-
2
-
-
0343133491
-
-
V.L. Ginzburg, Zh. Eksp. Teor. Fiz. 31, 202 (1956) [Sov. Phys. JETP 4, 153 (1957)].
-
(1957)
Sov. Phys. JETP
, vol.4
, pp. 153
-
-
-
4
-
-
0034894384
-
-
A. Huxley, I. Sheikin, E. Ressouche, N. Kernavanois, D. Braithwaite, R. Calemczuk, and J. Flouquet, Phys. Rev. B 63, 144519 (2001).
-
(2001)
Phys. Rev. B
, vol.63
, pp. 144519
-
-
Huxley, A.1
Sheikin, I.2
Ressouche, E.3
Kernavanois, N.4
Braithwaite, D.5
Calemczuk, R.6
Flouquet, J.7
-
6
-
-
0035846093
-
-
D. Aoki, A. Huxley, E. Ressouche, D. Braithwaite, J. Floquet, J. P. Brison, E. Lhotel, and C. Paulsen, Nature (London) 413, 613 (2001).
-
(2001)
Nature (London)
, vol.413
, pp. 613
-
-
Aoki, D.1
Huxley, A.2
Ressouche, E.3
Braithwaite, D.4
Floquet, J.5
Brison, J.P.6
Lhotel, E.7
Paulsen, C.8
-
7
-
-
0035811510
-
-
C. Pfleiderer, M. Uhlarz, S. M. Hayden, R. Vollmer, H. von Löhneysen, N.R. Bernhoeft, and G.G. Lonzarich, Nature (London) 412, 58 (2001).
-
(2001)
Nature (London)
, vol.412
, pp. 58
-
-
Pfleiderer, C.1
Uhlarz, M.2
Hayden, S.M.3
Vollmer, R.4
Von Löhneysen, H.5
Bernhoeft, N.R.6
Lonzarich, G.G.7
-
12
-
-
0000272114
-
-
I.A. Fomin, Pis'ma Zh. Eksp. Teor. Fiz. 74, 116 (2001) [JETP Lett. 74, 111 (2001)].
-
(2001)
JETP Lett.
, vol.74
, pp. 111
-
-
-
13
-
-
9744259105
-
-
note
-
We consider only cases where the ground state of the system is a flux lattice; other states are possible [12].
-
-
-
-
16
-
-
0001726581
-
-
A.A. Abrikosov, Zh. Eksp. Teor. Fiz. 32, 1442 (1957) [Sov. Phys. JETP 5, 1174 (1957)].
-
(1957)
Sov. Phys. JETP
, vol.5
, pp. 1174
-
-
-
18
-
-
39249083411
-
-
L. Radzihovsky, E. M. Ettouhami, K. Saunders, and J. Toner, Phys. Rev. Lett. 87, 027001 (2001).
-
(2001)
Phys. Rev. Lett.
, vol.87
, pp. 027001
-
-
Radzihovsky, L.1
Ettouhami, E.M.2
Saunders, K.3
Toner, J.4
-
19
-
-
9744264474
-
-
note
-
We have shown only that a hexagonal lattice leads to a local energy minimum for our final effective action, Eq. (6); the global minimum could have a different structure. The number and type of Goldstone modes would be the same, but the detailed form of the elastic energy would be different for a nonhexagonal lattice. See also Ref. [11].
-
-
-
-
21
-
-
9744283729
-
-
note
-
It is easy to verify that keeping terms of higher than quartic power in either order parameter in Eqs. (2) does not affect our conclusions.
-
-
-
-
22
-
-
9744247877
-
-
note
-
In conventional ferromagnets, the fluctuating vector potential leads to the dipole-dipole interaction. This is usually ignored for studying critical phenomena, despite its formal renormalization-group (RG) relevance, since it is very small compared to the exchange coupling. For the properties of a ferromagnetic superconductor, however, the coupling of the vector potential to the magnetization is crucial, as we will see.
-
-
-
-
23
-
-
9744268499
-
-
note
-
We consider only magnetic states which are rotationally invariant in the plane perpendicular to the direction of the spontaneous magnetization.
-
-
-
-
24
-
-
9744236133
-
-
note
-
To compare with Ref. [15], notice that these authors localized the potential in the second term and omitted both the last term and the subtraction leading to a instead of a in the next-to-last term. These approximations do not affect the leading elastic properties of the vortex-lattice.
-
-
-
-
25
-
-
9744249735
-
-
note
-
Note that this is the so-called left strain tensor, as opposed to the more commonly used right strain tensor [23]. A discussion of why the left strain tensor is appropriate for the situation at hand can be found in Ref. [24].
-
-
-
-
27
-
-
41349084958
-
-
T. C. Lubensky, R. Mukhopadhyay, L. Radzihovsky, and X. Xing, Phys. Rev. E 66, 011702 (2002).
-
(2002)
Phys. Rev. E
, vol.66
, pp. 011702
-
-
Lubensky, T.C.1
Mukhopadhyay, R.2
Radzihovsky, L.3
Xing, X.4
-
28
-
-
85088492555
-
-
note
-
2 is less suitable for our purposes since it it has a strong intrinsic spin anisotropy [4], and the same is true for URhGe.
-
-
-
|