Physics
Scientific paper
Jun 2009
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2009mss..confemi08l&link_type=abstract
"International Symposium On Molecular Spectroscopy, 64th Meeting, Held 22-26 June, 2009 at Ohio State University. http://molspec
Physics
Electronic
Scientific paper
We have shown that one and two-parameter analytical mapping functions such as
r(y;bar{r}, α)=bar{r}[1 + {1}/{α} tan(π y/2)] and r(y;bar{r})=bar{r} [ {1+ y}/{1-y} ] transform the conventional radial Schrödinger equation into equivalent alternate forms
{d^2φ(y)}/{dy^2} = [{π^2}/{4}+({2μ}/ {hbar^2} ) g^2(y) [E - U(r(y))]]φ(y) and {d^2φ(y)}/{dy^2} = ({2μ}/{hbar^2}) g^2(y)[E - U(r(y)) ]φ(y)
respectively, in which g(y)=dr(y)/dy . Such transformed equations are defined on the finite domain
yin [-1,1], and they may be solved routinely using standard numerical methods at all energies up to and including the potential asymptote. At the energy of the potential asymptote, the s-wave scattering length a_s can be expressed in terms of the logarithmic derivative of the wave function φ(y) at the right-hand boundary point:
a_s = bar{r}[{2}/ {πα} {1}/ {φ(y)} {dφ(y)}/ {dy}+1]_{y=1} and a_s = bar{r}[ 2 {1}/{φ(y)} {dφ(y)}/{dy} -1]_{y=1}
The required logarithmic derivative of φ(y) can be obtained efficiently by direct outward integration of the differential equation all the way to the end point y=1, which corresponds to the limit rto infty. This zero-energy wavefunction may also be combined with wavefunctions for ordinary bound states generated in the same manner^a to calculate photoassociation absorption matrix elements using any appropriately modified Franck-Condon computer program.
VVM is grateful to INTAS grant 06-1000014-5964 for support.
V.V. Meshkov, A.V. Stolyarov, and R.J. Le Roy, Phys. Rev. A 78, 052510 (2008)
Le Roy Robert J.
Meshkov Vladimir V.
Stolyarov Andrej V.
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