By International Symposium on Nuclear Structure Physics, Peter Von Brentano

Nuclear constitution physics is present process a big revival, choked with actions and pleasure. at the experimental part, this can be being made attainable by way of advances in detector expertise and accelerator functions that provide entry to info and nuclei (especially unique nuclei faraway from balance) by no means prior to available. at the theoretical aspect, new suggestions, rules and computational strategies are advancing our figuring out of powerful interactions, nucleonic correlations, and symmetries of constitution. This quantity covers a wide diversity of subject matters on nuclear constitution, together with: collective excitations; proton-neutron excitation modes; section transitions; signatures of constitution; isospin; constitution at either excessive- and low-angular momenta; fresh advancements in nuclear thought; the monstrous new realm of unique nuclei faraway from the valley of balance; and the most recent technological advances of detectors and amenities for you to lead this department of physics into the longer term.

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Extra info for International Symposium on Nuclear Structure Physics: Celebrating the Career of Peter Von Brentano : University of Gottingen, Germany 5-8 March 2001

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3 E2 Polarization Charge of Bound Particles in Drip Line Nuclei The features unique in drip line nuclei, which are relevant to polarization charge, are ; (i) loosely-bound nucleons cannot polarize the core ; (ii) "large" value of (N-Z)/A (or small value of Z/A) in neutron drip line nuclei can drastically change the ratio of polarization charge coming from the coupling with IS GQR and that with IV GQR. 5. 33 for both ! 4 Oi6 and |gCa 4 0 . 1) , , 8x B(EX; 0 -» A) < j a | kx(r) ^PO1JA,T*O-3(2A+1) i1> (hux) 3 - (AE21)2 (4) where the form factor of shape oscillations k\(r) is expressed by JR ^ or r ^ for IS modes, the nuclear radius by R, the vibration energy by hwx, and the energy difference of one-particle orbitals J2 and ji by AE2i=(E2—Ei).

Rev. C 60, 021302 (1999). 7. R. Bijker and A. Frank, Phys. Rev. C 62, 14303 (2000). 8. D. Mulhall, A. Volya, and V. Zelevinsky, nucl-th/0005014. 9. Lev Kaplan, Thomas Papenbrock, and Calvin W. Johnson, nuclth/0007013. 10. D. Kusnezov, nucl-th/0009076. This page is intentionally left blank 31 RENORMALIZATION OP ONE-PARTICLE M O M E N T S D U E TO CORE POLARIZATION - D R I P LINE NUCLEI V S . SE of Lund, Taking an example of static electric quadrupole polarization charge, which conies from the coupling to giant quadrupole resonances (GQR), the renormalization of one-particle moments in drip line nuclei is discussed, in comparison with /9-stable nuclei.

From Table 1 it is observed that the static E2 polarization charge for neutrons approaches to zero for orbitals with £=0 and 1, as the binding energies decrease to zero. Next, we examine at which one-particle eigen energy the strong dependence of e ^ ( i ? 2 , AE = 0) on £ values starts to appear. 0 H . ' \ ! 0 L. 0 Figure 1: Expectation values of (6), to which the static E2 polarization charge is proportional, as a function of ( 1 + ( E „ / / U 0 ) ) . For U 0 = 5 0 MeV ( l + ( E n / / U 0 ) ) = 0 .

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