IP Library Granted Patent US 8,500,276
Granted Patent B2
US 8,500,276 · App. 13/024,668 · Granted Aug 6, 2013

Non-reflective imaging optics for optical devices, particularly in opthalmology

Inventors: Jan Buchheister (Jena, DE); Lothar Müller (Ottendorf, DE); Marco Pretorius (Oberkochen, DE)
Assignee: Carl Zeiss Meditec AG
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Quick Facts
Patent No.
US 8,500,276
App. No.
13/024,668
Granted
Aug 6, 2013
Kind
B2
Abstract

Imaging optics for optical devices, with which reflections of the illumination light, which is guided through the same optical elements as the observation light, are kept from reaching the observation pupil of the imaging beam path. The non-reflective imaging optics include at least two refractive optical elements, which are utilized for illumination as well as observation. The at least two refractive optical elements are designed approximately wedge-shaped and are tilted at a random azimuth angle of at least 5° and/or are positioned off-center in the beam path to block out the single reflections of the illumination, occurring at the optical system surfaces, for the observation. The imaging optics are for optical devices, particularly in ophthalmology thought the invention is applicable to other ophthalmological devices as well as to optical devices outside of this field.

Claims (1042)

1. Non-reflective imaging optics for optical devices, in general and in ophthalmology,

comprising at least two refractive optical elements including a first refractive optical element and a second refractive optical element, which are utilized for illumination as well as observation, wherein the at least two refractive optical elements are approximately wedge-shaped and are tilted at a random azimuth angle of at least 5° and/or are positioned off-center in the beam path to completely block out single reflections of the illumination, occurring at the optical system surfaces, for the observation;

wherein at least two optical system surfaces of the at least two refractive optical elements, are designed as free-form surfaces, while remaining optical system surfaces of the at least two refractive optical elements are aspherical, toric or spherical in form.

2. Non-reflective imaging optics, according to claim 1 , wherein the optical system surfaces, designed as free-form surfaces, of the at least two refractive optical elements, which are designed approximately wedge-shaped and tilted in the beam path, are toric in form.

3. Non-reflective imaging optics, according to claim 1 , wherein exactly two refractive optical elements are designed approximately wedge-shaped and are tilted at a random azimuth angle of at least 5° and/or are positioned off-center in the beam path to completely block out single reflections of the illumination, occurring at the optical system surfaces, for the observation.

4. Non-reflective imaging optics, according to claim 1 , wherein anterior system surfaces of both refractive optical elements comprise free-form surfaces, a posterior system surface of the first refractive optical element is designed as torus, and a posterior system surface of the second refractive optical element is designed as sphere, and the overall design of the Non-reflective imaging optics is described as follows:

Surface

Radius [mm]

Thickness [mm]

Glass

Comment

SA = BQ

0.000000

127.023559

ZB

0.000000

33.434954

2 v

460.241355

40.000000

N-LAK8

XY polynomial

2 h

−112.724233

3.416369

Torus

3 v

67.330573

21.208847

N-LAK8

Sphere

3 h

−553.072593

49.259906

XY polynomial

P = IA

0.000000

17.000000Y

Ideal lens

f′ = 17 mm

R

0.000000

Position of the surfaces:

Translation of the coordinate systems:

Surface

X [mm]

Y [mm]

Z [mm]

2 v

−0.015804

−0.009449

0.000000

2 h

−0.176313

4.129852

0.000000

3 v

−1.160058

9.969841

0.000000

3 h

0.397186

4.114025

0.000000

P = IA

0.194216

2.831227

0.000000

Rotation of the coordinate systems with regard to eye pupil (in air):

Surface

Alpha [degree]

Beta [degree]

Gamma [degree]

2 v

−9.715970

−0.842779

0.000000

2 h

−14.376718

16.307588

0.000000

3 v

−9.946335

15.458494

0.000000

3 h

−11.913235

2.391050

0.000000

P = IA

1.482621

−0.261571

−0.138182

Description of the surface shapes of surfaces 2 v , 2 h , 3 h :

z

=

ρ

x

x

2

+

ρ

y

y

2

1

+

1

-

(

1

+

κ

x

)

ρ

x

2

x

2

-

(

1

+

κ

y

)

ρ

y

2

y

2

+

c

1

·

x

+

c

2

·

y

+

c

3

·

x

2

+

c

4

·

x

·

y

+

c

5

·

y

2

+

c

6

·

x

3

+

c

7

·

x

2

·

y

+

c

8

·

x

·

y

2

+

c

9

·

y

3

+

c

10

·

x

4

+

c

11

·

x

3

·

y

+

Surface 2 v :

    K x =

0.000000000E+00

    K y =

0.000000000E+00

1/ρ x =

262.029626

1/ρ y =

460.241355

c 1-3

−8.16682913E−02

  1.30744652E−02

  3.41935416E−03

c 4-6

−7.06926443E−04

  2.79954523E−03

−7.24668714E−05

c 7-9

−7.13866226E−05

−8.22329726E−05

−7.79315372E−05

c 10-12

−3.21596886E−07

  1.76630879E−07

−5.03015616E−07

c 13-15

−2.78639559E−07

−1.02664121E−06

  8.17043798E−09

c 16-18

  1.47741005E−08

  2.45319524E−08

−6.39279788E−09

c 19-21

  7.16686190E−09

−2.93771547E−09

  2.40054911E−11

c 22-24

  3.80865136E−12

  3.12139213E−10

−2.66011419E−10

c 25-27

−2.10800584E−10

  8.11033757E−11

  1.06969528E−11

Surface 2 h :

    K x =

0.000000000E+00

    K y =

0.000000000E+00

1/ρ x =

−192.389983

1/ρ y =

−112.724233

c 1-27

0.000000000E−00

Surface 3 h :

    K x =

0.000000000E+00

    K y =

0.000000000E+00

1/ρ x =

−626.781667

1/ρ y =

−553.072593

c 1-3

  1.46571567E−02

−4.19559905E−02

  2.47038454E−03

c 4-6

  1.30391601E−03

  4.05033404E−03

−1.10654287E−04

c 7-9

−1.18192140E−04

−1.08606641E−04

−1.01909142E−04

c 10-12

−9.70012347E−07

  5.68458154E−07

  3.06807937E−06

c 13-15

−1.85585147E−07

  5.49978310E−07

  1.31161920E−08

c 16-18

  2.50938306E−08

  2.12181386E−08

−4.80230112E−08

c 19-21

−4.51844849E−09

−1.37209572E−08

−2.41037488E−10

c 22-24

−9.94991837E−11

−1.48481266E−09

  3.35571849E−10

c 25-27

  5.06355656E−10

  7.62147783E−10

    3.68207235E−10.

5. Non-reflective imaging optics, according to claim 1 , wherein an anterior and a posterior system surface of the first refractive optical element, and the posterior system surface of the second refractive optical element comprise a free-form surface, and an anterior system surface of the second refractive optical element comprises an asphere and the overall design of Non-reflective imaging optics is described as follows:

Surface

Radius [mm]

Thickness [mm]

Glass

Comment

SA = BQ

0.000000

112.723657

ZB

0.000000

26.315884

2 v

460.241355

40.000000

N-LAK8

XY polynomial

2 h

−98.378083

2.432516

XY polynomial

3 v

69.369038

18.428907

N-LAK8

Asphere

3 h

−553.072593

45.324601

XY polynomial

P = IA

0.000000

17.000000Y

Ideal lens

f′ = 17 mm

R

0.000000

Position of the surfaces:

Translation of the coordinate systems:

Surface

X [mm]

Y [mm]

Z [mm]

2 v

−0.008249

−0.004878

0.000000

2 h

−3.632256

4.940808

0.000000

3 v

−7.513007

12.906752

0.000000

3 h

−6.767967

10.354774

0.000000

P = IA

−15.095604

20.046330

0.000000

Rotation of the coordinate systems with regard to eye pupil (in air):

Surface

Alpha [degree]

Beta [degree]

Gamma [degree]

2 v

−16.627633

−12.552204

0.000000

2 h

−2.975360

9.652402

0.000000

3 v

−18.533878

9.595629

0.000000

3 h

−17.902422

1.472894

0.000000

P = IA

−12.055657

−10.186383

−1.343352

z

=

ρ

x

x

2

+

ρ

y

y

2

1

+

1

-

(

1

+

κ

x

)

ρ

x

2

x

2

-

(

1

+

κ

y

)

ρ

y

2

y

2

+

c

1

·

x

+

c

2

·

y

+

c

3

·

x

2

+

c

4

·

x

·

y

+

c

5

·

y

2

+

c

6

·

x

3

+

c

7

·

x

2

·

y

+

c

8

·

x

·

y

2

+

c

9

·

y

3

+

c

10

·

x

4

+

c

11

·

x

3

·

y

+

Description of the surface shapes of surfaces 2 v , 2 h , 3 h :

Surface 2 v :

    K x =

  0.000000000E+00

    K y =

  0.000000000E+00

1/ρ x =

262.029626

1/ρ y =

460.241355

c 1-3

−1.076219235E−02

−1.939046941E−03

  1.997905625E−03

c 4-6

  1.746907059E−03

  2.461118134E−03

−6.571983437E−05

c 7-9

−9.883077652E−06

−5.445029935E−05

−1.632332880E−05

c 10-12

−3.984223970E−07

  6.025247976E−07

−3.447675743E−07

c 13-15

  6.588778570E−08

−9.912377449E−07

  6.020462360E−09

c 16-18

−1.953270172E−10

  7.786357428E−09

−1.948376196E−09

c 19-21

  7.040827309E−09

−8.579730212E−09

  1.890823354E−10

c 22-24

  1.545069767E−11

−3.939617920E−11

−1.872836301E−10

c 25-27

−1.433811680E−10

−3.180424756E−10

  5.075901345E−11

Surface 2 h :

    K x =

  0.000000000E+00

    K y =

  0.000000000E+00

1/ρ x =

−100.942861

1/ρ y =

−98.378083

c 1-3

  5.282970718E−03

−2.390734163E−02

  9.280180593E−04

c 4-6

  7.885552729E−04

−1.715965007E−03

  2.046197629E−05

c 7-9

  1.927024556E−05

  8.531615103E−05

−1.605061381E−05

c 10-12

  5.617458102E−07

  3.689124959E−07

  7.443694101E−07

c 13-15

−5.994160512E−07

  2.282951119E−07

−5.812076272E−09

c 16-18

−1.723649589E−09

−8.769239055E−09

−9.773820261E−10

c 19-21

−4.698271820E−09

−1.704652063E−08

  1.317751719E−10

c 22-24

  2.089880410E−10

  3.761425386E−10

  1.878879381E−10

c 25-27

−7.245340147E−11

−9.975912395E−11

−9.207989014E−11

Surface 3 h :

    K x =

  0.000000000E+00

    K y =

  0.000000000E+00

1/ρ x =

−626.781667

1/ρ y =

−553.072593

c 1-3

  2.487303401E−02

−6.337149712E−02

  5.842772050E−04

c 4-6

  3.650951912E−04

  3.800070084E−03

−6.340939346E−05

c 7-9

−4.948991848E−05

−1.560159975E−04

−2.586127402E−05

c 10-12

  9.681634924E−07

  9.072631039E−07

  1.675755763E−06

c 13-15

  9.789720502E−07

  5.079850594E−07

  9.057671419E−09

c 16-18

−5.038663621E−09

−6.726531096E−10

−2.375679687E−08

c 19-21

−3.868956663E−09

−1.420798036 − 08

−4.135849189E−10

c 22-24

−7.758610476E−11

−1.701714743E−09

−1.760333486E−11

c 25-27

−5.742161539E−10

−1.914559861E−11

−3.980153064E−10

Description of the surface shape of surface 3 v :

z

=

ρ

h

2

1

+

1

-

(

1

+

κ

)

ρ

2

h

2

+

k

=

1

c

k

h

2

k

+

2

    K =

  8.835330521E−02

1/ρ =

69.369038

c1-3

  0.000000000E−00

  0.000000000E−00

    0.000000000E−00.

6. Non-reflective imaging optics, according to claim 1 , wherein an anterior and a posterior system surface of the first refractive optical element, and a posterior system surface of the second refractive optical element comprise free-form surfaces, and an anterior system surface of the second refractive optical element is designed as a sphere, and an overall design of the Non-reflective imaging optics is described as follows:

Surface

Radius [mm]

Thickness [mm]

Glass

Comment

SA = BQ

0.000000

123.394223

ZB

0.000000

36.178305

2 v

460.241355

39.210908

N-LAK8

XY polynomial

2 h

−98.378083

2.041868

XY polynomial

3 v

69.665916

17.941242

N-LAK8

3 h

−553.072593

50.945958

XY polynomial

P = IA

0.000000

17.000000Y

Ideal lens

f′ = 17 mm

R

0.000000

Position of the surfaces:

Translation of the coordinate systems:

Surface

X [mm]

Y [mm]

Z [mm]

2 v

−0.011617

−0.016130

0.000000

2 h

0.974295

3.470584

0.000000

3 v

−3.363366

10.952433

0.000000

3 h

0.658348

5.474388

0.000000

P = IA

−0.182751

9.037957

0.000000

Rotation of the coordinate systems with regard to eye pupil (in air):

Surface

Alpha [degree]

Beta [degree]

Gamma [degree]

z

=

ρ

x

x

2

+

ρ

y

y

2

1

+

1

-

(

1

+

κ

x

)

ρ

x

2

x

2

-

(

1

+

κ

y

)

ρ

y

2

y

2

+

c

1

·

x

+

c

2

·

y

+

c

3

·

x

2

+

c

4

·

x

·

y

+

c

5

·

y

2

+

c

6

·

x

3

+

c

7

·

x

2

·

y

+

c

8

·

x

·

y

2

+

c

9

·

y

3

+

c

10

·

x

4

+

c

11

·

x

3

·

y

+

2 v

−11.950087

−1.103246

0.000000

2 h

−7.561127

12.292050

0.000000

3 v

−10.640443

13.236519

0.000000

3 h

−9.340704

1.838853

0.000000

P = IA

−3.992984

−0.936974

0.033760

Description of the surface shapes of surfaces 2 v , 2 h , 3 h :

Surface 2 v :

    K x =

  0.000000000E+00

    K y =

  0.000000000E+00

1/ρ x =

262.029626

1/ρ y =

460.241355

c 1-3

−7.816294472E−02

−6.769775549E−04

  3.512000519E−03

c 4-6

−1.933397623E−04

  3.323904852E−03

−7.073432239E−05

c 7-9

−5.175690025E−05

−4.246655458E−05

−5.977805266E−05

c 10-12

  1.661105408E−07

  2.387423681E−07

−2.140049981E−07

c 13-15

−2.624390743E−07

−1.155402838E−06

  5.256645482E−09

c 16-18

  1.507180023E−08

  2.590824277E−08

−9.019395714E−09

c 19-21

  8.408280778E−09

−9.933576982E−09

  1.024137839E−10

c 22-24

  8.699296183E−11

  3.577829179E−10

−2.664015377E−10

c 25-27

−1.672652883E−10

  1.189377902E−10

  5.791978628E−11

Surface 2 h :

    K x =

  0.000000000E+00

    K y =

  0.000000000E+00

1/ρ x =

−100.942861

1/ρ y =

−98.378083

c 1-3

−9.161670241E−03

−8.788093654E−02

  1.408964249E−03

c 4-6

  2.635200694E−04

−8.975033724E−04

−7.969861973E−06

c 7-9

  1.533812116E−05

  6.184418241E−05

−6.612799354E−06

c 10-12

  1.204845982E−06

−1.699698381E−07

  7.087299744E−07

c 13-15

−4.163252796E−07

  1.166367085E−07

−1.912225085E−08

c 16-18

  1.977850174E−09

−8.419477563E−09

−1.643242739E−08

c 19-21

−1.525863528E−08

−9.707951413E−09

  2.251616020E−10

c 22-24

  1.032924328E−10

  2.605738887E−10

  6.669331923E−11

c 25-27

−7.352489548E−13

  9.986952257E−12

  1.275821826E−10

Surface 3 h :

    K x =

  0.000000000E+00

    K y =

  0.000000000E+00

1/ρ x =

−626.781667

1/ρ y =

−553.072593

c1 -3

   9.589635860−04

−2.793454122E−02

  2.543402884E−03

c 4-6

  5.603206875E−04

  5.231844352E−03

   −749139943E−05

c 7-9

−1.274965695E−04

−1.490895306E−04

−8.223942953E−05

c 10-12

−7.767776527E−08

  8.031767435E−07

  2.666657937E−06

c 13-15

  1.243910582E−07

  4.703770967E−07

  2.285599114E−08

c 16-18

  2.782537511E−08

  1.728369546E−08

−4.077973829E−08

c 19-21

  2.806803694E−08

−1.355578289E−08

−3.765213129E−10

c 22-24

−1.470696533E−10

−1.629135913E−09

  1.752264004E−10

c 25-27

  3.089575802E−10

  1.268262112E−09

  −3.185215617E−10.

7. Non-reflective imaging optics, according to claim 1 , wherein three refractive optical elements are utilized, each of which is designed approximately wedge-shaped and tilted at a random azimuth angle of at least 5° and/or are positioned off-center in the beam path in order to block out single reflections of the illumination, occurring at the optical system surfaces, for the observation.

8. Non-reflective imaging optics, according to claim 7 , characterized in that at least one of the optical system surfaces of the three refractive optical elements, designed approximately wedge-shaped and tilted in the beam path, is designed as a free-form surface, while the remaining optical system surfaces of the three refractive optical elements, designed approximately wedge-shaped and tilted in the beam path, are aspherical, toric, or spherical in form.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 11, 2011
From: BUCHHEISTER, JAN; MUELLER, LOTHAR; PRETORIUS, MARCO
To: CARL ZEISS MEDITEC AG
Reel/Frame 026570/0034 →
Priority Claims (1)
DE 10 2010 008 629 · Feb 17, 2010 · national
Continuity (1)
Related Publication 20110199575A1 · Aug 18, 2011