Dynamics, Volume 3 (Handbook of Surface Science) by Eckart Hasselbrink, Bengt I. Lundqvist

By Eckart Hasselbrink, Bengt I. Lundqvist

This quantity of the guide of floor technological know-how covers all elements of the dynamics of floor tactics. dozen global major specialists during this box tackle the themes of power trade in gasoline atoms, floor collisions, the foundations governing dissociative adsorption on surfaces, the formation of nanostructures on surfaces by means of self-assembly, and the examine of floor phenomena utilizing ultra-fast lasers. The chapters are written for either newbies to the sector in addition to researchers. . Covers all elements of the dynamics of floor procedures . presents figuring out of this detailed box using a mess of exact experiments and complicated microscopic concept that enables quantum-level comparisons . offers the innovations and instruments proper past floor technology for catalysis, nanotechnology, biology, drugs, and fabrics

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By Eckart Hasselbrink, Bengt I. Lundqvist

This quantity of the guide of floor technological know-how covers all elements of the dynamics of floor tactics. dozen global major specialists during this box tackle the themes of power trade in gasoline atoms, floor collisions, the foundations governing dissociative adsorption on surfaces, the formation of nanostructures on surfaces by means of self-assembly, and the examine of floor phenomena utilizing ultra-fast lasers. The chapters are written for either newbies to the sector in addition to researchers. . Covers all elements of the dynamics of floor procedures . presents figuring out of this detailed box using a mess of exact experiments and complicated microscopic concept that enables quantum-level comparisons . offers the innovations and instruments proper past floor technology for catalysis, nanotechnology, biology, drugs, and fabrics

Show description

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This transition is referred to as a diabatic transition from state 1 to 2. Note that the center-of-mass trajectory branches near Rc , some being reflected without undergoing the 1 → 2 transition. Upon reflection at z = RT , the incident particle, now in state 2, hits the crossing point from the left where another branching is experienced. The time interval between passes at the crossing point is approximately Tv = 2π/ω0 where ω0 is the vibrational frequency associated with the bound state well.

2002). , 1996; Saalfrank, 2006). In particular, laser-induced-hot-electron-desorption studies have proliferated both because of their intrinsic interest and importance in surface dynamics and also because the internal electronic and TVR quantum states of the product (desorbate) can in principle be measured (Dai and Ho, 1995; Saalfrank, 2006; Frischkorn and Wolf, 2006). Still one must heed the cautionary warning of Wodtke et al. (2004) that the [frictional] theory rests on a ‘weak coupling approximation’.

Phys. Rev. A 74, 062902. , 1998. J. Chem. Phys. 109, 7702. , 1988. Adv. Chem. Phys. 70, 441. , 2007. Introduction to Quantum Mechanics: A Time-Dependent Perspective. University Science Books, Sausolito. , 2002. Phys. Rev. Lett. 88, 166802. , 2003. J. Chem. Phys. 119, 4539. , 1971. J. Chem. Phys. 76, 2412. , 1990. J. Chem. Phys. 93, 1061. , 2000a. Annu. Rev. Phys. Chem. 51, 153. , 2000b. Theor. Chem. Acc. 103, 173. , 2004. Surf. Sci. 566, 1. , 1983. Phys. Scripta T6, 27. , 1946. Phys. Rev. 70, 606.

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