bright new world norbert kroo hungarian academy of sciences dubna, 25.09.2008

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BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

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BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008. The Lycurgus Cup ( glass ; British Museum; 4 th Century A. D.). When illuminated from outside, it appears green. However, when - PowerPoint PPT Presentation

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Page 1: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

BRIGHT NEW WORLD

NORBERT KROO

HUNGARIAN ACADEMY OF SCIENCES

DUBNA, 25.09.2008

Page 2: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

TheThe Lycurgus Lycurgus CupCup ( (glassglass; British ; British Museum; 4Museum; 4thth CenturyCentury A. D.) A. D.)

When illuminated from outside, it appears green. However, whenilluminated from within the cup, it glows red. Red color is due to very small amounts of gold powder (about 40 parts per million)

Surface plasmon oscillationsMesoscopic:~1011 electrons

Page 3: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

SURFACE PLASMON POLARITONS are a

„NEW TYPE OF LIGHT”, they are

1.BOUND TO THE (METAL) SURFACE,

2.HAVE SPECIFIC DISPERSION PROPERTIES,

3.THE DIFFRACTION LIMIT DOES NOT APPLY,

4. MAY BE GUIDED,

5.REPRESENT VERY HIGH ELECTRIC FIELDS,

6.MAY BE LOCALIZED (e.g. to nanospheres or nanoshells)

7.MAY HAVE A BANDGAP,

8.MAY BE THE SUBJECT OF NONLINEAR PROCESSES

9. SHOW NON-CLASSICAL PROPERTIES

A POTENTIAL BASIS OF FUTURE NANOOPTICS

Page 4: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

ELECTRIC FIELD OF SURFACE PLASMONS

From Maxwell’s equations

1

Page 5: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

2

Excitation of SPO-s !!!?

Page 6: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

TYPICAL RESPONSE SIGNALS AND THEIR PART

USED FOR IMAGING

thermal

SPO

LASER PULSE EXCITED

SURFACE PLASMON NEAR FIELD STM

3

Page 7: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

23870

Ag SURFACE, W tip

200x200nm

Topographic, SPO and thermal images

Page 8: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

SURFACE PLASMON LIGHT GUIDE

38590+92

4000x4000nm

Gold images

Cut from

5000x5000nm images

4

Page 9: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

5GIANT ELECTRIC FIELDS!

Page 10: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

34300+02 Au

Cut from 200x200nm

images

100x100nm

Gold

Topography and

SPO near field

STM images

6

Page 11: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008
Page 12: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

WHAT IS THE ORIGIN OF THE COLORWHAT IS THE ORIGIN OF THE COLOR OF THE OF THE

LYCURGUS CUPLYCURGUS CUP? ANSWER: ``SURFAC? ANSWER: ``SURFACE E PLASMONS’’PLASMONS’’ An SPAn SPOO is a natural oscillation of the electron gas inside a is a natural oscillation of the electron gas inside a goldgold

nanospherenanosphere.. SPSPOO frequency depends on the frequency depends on the dielectricdielectric functionfunction of the gold, and the of the gold, and the

shapeshape of the nanoparticle. of the nanoparticle. For a For a spheresphere the plasma frequency is about the plasma frequency is about 0.580.58 times the bulk times the bulk

plasma frequency (being in the UV; the SPO frequency is in the plasma frequency (being in the UV; the SPO frequency is in the visible)visible) (~520nm) (~520nm)

electron sphere

Ionic background

Electron cloud oscillates with frequency of the SPO-s; ions provide restoring force.

(not to scale)

Page 13: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

SURFACE PLASMON ENERGY, OR MOMENTUM „GAPS”

Donor (chromophore), Acceptor (fluorophore)

7

Page 14: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

B:Similar arrangement, but simpler electronics for angular and spectral property studies of pulsed (790nm, 120fs) laser excited SPO emitted light

1.ARRANGEMENT FOR ANGULAR, LASER POWER AND TIME DEPENDENCE

MEASUREMENTS (A)

808nm SEMICONDUCTOR LASER

8

Page 15: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008
Page 16: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008
Page 17: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008
Page 18: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

23870

Ag SURFACE, W tip

200x200nm

9

Page 19: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

23950ss

FFT OF THE TOPOGRAPHIC

SURFACE PLASMON AND THERMAL

IMAGES

Page 20: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

SQUEEZING IN THE SPO IMAGE

Page 21: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

w = 4%

Page 22: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

APPLICATIONS OF LOCALIZED PLASMONS

Page 23: BRIGHT NEW WORLD NORBERT KROO HUNGARIAN ACADEMY OF SCIENCES DUBNA, 25.09.2008

THANK YOU FOR YOUR ATTENTION