Faraday effect in Sm3Ga5O12 at low temperatures

Sokolov, B. Yu.

doi:10.1134/1.1129907

Cited by 4 publications

(9 citation statements)

References 2 publications

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“…The most nanowires so far have been grown by Vapor-Liquid-Solid (VLS) method using gold as the catalyst. In this method, however, the nanowire is doped with the gold to degrade the crystalline [1,2]. Therefore, catalyst free growth of a nanowire is supposed to avoid the faults [3].…”

Section: Introductionmentioning

confidence: 99%

Catalyst free MBE‐VLS growth of GaAs nanowires on (111)Si substrate

Paek

Nishiwaki

Yamaguchi

et al. 2009

Phys. Status Solidi (c)

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The behaviour of catalyst free GaAs nanowire growth is investigated on (111)Si substrate by molecular beam epitaxy under different Ga and As fluxes. It is found that the diameter of nanowire is increased by increasing the Ga flux, while it is decreased by increasing the As flux. The growth rate along the wire axis is enhanced by increasing the As flux under a constant Ga flux. Moreover, the Ga droplet at the top disappears by the growth interruption and the growth along the wire axis is strictly prohibited. By adopting the last result, the growth of GaAs/AlGaAs core‐shell structure is attempted. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)

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Section: Introductionmentioning

confidence: 99%

Catalyst free MBE‐VLS growth of GaAs nanowires on (111)Si substrate

Paek

Nishiwaki

Yamaguchi

et al. 2009

Phys. Status Solidi (c)

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“…These quantities are of interest for constructing the field theoretic effective potential [1,2] of a 3d scalar field at the infrared fixed point or, in statistical mechanics language, for the formulation of the critical equation of state of the 3d Ising model universality class [3][4][5]. The computational methods, which so far have been used, include various approximate forms [6][7][8][9][10][11] of the renormalization group (RG), the field theoretic strong coupling expansion [2], the high temperature (HT) expansion [3,4,[12][13][14] and (single-or multi-cluster) MonteCarlo techniques [5,[15][16][17].…”

Section: Introductionmentioning

confidence: 99%

2n-point renormalized coupling constants in the three-dimensional Ising model:Estimates by high temperature series to orderΒ17

Butera

Comi

1997

Phys. Rev. E

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We compute the 2n-point renormalized coupling constants in the symmetric phase of the 3d Ising model on the sc lattice in terms of the high temperature expansions O(β 17 ) of the Fourier transformed 2n-point connected correlation functions at zero momentum.Our high temperature estimates of these quantities, which enter into the small field expansion of the effective potential for a 3d scalar field at the IR fixed point or, equivalently, in the critical equation of state of the 3d Ising model universality class, are compared with recent results obtained by renormalization group methods, strong coupling, stochastic simulations as well as previous high temperature expansions.

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“…Nd 3 Ga 5 O 12 [16], Gd 3 Ga 5 O 12 [17][18][19][20][21], Tb 3 Ga 5 O 12 [22,23], Dy 3 Ga 5 O 12 [24,25], Ho 3 Ga 5 O 12 [26] and Yb 3 Ga 5 O 12 [27] each have features indicative of a Néel transition below 1 K and appear to exhibit a wide variety of magnetic ground states. Here, the low temperature magnetic properties of Sm 3 Ga 5 O 12 [28,29] are studied. stoichiometric amounts of Sm 2 O 3 (or Y 2 O 3 ) and Ga 2 O 3 .…”

Section: Introductionmentioning

confidence: 99%