-
2
-
-
0001352146
-
-
A. V. Chaplik, Zh. Eksp. Teor. Fiz. 62, 746 (1972) [Sov. Phys. JETP 35, 395 (1972)].
-
(1972)
Sov. Phys. JETP
, vol.35
, pp. 395
-
-
Chaplik, A.V.1
-
11
-
-
3843106558
-
-
S. J. Allen, Jr., D. C. Tsui, and R. A. Logan, Phys. Rev. Lett. 38, 980 (1977).
-
(1977)
Phys. Rev. Lett.
, vol.38
, pp. 980
-
-
Allen, S.J.1
Tsui, D.C.2
Logan, R.A.3
-
15
-
-
16444377513
-
-
D. Olego, A. Pinczuk, A. Gossard, and W. Wiegmann, Phys. Rev. B 25, 7867 (1982).
-
(1982)
Phys. Rev. B
, vol.25
, pp. 7867
-
-
Olego, D.1
Pinczuk, A.2
Gossard, A.3
Wiegmann, W.4
-
17
-
-
0011134754
-
-
K. D. Maranowski, A. C. Gossard, K. Unterrainer, and E. Gornik, Appl. Phys. Lett. 69, 3522 (1996).
-
(1996)
Appl. Phys. Lett.
, vol.69
, pp. 3522
-
-
Maranowski, K.D.1
Gossard, A.C.2
Unterrainer, K.3
Gornik, E.4
-
19
-
-
0001489195
-
-
L. Wendler, T. Kraft, M. Hartung, A. Berger, A. Wixforth, M. Sundaram, J. H. English, and A. C. Gossard, Phys. Rev. B 55, 2303 (1997).
-
(1997)
Phys. Rev. B
, vol.55
, pp. 2303
-
-
Wendler, L.1
Kraft, T.2
Hartung, M.3
Berger, A.4
Wixforth, A.5
Sundaram, M.6
English, J.H.7
Gossard, A.C.8
-
26
-
-
0000170682
-
-
Academic Press, New York R. W. Hoffmann M. H. Francombe G. Hass
-
H. Raether, in Physics of Thin Films, edited by G. Hass, M. H. Francombe, and R. W. Hoffmann (Academic Press, New York, 1977), Vol. 9, p. 145.
-
(1977)
Physics of Thin Films
, vol.9
, pp. 145
-
-
Raether, H.1
-
28
-
-
0004148819
-
-
North-Holland, Amsterdam V. M. Agranovich D. L. Mills
-
A. A. Maradudin, in Surface Polaritons, edited by V. M. Agranovich and D. L. Mills (North-Holland, Amsterdam, 1982), p. 405.
-
(1982)
Surface Polaritons
, pp. 405
-
-
Maradudin, A.A.1
-
30
-
-
4243764139
-
-
U. Mackens, D. Heitmann, L. Prager, J. P. Kotthaus, and W. Beinvogl, Phys. Rev. Lett. 53, 1485 (1984).
-
(1984)
Phys. Rev. Lett.
, vol.53
, pp. 1485
-
-
Mackens, U.1
Heitmann, D.2
Prager, L.3
Kotthaus, J.P.4
Beinvogl, W.5
-
31
-
-
85037885987
-
-
It should be noted that in general there are two types of grating (or Wood’s) anomalies: (i) the Rayleigh wavelength-type and (ii) the resonance-type anomaly, which is connected with the excitation of a leaky surface wave propagating along the metallic grating. As shown in detail in Ref. 18 for the here discussed situation, the appearing tips and dips are caused by both types of Wood’s anomalies. This is true because in the far-infrared frequency range, both types of Wood’s anomalies occur at the same frequency and thus, cannot be distinguished. Because the onset of the Rayleigh wavelength-type anomaly is exactly determined by the onset (or disappearance) of a particular diffracted order of the propagating beam (in the substrate for transmission), in the present paper we call the appearing anomalies Rayleigh anomaly.
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It should be noted that in general there are two types of grating (or Wood’s) anomalies: (i) the Rayleigh wavelength-type and (ii) the resonance-type anomaly, which is connected with the excitation of a leaky surface wave propagating along the metallic grating. As shown in detail in Ref. 18 for the here discussed situation, the appearing tips and dips are caused by both types of Wood’s anomalies. This is true because in the far-infrared frequency range, both types of Wood’s anomalies occur at the same frequency and thus, cannot be distinguished. Because the onset of the Rayleigh wavelength-type anomaly is exactly determined by the onset (or disappearance) of a particular diffracted order of the propagating beam (in the substrate for transmission), in the present paper we call the appearing anomalies Rayleigh anomaly.
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