All-optical NAND logic gate using organic materials

Conventional electronic logic circuits in today's computers impose extreme limitations on computational speed, complexity, compactness. In highly dense electronic logic circuits the connections simply cannot handle electric signals swiftly and reliably. On the other hand, optical interconnections and optical integrated circuits are sought to provide answers to future computing and compactness demands. Optical devices are immune from electromagnetic interference and free from electrical short circuits. They have low-loss transmission and provide large bandwidth (i.e. multiplexing capability), and are manufacturable in compact sizes, are lightweight and inexpensive. Recently, we demonstrated an all-optical NAND logic gate having nanosecond response time by waveguiding two collinear nanosecond white light caused by focusing a pulsed Nd:YAG laser at 1064 nm along with a cw He-Ne laser at 632.8 nm through a polydiacetylene derivative of 2-methyl-4- nitroaniline (PDAMNA) thin film. The physics involved in the process was explained based on Z-scan studies of the same polymer using He-Ne laser. These studies show an induced absorption by an excited state, resulting in a reverse saturable absorption (RSA) in the system. The RSA figure of merit in PDAMNA was estimated. The size and sign of the real and imaginary parts of the third order nonlinearity were evaluated. These studies also demonstrate for the first time to our knowledge, that reverse saturable absorption in an optical system can be used to build similar logic gates.

[1]  G. M. Carter,et al.  Chapter III-3 – Degenerate Third-Order Nonlinear Optical Susceptibility of Polydiacetylenes , 1987 .

[2]  Kamjou Mansour,et al.  Organic Optical Limiter with a Strong Nonlinear Absorptive Response , 1996, Science.

[3]  Gary M. Carter,et al.  Excited-state dynamics and temporally resolved nonresonant nonlinear-optical processes in polydiacetylenes , 1987 .

[4]  M. L. Shand,et al.  Three-wave mixing in conjugated polymer solutions: Two-photon absorption in polydiacetylenes , 1980 .

[5]  K. Kawasaki,et al.  Third‐order nonlinear optical properties of retinal derivatives , 1990 .

[6]  Lei Zhang,et al.  Nonlinear absorption in metallo-porphyrin-like , 1994 .

[7]  J. Perry,et al.  Enhanced reverse saturable absorption and optical limiting in heavy-atom-substituted phthalocyanines. , 1994, Optics letters.

[8]  F. Kajzar,et al.  Chapter III-2 – Cubic Effects in Polydiacetylene Solutions and Films , 1987 .

[9]  Ray H. Baughman,et al.  Optical Nonlinearities in One-Dimensional-Conjugated Polymer Crystals. , 1976 .

[10]  Werner J. Blau,et al.  Picosecond degenerate four‐wave mixing in soluble polydiacetylenes , 1985 .

[11]  Li,et al.  Dynamic and steady-state behaviors of reverse saturable absorption in metallophthalocyanine. , 1994, Physical review. A, Atomic, molecular, and optical physics.

[12]  Donald O. Frazier,et al.  Photodeposition of amorphous polydiacetylene films from monomer solutions onto transparent substrates , 1995 .

[13]  Joseph Zyss,et al.  Nonlinear optical properties of organic molecules and crystals , 1987 .

[14]  Paul D. Townsend,et al.  Fabrication of waveguide structures from soluble polydiacetylenes , 1989 .

[15]  Donald O. Frazier,et al.  Photodeposition of Thin Polydiacetylene Films from Solution That Exhibit Large Third-Order Optical Nonlinearities , 1994 .

[16]  Mrinal Thakur,et al.  Correlation between photoinduced absorption and large off‐resonant nonlinear refractive index of polydiacetylene , 1992 .

[17]  Myoungsik Cha,et al.  Measurement of the complex nonlinear refractive index of single crystal p‐toluene sulfonate at 1064 nm , 1994 .