2 A ug 1 99 9 Breakdown of the magnetization plateau of the S = 1 / 2 ferromagnetic - ferromagnetic - antiferromagnetic trimerized spin chain with anisotropy

نویسنده

  • Kiyomi Okamoto
چکیده

We study the breakdown of the magnetization plateau at the magnetization M = MS/3 (MS is the saturation magnetization) of the S = 1/2 anisotropic spin chain with ferromagnetic-ferromagnetic-antiferromagnetic interactions. We consider the model with the isotropic ferromagnetic (trimer) coupling JF , and the anisotropic antiferromagnetic coupling (Jx = Jy = JAF and Jz = ∆JAF ). For the large γ ≡ JF /JAF limit, the model is equivalent to the S = 3/2 XXZ chain with the exchange anisotropy ∆. There is a phase transition between the plateau (small γ) and the no-plateau (large γ) regions. This phase transition is of the Berezinskii-Kosterlitz-Thouless type, and we determine the phase boundary from the numerical diagonalization data. Especially for ∆ = 1, the phase transition point between the plateau and the no-plateau regions is γc = 15.4.

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

4 D ec 1 99 9 Breakdown of the magnetization plateau of the S = 1 / 2 ferromagnetic - ferromagnetic - antiferromagnetic trimerized spin chain with anisotropy

We study the breakdown of the magnetization plateau at the magnetization M = MS/3 (MS is the saturation magnetization) of the S = 1/2 anisotropic spin chain with ferromagnetic-ferromagnetic-antiferromagnetic interactions. We consider the model with the isotropic ferromagnetic (trimer) coupling JF , and anisotropic antiferromagnetic coupling (Jx = Jy = JAF and Jz = ∆JAF ). For the limit of large...

متن کامل

امواج اسپین و ناهمسانگردی تک جهتی در دولایه‌ایهای نازک فرومغناطیسپادفرومغناطیسی

  In this paper a simple model calculation of spin wave is given for the ferromagtic layer in ultra thin ferromagnetic/antiferromagnetic bilayer. In this model the magnetic layer is assumed as an isolated layer but the effect of antiferromagnetic layer on ferromagnetic layer and unidirectional anisotropy, is given in the effective field applied on each spin. The thin layer is assumed as two-dim...

متن کامل

2 6 A ug 2 00 6 Ferrimagnetic States in S = 1 / 2 Frustrated Heisenberg Chains with Period 3 Exchange Modulation

Ground state properties of the S = 1/2 frustrated Heisenberg chain with period 3 exchange modulation are investigated using the numerical diagonalization and DMRG method. It is known that this model has a magnetization plateau at 1/3 of the saturation magnetization M s. On the other hand, the ground state is ferrimagnetic even in the absence of frustration if one of the nearest neighbour bond i...

متن کامل

Spin-wave theory of exchange-induced anisotropy

It is shown that exchange interactions of spins across the boundary between ferromagnetic and antiferromagnetic layers can cause a shift in the observed hysteresis loop of the ferromagnetic layer. The effect may be interpreted as a self-energy shift of each ferromagnetic spin due to emission and reabsorption of virtual antiferromagnetic spin waves. Emission of these waves by one ferromagnetic s...

متن کامل

Excitation Spectrum of the Spin-1/2 Ferromagnetic-Antiferromagnetic Alternating Heisenberg Chain

The natural explanation of the excitation spectrum of the spin1 antiferromagnetic Heisenberg chain is given from the viewpoint of the spin-1/2 ferromagnetic-antiferromagnetic alternating Heisenberg chain. The energy spectrum of the latter is calculated with fixed momentum k by numerical diagonalization of finite size systems. It consists of a branch of propagating triplet pair (triplet wave) an...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 1999