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A Newtonian approach to extraordinarily strong negative refraction

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Journal Club – 2012.09.14<br />

A <<strong>strong</strong>>New<<strong>strong</strong>>to</<strong>strong</strong>>nian</<strong>strong</strong>> <<strong>strong</strong>>approach</<strong>strong</strong>> <<strong>strong</strong>>to</<strong>strong</strong>> <<strong>strong</strong>>extraordinarily</<strong>strong</strong>> <strong>strong</strong><br />

<strong>negative</strong> <strong>refraction</strong><br />

Hosang Yoon, Kitty Y. M. Yeung, Vladimir Umansky & Donhee Ham<br />

Nature 488, 65-69 (2012)


Metamaterial and <strong>negative</strong> <strong>refraction</strong><br />

Metamaterial – having both m < 0, e < 0<br />

n = mre r <<br />

0<br />

http://en.wikipedia.org/wiki/Split-ring_resona<<strong>strong</strong>>to</<strong>strong</strong>>r<br />

<br />

sinq<br />

n<br />

sinq<br />

n<br />

=<br />

1 2<br />

2 1<br />

http://www.nature.com/nature/journal/v480/n7375/fig_tab/4800<br />

42a_F1.html


2D-electron system in semiconduc<<strong>strong</strong>>to</<strong>strong</strong>>r strip<br />

l=112mm, a=1.25mm, W=1mm<br />

and number of strip ~13<br />

Motion of 2DEG is induced<br />

by external EM field. (along<br />

xy-plane)


Band bending and modulation dopping<br />

Energy level of conduction band<br />

Energy level of conduction band<br />

(1) (2)<br />

AlGaAs : ~2eV GaAs : 1.42eV<br />

z-direction<br />

(3)<br />

Al+<br />

Al+<br />

Al+<br />

~ No free electrons<br />

Immigration of electron<br />

e- e- e- Fermi level<br />

Fermi level<br />

Energy level of conduction band<br />

Si<br />

S<br />

i<br />

Si<br />

Silicon doping<br />

Energy level of conduction band<br />

e- Al+<br />

(4)<br />

Si = +


2D-electron motion and kinetic inductance<br />

: Equation of motion<br />

i( kx-wt )<br />

Under AC field (eg. Electromagnetic wave) V ( x, t) = Ve<br />

With a definition of current in this system I = -n2DevW<br />

Z = iwL +<br />

R<br />

k ,2D<br />

: expression of impedance


Derivation of refractive index from L 2D,k<br />

With circuit equations in this system,<br />

After inserting V in induced by electromagnetic wave,


Derivation of refractive index from L 2D,k<br />

1<br />

- w V e ( e + e - 2) = V e<br />

2 ( wt-kma ) ika -ika ( wt-kma )<br />

0<br />

LK ,2DC<br />

0<br />

So, dispersion relation can be expressed as,<br />

From definition of refractive index,<br />

Negative value if w ><br />

wc


Comparison between 2D and 3D system<br />

Kinetic and magnetic inductance of single 3D gold nano particle<br />

Kinetic and magnetic inductance of 2DEG strip array<br />

2DEG strip system has larger kinetic inductance<br />

* Carrier density for silver is around 1 x 10 28 m -3


Result of simulated dispersion curve and current<br />

Dispersion curve indicates that group and phase velocity<br />

have opposite sign.<br />

Frequency above cu<<strong>strong</strong>>to</<strong>strong</strong>>ff creates high current density on the<br />

stripes.


Measurement of microwave<br />

Effective wavenumber<br />

can be extracted from S<br />

parameters


Transfer and scattering matrix


Temperature dependence<br />

In room temperature, strip has<br />

high resistance (~100kOhm)<br />

Kinetic inductance is reduced<br />

and system acts as open circuit


Effect of system dimension


Summary<br />

1. From the metamaterial having 2DEG Strong <strong>negative</strong> refractive index was<br />

observed in GHz range.<br />

2. Origin of <strong>negative</strong> <strong>refraction</strong> dominantly came from collective motion of<br />

electrons in the strip array which related <<strong>strong</strong>>to</<strong>strong</strong>> kinetic inductance.<br />

3. Temperature and size dependence of n was studied.

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