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Collective Response of Atom Clusters and Nuclei: Role of Chaos Trento April 2010 Mahir S. Hussein University of Sao Paulo
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Contents Metal Clusters Nuclei Giant dipole resonances Exit doorway model Damping width and Chaos Random matrix theory
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Metal Clusters Aggregate of N atoms Excite plasmon-type Mie resonances Electrons oscillate out of phase with respect to ions. Probes: Laser, electrons, other clusters. Multi-plasmon resonances
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PRL, 68, 3916 (1992). PRL,70, 2036 (1993).
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Energy and width of cluster plasmon resonances PRL,70, 2036 (1993).
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Multiphonon excitation in Na clusters PRL, 80, 1194 (1998). A perfect harmonic oscillator : n=4
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Plasmon excitation energy vs. size of Xe and Ar clusters Phys. Rev. Lett. 67, 3290 (1991).
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Plasmon excitation energy and width vs. size of Hg clusters Phys. Rev. Lett. 69, 3212 (1992).
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Nuclei Aggregate of N neutrons and Z protons Collective excitation of giant dipole and quadrupole resonances Probes: photons, electrons, other nuclei Neutrons oscillate against protons (dipole) Collective state is damped to chaotic configuration.
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J. G. Woodworth et al., Phys. Rev. C, 19, 1667 (1979); G. J. O’keefe et al., Nucl. Phys. A 649, 239 (1987).
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R. Schmidt et al. Phys. Rev. Lett. 70, 1767 (1993) Single- and double-phonon excitation in Xe nucleus.
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Rev.Mod.Phys., 47, 713 (1975). Shape is Lorentzian (spherical).
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Rev. Mod. Phys., 55, 287 (1983) Widths of giant dipole and quadrupole resonances in nuclei
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Rev.Mod.Phys., 47, 713 (1975). Excitation energy of giant dipole resonances in nuclei
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Pygmy giant resonances!
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Phys. Rev. Lett., 95, 132501 (2005).
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Split dipole state: Schrődinger cat? Z. Phys. A 355. 165 (1996)
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Exit doorway model Consider the many-body Hamiltonian with time-dependent interaction Intrinsic Hamiltonian of the system External perturbation System responds to action of and is excited to some collective state (not an eigenstate of )
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Calculation of excitation probabilities Write Use Get (taking ) Initial conditions Excitation probabilities
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Consider : dipole operator : electric field of external probe.
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Excitation of collective state with finite lifetime can be treated using the exit-doorway (ED) model Expanding
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Since, We get Model Uniform spectrum get
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Spreading or damping width, measures the degree of mixing of the collective state with the background (chaotic) states.
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Take does not mix excited states With ED hypothesis, get Write
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Get three coupled differential equations With Excitation probabilities
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And cross-section
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Ann. Phys. (New York), 284, 178 (2000). Calculation of excitation cross-section of a damped plasmon in sodium clusters
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Role of chaos Response function, spreading width Dynamical enhancement of multiphonon excitations.
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Dynamical enhancement of multiphonon excitation Owing to, to go from ground state to 2 phonon state (via 1 phonon) one may, if collision time, excite a single phonon on top of background which gives rise to
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Excitation probability Harmonic (Poissonian) Dynamical (Brink-Axel) Ann. Phys.(New York), 276, 111 (1999). Nucl. Phys. A 731, 163 (2004).
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Ann. Phys. (NY) 276,111 (1999); Nucl. Phys. A 690, 382 (2001). Coupling between collective and chaotic states.
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Evolution of density matrix with damping and dynamical chaos enhancement
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Phys. Rev. C, 60, 014604 (1999). Dynamical chaos enhancement of cross-section
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Ann. Phys.(New York), 276, 111 (1999). Nucl. Phys. A 731, 163 (2004). Dynamical enhancement could be as large as 80%.
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Conclusions Collective response of finite many-body systems is affected by the degree of chaoticity of the internal degrees of freedom. The system acquires a damping width: Damped harmonic oscillator Chaos leads to an enhanced excitation owing to the damping.
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Thanks to my collaborators: Brazil: C. A. Bertulani, L. F. Canto, B. V. Carlson, R. Donangelo, J. X. de Carvalho, M. P. Pato, A. F. R. de Toledo Piza Germany: T. Aumann, H. Emling USA: H. Feshbach, A. K. Kerman, V. Kharchenko, E. Timermmans
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Thank you!
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