system and the multilayer M-LIII equation. It is interesting to note that the integrable multilayer M-LIII equation contains constant magnetic field [Formula: see text]. It seems that this constant magnetic vector plays an important role in the theory of “integrable multilayer spin system” and in nonlinear dynamics of magnetic systems. Finally, we present some classes of integrable models of interacting vortices.


1987 ◽  
Vol 151 (Part_1_2) ◽  
pp. 25-33 ◽  
Author(s):  
Thomas C. Farrar ◽  
Rafael A. Quintero-Arcaya ◽  
Ilene C. Locker

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