By Stuart A. Rice, Aaron R. Dinner
Advances in Chemical Physics is the single sequence of volumes on hand that explores the innovative of analysis in chemical physics.
- This is the single sequence of volumes on hand that offers the leading edge of analysis in chemical physics.
- Includes contributions from specialists during this box of research.
- Contains a consultant cross-section of study that questions proven pondering on chemical solutions.
- Structured with an article framework that makes the ebook a good complement to a complicated graduate category in actual chemistry or chemical physics.
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Additional resources for Advances in Chemical Physics, Advances in Chemical Physics (Volume 156)
T. Genossar and M. Porat, IEEE 22, 449 (1992). 34. S. Orr, IEEE Transactions on Signal Processing 41, 122 (1993). 35. S. Qian and D. Chen, IEEE Trans. Signal Proc. 41, 2429 (1993). 36. J. A. Rice, J. Chem. Phys. 83, 5013 (1985). 37. R. A. Rice, P. Gaspard, S. J. Tannor, Chem. Phys. 139, 201 (1989). 38. P. A. Dahleh, and H. Rabitz, Phys. Rev. A 37, 4950 (1988). 39. S. Judson and H. Rabitz, Phys. Rev. Lett. 68, 1500 (1992). 40. M. E. S. R. Wullert, Opt. Lett. 15, 326 (1990). 41. A. Assion, T. Baumert, M.
92, 2087 (1988) and references therein. ENTROPY-DRIVEN PHASE TRANSITIONS IN COLLOIDS: FROM SPHERES TO ANISOTROPIC PARTICLES MARJOLEIN DIJKSTRA Soft Condensed Matter group, Debye Institute for Nanomaterials Science, Utrecht University, Princetonplein 5, 3584 CC Utrecht, The Netherlands CONTENTS I. Introduction II. Predicting Candidate Crystal Structures III. Free-Energy Calculations A. Fluid Phase B. Crystal Phase C. Plastic Crystal Phases D. Orientationally Ordered Crystal Phases IV. Bulk Phase Diagram and Kinetic Pathways A.
Right: Strong field manipulation of electronic motion in a diatomic molecule. For a color version of this figure, see the color plate section. As a preliminary illustration of the application of the pvb method to timedependent electronic dynamics, we solve Eq. (26) for the electronic wavepacket of a 1D atom in the combined field of near-infrared (NIR) and extreme ultraviolet (XUV) laser pulses. The Hamiltonian of this system is given as H(t) = H0 + V(t), (27) where H0 is the field-free Hamiltonian with a soft-core Coulomb potential: H0 = p2 Qe2 , − √ 2???? 4???????? x2 + a2 0 (28) and V(t) is the laser–electron coupling in the velocity gauge, e V(t) = − [ANIR (t) + AXUV (t)]p, ???? (29) where ANIR (t) and AXUV (t) are the vector potentials of the NIR and XUV laser pulses, respectively.