21.04.2014 Views

Quantum scattering - Chaos: Classical and Quantum

Quantum scattering - Chaos: Classical and Quantum

Quantum scattering - Chaos: Classical and Quantum

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Exercises<br />

35.1. Spurious orbits under the Krein-Friedel-Lloyd contruction.<br />

Draw examples for the three types of period<br />

orbits under the Krein-Friedel-Lloyd construction: (a)<br />

the genuine periodic orbits of the <strong>scattering</strong> region, (b)<br />

spurious periodic orbits which can be removed by the<br />

subtraction of the reference system, (c) spurious periodic<br />

orbits which cannot be removed by this subtraction.<br />

What is the role of the double limit η → 0, container size<br />

b → ∞?<br />

a<br />

R<br />

a<br />

35.2. The one-disk <strong>scattering</strong> wave function. Derive the<br />

one-disk <strong>scattering</strong> wave function.<br />

(Andreas Wirzba)<br />

35.3. <strong>Quantum</strong> two-disk <strong>scattering</strong>. Compute the quasiclassical<br />

spectral determinant<br />

⎛<br />

∏<br />

Z(ε) = ⎜⎝ 1 −<br />

p, j,l<br />

t p<br />

Λ j+2l<br />

p<br />

⎞<br />

⎟⎠<br />

j+1<br />

for the two disk problem. Use the geometry<br />

The full quantum mechanical version of this problem<br />

can be solved by finding the zeros in k for the determinant<br />

of the matrix<br />

M m,n = δ m,n + (−1)n<br />

2<br />

J m (ka)<br />

H n<br />

(1) (ka)<br />

(<br />

H<br />

(1)<br />

m−n(kR) + (−1) n H (1)<br />

m+n(k<br />

where J n is the nth Bessel function <strong>and</strong> H n<br />

(1) is the Hankel<br />

function of the first kind. Find the zeros of the determinant<br />

closest to the origin by solving det M(k) = 0.<br />

(Hints: note the structure M = I + A to approximate the<br />

determinant; or read <strong>Chaos</strong> 2, 79 (1992))<br />

35.4. Pinball topological index. Upgrade your pinball simulator<br />

so that it computes the topological index for each<br />

orbit it finds.<br />

References<br />

[35.1] W. Thirring, <strong>Quantum</strong> mechanics of atoms <strong>and</strong> molecules, A course in<br />

mathematical physics Vol. 3 (Springer, New York, 1979). (Springer, Wien<br />

1979).<br />

[35.2] A. Messiah, <strong>Quantum</strong> Mechanics, Vol. I (North-Holl<strong>and</strong>, Amsterdam,<br />

1961).<br />

[35.3] M.G. Krein, On the Trace Formula in Perturbation Theory, Mat. Sborn.<br />

(N.S.) 33, 597 (1953) ; Perturbation Determinants <strong>and</strong> Formula for Traces<br />

of Unitary <strong>and</strong> Self-adjoint Operators, Sov. Math.-Dokl. 3, 707 (1962).<br />

[35.4] M.Sh. Birman <strong>and</strong> M.G. Krein, On the Theory of Wave Operators <strong>and</strong><br />

Scattering Operators, Sov. Math.-Dokl. 3, 740 (1962); M.Sh. Birman <strong>and</strong><br />

D.R. Yafaev, St. Petersburg Math. J. 4, 833 (1993).<br />

[35.5] E. Beth <strong>and</strong> G.E. Uhlenbeck, Physica 4, 915 (1937).<br />

refsScatter - 11aug2005 <strong>Chaos</strong>Book.org version13, Dec 31 2009

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!