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Photonic crystals in biology

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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

Diamagnetic Susceptibility <strong>in</strong> Quantum Well<br />

Hasan Akbas 1 * and 1<br />

1 Department of Physics, Trakya University, Edirne 22030,Turkey<br />

Abstract-The d iamagnetic susceptibility of a hydrogenic donor placed <strong>in</strong> Si,Ge,GaAs quantum wells with <strong>in</strong>f<strong>in</strong>ite conf<strong>in</strong>ement<br />

potential has been <strong>in</strong>vestigated as function of the well sizes us<strong>in</strong>g anisotropic effective masses. For the Ge the diamagnetic<br />

susceptibility is found to be<br />

The diamagnetic plays an important roles <strong>in</strong> optical and<br />

transport phenomena of semiconductor nanostructers. The<br />

optical properties of quantum wells are of significant<br />

importance <strong>in</strong> possible device applications. A few physical<br />

quantities that depend on the donor wave function directly<br />

are diamagnetic susceptibility, polarizab ility and oscillator<br />

strengths.<br />

In present work, we study a hydrogenic impurity with<strong>in</strong><br />

an <strong>in</strong>f<strong>in</strong>ite quantum well with anisitropic effective mass of<br />

electron. Therefore, the motion of the electron <strong>in</strong> the<br />

longitud<strong>in</strong>al directions is different from that <strong>in</strong> the<br />

transverse direction.<br />

The aim of this work is to obta<strong>in</strong> the diamagnetic<br />

susceptibility of the hydrogenic donor and to understand<br />

how the transverse and longitud<strong>in</strong>al parts of susceptibility<br />

reflect charge <strong>in</strong> the quantum well size. The calculation of<br />

the donor wawe function are performed us<strong>in</strong>g effective<br />

mass approximation with<strong>in</strong> a variational approach.<br />

The Hamiltonian of the hydrogenic donor impurity,<br />

<strong>in</strong> the cyl<strong>in</strong>drical coord<strong>in</strong>ate system is<br />

(a.u.)<br />

0<br />

-0.04<br />

-0.08<br />

-0.12<br />

-0.16<br />

-0.2<br />

dia<br />

<br />

z<br />

0 200 400 600 800 1000<br />

L(A o )<br />

Figure 1. Variation of the transverse, longitudial,<br />

and total susceptibility as function of the well width<br />

for Ge.<br />

where and denote transverse and longitud<strong>in</strong>al<br />

effective masses of electron , respectively , and is a<br />

static dielectric constant. The conf<strong>in</strong><strong>in</strong>g potential is given<br />

by<br />

The anisotropy destroys spherical symmetry of the<br />

hydrogenic donor. We therefore choose two-parametric<br />

trial wave function of the ground state.<br />

<br />

where and are the variational parameters. The ground<br />

state donor b<strong>in</strong>d<strong>in</strong>g energy is given by<br />

The diamagnetic susceptibility of the hydrogenic donor<br />

is given by<br />

=<br />

We calculate a b<strong>in</strong>d<strong>in</strong>g energy of the hydrogenic donor<br />

with various effective mass anisotropy parameters;<br />

, GaAs , Si and<br />

Ge . Our results of the b<strong>in</strong>d<strong>in</strong>g energy agrees<br />

with results <strong>in</strong> .<br />

The variation of for and<br />

Ge is given <strong>in</strong> Fig 1.<br />

In case of small , Ge<br />

, total susceptibility is<br />

found to be<br />

Corrrespond<strong>in</strong>g author: 0Thasan22ak@yahoo.com<br />

[1] P.Andreev, T.V.Pavlova, PhysicaE 40, 1551,2008,<br />

Hydrogenic impurity states <strong>in</strong> semiconduct<strong>in</strong>g nanostructers with<br />

anisotropic effective mass.<br />

[2] <br />

Microstructures 46 ,817,2009 ,The diamagnetic susceptibilities of<br />

donors <strong>in</strong> quantum wells anisotropic effective mass.<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 313

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