Lecture 12 – Nanophotonics in Microscopy
EECS 598-002 Winter 2006 Nanophotonics and Nano-scale Fabrication P.C.Ku Schedule for the rest of the semester
Introduction to light-matter interaction (1/26):
How to determine ε(r)?
The relationship to basic excitations. Basic excitations and measurement of ε(r). (1/31) Structure dependence of ε(r) overview (2/2) Surface effects (2/7):
Surface EM wave
Surface polaritons
Size dependence Case studies (2/9 – 2/16):
Quantum wells, wires, and dots
Nanophotonics in microscopy
Nanophotonics in plasmonics Dispersion engineering (2/21 – 3/7):
Material dispersion
Waveguide dispersion (photonic crystals)
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 2 Principles of optical microscopy
The information contained in the object/image is carried by the light wave to the detector (e.g. eyes).
Information = F(x,y) Æ F(,kkxy )
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 3 Optical vs electron microscopy
Advantages of optical microscopes
Photon energy is low (~ eV). Electron energy is high (~10-100 keV) -27 Photon momentum is low (~ 10 kg m/s). Electron momentum is high (~ 10-23 -10-22 kg m/s)
Especially good to study optical processes (including nonlinear optical response) in the sample
Ultra-short optical pulse is available to study ultra-fast processes
Can make the fluorescence work Æ useful for biological imaging
Disadvantages of optical microscopes
Photon does not have charge. Cannot study the Coulomb interaction in the sample.
Photon does not reveal information regarding the chemical composition of the sample (unless we go to the x-ray wavelength).
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 4 Resolution limits of optical microscopes
Small features correspond to large (kx, ky) components.
In traditional optical microscopes, the detector sees the light in the far fieldk region.
2 2 222 k==++ωµε0 kkkxyz
22 ⇒+<⇒kkxyω nck/2/&,max =πλ n
17.5 15 Resolving power 12.5
k-space real-space 10 = λλ/2( n)≡ eff /2 7.5 5 = diffraction limit 2.5
−2/π n λ 2/π n λ k& -2 -1 1 2 λ / n
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 5 Finite-size lens
In a real system, the cutoff spatial frequency is often limited by the size of the lens which is quantitatively described by a numerical aperture (NA).
NA≡ n sinθ θ
k&,max 2π ⇒=⇒=sink&,max NA k λ
θ Resolving power Æ
λλ/2NA( )≡ eff /2
where λeff = λ /NA
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 6 Resolution enhancement
Shortening of wavelength:
Decrease the wavelength of light source
Increase the refractive index (e.g. immersion microscope)
Using nonlinear optical effect (e.g. frequency doubling)
Increase the detectable spatial frequency
Moire grating
Near field optics to detect the evanescent waves
Ref: S. Kawata, chapter 2, figure 1.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 7 Scanning Near-field Optical Microscope
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 8 Different modes of SNOM
Ref: Prasad, chapter 3, figure 7.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 9 Detection of near field intensity modulation
The modulation of the near-field intensity can be detected at the far-field region:
e.g. Thin slab photon tunneling d = wavelength/4 1 Transmission 0.9 Reflection 0.8
0.7
0.6
0.5
0.4
0.3
0.2
0.1
0 0 20 40 60 80 100 Incident Angle
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 10 Configuration of SNOM
Ref: Prasad, chapter 3, figure 8.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 11 Near-field probes
(aperture in an opaque screen)
(e.g. PSTM)
Green: evanescent wave
Ref: S. Kawata, chapter 2, figure 6.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 12 Advantages of apertureless probes
No cutoff frequency as existing in a metal-coated fiber optics probe
Field enhancement due to surface plasmon polaritons
The probe size can be made much smaller
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 13 Controlling the probe-sample distance
feedback (1) laser excitation (2) laser
beam splitter segment ed photodiod e
The tip-sample distance changes the damping sampl e cant i l ever of the resonance oscillator.
Ref: Prasad, chapter 3, figure 9.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 14 Laser trapping for probe
Ref: S. Kawata, chapter 8.
e.g. 2.5W Nd-YLF traps a gold particle (~ 10-100 nm) with a 100X NA=1.35 objective (oil immersion)
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 15 Examples of SNOM images 1
Single molecule fluorescence detection
location
Laser detuning
Ref: W. E. Moerner, Science 265 (1994) 46.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 16 Examples of SNOM images 2
Single quantum dot
Ref: T. Saiki and Y. Narita, Jpn. J. Appl. Phys., 37 (1998) 1638.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 17 Examples of SNOM images 3
Dynamics using pump-probe technique t = 30 ps
t = 0 ps
Ref: Y. Shen et al., J. Phys. Chem. B 107 (2003) 13551.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 18 Examples of SNOM images 4
Topography
0 14500 0 28000
830,25nm
21000 829,53nm 0 21000 0 14000 SNOM 0
6000
0 Background
0 80000 0 1300 0
0 61000 0 18000
VCSEL 15 microns scan range Taken from presentation materials of WITEC. 0 8000 0 120 00 EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 19 Examples of SNOM images 5
MFM - Magnetic Force Microscopy
80 microns scan range 20 microns scan range 5 microns scan range
PC hard drive
Taken from presentation materials of WITEC.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 20 Examples of SNOM images 5
Semiconductor Surface Study
Topography SNOM
20% In (a) (b) (c)
24% In (d) (e) (f)
InGaN films
Jeongyong Kim et al., University of Illinois, see also APL Vol. 80, 6, 989 (2002). 27% In (g) (h) (i)
10 microns scan range
Taken from presentation materials of WITEC.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 21 Examples of SNOM images 7
Topography Adhesion 5 microns scan range
Bodyguard adhesive tape Taken from presentation materials of WITEC.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 22 Reading
S. Kawata, chapter 2.
EECS 598-002 Nanophotonics and Nanoscale Fabrication by P.C.Ku 23