x-ray phase imaging with grating interferometers · suitable for radiography and tomography...

30
Timm Weitkamp , Ana Diaz, Christian David Laboratory for Micro- and Nanotechnology, Paul Scherrer Institut, Villigen, Switzerland Oliver Bunk, Amela Groso, Marco Stampanoni, Franz Pfeiffer Swiss Light Source, Paul Scherrer Institut, Villigen, Switzerland Peter Cloetens, Eric Ziegler European Synchrotron Radiation Facility, Grenoble, France Coherence 2005 Workshop, Porquerolles, 15 June 2005 X-ray phase imaging with grating interferometers See copyright notice and terms of use on next slide

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Page 1: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Tim

m W

eitkam

p,

Ana D

iaz,C

hristian D

avid

Labora

tory

for

Mic

ro-

and N

anote

chnolo

gy,

Paul S

cherr

er

Institu

t, V

illig

en, S

witzerland

Oliv

er

Bunk, A

mela

Gro

so,

Marc

oS

tam

panoni, F

ranz

Pfe

iffe

rS

wis

s L

ight S

ourc

e,P

aul S

cherr

er

Institu

t, V

illig

en, S

witzerland

Pete

rC

loete

ns,

Eric Z

iegle

rE

uro

pean S

ynchro

tron R

adia

tion

Facili

ty,

Gre

noble

, F

rance

Cohere

nce 2

005 W

ork

shop, P

orq

uero

lles, 15 J

une 2

005

X-r

ay p

hase im

agin

g w

ith g

rating inte

rfero

mete

rs

See c

opyright notice a

nd term

s o

f use o

n n

ext slid

e

Page 2: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Co

pyri

ght notice a

nd t

erm

s o

f use

The m

ate

rial in

this

file

is c

op

yrighte

d.

You m

ay

do

wn

load a

nd v

iew

the f

ile f

rom

its

we

b r

ep

ository

, but

ple

ase

•do n

ot

redis

trib

ute

this

file

or

an

y part

of

it o

r its c

onte

nts

in a

ny

form

,•

do n

ot

use a

ny o

f th

e c

onte

nts

of

this

file

in p

resenta

tions o

r public

atio

ns

without

pri

or

wri

tte

n c

onse

nt

of

the a

uth

ors

.

Thank y

ou.

Auth

ors

can b

e r

eached a

t th

e f

ollo

win

g a

ddre

sses:

Tim

mW

eitkam

p,

ES

RF

, 6 r

ue J

ule

s H

oro

witz,

38043 G

reno

ble

, F

rance

E-m

ail

tim

m.w

eitkam

p@

psi.ch,

we

itkam

p@

esrf

.fr

Christia

n D

avid

, P

aul S

cherr

er

Institu

t, 5

232 V

illig

en

PS

I, S

witzerla

nd

E-m

ail

christia

n.d

avid

@psi.ch

11 J

uly

20

05

Page 3: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Motivation

•H

ard

X r

ays

well

suite

dfo

rra

dio

gra

ph

ic im

agin

g(lon

g p

en

etr

ation

de

pth

, neglig

ible

refr

action

)

•G

enera

l se

tup u

ses a

bso

rpti

on

co

ntr

ast:

Are

a d

ete

cto

r behin

d s

am

ple

reco

rds inte

nsity v

ariations

cause

d b

y a

ttenuatio

n p

rofile

of th

e s

am

ple

•T

om

og

rap

hy:

takin

g 2

D r

ad

iogra

phs a

t diffe

rent

vie

win

g

ang

les y

ield

s 3

D d

istr

ibutio

n µ

(x,y

,z)

•B

ut fo

r lig

ht

mate

rials

(bio

log

ical tissue,

poly

mers

...)

, and

hig

h p

ho

ton

en

erg

ies,

ab

so

rpti

on

co

ntr

ast

is r

ela

tively

w

eak

•B

ett

er

image c

ontr

ast w

ould

resu

lt in

–S

ho

rter

exp

osu

re t

imes

(mate

rials

scie

nce a

pplic

ations)

–R

ed

uced

do

se d

ep

osit

ion

(bio

logy, m

edic

al im

agin

g)

Page 4: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Phase r

adio

gra

phy m

eth

ods

Cry

sta

l in

terf

ero

mete

rsB

onse

& H

art

19

65

Fre

e-s

pace p

ropagation

(“In

line p

hase c

ontr

ast”

)S

nig

irev

1995, W

ilkin

s 1

995, C

loete

ns

1996

Analy

zer-

cry

sta

l based

(“diffr

action-e

nhanced

imagin

g”,

DE

I)In

gal&

Belia

evska

ya

1995

D

�Lots

of diffe

rent

schem

es a

lre

ady

Page 5: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Why y

et ano

ther

meth

od?

•F

or

the c

om

bin

ation o

f...

–la

rge

fie

ld o

f vie

w(m

od

era

te r

eso

lutio

n),

–p

ossib

ility

of

use

with

an

X-r

ay t

ub

eso

urc

e,

•... th

e e

xis

ting m

eth

ods h

ave p

roble

ms:

–B

on

se

-Ha

rt:

cry

sta

l siz

e lim

its F

OV

–D

EI:

mo

no

ch

rom

aticity, co

llim

atio

n �

ne

ed

s S

R

–F

SP

: e

xce

llen

t fo

r h

igh

re

so

lutio

n,

bu

t a

t m

od

era

te r

eso

lutio

n,

larg

e d

ista

nce

s r

eq

uir

ed

•G

rating inte

rfero

mete

r:m

ay fill

this

dom

ain

Page 6: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

d

beam

-split

ter

phase

gra

ting

inte

rfe

rence

patt

ern

s

•P

hase g

rating

as a

beam

split

ter

•W

avele

ngth�

1 �

, gra

ting p

eriod �

1 µ

m�

sm

all

diffr

action a

ng

les

�beam

s o

verl

ap

Ho

w c

an w

e d

ete

ct

the

local fr

inge p

ositio

n?

Gra

tin

g in

terf

ero

me

try

Page 7: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

ca

mera

beam

-split

ter

phase

gra

ting

analy

zer

am

plit

ude

gra

ting

inte

rfe

rence

patt

ern

•A

bsorp

tio

n g

rating

with

sam

eperio

das f

ring

es

•A

cts

as t

ransm

issio

nm

ask

(not

as d

iffr

active

ele

ment!

)•

Tra

nsfo

rms

frin

ge

positio

ns

into

inte

nsity

sig

nal

�M

ay

use

dete

cto

rw

ith

pix

els

larg

er

than

frin

ge

wid

th

Gra

tin

g in

terf

ero

me

try

Page 8: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

ca

mera

beam

-split

ter

phase

gra

ting

analy

zer

am

plit

ude

gra

ting

inte

rfe

rence

patt

ern

phase

obje

ct �

Diffe

rentia

lph

ase

contr

ast

imagin

gB

ut

how

to s

epara

te p

hase info

rmation f

rom

absorp

tion?

-O

bje

ct

in b

ea

m-

Dis

tort

sw

ave

front,

i.e

., d

eflects

beam

-F

ringes

loca

llydis

pla

ced

-D

iffe

rent

inte

nsity

on d

ete

cto

r-

Inte

nsity

corr

ela

ted

to f

irst

derivative

of

wa

vefr

ont

phase

Gra

tin

g in

terf

ero

me

try

Page 9: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

(sam

ple

here

:poly

sty

ren

esp

here

100 a

nd 2

00

µm

)

Sam

ple

Beam

split

terA

naly

zer

scan

ned

Dete

cto

r

ES

RF

BM

5,

E=

12.4

keV

, p

1=

4 µ

m,

p2=

2.0

04 µ

m

Phase

-ste

ppin

gin

terf

ero

metr

yLin

ear

transvers

e s

can

of

one o

f th

e g

ratings:

�sig

nal oscill

ate

s

Page 10: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Phase

-ste

ppin

gin

terf

ero

metr

y

Page 11: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Phase

-ste

ppin

gin

terf

ero

metr

yC

onsid

er

indiv

idual

pix

els

:In

tensity

oscill

ate

s

Page 12: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Phase

-ste

ppin

gin

terf

ero

metr

y

�1�

2

a2

a1

aij

�P

rocessed

images:

�ij

Page 13: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Phase

-ste

ppin

gin

terf

ero

metr

y

�ij

Ph

ase g

rad

ien

tim

ag

e(p

erp

endic

ula

rto

gra

ting

lines)

---

all

absorp

tio

ncontr

ibutions

elim

inate

d

Can

be

inte

gra

ted

to y

ield

pro

jecte

dp

hase

shift

of

sam

ple

aij

�S

uited

for

tom

ogra

phic

reco

nstr

uction

�Q

uantita

tive:

(suited

for

tom

ogra

phic

reco

nstr

uction)

Mix

ture

of

absorp

tion

and in

line

phase

contr

ast

---

the

sam

eim

ag

e t

hat

wo

uld

be

ob

serv

ed

wit

ho

ut

the

inte

rfero

mete

rin

th

eb

eam

),

()

,(

2y

xdp

x

yx

ϕλ

=∂

Φ∂

Page 14: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Phase

-ste

ppin

g t

om

ogra

phy

Sam

ple

Beam

split

ter

Dete

cto

r

Fast axis

:phase s

teppin

gS

low

axis

:to

mo

rota

tion

Analy

zer

•T

wo s

can a

xes:

pro

jection a

ng

leand inte

rfero

mete

r phase

•N

um

ber

of pro

jection

angle

s:

100…

10

00

•N

um

ber

of phase-s

tepp

ing p

oin

tsper

angle

: 4 o

r m

ore

•R

esu

lts:

3D

dis

trib

utions �

(x,y

,z)

and µ

(x,y

,z)

ES

RF

ID

19, Jun

e 2

004

E=

12.4

keV

, p

1=

4 µ

m,

p2=

2 µ

m,

d=

23 m

m

Page 15: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Beam

split

ter

phase

gra

ting

(p=

4 µ

m)

and a

naly

zer

absorp

tion

gra

ting

(p=

2 µ

m)

4 µ

m4 µ

m4 µ

m

Phase g

rating

(Si)

Absorp

tion g

rating

(Au in S

i)

•S

ilicon w

et-

etc

hed

•D

epth

of str

uctu

res c

hosen s

o that

phase s

hift is

��

no z

ero

ord

er

•�

Effic

iency lim

it: 80 %

(fra

ction o

f usefu

l photo

ns)

•G

old

in g

aps o

f sili

con g

rating

•G

row

n e

lectr

ochem

ically

•P

eriod is h

alf that of S

igra

ting

•E

ffic

iency lim

it: 50 %

(fra

ction o

f tr

ansm

itte

d inte

nsity)

�P

oste

r P

9, A

. D

iaz e

t al.

Page 16: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

1m

m0.5

mm

Tom

ogra

phy o

f a s

pid

er:

Isosurf

ace

renderi

ng o

f X

-ray r

efr

active in

de

x

Page 17: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

1m

m0.5

mm

Tom

ogra

phy o

f a s

pid

er:

De

nsity-p

roje

ctio

n r

enderi

ng o

f X

-ray r

efr

active ind

ex

Page 18: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Non-i

nte

rfero

metr

icpro

jection

Non-i

nte

rfero

metr

icto

mogra

mIn

terf

ero

metr

icphase t

om

ogra

m

Inte

rfero

metr

icphase p

roje

ctio

n

0.5

mm

0.5

mm

0.5

mm

0.5

mm

Page 19: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Qua

ntita

tive p

hase r

econstr

uction I

Exa

mp

le:

ph

ase

pro

file

of

pa

rab

olic

re

fra

ctive

len

se

s

R

Bery

llium

refr

active lens,

R=

0.2

mm

�f=

61 m

at 14.4

keV

Be

ES

RF

BM

5,

9 J

une 2

005

Positio

n (

mm

)

Position (mm) Phase (�)P

hase (�

)

Colla

bora

tion w

ith J

. P

ato

mm

el, B

. Lengele

r(R

WT

H),

C. S

chro

er

(HA

SY

LA

B)

Page 20: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Qua

ntita

tive p

hase r

econstr

uction I

Page 21: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Qua

ntita

tive p

hase r

econstr

uction I

I:

pin

k-b

ea

m t

om

ogra

phy

Inte

rfero

metr

icphase t

om

ogra

mN

on-i

nte

rfero

metr

icto

mogra

m

Thre

efibers

•P

oly

am

ide Ø

225 µ

m•

Boro

n Ø

200 µ

m,

core

: W

Ø 1

0 µ

m•

PB

T Ø

190 µ

m

Sam

ple

:

SLS

Mate

rials

Scie

nce b

eam

line

July

200

4

E=

17.5

keV

,�

E=

1 k

eV

Page 22: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Poly

chro

matic

radia

tion

ca

mera

beam

-split

ter

phase

gra

ting

analy

zer

am

plit

ude

gra

ting

inte

rfe

rence

patt

ern

phase

obje

ct

� 1� 2

�Q

uasi-a

chro

matic

instr

um

ent

Page 23: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Lim

its o

f achro

maticity

•In

ter-

gra

ting d

ista

nce:

devia

tes fro

mT

alb

ot conditio

n,

•B

eam

split

ter:

phase s

hift

devia

tes fro

m �

,

•A

naly

zer:

changes

absorp

tion.

Effects

of energ

y c

hange (

aw

ay fro

m d

esig

n e

nerg

y)

on e

ffic

iency o

f a g

iven s

etu

p:

Measure

ment

(moiré f

ring

es)

Fit t

o t

heory

Desig

nenerg

y:

14.4

keV

(Gra

ting p

eri

od

s p

1=

4 µ

m, p

2=

2 m

, 3

rdT

alb

ot dis

tance d

3=

69

.7 m

m)

Data

taken a

t E

SR

F B

M5,

11 J

une 2

00

5

FW

HM

:

> 2

keV

Effic

iency v

s. energ

y

Page 24: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Bio

logic

al tissue s

am

ple

sin

aqu

eous e

nviron

ment

•C

on

ditio

ns s

imila

r to

na

tura

l e

nvir

on

me

nt,

i.e

., to

in-v

ivo

im

ag

ing

•C

on

tra

st

be

twe

en

tis

su

e a

nd

wa

ter

is v

ery

we

ak,

i.e

., a

re

al ch

alle

ng

e

•L

arg

e o

bje

ct,

mo

de

rate

re

so

lutio

n e

no

ug

h�

test ca

se

•O

ur

firs

t sa

mp

le:

the

he

art

of

a r

at, in

fo

rma

lin

Page 25: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Rat

heart

in f

orm

alin

-W

alls

of

vessels

cle

arl

y vis

ible

in t

he p

hase-c

ontr

ast

image

-…

but

not

in the a

bsorp

tion im

age

acquired w

ith t

he s

am

e d

ose

Absorp

tio

n im

age

3 m

m

Pix

el siz

e 1

4 µ

mIm

age s

titc

hed f

rom

5x4 d

ete

cto

r fr

am

es

SLS

beam

line

4S

, 29 J

an 2

00

5

Sam

ple

by T

. K

han,

Univ

. ho

spital Z

ürich

Page 26: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Rat

heart

in f

orm

alin

Phase-g

radie

nt

image

3 m

m

-W

alls

of

vessels

cle

arl

y vis

ible

in t

he p

hase-c

ontr

ast

image

-…

but

not

in the a

bsorp

tion im

age

acquired w

ith t

he s

am

e d

ose

-F

ield

of

vie

w h

ere

on

ly lim

ite

d b

ysynchro

tro

n b

eam

siz

e--

-not

by

the inte

rfero

mete

r

Pix

el siz

e 1

4 µ

mIm

age s

titc

hed f

rom

5x4 d

ete

cto

r fr

am

es

SLS

beam

line

4S

, 29 J

an 2

00

5

Sam

ple

by T

. K

han,

Univ

. ho

spital Z

ürich

Page 27: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

X-r

ay tube?

•P

roble

m: cohere

nt flux

•H

ave to u

se m

icro

focus

sourc

eor

slit

a u

sual sourc

e d

ow

n

•N

o b

etter

solu

tion?

(i.e

., h

igher

flux)

–w

e d

on’t n

eed the h

igh

resolu

tion o

f a m

icro

focus

•M

aybe u

sin

g …

anoth

er

gra

ting?

Page 28: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Arr

ayed s

ourc

e

s

Ld

p0

p1

p2

Tra

de r

esolu

tion f

or

flu

x,

keep

ing c

ohere

nce

•F

ringe p

attern

s fro

m the d

iffe

rent virtu

al sourc

es s

uperim

pose

incohere

ntly, but constr

uctively

.•

Spatial re

solu

tion d

egra

des to (

s d

/ L

).•

But flux is incre

ased b

y a

facto

r of N

.

Nslit

s(v

irtu

al

sourc

es)

C. D

avid

, F

. P

feiffe

r, T

. W

eitkam

p,

pate

nt

pendin

g

Page 29: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

X-r

ay t

ube r

esults

Page 30: X-ray phase imaging with grating interferometers · Suitable for radiography and tomography application s with large fields of view, moderate resolution Posters: • Wavefront sensing

Sum

mary

•G

ratin

g in

terf

ero

me

ter

giv

es d

iffe

ren

tia

l p

ha

se

con

tra

st

(d�

/dx)

•P

ha

se

ste

pp

ing

se

pa

rate

s a

bso

rptio

n f

rom

ph

ase

, yie

ldin

g b

oth

p

ha

se

�a

nd

tra

nsm

issio

n s

ign

al

•P

ha

se

-ste

pp

ing

to

mo

gra

ph

yyie

lds r

efr

active

in

de

x �

(x,y

,z)

•R

esu

lts a

re q

ua

ntita

tive

•In

str

um

en

t is

la

rge

ly a

ch

rom

atic

•S

tab

le,

rob

ust,

alm

ost

no

alig

nm

en

t

•B

ett

er

co

ntr

ast

tha

n in

ab

so

rptio

n im

ag

ing

with

th

e s

am

e d

ose

•W

ith

an

arr

aye

d s

ou

rce

, e

ffic

ien

t u

se w

ith

X-r

ay t

ub

e

•C

an

be

sca

led

up

to h

igh

er

en

erg

ies a

nd

la

rge

r fie

lds o

f vie

w

�S

uita

ble

fo

r ra

dio

gra

ph

y a

nd

to

mo

gra

ph

y a

pp

lica

tio

ns w

ith

larg

e f

ield

s o

f vie

w,

mo

de

rate

re

so

lutio

nP

oste

rs:

•W

avefr

on

tsensin

g w

ith m

oiré inte

rfe

rom

etr

y(P

8,

Christian D

avid

et al.)

•F

abrication o

f g

ratings (

P9, A

na D

iaz e

t al.)

•C

ohere

nce c

hara

cte

rization (

P44, F

ranz P

feiffe

r et al.)