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HIGHER HARMONIC A.C. POLAROGRAPHY OF MULTICOMPONENT SYSTEMSDEVAY J; GARAI T; PALAGYI FENYES B et al.1973; ACTA CHIM. ACAD. SCI. HUNGAR.; HONGR.; DA. 1973; VOL. 76; NO 1; PP. 29-50; ABS. RUSSE; BIBL. 15 REF.Serial Issue

THE EFFECT OF THE CELL RESISTANCE IN HIGHER HARMONIC A.C. POLAROGRAPHY IN THE CASE OF DIFFUSION POLARIZATIONDEVAY J; GARAI T; MESZAROS L et al.1973; ACTA CHIM. ACAD. SCI. HUNGAR.; HONGR.; DA. 1973; VOL. 75; NO 4; PP. 331-349; ABS. RUSSE; BIBL. 28 REF.Serial Issue

FREE-ELECTRON LASERS OPERATING IN HIGHER HARMONICSCOLSON WB.1981; PHYS. REV. A; ISSN 0556-2791; USA; DA. 1981; VOL. 241; NO 1; PP. 639-641; BIBL. 11 REF.Article

INTERACTIONS NON LINEAIRES DES ONDES DANS LES CRISTAUX A CONSTANTE DIELECTRIQUE SCALAIREBELYJ VN; LOPASHIN FA; SERDYUKOV AN et al.1976; ZH. PRIKL. SPEKTROSK., BELORUS. S.S.R.; S.S.S.R.; DA. 1976; VOL. 24; NO 3; PP. 501-507; BIBL. 8 REF.Article

SATURATION OF RESONANT TWO-PHOTON TRANSITIONS IN THALLIUM VAPOR.WANG CC; DAVIS LI JR.1975; PHYS. REV. LETTERS; U.S.A.; DA. 1975; VOL. 35; NO 10; PP. 650-653; BIBL. DISSEM.Article

TENSORS IN CIRCULAR-CYLINDRICAL COORDINATES FOR THE DESCRIPTION OF HARMONIC GENERATION OF CIRCULARY POLARIZED LASER LIGHT. = TENSEURS EN COORDONNEES CYLINDRIQUES CIRCULAIRES POUR LA DESCRIPTION DE LA GENERATION D'HARMONIQUES DANS LA LUMIERE D'UN LASER A POLARISATION CIRCULAIREOZGO Z; KIELICH S.1976; PHYSICA B+C; PAYS-BAS; DA. 1976; VOL. 81; NO 1; PP. 151-157; BIBL. 14 REF.Article

ETUDE DES CARACTERISTIQUES SPECTRALES, ANGULAIRES, ET DE TEMPERATURE DES CRISTAUX NON LINEAIRES HIO3, LIIO3, CDA, DKDP, KDP, ADP, EN REGIME DE GENERATION DES HARMONIQUES DEUX ET QUATREANDREEV RB; VOLOSOV VD; KALINTSEV AG et al.1974; OPT. I SPEKTROSK.; S.S.S.R.; DA. 1974; VOL. 37; NO 2; PP. 294-299; BIBL. 9 REF.Article

FIFTH HARMONIC GENERATION MECHANISMS IN A TWO-SPECIES SYSTEMNEW GHC.1981; OPT. COMMUN.; ISSN 0030-4018; NLD; DA. 1981; VOL. 38; NO 3; PP. 189-192; BIBL. 7 REF.Article

THIRD HARMONIC GENERATION IN PHASE-MATCHED ALKALI METAL VAPORS.BLOOM DM; BEKKERS GW; YOUNG JF et al.1975; APPL. PHYS. LETTERS; U.S.A.; DA. 1975; VOL. 26; NO 12; PP. 687-689; BIBL. 8 REF.Article

PHASE-MATCHED THIRD-HARMONIC GENERATION IN DYE SOLUTIONS.DIELS JC; SCHAEFER FP.1974; APPL. PHYS.; GERM.; DA. 1974; VOL. 5; NO 3; PP. 197-202; BIBL. 14 REF.Article

Carbon aerogel plumes as an efficient medium for higher harmonic generation in the 40―90 nm rangeGANEEV, Rashid A; NAIK, Prasad A; CHAKERA, Juzer A et al.Journal of the Optical Society of America. B, Optical physics (Print). 2011, Vol 28, Num 3, pp 360-364, issn 0740-3224, 5 p.Article

A comparative study for an eighth harmonic cusptron tube operating in the π mode and 2π modeKUO, S. P; TIONG, K. K; MILLER, P. E et al.The Physics of fluids. 1988, Vol 31, Num 6, pp 1821-1823, issn 0031-9171Article

SYSTEMES HARMONIQUES ACTIFS, DE L'ORDRE SUPERIEUR AU DEUXIEME, SOUMIS A UNE ACTION EXTERIEUREBODUNOV VP.1975; RADIOTEKHNIKA; S.S.S.R.; DA. 1975; VOL. 30; NO 9; PP. 70-77; BIBL. 6 REF.Article

HARMONIC GENERATION AND FREQUENCY MIXING IN LASER-PRODUCED PLASMAS.PING LEE; GIOVANIELLI DV; GODWIN RP et al.1974; APPL. PHYS. LETTERS; U.S.A.; DA. 1974; VOL. 24; NO 9; PP. 406-408; BIBL. 8 REF.Article

SEMI-CLASSICAL THEORY OF TWO-PHOTON RESONANT THIRD-HARMONIC GENERATION.ELGIN JN; NEW GHC.1976; OPT. COMMUNIC.; NETHERL.; DA. 1976; VOL. 16; NO 2; PP. 242-246; BIBL. 17 REF.Article

THIRD-HARMONIC GENERATION OF ND: YAG LASER IN LITHIUM FORMATE MONOHYDRATE.KATO K.1976; OPT. QUANTUM ELECTRON.; G.B.; DA. 1976; VOL. 8; NO 3; PP. 261-262; BIBL. 7 REF.Article

MIXED METAL VAPOR PHASE MATCHING FOR THIRD-HARMONIC GENERATION.BLOOM DM; YOUNG JF; HARRIS SE et al.1975; APPL. PHYS. LETTERS; U.S.A.; DA. 1975; VOL. 27; NO 7; PP. 390-392; BIBL. 4 REF.Article

SECOND-ORDER CORRELATION TENSOR OF N-HARMONICALLY SCATTERED LIGHT INTENSITY.KIELICH S; KOZIEROWSKI M; TANAS R et al.1975; OPT. COMMUNIC.; NETHERL.; DA. 1975; VOL. 15; NO 1; PP. 131-134; BIBL. 18 REF.Article

INFRARED-PUMPED THIRD-HARMONIC AND SUM-FREQUENCY GENERATION IN DIATOMIC MOLECULES.SHE CY; BILLMAN KW.1975; APPL. PHYS. LETTERS; U.S.A.; DA. 1975; VOL. 27; NO 2; PP. 76-79; BIBL. 18 REF.Article

Observation of bifurcation to chaos in an all-optical Fabry-Perot resonatorHARRISON, R. G; FIRTH, W. J; AL-SAIDI, I. A et al.Physical review letters. 1984, Vol 53, Num 3, pp 258-261, issn 0031-9007Article

COMPARISON OF FIFTH AND THIRD HARMONIC CONVERSION IN HELIUMREINTJES J; SHE CY.1978; OPT. COMMUNIC.; NLD; DA. 1978; VOL. 27; NO 3; PP. 469-474; BIBL. 15 REF.Article

TWO-PHOTON RESONANT, OPTICAL THIRD-HARMONIC GENERATION IN CESIUM VAPOR.LEUNG KM; WARD JF; ORR BJ et al.1974; PHYS. REV., A; U.S.A.; DA. 1974; VOL. 9; NO 6; PP. 2440-2448; BIBL. 20 REF.Article

Real-time mass sensing by nanomechanical resonators in fluidGHATKESAR, Murali K; BARWICH, V; BRAUN, T et al.IEEE Sensors conference. 2004, isbn 0-7803-8692-2, 3Vol, vol 2, 1060-1063Conference Paper

SPHERICAL HARMONIC ANALYSIS IN THE PRESENCE OF HIGH HARMONICSALLDREDGE LR; KAWASAKI K.1981; J. GEOMAGN. GEOELECTR.; ISSN 0022-1392; JPN; DA. 1981; VOL. 33; NO 9; PP. 503-515; BIBL. 5 REF.Article

THEORIE DER OPTIMALEN FOKUSSIERUNG FUER DIE DIREKTE ERZEUGUNG HOEHERER OPTISCHER HARMONISCHER = THEORIE DE LA FOCALISATION OPTIMALE POUR L'OBTENTION DIRECTE D'HARMONIQUE X OPTIQUE D'ORDRE ELEVEFISCHER R; WIECZOREK LW.1978; ANN. PHYS.; DDR; DA. 1978; VOL. 35; NO 5; PP. 389-400; ABS. ENG; BIBL. 14 REF.Article

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