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Quantum Mechanical Properties of Nuclei: Lecture 4 - Nuclear Sizes, Shapes, and Moments - , Study notes of Chemistry

A portion of a university lecture on quantum mechanical properties of nuclei. It covers topics such as nuclear sizes and shapes, nuclear spin and parity, and electric and magnetic moments. The document also includes formulas and values for various nuclear properties.

Typology: Study notes

Pre 2010

Uploaded on 08/30/2009

koofers-user-zgo
koofers-user-zgo 🇺🇸

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Download Quantum Mechanical Properties of Nuclei: Lecture 4 - Nuclear Sizes, Shapes, and Moments - and more Study notes Chemistry in PDF only on Docsity! Quantum Mechanical Properties of Nuclei Lecture 4 Sizes and Shapes of Nuclei • How big are nuclei? • 1-10 fm • sharp cutoff model, R=r0A1/3 fm r0=1.07 r0=1.2 r0=1.44 The “Halo Nuclei” 208 Ph jj Nuclear Spin and Parity • Nuclei have an intrinsic “spin” angular momentum, akin to the spin of the electron. • For odd A nuclei, the spin J is half integer. (1/2,3/2, etc.) For even A nuclei, the spin J is integer. (0,1,2,etc.). The magnitude of the spin is multiple of hbar. Parity (the symmetry properties of the nuclear wave function) ! "(r,s) = +"(#r,#s) $ = + "(r,s) = #"(#r,#s) $ = # For a central potential, V=V(r) ! " = (#1)l A=4 2=0 a2 a=3 Sphere Quadrupoles Octupoles Hexadecapoles OBLATE y ~ ‘ J - V9 Vv PROLATE 2 -@- Neutrons Octupoles K isomers spherical Shape coexistence, shape transitions spherical —> strongly deformed Protons Electric and magnetic moments • Electric moments are measures of the distribution of electric charge. Magnetic moments measure the distribution of electric currents. Classical Analogy ! magnetic dipole moment = iA µ = iA = ev 2"r # $ % & ' ( "r2( ) = evr 2 l = mvr µ = evr 2 • m m = el 2m gyromagnetic ratio = ) = µ l = e 2m Electric Quadrupole Moments ! charge at point = "d# = " r2drsin$d$d%( ) potential at P = d& d& = "d# ' = "d# D 2 + r2 ( 2Drcos$( ) 1/ 2 P2 cos$( ) = 3 2 cos2$ ( 1 2 P1 cos$( ) = cos$ d& = "d# D 1+ r D P1 cos$( ) + r D ) * + , - . 2 P2 cos$( ) +L / 0 1 2 3 4 V = 1 D "d# volume 5 / 0 1 2 3 4 + 1 D 2 "rcos$d# volume 5 / 0 1 2 3 4 + 1 D 3 "r2 3 2 cos2$ ( 1 2 ) * + , - . d# +L volume 5 / 0 1 2 3 4 ! Q = r 2"(r) 3 2 cos 2# $ 1 2 % & ' ( ) * r 2 drsin#d#d+,,, ! R 2 = 1 2 a 2 + c 2( ) = r0A1/ 3 Q = 2 5 Ze a 2 " c 2( ) oe \f J \ | a “—y | | 7 04} — 814 4050 82, 1 OS; = 06, -o71 4 ~0a} 09] 4 o 10 2 30 4 50 60 70 80 90 100 110 120 190 140 150 Zon
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