Microscopy from Carl Zeiss Info-forum
Transcript of Microscopy from Carl Zeiss Info-forum
Info-forum
Information forum:
Polarization microscopy
M i c r o s c o p y f r o m C a r l Z e i s s
Michel Lévy Color ChartPolarized LightConoscopic Determination
ZEI1202_ColorChart.GB 07.11.2002 13:18 Uhr Seite 1
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Eye
Eyepiece
Intermediate image plane
Tube lensBertrand lens plane
Intermediate image plane
Bertrand systemDepolarizer
AnalyzerCompensator plane
Objective pupil
Objective
Specimen plane
Condenser
Aperture diaphragm
Polarizer
Luminous field diaphragm
Collector
Light source (filament)
Inte
rmed
iate
tu
be
Pol
Orthoscopy Conoscopy
Polarization in transmitted light
Orthoscopy and conoscopy are the most
important techniques in classical trans-
mitted light polarization microscopy.
With their different ways of examining,
they provide different options, e.g. in
mineral diagnosis in geological micros-
copy. In orthoscopy, each pixel corre-
sponds to a dot in the specimen.
Analyzing minerals is based on such
morphological and optical features as
form, cracks, color, pleochroisms, and
their characteristic interference colors.
In conoscopy, each pixel corresponds to a
direction in the specimen. This technique
requires the use of the highest objective
and condenser aperture possible.
Particularly suitable objectives are CP-
Achromat 50x/0.80 Pol, Plan-Neofluar
40x/0.85 Pol or Plan-Neofluar 100x/1.30
Oil Pol. When the Betrand lens is placed
in the light path, the interference or
axial image in the back focal plane of the
specimen becomes visible. Conoscopy is
used when additional information about
the specimen is necessary for analysis. It
provides interference images that can be
seen through the eyepiece and enable dif-
ferentiation according to 1 or 2 axes and
with compensator λ (λ-lamina, Red I),
according to 1-axis positive/negative or
2-axis positive/negative.
The intermediate tube Pol is designed for
high-performance conoscopy. Thanks to
its two additional intermediate image
planes with suspended crosshair and
field of view diaphragm, it permits the
conoscopy of crystals larger than 10 µm.
*Field of view
diaphragm
*
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d
Second OrderFirst Order
Birefringence(nγ – nα)
d [µm]
50
40
30
20
10
0
Thic
knes
s
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-0.040
-0.045
-0.050
-0.055
-0.060
-0.065-0.070
-0.080
-0.090
-0.120
-0.180
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1400
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1101
1128
1151
1258
1334
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l pur
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let-
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y-bl
ue
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l sea
gre
en
Blui
sh g
reen
TephroiteMeioniteAegerine-augiteGruneriteDatolite
TalcMonaziteZirconAegirine
Astrophyllite
Basaltic HornblendeOxyhornblende
AschariteAnatase
Siderophyllite
Baddeleyite
SpheneBrookiteColumbiteAragoniteCalciteDolomiteMagnesiteSideritePyrophaniteHematiteRutileGeikieliteLepidocrocite
TilleyiteSpurrite
Biotite
Carborundum
Diaspore
Cholesterole
Silk
Nylon
Cellulose
Maltose
Bicalciumferrite
BrownmilleriteGlucose
Carbamide
Monocalciumferrite
LåveniteNontronite
PhengiteTitanbiotiteAnhydrite
PyrophylliteFayaliteIlvaite
Piemontite
Kieserite
Stilpno melane
Cassiterite
Xenotime
Goethite
WhewelliteLudwigite
Path difference [nm](1000nm = 1µm = 10-3mm)
Third Order
0,0380,039
0,0410,0430,0440,0450,0470,0480,0490,0500,052
0,055
0,0600,063
0,0650,0700,073
0,080
0,0900,096
0,107
0,1200,1400,1500,1560,1720,1800,1950,2410,2700,2800,2860,360,57
Michel Lévy
Color Chart
We make it visible.
ZEI1202_ColorChart.GB 07.11.2002 13:19 Uhr Seite 4
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Linear and circular polarized light
Determination of optical character
Behavior of optically
anisotropic crystals in linearly
and circularly polarized light
in orthoscopic and
conoscopic observation.
Determination of the optical
character of uniaxial and
biaxial minerals in linearly
and circularly polarized light.
The reference direction ny of
the λ-compensators is oriented
NE-SW.
linear
linear
biaxial
State of polarization of the light
linear circular
compensator λ
without with without with without with without with
normal position diagonal position normal position diagonal position
positive
barite
negative
muskovite
0° 45° 90° 135° 180°Zir
con
Muscovit
e
Specim
en
State of polariza-
tion of the light
Rotation of the microscope stage
State of polarization of the light
linear circular
compensator λ
without with without with
circular
uniaxial
positive
quartz
negative
calcite
circular
ZEI1202_ColorChart.GB 07.11.2002 13:19 Uhr Seite 5
Axi
osko
p 40
A P
olA
xios
kop
40 P
ol
Stands
Transmitted light
(basic version)
Transmittedlight
Transmittedand reflectedlight
Transmittedlight
Transmittedand reflectedlight
Reflected light
Tubes
Binocular tube30°/23 or binoculartube with photo-port 20°/20 Pol orergotube 20°/23and other tubes ifdesired
Binocular tube withphoto port 30°/25with slider prism orwith 2 ports, TVtube mio. with 2ports and furthertubes from theAxioskop 2 pro-gram if desired
Polarizers
All polarizersexcept CircularPolarizer D
Transmitted light:Polarizer (switch-able), polarizer(rotatable with 0°and 90° stop),polarizer (switch-able with λ-plate,rotatable)Reflected light:Reflector modulePol, reflector mod-ule Pol for HBO 103
Transmitted light:Polarizer (switch-able), polarizer(rotatable with 0°and 90° stop),polarizer (switch-able with λ-plate,rotatable)Reflected light:Reflector module Pol,reflector module Polfor HBO 103
Analyzers
Analyzer slider oranalyzer slider with λ-plate
Analyzer module ormeasurement ana-lyzer with 0.1°splitting, 180°rotatable
Analyzer module oranalyzer slider oranalyzer slider withanalyzer and λ-plate, rotatable +/-10° or measure-ment analyzer with0.1° splitting, 360°rotatable
Bertrand system
Diopter or auxiliarymicroscope
Fixed focus Betrandmodule andswitchable pin holediaphragm or inter-mediate tube Polwith centerableBetrand lens;crosshair and fieldof view diaphragmin additional inter-mediate imageplanes
Intermediate tubePol with centerableBetrand lens;crosshair and fieldof view diaphragmin additional inter-mediate imageplanes
Nosepieces
6 position H
6 position Pol (5xW0.8 screw thread,1xM27 screwthread for HD DICobjective), individu-ally centerable
6 position Pol,encoded (5xW 0.8screw thread,1xM27 screwthread for HD DICobjective), individu-ally centerable
Reflector turrets
5 position, changeof Push&Click mod-ule without tools
8 position, manualor motorized,change ofPush&Click modulewithout tools
Axi
opla
n 2
imag
ing
Pol
Polarization microscopy from
Carl Zeiss
Polarization microscopy from Carl Zeiss is based on
Axioskop 40 Pol and Axioplan 2 imaging Pol. Two
powerful microscopes that are tailor-made for your
individual applications and designed to meet the
growing needs of polarization microscopy – easier
and more effectively than ever before.
Dunite thin section, transmitted light polar-
ization
Carl ZeissLight Microscopy
P.O.B. 404137030 GöttingenGERMANYPhone: ++49 551 5060 660Telefax: ++49 551 5060 464E-Mail: [email protected]
www.zeiss.de/microSubject to change
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ZEI1202_ColorChart.GB 07.11.2002 13:19 Uhr Seite 6