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Learning from Giants' Mistakes in Cataract Surgery Fedorov 67 vs Fyodorov 75

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Abstract and Figures

One of the most influential papers in the history of cataract surgery is Fedorov and Kolinko's 1967 paper. All so called third and fourth generation intraocular lens calculation formulas implemented to this day are based on it. We show that the actual expression given in the 1967 article is incorrect and was subsequently corrected by Fedorov and colleagues in 1975. We show the source of error and comment on implications for modern day intraocular power calculations for cataract surgery.
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Learning from Giants’ Mistakes in Cataract Surgery
Fedorov 67 vs Fyodorov 75
Samir I Sayegh, MD, PhD, FACS, FAAO, FASRS
The EYE Center, Champaign, IL, USA
sayegh@umich.edu
Abstract
One of the most influential papers in the history of cataract surgery is Fedorov and Kolinko’s
1967 paper. All so called third and fourth generation intraocular lens calculation formulas
implemented to this day are based on it. We show that the actual expression given in the 1967
article is incorrect and was subsequently corrected by Fedorov and colleagues in 1975. We
show the source of error and comment on implications for modern day intraocular power
calculations for cataract surgery.
Introduction
Slava Fedorov’s contributions to Ophthalmology are profound and lasting. In a paper with
Albina Kolinko in 1967 they attempted a rational theoretical approach to the computation of
intraocular lens (IOL) power based on biometry of the patient’s eye1. The paper was written in
Russian and was followed by a few similar attempts by mainly European ophthalmologists. In
1975, together with Galin and Linksz, Fedorov (Fyodorov) contributed a similar article and
computation to the English literature2. This made the approach more accessible to a wider
readership and was followed by the (re)introduction of regression methods exemplified by
SRK3,4 and somewhat later, by a realization that theoretical methods were foundational and
need be adopted albeit with a grain of tweaking! This is represented by some of the major
third generation” or “vergence basedformulas such as Holladay1, SRKT and HofferQ5,6,7, all of
which cite at least one of the Fyodorov and colleagues papers and are in turn some of the most
cited and implemented papers in the IOL power calculation literature.
To our knowledge, there is no systematic comparison that has been attempted between the
1967 and 1975 versions of Fedorov and colleagues’ articles. In fact, a number of papers have
cited both the 1967 and 1975 articles without mention of any discrepancy4,6,8. Others will cite
only one9 or the other3,10,11. Some will mention a date and cite the article from the other
date12. Yet others, surprisingly, cite neither13. In the present work we start by a direct
comparison of the key formulas and their differences including numeric estimates and clinical
implications. We follow with an analysis of the original sources and the sources of errors and
draw conclusions as to lessons to be learned.
The 1967 and 1975 formulas of Fedorov and colleagues are different. One is incorrect.
1967 version1
!"#$ %&'( !
r)
* ( + ,&+
'&
-
.
* ( +
/0
&1(&+!
r
'&
2.
345
/
1975 version2
!6%& ' ( 7!8
.
7( +
/)
1(&+!8
'&
-.
359
/
where the symbols used in the corresponding articles and in our presentation are given in
tables 1 and 2 where ACD = Anterior Chamber Depth and ELP = Effective Lens Position.
Power
F67
F75
Sayegh
Cornea power
!r
!8
K
IOL power
!"#$
!:
L
EYE Power
!;<=
-
E
Table 1 Notations for Powers
Linear Measure
F67
F75
Sayegh
Sayegh-
Reduced
Axial length
*
a
a
>
Focal length
?@
-
f
A
Postoperative ACD (“ELP”)
k
k
e
B
Second principal plane to IOL
C@
-
*
D
Table 2 Notations for Distances and Reduced Distances
Our notation eliminates the use of subscripts, and while using familiar eye-specific symbols,
improves readability and makes explicit use of reduced distances. Powers are denoted by
capital Latin letters usually related to the corresponding refracting surface designation.
Distances are denoted by lower case Latin letters and the corresponding reduced distances
(distance/index of refraction) by the corresponding Greek letter.
The F67 F75 difference and some numerical comparisons
Using Sayegh’s notation, F67 can be written as
E %&1(
)
>( F,&F
'&
-
G
.
> ( F
/.
&1(&FG
/
And F75 would read in same notation
E %& 1( >G
.
>( F
/.
&1(&FG
/
& &
H
.3I/.JKLMLNLOPQRKSTU/
V
the difference D = F67-F75 can then be expressed as
W&% BG
)
'( 1
'
-
.
> ( F
/.
1(BG
/.
W
/
Numerical examples are illustrated in Figure 1 where
W
is plotted as a function of the
postoperative ACD or ELP. For example, using a 3.2 mm anterior chamber depth, the average
reported by the authors, and for average values of keratometry and axial length, one finds a D
just short of 2 D between F67 and F75 with F67 ~ F75 + 2 D. Given that the F75 is the correct
derivation it is interesting to notice that the 67 paper comments that it is best to leave the
patients with 1-2 D of myopia as they will have no accommodation left1. Note that D is a strictly
increasing function of ELP and nearly doubles for an IOL placed in the bag of a “typical” eye.
Figure 1 The difference in diopters between the IOL power prediction of Fedorov 1967 and Fyodorov 1975
1967 Fedorov and Kolinko approach and error. Sources and sources of error.
F67 relies on and cites findings from the 1950 edition of a Russian language physiological optics
work by Kravkov (Кравков)14. The relations used are identical to those in Gullstrand 1909 and
191115. The approach of Fedorov 1967 boils down to the following: Treat the pseudophakic eye
as a “thick lens” with the first refractive surface being the cornea and the second the IOL.
Express the power of that eye in two ways. One as the combination of the power of the cornea
and that of the IOL, with the “thickness” being the postoperative ACD. The other as being the
inverse of the focal length (i.e. the reduced second principal plane distance from the retina),
which is expressed in terms of quantities including the axial length. Equating these two forms
for the power of the eye yields the expression of the IOL power in terms of axial length,
postoperative ACD, corneal power, and index of refraction of the aqueous/vitreous.
In more detail, what is done is the following.
1) Use the thick lens equation with the cornea and IOL as the two powers being combined
and the (postoperative) anterior chamber depth as the “thickness” of the combination
thick lens. The thick lens relation is referenced to Kravkov book p. 38. This approach
results in an expression for the power of the eye as a function of the powers of cornea
and IOL, the anterior chamber depth, and the index of refraction.
Referring to tables 1 and 2 and the description above, we have 3 powers and 4 reduced
lengths for a total of 7 variables. We can now write, in our compact notation, the two
equations involving the power of the eye:
X % G , E ( &F&G&E
0
.1/
(YZ[\+&*]'^&]_`7Y[a'
2
And:
X % 1
A&
.
b
/
(
.
?a\7*&*]'cYZ ( dae]f&f]*7Y[a'
/
2) Draw a diagram with 4 surfaces, A, B, C, D with A being the cornea plane and D the
retina plane with C being the IOL plane and B the second principal plane of the eye
(Figure 2).
Figure 2 Ada pted from Fedorov 67 with typos corr ected in green
Simple geometry shows
&&&&&&&&&&&&&&&&&g! %h!(hi ,gi
Or,
&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&?@% * ( + ,&C@
Where l is the axial length and k is the anterior chamber depth. In our compact notation:
? % 7 ( ], *
Or, equivalently, after division by the index of refraction
'
:
A % > ( F , D
.
j
/
3) In Fedorov 1967 article
?@
and
C@
are then expressed in terms of relationships known to
relate the powers and distances to the principal planes’ distances. Kravkov’s book14 has
a discussion of this based partially on Gullstrand’s contribution in von Helmholzthird
edition of Physiological Optics (1909) and his 1911 monograph15. The main error in
Fedorov’s paper is introduced at this stage and the error is misinterpretation of a
formula in Kravkov and using a length instead of a reduced length (Figure 3). It is worth
noting that this 1967 paper by Fedorov is not cited in Fedorov 19752.
Finally, we express
D
in terms of the fraction of
F
:
D %&G
X&F
.
k
/
With four equations (1-4) we can, out of the 7 variables, eliminate 3, namely, E,
AlD
, leaving us
with one relation between the 4 remaining variables, L, K,
>
and
F
and we can thus express L in
terms of the other 3 variables as follows:
E %& 1
> ( F1(>G
1(FG
.
3I
/
This is trivially equivalent to F75 but not to F67. In Figure 3 we illustrate the error and the
correction that leads to results equivalent to F75.
Figure 3 Ada pted from Fedorov 67 with typos corrected in green and errors in red
The thick lens equation in its modern form can be attributed to Gauss16. More recent
treatments (prior to and following the Fedorov publications) can be easily found in the Optics
literature, from monumental foundational work17,18 to very useful practical manuals19. Prior to
the 1967 article, reviews of the classic Born and Wolf Optics text were already appearing
including in the biology literature.20
Discussion
Fedorov and Kolinko’
^
foundational equation as formulated in 1967 is a simple yet profoundly
insightful and influential approach to the calculation of the power of IOLs, yet it is incorrect. It
has been praised and cited for decades by generations of leading ophthalmologists that
proceeded to build on their legacy. The apparent lack of awareness or mention of the
differences between the 1967 version and the 1975 is stunning! This may be due to the fact
that the article was in Russian and published in the Russian literature. This is only partially
reasonable since there was a significant interest in “monitoring” Russian publications at the
height of the Cold War21 and even decades earlier keen interest in the scientific Russian
literature had already developed22. It is also worth mentioning that even current Russian
Ophthalmology literature continues to refer to that paper as foundational23.
Dogmatic views have sometimes persisted in Ophthalmology and in Medicine. Fairly recent
examples from cataract surgery include the A constantthat has “no units” (AAO Basic and
Clinical Sciences, Lens and Cataract, various earlier editions, and persistent in recent quotes 24
despite clarifications 25) and the “constant” 30 degrees rotation for total loss of astigmatism
corrected by a toric IOL, and shown to be variable, implicitly by Felipe et al26 and explicitly by
Sayegh27. Various beliefs, rather than rigorous insight, continue to pervade the medical and
ophthalmological communities including a rising belief that artificial intelligence methods are all
powerful and can be a substitute for rigorously established scientific methodologies. It is
imperative to debunk such naïve beliefs and make sure that the rising generation of
ophthalmologists and vision scientists are schooled in the most rigorous intellectual tradition.
It is undeniable that the work by Fedorov and Kolinko constitutes one of the pillars of a
paradigm shift that, along with high quality intraocular lenses delivered through smaller
incisions and a number of other innovations, moved cataract surgery from a risk prone
procedure with moderate outcomes to one of the most sophisticated and successful
procedures in the history of Medicine12,28. This shift took place mainly in the last quarter of the
20th century and is ongoing. To continue building on this success it behooves us to reach a full
assimilation of the process it took to get where we are and delve into the methods and their
derivations. Maintaining a healthy centuries-old intellectual and scientific tradition is also likely
to accelerate our future progress towards better results for our patients.
Fully understanding giants’ mistakes, while standing on their shoulders, is a most valuable
building block of our next glorious pyramid!
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ResearchGate has not been able to resolve any citations for this publication.
Preprint
Full-text available
Purpose: To demonstrate that the total loss of astigmatism as a consequence of misalignment or rotation of a toric intraocular lens (tIOL) can occur much earlier than the widely believed and taught 30 degrees. To give a precise surgically useful estimate of that value. To clarify the role of mismatch and misalignment of toric intraocular lenses in cataract surgery beyond what is commonly recognized in the literature and make corresponding surgical recommendations. Setting: Private Practice and Research Center. The EYE Center. Champaign, IL, USA. Design: Formal Analytical Study Methods: The astigmatism addition approach is used in its simplest form along with analytical tools to derive new results concerning mismatch, misalignment and rotation of toric intraocular lenses. Results: The often stated results of total loss of astigmatic correction by 30-degree rotation and 3.3 % loss per degree represent a usually poor approximation to realistic surgical cases. We show how they constitute a very special case in the context of a more general framework relevant to procedures performed by refractive cataract surgeons dealing with the surgical correction of astigmatism with tIOLs. Total loss of astigmatic correction can occur with as little as 20 degrees of misalignment and less than 10 degrees of tIOL rotation. A practical approximation for that angle of doom, Δ, in the surgically relevant range can be expressed by Δ ≈ 30 − 15 ω degrees, where ω = (L − A) ÷ A is the fractional overcorrection of L, the cylinder of the tIOL, and A, the astigmatism to be corrected. Similarly for undercorrection we show that Δ ≈ 30 + 15 μ degrees where μ = (A − L) ÷ A represents the corresponding fractional undercorrection. That is to say the angle of doom is extended beyond the 30 degrees for cases of undercorrection of the astigmatism. We also demonstrate that overcorrection of astigmatism results in a significantly faster decline in astigmatism correction per degree of misalignment/rotation. The significant clinical implications and surgical recommendations, including for optimal degree of overcorrection, are a natural consequence of these novel results. Conclusions: Total loss of astigmatism correction can occur at a significantly smaller angle than commonly believed and overcorrected astigmatism residual rises with tIOL misalignment or rotation significantly faster than undercorrected astigmatism. We provide the methodology and explicit solution for determining this behavior.
Book
Cambridge Core - Electronic, Optoelectronic Devices, and Nanotechnology - Principles of Optics - by Max Born
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To analyze changes in the eye's refractive properties when a toric intraocular lens (IOL) rotates. Fundación Oftalmológica del Mediterráneo, Valencia, Spain. Experimental study. The matrix definition of astigmatism was used in this theoretical study and compared with another vector representation. Two methods were compared: (1) The cylinder, C, resulting from the addition of 2 cylinders C(1) and C(2) whose axes form an angle a, is obtained by the addition of 2 vectors of values C(1) and C(2) forming an angle 2a; (2) the power matrix, F, of a thin astigmatic dioptric system that decomposes naturally into 3 orthogonal components: the purely spherical part F(nes,) the ortho-astigmatism F(or), and oblique astigmatism F(ob). The residual cylinder was one third of the corneal astigmatism when a toric IOL rotated ±10 degrees when the cylinder values for the cornea (C(1)) and IOL (C(2)) were equal. Nevertheless, in most cases C(1) is greater than C(2); therefore, the residual astigmatism did not change noticeably with small rotations. The angle of rotation, b, which annuls the astigmatism correction, could be obtained from the following: cos(π + 2b) = -r/2, with r being the ratio between the IOL and cornea cylinders. The 2 methods gave equivalent results. When the IOL cylinder had a value different from that of the corneal astigmatism, a better choice would be a lower, rather than higher, cylinder value to reduce residual astigmatism. In general, toric IOL rotations less than 10 degrees changed the eye's refraction less than 0.50 diopter. Thus, small axis rotations are not an obstacle for satisfactory astigmatism correction with toric IOLs. No author has a financial or proprietary interest in any material or method mentioned.
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A three-part system that determines the correct power for an intraocular lens (IOL) to achieve a desired postoperative refraction is presented. The three components are (1) data screening criteria to identify improbable axial length and keratometry measurements, (2) a new IOL calculation formula that exceeds the current accuracy of other formulas for short, medium, and long eyes, and (3) a personalized "surgeon factor" that adjusts for any consistent bias in the surgeon's results, from any source, based on a reverse solution of the new formula; the reverse solution uses the postoperative stabilized refraction, the dioptric power of the implanted IOL, and the preoperative corneal and axial length measurements to calculate the personalized surgeon factor. The improved accuracy of the new formula was proven by performing IOL power calculations on 2,000 eyes from 12 surgeons and comparing the results to seven other currently used formulas.
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