gisaxs による高分子薄膜構造解析

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GISAXS による高分子薄膜構造解析. 東京大学 大学院新領域創成科学研究科 基盤科学研究系 物質系専攻 横山英明. yokoyama@molle.k.u-tokyo.ac.jp. Outline. Nanocellular thin films GISAXS What can we obtain using GISAXS? Distorted Wave Born Approximation (DWBA) ‏ Quantitative analysis of nanocellular thin films using DWBA - PowerPoint PPT Presentation

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GISAXSGISAXS による高分子薄膜構造解による高分子薄膜構造解析析

東京大学東京大学 大学院新領域創成科学研究科大学院新領域創成科学研究科基盤科学研究系基盤科学研究系 物質系専攻物質系専攻

横山英明横山英明

yokoyama@molle.k.u-tokyo.ac.jp

yokoyama@molle.k.u-tokyo.ac.jp2

Outline

• Nanocellular thin films• GISAXS• What can we obtain using GISAXS?• Distorted Wave Born Approximation

(DWBA)• Quantitative analysis of nanocellular thin

films using DWBA• Analysis of vertically and horizontally

aligned nanosheets

yokoyama@molle.k.u-tokyo.ac.jp3

Foaming

• Styrofoam– Macroscopic foam

• Macrocells• Microfoaming with supercritical carbon

dioxide– Microscopic foam

• Microcells• Target: smaller foams(cells)

– Nanofoaming• Nanocells

yokoyama@molle.k.u-tokyo.ac.jp4

Accessible critical point (Tc = 31.1 & Pc = 7.4 MPa)

Tunable density & solvent quality

Environmentally friendly

High diffusivity

Supercritical Carbon Dioxide

Tc

Pre

ssur

e

Pc

Temperature

Gas

Liquid

SCFSol

id

yokoyama@molle.k.u-tokyo.ac.jp5

Conventional CO2 foaming Process

Rapid depressurization Limited accessible size.> 1 m

10m

*K. A. Arora, A. J. Lesser and T. J. McCarthy Macromolecules 1998, 31, 4614-4620

Example: polystyrene

yokoyama@molle.k.u-tokyo.ac.jp6

Self-assembly of block copolymers

M. W. Matsen and M. Scick, Phys. Rev. Lett. 72 , 2660 (1994).

Block Copolymers present a variety of domain structures of the order of 5 – 50 nm.

yokoyama@molle.k.u-tokyo.ac.jp7

5~50 nm

Poly(styrene-block-perfluorooctylethyl methacrylate) (PS-PFMA)

Poly(methyl methacrylate-block-perfluorooctylethyl methacrylate) (PMMA-PFMA)

PFMA is soluble in SC CO2

(CO2-philic)

Block copolymer with fluorinated block

yokoyama@molle.k.u-tokyo.ac.jp8

CO2 Process

Time / h

Tem

pera

ture

/ºC 60 ºC

0 ºC1 h

isobaric

Depressurization

CO2 pump

Back pressure regulator

High pressure vessel

TcP

ress

ure

Pc

Temperature

Gas

Liquid

SCFSol

id

Failed:Microcells appear

?

2 m

yokoyama@molle.k.u-tokyo.ac.jp9

(A) SAXS profiles of PS-PFMA processed in 7.5-30 MPa of CO2. Domain spacing increase with pressure. (B) A schematic picture of nanofoams and PS-PFMA chains.

Structures of nanofoams

PFMA domain

PS domain

Nanocell

A B

yokoyama@molle.k.u-tokyo.ac.jp10

Nanoces in thin films

70 nm

(110 nm?)

100 nm

ScCO2

pressurize

ScCO2

depressurize

yokoyama@molle.k.u-tokyo.ac.jp11

Exposing cell structures by RIE

0 nm 10 nm

13 nm

15 nm

20 nm

40 nm

200 nm

Etching

yokoyama@molle.k.u-tokyo.ac.jp

Refractive index (density) is controlled by the processing pressure of CO2.

Reduction of refractive index  = porosity

0 5 10 15 20 25 301.1

1.2

1.3

1.4

1.5

1.6

Ref

ract

ive

Ind

ex

P / MPa

0.0

0.1

0.2

0.3

0.4

0.5

0.6

Vo

lum

e F

rac

tio

n o

f ce

lls

yokoyama@molle.k.u-tokyo.ac.jp13

Quantitative measurement of nanocells

• Prepare a single layer of nanocells (60 nm thick film)– 2-D hexagonal lattice– inter-cell scattering is restricted in the film

plane– Foam factor of cells is 3D

• Size• Structure of block copolymers around the

voids

yokoyama@molle.k.u-tokyo.ac.jp14

Grazing incident small angle X-ray scattering (GISAXS)

http://www.spring8.or.jp/wkg/BL40B2/instrument/lang-en/INS-0000001280/instrument_summary_view

yokoyama@molle.k.u-tokyo.ac.jp15

GISAXS Patterns

qz

qy

yokoyama@molle.k.u-tokyo.ac.jp16

Theory of GISAXS

• Reflectivity– Fresnel law

• Small Angle Scattering– Born Approximation– Fourier transform of model

• GISAXS(DWBA)– Calculate 4 beam intensities using Fresnel

law– Apply Born approximation

yokoyama@molle.k.u-tokyo.ac.jp17

Distorted Wave Born Approximation (DWBA)(1)

Compute Reflectivity.......

yokoyama@molle.k.u-tokyo.ac.jp18

DWBA(2)Compute scattering.......

TfT

i

Rf

Ti

Tf

Rf

Ri

Ri

yokoyama@molle.k.u-tokyo.ac.jp19

Model

R1

R2

1

F

qR

Paracrystal distortion

Lattice Form factor of cells

yokoyama@molle.k.u-tokyo.ac.jp20

GISAXS and DWBA

incident angle: 0.15 degree

incident angle: 0.225 degree

yokoyama@molle.k.u-tokyo.ac.jp21

Interference of reflected wavesincident angle: 0.15 degree incident angle: 0.225 degree

@ critical angle @ critical angle

yokoyama@molle.k.u-tokyo.ac.jp22

Model fitting

F

qR

Sphere

SCS

R1

R2

1

yokoyama@molle.k.u-tokyo.ac.jp23

Self-assembly of block copolymers

M. W. Matsen and M. Scick, Phys. Rev. Lett. 72 , 2660 (1994).

Block Copolymers present a variety of domain structures of the order of 5 – 50 nm.

yokoyama@molle.k.u-tokyo.ac.jp24

As cast morphologies

• Trifluorotoluene (TFT)

– Non-selective

– Cylinders oriented in the surface plane

• Hexafluorobenzene (HFB)

– Selective for PFMA

– Fat cylinders of PS oriented vertically ?

TFT Top View HFB Top View

HFB Side View

yokoyama@molle.k.u-tokyo.ac.jp25

GISAXS of as-cast morphologies  

• Trifluorotoluene (TFT)

– Non-selective

– Cylinders oriented in the surface plane

• Hexafluorobenzene (HFB)

– Selective for PFMA

– Fat cylinders of PS oriented vertically ?

TFT GISAXS

HFB GISAXS

yokoyama@molle.k.u-tokyo.ac.jp

CO2 process

As-cast films CO2 processTemplated

porous films?

yokoyama@molle.k.u-tokyo.ac.jp27

“Porous” structure (HFB)Standing nanosheets

200 nm

yokoyama@molle.k.u-tokyo.ac.jp28

GISAXS of standing nanosheets

qy / nm-1

q z / nm

-1

-1.2 -1.0 -0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2

1.4

1.2

1.0

0.8

0.6

0.4

0.2

0.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.510

0

101

102

103

104

105

0.10

0.15

0.20

Inte

nsi

ty, a

.u.

qy / nm

-1

yokoyama@molle.k.u-tokyo.ac.jp

Standing nanosheets

• Capillary condensation• Constraint by substrate• 22.4 nm and 20.3 nm

Top view

200 nm

yokoyama@molle.k.u-tokyo.ac.jp30

“Porous” structure (TFT)stacking nanosheets

200 nm

yokoyama@molle.k.u-tokyo.ac.jp31

Out of plane scattering

= 0 .20 = 0 .1 5 RT 3

TT 3

RT 2

TT 2

RT 1TT 1

Y oneda

0 1 .2-1.20 1 .2-1 .2

qy / n m - 1

qz /

nm

-1

0

1 .4

qy / n m -1

yokoyama@molle.k.u-tokyo.ac.jp

Decomposing to two components

• Stacking nanosheets

• 20.9±0.4 nm from 2/qz of two sets of peaks

0.0 0.5 1.0 1.510

2

103

104

105

106

107

108

3'

3'

2'

2'

1'

1'

= 0.15 = 0.20

1

2

3

3

2

1

Inte

nsi

ty,

a.u

.

qz / nm- 1

1,2,3

1',2',3'

yokoyama@molle.k.u-tokyo.ac.jp33

Summary

• GISAXS reveals cellular structures quantitatively

• GISAXS is useful method for the analysis of thin films on substrate

• DWBA simulation is essential for quantitative analysis

yokoyama@molle.k.u-tokyo.ac.jp34

Acknowledgment

• C. Dutriez, L. Li and R. Zhang (AIST)

• K. Sugiyama (TIT)

• S. Sasaki, H. Masunaga and M. Takata (JASRI)

• H. Okuda (Kyoto U.)

yokoyama@molle.k.u-tokyo.ac.jp35

In plane scattering

- 1 . 5 -1 .0 - 0 . 5 0 .0 0 . 5 1 . 0 1 .5

1 0 2

1 0 3

1 0 4

1 0 5

1 0 6

1 0 7

I,

a.u

.

q

y

/ n m - 1

1 0 %

3 4 %

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