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Molecular physics

Rotational syimnetry is used here as an example to explain the motivation for using syimnetry in molecular physics it will be discussed in more detail in section AT4.3.2. [Pg.137]

Dalgarno A and Lepp S 1996 Applications of atomic and molecular physics to astrophysics Atomic, Moiecuiar, and Opticai Physics Handbook ed G W F Drake (Woodbury, NY AlP)... [Pg.828]

Figure Bl.7.12. A schematic diagram of a typical selected-ion flow (SIFT) apparatus. (Smith D and Adams N G 1988 The selected ion flow tube (SIFT) studies of ion-neutral reactions Advances in Atomic and Molecular Physics vol 24, ed D Bates and B Bederson p 4. Copyright Academic Press, Inc. Reproduced with pennission.)... Figure Bl.7.12. A schematic diagram of a typical selected-ion flow (SIFT) apparatus. (Smith D and Adams N G 1988 The selected ion flow tube (SIFT) studies of ion-neutral reactions Advances in Atomic and Molecular Physics vol 24, ed D Bates and B Bederson p 4. Copyright Academic Press, Inc. Reproduced with pennission.)...
McDaniel E W and Mansky E J 1994 Guide to bibliographies, books, reviews and compendia of data on atomic collisions Advances in Atomic and Molecular Physics vol 33, ed B Bederson and FI Walther p 389... [Pg.2058]

Bates D R and Estermann I (eds) 1965 Advances in Atomic and Molecular Physics vol 1... [Pg.2058]

Luckliurst G R and Gray G W (eds) 1979 The Molecular Physics of Liquid Crystals (London Academic) de Gennes P G and Prost J 1993 The Physics of Liquid Crystals 2nd edn (Oxford Oxford University Press)... [Pg.2572]

In molecular physics, the topological aspect has met its analogue in the Jahn-Teller effect [47,157] and, indeed, in any situation where a degeneracy of electronic states is encountered. The phase change was discussed from various viewpoints in [144,158-161] and [163]. [Pg.105]

The adiabatic picture developed above, based on the BO approximation, is basic to our understanding of much of chemistry and molecular physics. For example, in spectroscopy the adiabatic picture is one of well-defined spectral bands, one for each electronic state. The smicture of each band is then due to the shape of the molecule and the nuclear motions allowed by the potential surface. This is in general what is seen in absorption and photoelectron spectroscopy. There are, however, occasions when the picture breaks down, and non-adiabatic effects must be included to give a faithful description of a molecular system [160-163]. [Pg.276]

JCAMP. jdx,. dx,. cs Joint Committee on Atomic and Molecular Physical Data structure and spectroscopic format nmm.jcamp. org/ 56... [Pg.46]

Distributed multipole models for Nj and HF. (Figure adapted from Stone A j and M Alderton 19S5. ibuted Multipole Analysis Methods and Applications. Molecular Physics 56 3 047-1064.)... [Pg.214]

J A, R A Fisher and R O Watts 1971. Liquid Argon Monte Carlo and Molecular Dynamics Iculations. Molecular Physics 21 657-673. [Pg.266]

Rodger P M, A J Stone and D J Tildesley 1988. The Intermolecular Potential of Chlorine. A Three Phase Study. Molecular Physics 63 173-188. [Pg.269]

Friedman H L 1975. Image Approximation to the Reaction Field. Molecular Physics 29 1533-1543. [Pg.365]

Gunsteren W F and H J C Berendsen 1982. Algorithms for Brownian Dynamics. Molecular Physics 45 637-547. [Pg.424]

Gunsteren W F, H J C Berendsen and J A C Rullmann 1981. Stochastic Dynamics for Molecules with Constraints. Brownian Dynamics of n-Alkanes. Molecular Physics 44 69-95. [Pg.424]

The insertion of a three-unit molecule onto the lattice shown, starting at point S, can he achieved in only ay (see text). (Figure adapted from Siepmann J11990. A Method for the Direct Calculation of Chemical tialsfor Dense Chain Systems. Molecular Physics 70 1145-1158.)... [Pg.460]

Pablo J J, M Laso, JI Siepmann and U W Suter 1993. Continuum-Configurational Bias Monte Carlo Simulations of Long-chain Alkanes. Molecular Physics 80 55-63. [Pg.470]

Panagiotopoulos A Z 1987. Direct Determination of Phase Coexistence Properties of Fluids by Mon Carlo Simulation in a New Ensemble. Molecular Physics 61 813-826. [Pg.471]

Siepmann J I 1990. A Method for the Direct Calculation of Chemical Potentials for Dense Cha Systems. Molecular Physics 70 1145-1158. [Pg.471]

Siepmann J I and D Frenkel 1992. Configurational Bias Monte Carlo A New Sampling Scheme f Flexible Chains. Molecular Physics 75 59-70. [Pg.471]

Bernier D K and P A Madden 1990. Molecular Dynamics without Effective Potentials via the Car ParrineUo Approach. Molecular Physics 70 921-966. [Pg.653]

A computer file of about 19,000 peak wavenumbers and intensities, along with search software, is distributed by the Infrared Data Committee of Japan (IRDC). Donated spectra, which are evaluated by the Coblentz Society in coUaboration with the Joint Committee on Atomic and Molecular Physical Data (JCAMP), are digitized and made avaUable (64). Almost 25,000 ir spectra are avaUable on the SDBS system developed by the NCLl as described. A project was initiated at the University of California, Riverside, in 1986 for the constmction of a database of digitized ftir spectra. The team involved also developed algorithms for spectra evaluation (75). Other sources of spectral Hbraries include Sprouse Scientific, Aston Scientific, and the American Society for Testing and Materials (ASTM). [Pg.121]

Data Analysis. The computerization of spectrometers and the concomitant digitization of spectra have caused an explosive increase in the use of advanced spectmm analysis techniques. Data analysis in infrared spectrometry is a very active research area and software producers are constantly releasing more sophisticated algorithms. Each instmment maker has adopted an independent format for spectmm files, which has created difficulties in transferring data. The Joint Committee on Atomic and Molecular Physical Data has developed a universal format for infrared spectmm files called JCAMP-DX (52). Most instmment makers incorporate in thek software a routine for translating thek spectmm files to JCAMP-DX format. [Pg.200]

G. R. Luckhurst and G. W. Gray, eds.. The Molecular Physics of Eiquid Cystals, Academic Press, Inc., New York, 1979. [Pg.205]

Kahn, F. The Molecular Physics of Liquid-Crystal Devices. Physics Today (May 1982), pp, 66-74... [Pg.161]


See other pages where Molecular physics is mentioned: [Pg.158]    [Pg.175]    [Pg.176]    [Pg.177]    [Pg.33]    [Pg.40]    [Pg.322]    [Pg.636]    [Pg.636]    [Pg.636]    [Pg.676]    [Pg.713]    [Pg.733]    [Pg.441]    [Pg.180]    [Pg.266]    [Pg.424]    [Pg.424]    [Pg.654]    [Pg.47]    [Pg.486]   
See also in sourсe #XX -- [ Pg.245 ]

See also in sourсe #XX -- [ Pg.221 , Pg.222 , Pg.223 , Pg.224 , Pg.225 ]




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A physical basis for the VSEPR model of molecular geometry

From the Standard Model of Physics to Molecular Parity Violation

Molecular dynamics physical simulation

Molecular mass distribution physical property

Molecular mechanics, physical

Molecular modelling physical constant values

Molecular orbital physical significance

Molecular orbitals physical significance

Molecular physical parameters

Molecular physically entrapped (adsorbed

Molecular recognition physical basis

Molecular sieves physical properties

Molecular structure approach chemistry physics

Molecular structure physical properties

Molecular structures structural physical effects

Nuclear physics, molecular spectroscopy

PHYSICAL FORCES AND MOLECULAR INTERACTIONS

Pertinent Topics from Atomic, Molecular, and Optical Physics

Physical Description of Molecular Transport Junctions

Physical Significance of Molecular Connectivity Indexes

Physical and molecular interactions

Physical hazards, molecular design

Physical properties Molecular configuration

Physical properties molecular dynamics

Physical properties molecular structure and

Physical properties, estimation methods molecular simulations

Physical states kinetic-molecular view

Simple molecular compounds, physical

Simple molecular compounds, physical properties

Singlet Molecular Oxygen, Physical Quenchers of (Bellus)

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