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Results 1 to 25 of 364

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ON THE H+F2->HF+F REACTION. AN AB INITIO POTENTIAL ENERGY SURFACEO'NEIL S; PEARSON PK; SCHAEFER HF III et al.1973; J. CHEM. PHYS.; U.S.A.; DA. 1973; VOL. 58; NO 3; PP. 1126-1131; BIBL. 37 REF.Serial Issue

PURE ROTATIONAL RAMAN SPECTRUM OF FLUORINE.EDWARDS HGM; GOOD EAM; LONG DA et al.1976; J. CHEM. SOC., FARADAY TRANS., 2; G.B.; DA. 1976; VOL. 72; NO 5; PP. 984-987; BIBL. 6 REF.Article

VIBRATIONAL RELAXATION OF FLUORINE BY A SHOCK TUBE SCHLIEREN METHOD.DIEBOLD GJ; SANTORO RJ; GOLDSMITH GJ et al.1974; J. CHEM. PHYS.; U.S.A.; DA. 1974; VOL. 60; NO 11; PP. 4170-4174; BIBL. 28 REF.Article

MONTE CARLO CALCULATIONS OF REACTIONS RATES AND ENERGY DISTRIBUTIONS AMONG REACTION PRODUCTS. III. H+F2->HF+F AND D+F2->DF+FWILKINS RL.1973; J. CHEM. PHYS.; U.S.A.; DA. 1973; VOL. 58; NO 6; PP. 2326-2332; BIBL. 18 REF.Serial Issue

IONIZATION POTENTIALS AND BOND LENGTHS FOR CO, N2, AND F2 USING THE SCF-XALPHA -SW METHOD: A STUDY OF THE EFFECT OF OVERLAPPING SPHERES.SALAHUB DR; MESSMER RP; JOHNSON KH et al.1976; MOLEC. PHYS.; G.B.; DA. 1976; VOL. 31; NO 2; PP. 529-534; BIBL. 27 REF.Article

THE STRUCTURE OF THE DIATOMIC MOLECULAR SOLIDS.ENGLISH CA; VENABLES JA.1974; PROC. R. SOC. LONDON, A; G.B.; DA. 1974; VOL. 340; NO 1620; PP. 57-80; BIBL. 39 REF.Article

ELASTIC SCATTERING OF ELECTRONS FROM F2.SCHNEIDER BI; HAY PJ.1976; J. PHYS. B; G.B.; DA. 1976; VOL. 9; NO 6; PP. L165-L167; BIBL. 5 REF.Article

EXACT QUANTUM MECHANICAL TRANSITION PROBABILITIES FOR THE COLLINEAR REACTION: H+F2(V=0)->HF (U' <OU= 11)+F.CONNOR JNL; JAKUBETZ W; MANZ J et al.1976; CHEM. PHYS. LETTERS; NETHERL.; DA. 1976; VOL. 39; NO 1; PP. 75-78; BIBL. 19 REF.Article

ONE-BODY GREEN'S FUNCTION FOR ATOMS AND MOLECULES: THEORY AND APPLICATION.CEDERBAUM LS.1975; J. PHYS. B; G.B.; DA. 1975; VOL. 8; NO 2; PP. 290-303; BIBL. 33 REF.Article

A QUASICLASSICAL TRAJECTORY STUDY OF THE H2+F2 REACTIONS.THOMPSON DL; MCLAUGHLIN DR.1975; J. CHEM. PHYS.; U.S.A.; DA. 1975; VOL. 62; NO 11; PP. 4284-4299; BIBL. 1 P.Article

MOLECULAR POLARIZABILITY ESTIMATES FOR VIBRATIONAL SPECTRALINTERPRETATION.JAO TC; BEEBE NHF; PERSON WB et al.1974; CHEM. PHYS. LETTERS; NETHERL.; DA. 1974; VOL. 26; NO 4; PP. 474-478; BIBL. 31 REF.Article

NON-EMPIRICAL VALENCE-ELECTRON MOLECULAR ORBITAL CALCULATIONS. THE NEVE METHOD FOR FIRST-ROW DIATOMIC MOLECULES.PEEL JB.1974; AUSTRAL. J. CHEM.; AUSTRAL.; DA. 1974; VOL. 27; NO 5; PP. 923-931; BIBL. 15 REF.Article

AB INITIO-RECHNUNGEN ZUM F2-MOLEKUEL = CALCULS AB INITIO SUR LA MOLECULE F2KASSECKERT E.1973; Z. NATURFORSCH., A; DTSCH.; DA. 1973; VOL. 28; NO 5; PP. 704-708; ABS. ANGL.; BIBL. 21 REF.Serial Issue

PRECISION DU CALCUL DES COURBES DE POTENTIEL ET DES CONSTANTES SPECTROSCOPIQUES DANS LA METHODE SCF-XALPHA DES ONDES DIFFUSEESGEGUZIN II; TOPOL IA.1980; ZH. STRUKT. KHIM.; SUN; DA. 1980; VOL. 21; NO 1; PP. 155-156; BIBL. 5 REF.Article

SADDLE POINT GEOMETRY AND BARRIER HEIGHT FOR H+F2->HF+F.BENDER CF; BAUSCHLICHER CW JR; SCHAEFER HF III et al.1974; J. CHEM. PHYS.; U.S.A.; DA. 1974; VOL. 60; NO 9; PP. 3707-3708; BIBL. 12 REF.Article

ETUDE DE LA RELAXATION VIBRATIONNELLE DES MOLECULES CO2(00O1) SUR DES MOLECULES DE F2, HF, CCL4, C2H2, NH3, PH3, CH3OHAGROSKIN V YA; VASIL'EV GK; KIR'YANOV VI et al.1974; KHIM. VYS. ENERG.; S.S.S.R.; DA. 1974; VOL. 8; NO 3; PP. 283-284; BIBL. 8 REF.Article

Selective removal of F2 impurity from NF3/Xe/Ne, XeF laser mixturesMANDL, A; SLATER, R; APPEL, C. H et al.SPIE milestone series. 2000, Vol 159, pp 332-336, issn 1050-0529Article

Novel F2 detector for the gas monitor of an excimer laserHAKUTA, K; MUKAI, N; MIKI, S et al.Review of scientific instruments. 1986, Vol 57, Num 10, pp 2529-2531, issn 0034-6748Article

TOPOGRAPHY OF POTENTIAL ENERGY SURFACES: DIM SURFACE FOR H+F2DUGGAN JJ; GRICE R.1983; JOURNAL OF CHEMICAL PHYSICS; ISSN 0021-9606; USA; DA. 1983; VOL. 78; NO 6; PART. 2; PP. 3842-3849; BIBL. 22 REF.Article

BASIS SET EXPANSIONS OF RELATIVISTIC MOLECULAR WAVE EQUATIONSSCHWARZ WHE; WALLMEIER H.1982; MOL. PHYS.; ISSN 0026-8976; GBR; DA. 1982; VOL. 46; NO 5; PP. 1045-1061; BIBL. 25 REF.Article

THEORETICAL STUDY OF THE F2 MOLECULE USING THE VARIATIONAL CELLULAR METHODLIMA MAP; LEITE JR; FAZZIO A et al.1981; J. PHYS. B; ISSN 0022-3700; GBR; DA. 1981; VOL. 14; NO 16; PP. L533-L535; BIBL. 14 REF.Article

FOURTH-ORDER DIAGRAMMATIC MB-RSPT CALCULATIONS OF THE CORRELATION ENERGY: N2, CO, F2 AND THE REACTION ENERGY OF THE PROCESS 1/2F2+1/2H2=HFKELLO V; URBAN M.1980; INT. J. QUANTUM CHEM.; ISSN 0020-7608; USA; DA. 1980; VOL. 18; NO 6; PP. 1431-1448; ABS. FRE/GER; BIBL. 59 REF.Article

CHARGE DISTRIBUTION ANALYSIS IN TERMS OF BERLIN'S BINDING AND ANTIBINDING REGIONS FOR LI2 AND F2.ZUVIA M; LUDENA EV.1978; INTERNATION. J. QUANTUM CHEM.; USA; DA. 1978; VOL. 14; NO 1; PP. 1-11; BIBL. 52 REF.Article

DETAILED PRODUCT ENERGY DISTRIBUTIONS FOR EXOTHERMIC TRIATOMIC EXCHANGE REACTIONS FROM A STATISTICAL DYNAMIC MODELVENZL G; FISCHER SF.1978; CHEM. PHYS.; NLD; DA. 1978; VOL. 33; NO 2; PP. 305-312; BIBL. 29 REF.Article

SELF-CRYSTALLIZING MOLECULAR MODELS. V. MOLECULAR CHARGE DENSITY CONTOURS.KIHARA T; SAKAI K.1978; ACTA CRYSTALLOGR.; DANEM.; DA. 1978; VOL. 34; NO 2; PP. 326-329; BIBL. 8 REF.Article

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