-
2
-
-
61849178092
-
-
and references therein
-
T. Dahm et al.: Nat. Phys. 5(2009) 217, and references therein.
-
(2009)
Nat. Phys.
, vol.5
, pp. 217
-
-
Dahm, T.1
-
18
-
-
45249120773
-
-
details of setup geometry can be found in
-
The details of setup geometry can be found in D. S. Inosov et al.: Phys. Rev. B 77(2008) 212504.
-
(2008)
Phys. Rev. B.
, vol.77
, pp. 212504
-
-
Inosov, D.S.1
-
19
-
-
73949119959
-
-
In investigation of three-dimensionality of iron pnictides ARPES studies concentrate on the undoped and electron-doped samples
-
In investigation of three-dimensionality of iron pnictides ARPES studies concentrate on the undoped and electron-doped samples [W. Malaeb et al.: J. Phys. Soc. Jpn. 78(2009) 123706;
-
(2009)
J. Phys. Soc. Jpn.
, vol.78
, pp. 123706
-
-
Malaeb, W.1
-
21
-
-
79951592084
-
-
z-averaged ones of the real three-dimensional structure, should provide fairly good accuracy in our case
-
z-averaged ones of the real three-dimensional structure, should provide fairly good accuracy in our case.
-
-
-
-
23
-
-
4243352027
-
-
xx is consistent with
-
xx is consistent with J. M. Harris et al.: Phys. Rev. Lett. 75(1995) 1391;
-
(1995)
Phys. Rev. Lett.
, vol.75
, pp. 1391
-
-
Harris, J.M.1
-
24
-
-
0038035162
-
-
although rewritten in a form more convenient for the present consideration
-
N. E. Hussey: Eur. Phys. J. B 31(2003) 495, although rewritten in a form more convenient for the present consideration.
-
(2003)
Eur. Phys. J. B.
, vol.31
, pp. 495
-
-
Hussey, N.E.1
-
25
-
-
79951629380
-
-
∇ε
-
2ε · |∇ε| - (∇|∇ε|, ∇ε)/(∇ε, ∇ε).
-
-
-
-
27
-
-
67650296128
-
-
H is very close to the one, resulting from the rigorously calculated band structure A. N. Yaresko: private communication. Details of the band structure calculation are available in
-
H is very close to the one, resulting from the rigorously calculated band structure (A. N. Yaresko: private communication). Details of the band structure calculation are available in A. N. Yaresko et al.: Phys. Rev. B 79(2009) 144421.
-
(2009)
Phys. Rev. B.
, vol.79
, pp. 144421
-
-
Yaresko, A.N.1
-
35
-
-
79951653481
-
-
Presented here considerations rely on the results, obtained in the Fermi-liquid-like approach. Though pure Fermi liquid theory is not always applicable to the electrons in solids, e.g., in the vicinity of phase transition and importance of order fluctuations see ref. 45 and references therein, the natural extension of this transparent theory may be useful even in description of correlated systems. In particular, the band dispersion, extracted from the spectral function measured in ARPES experiments, should well represent the effective band dispersion and Fermi surface, defining the electron dynamics
-
Presented here considerations rely on the results, obtained in the Fermi-liquid-like approach. Though pure Fermi liquid theory is not always applicable to the electrons in solids, e.g., in the vicinity of phase transition and importance of order fluctuations (see ref. 45 and references therein), the natural extension of this transparent theory may be useful even in description of correlated systems. In particular, the band dispersion, extracted from the spectral function (measured in ARPES experiments), should well represent the effective band dispersion and Fermi surface, defining the electron dynamics.
-
-
-
-
37
-
-
79951659108
-
-
A manuscript with the calculation of the LiFeAs Hall coefficient from ARPES and comparison to the magnetotransport measurements is under preparation. Measurements of the Hall effect on LiFeAs are described in O. Heyer et al.: arXiv:1010.2876
-
A manuscript with the calculation of the LiFeAs Hall coefficient from ARPES and comparison to the magnetotransport measurements is under preparation. Measurements of the Hall effect on LiFeAs are described in O. Heyer et al.: arXiv:1010.2876.
-
-
-
-
39
-
-
79951620203
-
-
T Yoshida et al.: arXiv:1008.2080
-
T Yoshida et al.: arXiv:1008.2080.
-
-
-
|