-
3
-
-
0004324756
-
-
Materials Research Society, Pittsburgh, PA
-
R. Crane, K. Lewis, E. Van Stryland, M. Koshnevisan, Eds., Materials for Optical Limiting (Materials Research Society, Pittsburgh, PA, 1995), vol. 374.
-
(1995)
Materials for Optical Limiting
, vol.374
-
-
Crane, R.1
Lewis, K.2
Van Stryland, E.3
Koshnevisan, M.4
-
6
-
-
0028441927
-
-
B. L. Justus, A. J. Campillo, A. L. Huston, Opt. Lett. 19, 673 (1994); B. L. Justus, Z. H. Kafafi, A. L. Huston, ibid. 18, 1603 (1993).
-
(1994)
Opt. Lett.
, vol.19
, pp. 673
-
-
Justus, B.L.1
Campillo, A.J.2
Huston, A.L.3
-
7
-
-
0027678858
-
-
B. L. Justus, A. J. Campillo, A. L. Huston, Opt. Lett. 19, 673 (1994); B. L. Justus, Z. H. Kafafi, A. L. Huston, ibid. 18, 1603 (1993).
-
(1993)
Opt. Lett.
, vol.18
, pp. 1603
-
-
Justus, B.L.1
Kafafi, Z.H.2
Huston, A.L.3
-
10
-
-
0000661016
-
-
J. S. Shirk, R. G. S. Pong, F. J. Bartoli, A. W. Snow, Appl. Phys. Lett. 63, 1880 (1993).
-
(1993)
Appl. Phys. Lett.
, vol.63
, pp. 1880
-
-
Shirk, J.S.1
Pong, R.G.S.2
Bartoli, F.J.3
Snow, A.W.4
-
12
-
-
85168196509
-
-
U.S. Patent 5,080,469 (1992)
-
S. W. McCahon and L. W. Tutt, U.S. Patent 5,080,469 (1992).
-
-
-
McCahon, S.W.1
Tutt, L.W.2
-
18
-
-
33947487561
-
-
M. K. Lowery, A. J. Starshak, J. N. Esposito, P. C. Krueger, M. E. Kenney, ibid. 4, 128 (1965); B. L. Wheeler et al., J. Am. Chem. Soc. 106, 7404 (1984); S. A. Mikhalenko, S. V. Barkanova, O. L. Lebedev, E. A. Luk'yanets. Zh. Obshch Khim. 41, 2735 (1971); K.-Y. Law, Inorg. Chem. 24, 1778 (1985).
-
(1965)
Inorg. Chem.
, vol.4
, pp. 128
-
-
Lowery, M.K.1
Starshak, A.J.2
Esposito, J.N.3
Krueger, P.C.4
Kenney, M.E.5
-
19
-
-
0021520454
-
-
M. K. Lowery, A. J. Starshak, J. N. Esposito, P. C. Krueger, M. E. Kenney, ibid. 4, 128 (1965); B. L. Wheeler et al., J. Am. Chem. Soc. 106, 7404 (1984); S. A. Mikhalenko, S. V. Barkanova, O. L. Lebedev, E. A. Luk'yanets. Zh. Obshch Khim. 41, 2735 (1971); K.-Y. Law, Inorg. Chem. 24, 1778 (1985).
-
(1984)
J. Am. Chem. Soc.
, vol.106
, pp. 7404
-
-
Wheeler, B.L.1
-
20
-
-
0000525971
-
-
M. K. Lowery, A. J. Starshak, J. N. Esposito, P. C. Krueger, M. E. Kenney, ibid. 4, 128 (1965); B. L. Wheeler et al., J. Am. Chem. Soc. 106, 7404 (1984); S. A. Mikhalenko, S. V. Barkanova, O. L. Lebedev, E. A. Luk'yanets. Zh. Obshch Khim. 41, 2735 (1971); K.-Y. Law, Inorg. Chem. 24, 1778 (1985).
-
(1971)
Zh. Obshch Khim.
, vol.41
, pp. 2735
-
-
Mikhalenko, S.A.1
Barkanova, S.V.2
Lebedev, O.L.3
Luk'yanets, E.A.4
-
21
-
-
0000301427
-
-
M. K. Lowery, A. J. Starshak, J. N. Esposito, P. C. Krueger, M. E. Kenney, ibid. 4, 128 (1965); B. L. Wheeler et al., J. Am. Chem. Soc. 106, 7404 (1984); S. A. Mikhalenko, S. V. Barkanova, O. L. Lebedev, E. A. Luk'yanets. Zh. Obshch Khim. 41, 2735 (1971); K.-Y. Law, Inorg. Chem. 24, 1778 (1985).
-
(1985)
Inorg. Chem.
, vol.24
, pp. 1778
-
-
Law, K.-Y.1
-
22
-
-
85168215104
-
-
note
-
4 was isolated as a single isomer by crystallization from ether-ethanol solution. We measured the fluence-dependent transmittance of the series of compounds by using 8-ns, 532-nm laser pulses from a frequency-doubled Q-switched Nd:yttrium-aluminum-garnet laser.
-
-
-
-
23
-
-
0027191786
-
-
o are the ground state, excited state, and total number densities, respectively. The propagation equation is solved numerically by a finite-element approach where each element is chosen to be optically thin such that beam attenuation within the element can be neglected. The attenuation of the beam is calculated as the pulse is passed sequentially through each element, with the output energy of an element used as the input energy for the next element. See, for example, K. Mansour et al. Proc. SPIE 1853, 132 (1993).
-
(1993)
Proc. SPIE
, vol.1853
, pp. 132
-
-
Mansour, K.1
-
24
-
-
0000010232
-
-
Use of tandem cells of a Pc excited-state absorber has achieved a comparable blocking level in a slower optical system (f/10), but with the chromophore and the tandem cell device design utilized, the linear transmittance was rather low (20%) [D. J. Hagan et al., Int. J. Nonlinear Opt. Phys. 2, 483 (1993)].
-
(1993)
Int. J. Nonlinear Opt. Phys.
, vol.2
, pp. 483
-
-
Hagan, D.J.1
-
25
-
-
85168209064
-
-
note
-
effL. A much higher (nonhomogeneously distributed) concentration would be needed to achieve an attentuation of 540 and would result in a linear transmission of 0.12. 22. This work was performed in part at the Jet Propulsion Laboratory as part of its Center for Space Microelectronics Technology and was supported by the Ballistic Missile Defense Organization, Innovative Science and Technology Office, and the U.S. Air Force Wright Laboratory through an agreement with NASA. Work at the Beckman Institute was supported by the Office of Naval Research, the Defense Advanced Research Projects Agency, the Office of Naval Research through the Center for Advanced Multifunctional Molecular Assemblies and Polymers, and the Air Force Office of Scientific Research P.V.B. is the recipient of a postdoctoral fellowship from the James Irvine Foundation.
-
-
-
|