-
1
-
-
85075918556
-
-
10.1117/12.150601
-
A. E. Siegman, Proc. SPIE 1868, 2 (1993). 10.1117/12.150601
-
(1993)
Proc. SPIE
, vol.1868
, pp. 2
-
-
Siegman, A.E.1
-
2
-
-
0004142577
-
-
Cambridge University Press, Cambridge, UK
-
P. Hariharan, Optical Holography (Cambridge University Press, Cambridge, UK, 1996), pp. 74-75.
-
(1996)
Optical Holography
, pp. 74-75
-
-
Hariharan, P.1
-
3
-
-
0000233116
-
-
10.1063/1.123502
-
H. Kosaka, Appl. Phys. Lett. 74, 1212 (1999). 10.1063/1.123502
-
(1999)
Appl. Phys. Lett.
, vol.74
, pp. 1212
-
-
Kosaka, H.1
-
5
-
-
20444442786
-
-
10.1063/1.1830675;
-
R. Iliew, Appl. Phys. Lett. 85, 5854 (2004) 10.1063/1.1830675
-
(2004)
Appl. Phys. Lett.
, vol.85
, pp. 5854
-
-
Iliew, R.1
-
6
-
-
0347764674
-
-
10.1364/OL.29.000050
-
D. W. Prather, Opt. Lett. 29, 50 (2004). 10.1364/OL.29.000050
-
(2004)
Opt. Lett.
, vol.29
, pp. 50
-
-
Prather, D.W.1
-
7
-
-
32844465934
-
-
10.1103/PhysRevE.73.016601
-
K. Staliunas and R. Herrero, Phys. Rev. E 73, 016601 (2006). 10.1103/PhysRevE.73.016601
-
(2006)
Phys. Rev. e
, vol.73
, pp. 016601
-
-
Staliunas, K.1
Herrero, R.2
-
10
-
-
33846451396
-
-
10.1103/PhysRevB.75.014304;
-
I. Pérez-Arjona, Phys. Rev. B 75, 014304 (2007) 10.1103/PhysRevB.75.014304
-
(2007)
Phys. Rev. B
, vol.75
, pp. 014304
-
-
Pérez-Arjona, I.1
-
11
-
-
35748977134
-
-
10.1103/PhysRevB.76.140302
-
V. Espinosa, Phys. Rev. B 76, 140302 (R) (2007). 10.1103/PhysRevB.76. 140302
-
(2007)
Phys. Rev. B
, vol.76
, pp. 140302
-
-
Espinosa, V.1
-
12
-
-
65549104297
-
-
The efficiency of the projection is in general determined by the vector product between the eigenvectors of Bloch mode with the vector of the corresponding plane-wave component. The study of the projection in the particular case studied is to be published elsewhere.
-
The efficiency of the projection is in general determined by the vector product between the eigenvectors of Bloch mode with the vector of the corresponding plane-wave component. The study of the projection in the particular case studied is to be published elsewhere.
-
-
-
-
14
-
-
65549098136
-
-
The detailed study of the excitation reprojection in Eq. 4 is to be presented elsewhere.
-
The detailed study of the excitation reprojection in Eq. 4 is to be presented elsewhere.
-
-
-
-
15
-
-
34249851293
-
-
10.1016/j.physrep.2007.02.011
-
K. Busch, Phys. Rep. 444, 101 (2007). 10.1016/j.physrep.2007.02.011
-
(2007)
Phys. Rep.
, vol.444
, pp. 101
-
-
Busch, K.1
-
17
-
-
19544388569
-
-
10.1103/PhysRevLett.93.083905
-
D. Neshev, Phys. Rev. Lett. 93, 083905 (2004). 10.1103/PhysRevLett.93. 083905
-
(2004)
Phys. Rev. Lett.
, vol.93
, pp. 083905
-
-
Neshev, D.1
-
18
-
-
65549159170
-
-
We note that the expansion 2 leading to Eq. 3 is possible without paraxial approximation, and the discussions concerning the projecting of the excitation on the slopes of dispersion curves is qualitatively correct also for nonparaxial case. In this nonparaxial case, the dispersion curves are circles instead of parabolas in the paraxial case considered in the present paper.
-
We note that the expansion 2 leading to Eq. 3 is possible without paraxial approximation, and the discussions concerning the projecting of the excitation on the slopes of dispersion curves is qualitatively correct also for nonparaxial case. In this nonparaxial case, the dispersion curves are circles instead of parabolas in the paraxial case considered in the present paper.
-
-
-
|