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14
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85037911936
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There is by now sizable literature on this subject, and we apologize for not listing much of the recent work except where directly germane to the topic of this paper.
-
There is by now sizable literature on this subject, and we apologize for not listing much of the recent work except where directly germane to the topic of this paper.
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15
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C. Timm, S. M. Girvin, and H. A. Fertig, Phys. Rev. B 58, 10 634 (1998), and references therein.
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Zheng, L.6
Yoshioka, D.7
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21
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For related work, see B. E. Kane, L. N. Pfeiffer, and K. W. West, Phys. Rev. B 46, 7264 (1992);
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Phys. Rev. B
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Kane, B.E.1
Pfeiffer, L.N.2
West, K.W.3
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26
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85037913565
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K. Lejnell, thesis, Stockholm University, 1996.
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K. Lejnell, thesis, Stockholm University, 1996.
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27
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0001461268
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M. Abolfath, J. J. Palacios, H. A. Fertig, S. M. Girvin, and A. H. MacDonald, Phys. Rev. B 56, 6795 (1997).
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Palacios, J.J.2
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Kyungsun Moon and Kieran Mullen, Phys. Rev. B 57, 14 833 (1998).
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Phys. Rev. B
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30
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85037920624
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For (Formula presented) and (Formula presented) equals (Formula presented) and (Formula presented) respectively.
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For (Formula presented) and (Formula presented) equals (Formula presented) and (Formula presented) respectively.
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-
-
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34
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0003498504
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Academic Press, New York
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See, e.g., I. S. Gradshteyn and I. M. Ryzhik, Table of Integrals, Series, and Products (Academic Press, New York, 1980).
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Table of Integrals, Series, and Products
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Gradshteyn, I.S.1
Ryzhik, I.M.2
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35
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85037879911
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Ar. Abanov and V. L. Pokrovsky, cond-mat/9801114(unpublished).
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Pokrovsky, V.L.1
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0008792394
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D. Lilliehöök, K. Lejnell, A. Karlhede, and S. L. Sondhi, Phys. Rev. B 56, 6805 (1997).
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Phys. Rev. B
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Sondhi, S.L.4
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37
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0003474751
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Cambridge University Press, Cambridge, England
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W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes in C (Cambridge University Press, Cambridge, England, 1988).
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(1988)
Numerical Recipes in C
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Press, W.H.1
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Flannery, B.P.4
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38
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85037906919
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The shooting method cannot be used directly since the origin is a critical point: The value of the function and of its first derivative at the origin do not specify the solution uniquely.
-
The shooting method cannot be used directly since the origin is a critical point: The value of the function and of its first derivative at the origin do not specify the solution uniquely.
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39
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85037901449
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An alternative method would be to use the sigma model solution near (Formula presented) We would then have to minimize the energy with respect to additional parameters (corresponding to unknown derivatives of f at the origin) and this would necessarily involve several relaxation solutions. This is quite time consuming and also has other numerical disadvantages.
-
An alternative method would be to use the sigma model solution near (Formula presented) We would then have to minimize the energy with respect to additional parameters (corresponding to unknown derivatives of f at the origin) and this would necessarily involve several relaxation solutions. This is quite time consuming and also has other numerical disadvantages.
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-
-
-
40
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85037914688
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We give the energies to create one Skyrmion at fixed particle number and fixed magnetic field. These energies are equal for the Skyrmion and anti-Skyrmion (with the same value of (Formula presented).
-
We give the energies to create one Skyrmion at fixed particle number and fixed magnetic field. These energies are equal for the Skyrmion and anti-Skyrmion (with the same value of (Formula presented).
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41
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85037915552
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The deviation is probably partly due to finite-size effects in the Hartree-Fock calculation for which the boundary condition is (Formula presented) at (Formula presented) while in the effective action calculation we have (Formula presented)
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The deviation is probably partly due to finite-size effects in the Hartree-Fock calculation for which the boundary condition is (Formula presented) at (Formula presented) while in the effective action calculation we have (Formula presented)
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