This paper presents a new graphical method for selecting a pair of optical glass and housing materials to simultaneously achromatize and athermalize a multilens system composed of many elements. To take into account the lens spacing and housing, we quantify the lens power, chromatic power, and thermal power by weighting the ratio of the paraxial ray height at each lens to them. In addition, we introduce the equivalent single lens and the expanded athermal glass map including a housing material. Even though a lens system is composed of many elements, we can simply identify a pair of glass and housing materials that satisfies the athermal and achromatic conditions. Applying this method to design a black box camera lens equipped with a 1/4inch image sensor having a pixel width of 2 μm, the chromatic and thermal defocusings are reduced to less than the depth of focus, over the specified ranges in temperature and frequency.
I. INTRODUCTION
In modern optical instruments such as mobile and black box cameras, plastic materials are widely used. The merits of plastic material include its being light, cheap, and easy to mold into aspherical surfaces. Because of its inherent temperature sensitivity, however, variation in ambient temperature significantly induces changes in refractive index, curvature of the lens, and thickness rather than glass. Since the thermal defocusing caused by such changes degrades image quality, a lens system using plastics should be designed to have stable performance over a specified temperature range.
defocusings, which are mainly induced by the large variations of refractive index with temperature and wavelength. In the infrared waveband, many design methods to reduce these defocusings have been reported
[1

3]
. However, these methods have difficulties in finding proper combinations of materials and lens powers.
As an alternative approach to overcome these problems, a graphical method has been developed
[4

7]
. Although this method is robust, it requires a complex process and calculations to achieve an athermalized and achromatized system having more than three elements. To solve these difficulties, another graphical selection method for optical materials, using an athermal glass map and equivalent single lens, has been developed
[8]
. This method is useful for finding proper combinations of materials for an athermal and achromatic system with multiplelenses in contact. Because it does not take into account the lens spacing and housing, however, approximate solutions are obtained.
To consider the lens spacing and housing, in this paper we quantify the lens power, chromatic power, and thermal power by weighting the ratio of the paraxial ray height at each lens to them. In addition, we introduce the equivalent single lens and the expanded athermal glass map including a housing material
[6

8]
. Even though a lens system is composed of many elements, we can simply identify a pair of materials that satisfies the athermal and achromatic conditions by selecting the corresponding materials from an expanded athermal glass map.
By applying this method to design a black box camera lens composed of one glass and four plastic elements, a good solution having small chromatic and thermal defocusings is obtained.
II. ATHERMAL AND ACHROMATIC CONDITIONS
For a single thin lens of power
ϕ_{i}
and Abbe number
v_{i}
, the thermal power
γ_{i}
and chromatic power
ω_{i}
are given as follows
[5
,
6]
:
where
n_{i}
is the refractive index at the center wavelength,
α_{i}
is the lens material’s coefficient of thermal expansion (CTE), and
T
is the temperature. In some papers, chromatic power is designated as an inverse Abbe number (1/
v
), and thermal power as a thermal glass constant
[4
,
8]
.
Figure 1
illustrates an optical system composed of
k
thin lenses, in which
L_{i}
denotes the
i
th lens with power
ϕ_{i}
, chromatic power
ω_{i}
, and thermal power
γ_{i}
. In that figure,
h_{i}
and
h_{k}
are the paraxial ray heights at the
i
th and final lenses respectively, and the focal plane of the system is assumed to be fixed to the lens housing. In a real optical system, there are a housing structure and spacings between lenses, but previous studies proposed achromatic and athermal conditions that did not take into account the expansion of the housing or spacings between lenses
[7
,
8]
. In this study, to solve these problems the lens power, chromatic power, and thermal power are defined by weighting the ratio of the paraxial ray height at each lens to them:
Reconfiguration of an optical system due to a temperature change.
In such an optical system with an arbitrary number of elements, the following equations must be satisfied for axial color to be corrected
[5

11]
:
The thermal defocusing can be expressed as the difference between the thermal expansion of the housing and the change in back focal length (Δ
f_{b}
) with temperature. Therefore, for the system to be athermal, being mounted in a housing with a CTE of
α_{h}
the system must also satisfy the following equation:
where
L
is the flange back distance of the mechanical structure
The athermal and achromatic conditions for a doublet are given by
For a doublet to be achromatic, each element must have the power given in Eq. (9) by solving the Eqs. (6) and (7), as follows:
Inserting Eq. (9) into Eq. (8) results in an expression for the athermal and achromatic conditions for a doublet:
Assuming that the flange back distance is approximately equal to the back focal length, i.e.
, then the athermal and achromatic conditions given by Eq. (10) are rewritten as follows:
III. EXPANDED ATHERMAL GLASS MAP AND EQUIVALENT SINGLE LENS
 3.1. Expanded Athermal Glass Map
Figure 2
shows the expanded athermal glass map that plots chromatic power on the horizontal axis and thermal power on the vertical axis for a housing material; these powers are weighted by the relative paraxial ray heights. From the athermal glass map and Eq. (11), we can visually identify two materials that satisfy the athermal and achromatic conditions.
Expanded athermal glass map.
In an expanded athermal glass map, if two materials of
M′
_{1}
and
M′
_{2}
are assumed to provide an athermal and achromatic system, then the line connecting two materials crosses the
y
axis at the
y
intercept
. To prove this, consider the equation for a line,
y
=
ax
+
b
. First, substitute the slope in the two given data points
M′
_{1}
(
ω′
_{1}
,
γ′
_{1}
) and
M′
_{2}
(
ω′
_{2}
,
γ′
_{2}
):
Then, rearranging Eq. (12) to solve for
b
gives the expression
Next, rearranging Eq. (11) results in an expression for
, as follows:
From Eqs. (12) to (14), we see that the line
y
=
ax
+
b
has a
y
intercept of
and a slope of
Thus, in an expanded athermal glass map, two materials can be selected to satisfy the athermal and achromatic conditions on the line connecting them, which is given by
From Eq. (15) we see how simple and intuitive it is to include the housing material. When two materials are given, unlike some of the previous methods
[5

8]
, the proposed method can be used to visually determine exactly what CTE of the housing is required to athermalize and achromatize a system. Meanwhile, if any material
M′
_{1}
(
ω′
_{1}
,
γ′
_{1}
) and housing are given, then the counterpart material
M′
_{2}
(
ω′
_{2}
,
γ′
_{2}
) can be determined to satisfy the athermal and achromatic conditions of Eq. (11).
 3.2. Equivalent Single Lens
An athermal and achromatic doublet can be simply obtained from Eq. (11), but a very complicate process is required to have a lens system with many elements be athermal and achromatic simultaneously
[4

7]
. In this study, a lens system with many elements is substituted by an equivalent single lens that has the equivalent power, equivalent chromatic power, and equivalent thermal power. This equivalent single lens is useful in selecting a pair of glasses on the athermal glass map, like a doublet
[8]
.
To consider the spacings between lenses, the equivalent lens power
ϕ_{e}
, equivalent chromatic power
, and equivalent thermal power
are expressed by summing the contribution of each lens, weighted by the ratio of the paraxial ray heights at each lens:
Although this is a multilens system, from Eqs. (17) and (18), its chromatic and thermal powers can be obtained simply. Thus, this equivalent single lens reduces the problem to that of a twoelement system as a doublet. Consequently, a pair of materials that satisfies Eq. (11) can graphically be selected to simultaneously achromatize and athermalize an imaging lens. Unlike previous methods using a complex process
[5

7]
, we can use this method to visually determine exactly what materials and housing are required to achromatize and athermalize a multilens system.
IV. ATHERMAL AND ACHROMATIC DESIGN EXAMPLE USING EXPANDED ATHERMAL GLASS MAP AND EQUIVALENT SINGLE LENS
 4.1. Analysis of a Starting Lens
A black box camera lens composed of two glasses and three plastics (2G+3P), equipped with a 1/4inch image sensor having a pixel width of 2 μm, is given as a starting point, as shown in
Fig. 3
[12]
. This patented lens has an
f
number of F/2.64, focal length of 2.2953 mm, and field of view of 90º. The depth of focus
δ
of this lens is given by
[11]
:
Layout of a patented lens for a black box camera.
This lens has small variations in back focal length (ΔBFL) and flange back distance (ΔFBD) from −40℃ to 80℃: ΔBFL = ±3.39 μm and ΔFBD = ∓3.22 μm, as shown in
Fig. 4
. The change in effective focal length, ΔEFL = ±18.05 μm, is greater than the depth of focus. Note that the signs of ΔBFL and ΔEFL are opposite that of ΔFBD, which induces additional thermal defocusing at extreme temperature. The modulation transfer function (MTF) is unstable at both extreme temperatures, as shown in
Fig. 9(a)
.
Thermal shifts of a patented lens for effective focal length (EFL), back focal length (BFL), and flange back distance (FBD).
A comparison of the MTF at 180 lp/mm with temperature. (a) Patented lens, (b) athermal and achromatic lens.
This patented lens partially fulfills the requirements of a black box camera over the specified temperature range; however, it consists of two expensive glasses. Because the plastic material has advantages over glass in cost and aspheric molding, in this research we replace the front glass (NSK16) with plastic (E48R) having similar index and Abbe number. Consequently, this lens has the configuration of one glass (
L
_{4}
) and four plastic elements, instead of 2G+3P.
Figure 5
illustrates this temporary lens, which still has not been corrected for color and thermal errors. In this study the achromatic and passively athermalized design will be discussed to graphically select the material of the positively powered lens
L
_{4}
, using an expanded athermal glass map.
Layout of a temporary lens for black box camera design.
 4.2. Graphical Selection of a Material Pair and Optimized Design
Figure 6
shows the expanded athermal glass map plotted for visible Schott and Ohara glasses, including housing material AL6061 (
α_{h}
= 23.4 × 10
^{−6}
/℃)
[8
,
13

16]
. In the temporary lens of
Fig. 5
, there are five combinations for an equivalent single lens: case 1 (
L
_{1234}
), case 2 (
L
_{1235}
), case 3 (
L
_{1245}
), case 4 (
L
_{1345}
), and case 5 (
L
_{2345}
). To have the configuration of one glass plus four plastics, among five combinations, case 2 is uniquely selected; the other four combinations contain two glasses plus three plastics. Thus, four elements of
L
_{1}
,
L
_{2}
,
L
_{3}
, and
L
_{5}
are chosen such that they create an equivalent single lens. This equivalent lens is then used to determine the material of the fourth element
L
_{4}
, to realize an athermal and achromatic system. The chromatic power
and thermal power
of an equivalent single lens in case 2 are calculated from Eqs. (17) and (18):
Graphical selection of a glass material on an expanded athermal glass map.
The equivalent single lens having
and
given in Eqs. (20) and (21) is located at
in
Fig. 6
. By connecting this point
to the yintercept of
with a line, the material of the fourth element
L
_{4}
can be selected from the glasses lying on this line, satisfying both athermal and achromatic conditions. From case 2 of
Fig. 6
, the glass of the fourth element is graphically selected to be SFPL53 from Ohara. This material combination also satisfies Eq. (11).
After replacing the fourth element’s glass with SFPL53, the temporary lens has been reoptimized using CodeV. Finally, a black box camera lens having good performance is obtained, as shown in
Fig. 7
. The thermal shifts of this lens are significantly reduced, as illustrated in
Fig. 8
. The variations of effective focal length, back focal length, and flange back distant over −40℃ to 80℃ are ΔEFL = ∓10.21 μm, ΔBFL = ∓6.69 μm, and ΔFBD = ∓3.49 μm respectively. Note that here the signs of ΔBFL and ΔEFL are the same as that of ΔFBD, which reduces the thermal defocusings over the whole range of temperatures. Thus, all thermal shifts due to temperature are less than the depth of focus. The chromatic focal shift between C and Flines is reduced to 1.45 μm, less than the 5.83 μm of the starting patented lens. In conclusion, the designed lens is achromatic in visible light and passively athermalized over the range −40℃ to 80℃.
Layout of an athermal and achromatic lens for a black box camera.
Thermal shifts of an athermal and achromatic lens for effective focal length (EFL), back focal length (BFL), and flange back distance (FBD).
Figure 9
shows the modulation transfer functions (MTFs) of two lenses with temperature. The MTF of the lens designed from athermal and achromatic process, even though its front element has been replaced with plastic, is much more stable than that of the starting patented lens over the specified temperature range. Also, the MTF at maximum frequency of 180 lp/mm is greater than 36% over all fields. The final lens design for a black box camera has an
f
number of 2.64, focal length of 2.2953 mm, and stable chromatic and thermal focusing. Consequently, this lens has sufficient performance to fulfill the requirements of a modern camera.
V. CONCLUSION
To realize an achromatic and athermal multilens system, the lens spacing and housing have been taken into account in plotting an expanded athermal glass map. By graphically selecting the corresponding materials from an expanded athermal glass map, we can simply identify a pair of optical and housing materials that satisfies the athermal and achromatic conditions. By utilizing this method to design a black box camera lens with five elements, a good solution having small chromatic and thermal defocusings has been found. The chromatic focal shift is 1.45 μm between C and Flines, and the thermal defocusings over −40℃ to 80℃ are found to be less than the depth of focus. This lens is consequently achromatized and passively athermalized. In conclusion, this graphical method for selecting materials is expected to serve as a simple and powerful way to find design solutions.
Jamieson H.
1981
“Thermal effects in optical systems,”
Opt. Eng.
20
156 
160
Rogers P. J.
1990
“Athermalized FLIR optics,”
Proc. SPIE
1354
742 
751
Kurbitz G.
1991
“Automatic active athermalization of infrared optical systems,”
Proc. SPIE
1540
612 
621
Rayces L.
,
Lebich L.
1990
“Thermal compensation of infrared achromatic objectives with three optical materials,”
Proc. SPIE
1354
752 
759
Tamagawa Y.
,
Wakabayashi S.
,
Tajime T.
,
Hashimoto T.
1994
“Multilens system design with an athermal chart,”
Appl. Opt.
33
8009 
8013
DOI : 10.1364/AO.33.008009
Tamagawa Y.
,
Tajime T.
1996
“Expansion of an athermal chart into a multilens system with thick lenses spaced apart,”
Opt. Eng.
35
3001 
3006
DOI : 10.1117/1.600984
Schwertz K.
,
Dillon D.
,
Sparrold S.
2012
“Graphically selecting optical components and housing material for color correction and passive athermalization,”
Proc. SPIE
8486
84860E 
Kim Y. J.
,
Kim Y. S.
,
Park S. C.
2015
“Simple graphical selection of optical materials for an athermal and achromatic design using equivalent abbe number and thermal glass constant,”
J. Opt. Soc. Korea
19
182 
187
DOI : 10.3807/JOSK.2015.19.2.182
Liu Y.
,
Sun Q.
,
Lu Z.
,
Yue J.
,
Zhang H.
,
Zhu R.
2009
“Athermal design of hybrid refractive/harmonic diffractive optical system for farinfrared multiband,”
Proc. SPIE
7282
72823Q 
Gao D.
,
Fu Q.
,
Zhao Z.
,
Zhao B.
,
Zhong L.
,
Zhan J.
2014
“Design of polarized infrared athermal telephoto objective for penetrating the fog,”
Proc. SPIE
9300
93001W 
Rogers P. J.
,
Roberts M.
2009
Handbook of Optics
3rd ed
McGrawHill
New York, USA
“Thermal compensation techniques,”, Chapter 8
Lee D. J.
2012
“Wideangle lens system for visible ray and near infrared rays,”
Korea Patent
1013564030000
2012
Optical Glass Catalogue Excel
Schott Inc.
Germany
2008
Schott Technical Information
Schott Inc.
Germany
“TIE19: Temperature coefficient of the refractive index,”
2012
Optical Glass Catalog Excel
Ohara Inc.
Japan
Baumer S.
2010
Handbook of Plastic Optics
2nd ed
WILEYVCH
Germany
Chapter 5