In the world of optics, the hunt for precision and clarity has always been a compelling and ever-evolving journey. Among the remarkable advancements, the achromatic triplet stands out as a testament to mankind's pursuit of excellence. Today, we delve into the principles and characteristics of achromatic triplets, with a special focus on the groundbreaking innovations brought to you by Hyperion Optics.

Goto CLZ to know more.

Understanding the Basics of Achromatic Triplets

Achromatic triplets are optical lens systems comprising three lenses designed to minimize chromatic aberration. By combining two lenses of different materials, the spread of wavelength-dependent focal points is significantly reduced. As a result, these triplets are ideal for applications where color correction and enhanced imaging performance are critical.

The Role of Hyperion Optics in Achromatic Triplets

Hyperion Optics, a renowned brand at the forefront of precision optics, has made significant strides in the development and manufacturing of achromatic triplets. With our expertise and state-of-the-art facilities, we have revolutionized the industry by producing achromatic lenses that exhibit exceptional color correction capabilities and optical performance.

Unveiling Hyperion Optics' Achromatic Triplet Innovations

Hyperion Optics' dedication to pushing the boundaries of optical technology is evident in their range of achromatic triplets. Utilizing advanced materials and cutting-edge manufacturing techniques, Hyperion Optics has developed achromatic lenses that offer unrivaled color correction across a wide range of wavelengths, ensuring striking clarity and precision in imaging applications.

Furthermore, Hyperion Optics' achromatic triplets boast low dispersion characteristics, enabling them to produce highly accurate images without the distortion caused by chromatic aberration. These lenses have found widespread applications in industries such as microscopy, photography, and various scientific research fields.

Advantages and Future Implications of Achromatic Triplets

Achromatic triplets have become indispensable in modern optics, and Hyperion Optics' contributions have only further strengthened their allure. The advantages of these triplets span far and wide, with enhanced color correction, reduced image distortion, and improved resolution topping the list. These benefits have opened new avenues for scientific discoveries, medical diagnostics, and high-resolution imaging across industries.

Looking ahead, the future of achromatic triplets holds immense potential. Hyperion Optics continues to invest in research and development, striving to further enhance the optical performance of their achromatic lenses. With ongoing advancements in materials, coatings, and design techniques, the realm of precision optics is poised to achieve even higher levels of precision and optical fidelity.

As we conclude our exploration of achromatic triplets, it becomes evident that these lenses have transformed the way we perceive imaging and precision optics. Hyperion Optics has played a pivotal role in introducing revolutionary achromatic triplets characterized by unparalleled color correction capabilities and exceptional optical performance. Innovations like these make us excited for what the future holds, promising ever-improving imaging technology in various industrial sectors. Next time you gaze upon a remarkable image, take a moment to appreciate the invisible marvels behind it – the achromatic triplets by Hyperion Optics.

Click for Details
[APPLIST] [APPLIST] Triplet Fiber Collimation Packages can be used for collimator-to-collimator coupling with separation distances from 50 mm to 2 m. The separation distance is the distance between the front lens' surfaces.

Features

• Prealigned for 405 nm, 532 nm, 543 nm, 633 nm, 780 nm, 850 nm, 980 nm, nm, nm, nm, or 2 µm
• Available with 6 mm, 12 mm, 18 mm, or 25 mm Effective Focal Length
• Can be Used as a Coupler or Collimator
• Full-Angle Divergence: ≤0.119° (See Tables Below for Details)
• Available with Either an FC/PC or FC/APC 2.2 mm Wide Key Connector
• Low Pointing Error
• FC/PC: 2 mrad (Max)
• FC/APC: 3 mrad (Max)
• Each Collimator Includes a Test Data Sheet
• Non-Magnetic Stainless Steel Housing

Thorlabs' Triplet Fiber Collimators use air-spaced triplet lenses that produce beam quality superior to aspheric lens collimators. The benefits of the low-aberration triplet design include an M2 term closer to 1 (Gaussian), less divergence, and less wavefront error. Detailed performance testing results comparing these triplet collimators to our fixed aspheric collimators are presented on the Performance tab.

Our triplet fiber collimators are available from stock with alignment wavelengths ranging from 405 nm to 2 μm, effective focal lengths (EFL) of approximately 6 mm, 12 mm, 18 mm, or 25 mm, and either an FC/PC or FC/APC connector. The exact focal length at the specified wavelength for each collimator is given in the tables below. Each lens in the collimator has a broadband antireflection coating (see the Coatings tab) in order to minimize losses caused by surface reflections.

In order to take full advantage of the superior beam quality, we recommend using our triplet collimators with our AR-coated single mode or polarization-maintaining fiber optic patch cables. These cables, which are available with either an FC/PC or FC/APC 2.0 mm narrow key connector, have an antireflective coating on one fiber end for increased transmission and improved return loss at the fiber-to-free-space interface.

Zemax Files Click on the red Document icon next to the item numbers below to access the Zemax file download. Our entire Zemax Catalog is also available.

These triplet collimator packages use high-precision 2.2 mm wide key connectors with tightly toleranced ceramic sleeves that provide excellent pointing repeatability, allowing the user to easily remove and replace the fiber. Please note that careful alignment is needed when mating a narrow key PM fiber with the collimator's wide key receptacle. The receptacles for the APC versions are angled so that light exiting the fiber enters the collimator perpendicular to the focal plane. All of our triplet collimators are compatible with the AD12BA, AD12F, AD12NT, KAD12F, or KAD12NT collimator mounting adapters. The longer collimators have a housing design that makes them compatible with additional adapters; triplet collimators with an EFL of approximately 18 mm are also compatible with the AD15F, AD15NT, and AD15F2 adapters, while those with an EFL of approximately 25 mm are also compatible with the AD16F and AD16NT adapters. The collimation packages with external M12 x 0.5 threading are compatible without an adapter with our cage plate CP1M12(/M) to be integrated into our 30 mm cage system.

For triplet collimators aligned to a wavelength other than what is available from stock, please contact Tech Support for additional information. Performance of each collimator over an extended wavelength range can be obtained by the using the black box Zemax files. Please see the Zemax Files tab for more information on these files.

When using these collimators as a free-space coupler, precise alignment is needed for good coupling efficiency. We recommend using a kinematic tip and tilt mount paired with an XYZ adjustable platform (such as our KM100V and MT3 (MT3/M), or our 6-axis kinematic mount paired with a lens tube coupler (K6XS with AD12F or AD16F). Additional collimator mounting adapters are also available, including Ø1/2" and Ø1" unthreaded versions and externally threaded SM05 (0.535"-40), RMS (0.800"-36), or SM1 (1.035"-40) versions. Additionally, these couplers may be used in pairs with a free-space beam between the lenses. This free-space beam can be manipulated with many types of optics prior to entering the second lens. See the Performance Tab for back-coupling efficiency graphs for these collimators.

We also offer a line of aspheric fiber collimators, including our fixed collimators and our FiberPort adjustable collimation packages, that are well suited for use with a wide range of wavelengths. For our complete line of collimation and coupling options, please see the Collimator Guide tab.

Damage Threshold Specifications Item # Suffix Damage Threshold -405
-532
-543
-633 3 J/cm2 (532 nm, 10 Hz, 10 ns, Ø408 µm) -780
-850
-980 7.5 J/cm2 (810 nm, 10 Hz, 10 ns, Ø76.9 µm) -
-
- 3 J/cm2 ( nm, 1 Hz, 10 ns, Ø268 µm) - 2 J/cm2 (2.05 µm, 10 Hz, 10 ns, Ø186 µm)

Damage Threshold Data for Triplet Collimator/Coupler AR Coatings

The specifications to the right are measured data for the antireflective (AR) coatings deposited onto the optical surface of our triplet fiber optic collimators and couplers. Damage threshold specifications are constant for a given coating type, regardless of the focal length and connector type.

Laser Induced Damage Threshold Tutorial

The following is a general overview of how laser induced damage thresholds are measured and how the values may be utilized in determining the appropriateness of an optic for a given application. When choosing optics, it is important to understand the Laser Induced Damage Threshold (LIDT) of the optics being used. The LIDT for an optic greatly depends on the type of laser you are using. Continuous wave (CW) lasers typically cause damage from thermal effects (absorption either in the coating or in the substrate). Pulsed lasers, on the other hand, often strip electrons from the lattice structure of an optic before causing thermal damage. Note that the guideline presented here assumes room temperature operation and optics in new condition (i.e., within scratch-dig spec, surface free of contamination, etc.). Because dust or other particles on the surface of an optic can cause damage at lower thresholds, we recommend keeping surfaces clean and free of debris. For more information on cleaning optics, please see our Optics Cleaning tutorial.

Testing Method

Thorlabs' LIDT testing is done in compliance with ISO/DIS  and ISO specifications.

First, a low-power/energy beam is directed to the optic under test. The optic is exposed in 10 locations to this laser beam for 30 seconds (CW) or for a number of pulses (pulse repetition frequency specified). After exposure, the optic is examined by a microscope (~100X magnification) for any visible damage. The number of locations that are damaged at a particular power/energy level is recorded. Next, the power/energy is either increased or decreased and the optic is exposed at 10 new locations. This process is repeated until damage is observed. The damage threshold is then assigned to be the highest power/energy that the optic can withstand without causing damage. A histogram such as that below represents the testing of one BB1-E02 mirror.

The photograph above is a protected aluminum-coated mirror after LIDT testing. In this particular test, it handled 0.43 J/cm2 ( nm, 10 ns pulse, 10 Hz, Ø1.000 mm) before damage. Example Test Data Fluence # of Tested Locations Locations with Damage Locations Without Damage 1.50 J/cm2 10 0 10 1.75 J/cm2 10 0 10 2.00 J/cm2 10 0 10 2.25 J/cm2 10 1 9 3.00 J/cm2 10 1 9 5.00 J/cm2 10 9 1

According to the test, the damage threshold of the mirror was 2.00 J/cm2 (532 nm, 10 ns pulse, 10 Hz, Ø0.803 mm). Please keep in mind that these tests are performed on clean optics, as dirt and contamination can significantly lower the damage threshold of a component. While the test results are only representative of one coating run, Thorlabs specifies damage threshold values that account for coating variances.

Continuous Wave and Long-Pulse Lasers

When an optic is damaged by a continuous wave (CW) laser, it is usually due to the melting of the surface as a result of absorbing the laser's energy or damage to the optical coating (antireflection) [1]. Pulsed lasers with pulse lengths longer than 1 µs can be treated as CW lasers for LIDT discussions.

When pulse lengths are between 1 ns and 1 µs, laser-induced damage can occur either because of absorption or a dielectric breakdown (therefore, a user must check both CW and pulsed LIDT). Absorption is either due to an intrinsic property of the optic or due to surface irregularities; thus LIDT values are only valid for optics meeting or exceeding the surface quality specifications given by a manufacturer. While many optics can handle high power CW lasers, cemented (e.g., achromatic doublets) or highly absorptive (e.g., ND filters) optics tend to have lower CW damage thresholds. These lower thresholds are due to absorption or scattering in the cement or metal coating.

Pulsed lasers with high pulse repetition frequencies (PRF) may behave similarly to CW beams. Unfortunately, this is highly dependent on factors such as absorption and thermal diffusivity, so there is no reliable method for determining when a high PRF laser will damage an optic due to thermal effects. For beams with a high PRF both the average and peak powers must be compared to the equivalent CW power. Additionally, for highly transparent materials, there is little to no drop in the LIDT with increasing PRF.

In order to use the specified CW damage threshold of an optic, it is necessary to know the following:

1. Wavelength of your laser
2. Beam diameter of your beam (1/e2)
3. Approximate intensity profile of your beam (e.g., Gaussian)
4. Linear power density of your beam (total power divided by 1/e2 beam diameter)

Thorlabs expresses LIDT for CW lasers as a linear power density measured in W/cm. In this regime, the LIDT given as a linear power density can be applied to any beam diameter; one does not need to compute an adjusted LIDT to adjust for changes in spot size, as demonstrated by the graph to the right. Average linear power density can be calculated using the equation below. 

The calculation above assumes a uniform beam intensity profile. You must now consider hotspots in the beam or other non-uniform intensity profiles and roughly calculate a maximum power density. For reference, a Gaussian beam typically has a maximum power density that is twice that of the uniform beam (see lower right).

Now compare the maximum power density to that which is specified as the LIDT for the optic. If the optic was tested at a wavelength other than your operating wavelength, the damage threshold must be scaled appropriately. A good rule of thumb is that the damage threshold has a linear relationship with wavelength such that as you move to shorter wavelengths, the damage threshold decreases (i.e., a LIDT of 10 W/cm at nm scales to 5 W/cm at 655 nm):

Contact us to discuss your requirements of Custom Optical Triplet Lenses. Our experienced sales team can help you identify the options that best suit your needs.

While this rule of thumb provides a general trend, it is not a quantitative analysis of LIDT vs wavelength. In CW applications, for instance, damage scales more strongly with absorption in the coating and substrate, which does not necessarily scale well with wavelength. While the above procedure provides a good rule of thumb for LIDT values, please contact Tech Support if your wavelength is different from the specified LIDT wavelength. If your power density is less than the adjusted LIDT of the optic, then the optic should work for your application. 

Please note that we have a buffer built in between the specified damage thresholds online and the tests which we have done, which accommodates variation between batches. Upon request, we can provide individual test information and a testing certificate. The damage analysis will be carried out on a similar optic (customer's optic will not be damaged). Testing may result in additional costs or lead times. Contact Tech Support for more information.

Pulsed Lasers

As previously stated, pulsed lasers typically induce a different type of damage to the optic than CW lasers. Pulsed lasers often do not heat the optic enough to damage it; instead, pulsed lasers produce strong electric fields capable of inducing dielectric breakdown in the material. Unfortunately, it can be very difficult to compare the LIDT specification of an optic to your laser. There are multiple regimes in which a pulsed laser can damage an optic and this is based on the laser's pulse length. The highlighted columns in the table below outline the relevant pulse lengths for our specified LIDT values.

Pulses shorter than 10-9 s cannot be compared to our specified LIDT values with much reliability. In this ultra-short-pulse regime various mechanics, such as multiphoton-avalanche ionization, take over as the predominate damage mechanism [2]. In contrast, pulses between 10-7 s and 10-4 s may cause damage to an optic either because of dielectric breakdown or thermal effects. This means that both CW and pulsed damage thresholds must be compared to the laser beam to determine whether the optic is suitable for your application.

Pulse Duration t < 10-9 s 10-9 < t < 10-7 s 10-7 < t < 10-4 s t > 10-4 s Damage Mechanism Avalanche Ionization Dielectric Breakdown Dielectric Breakdown or Thermal Thermal Relevant Damage Specification No Comparison (See Above) Pulsed Pulsed and CW CW

When comparing an LIDT specified for a pulsed laser to your laser, it is essential to know the following:

1. Wavelength of your laser
2. Energy density of your beam (total energy divided by 1/e2 area)
3. Pulse length of your laser
4. Pulse repetition frequency (prf) of your laser
5. Beam diameter of your laser (1/e2 )
6. Approximate intensity profile of your beam (e.g., Gaussian)

The energy density of your beam should be calculated in terms of J/cm2. The graph to the right shows why expressing the LIDT as an energy density provides the best metric for short pulse sources. In this regime, the LIDT given as an energy density can be applied to any beam diameter; one does not need to compute an adjusted LIDT to adjust for changes in spot size. This calculation assumes a uniform beam intensity profile. You must now adjust this energy density to account for hotspots or other nonuniform intensity profiles and roughly calculate a maximum energy density. For reference a Gaussian beam typically has a maximum energy density that is twice that of the 1/e2 beam.

Now compare the maximum energy density to that which is specified as the LIDT for the optic. If the optic was tested at a wavelength other than your operating wavelength, the damage threshold must be scaled appropriately [3]. A good rule of thumb is that the damage threshold has an inverse square root relationship with wavelength such that as you move to shorter wavelengths, the damage threshold decreases (i.e., a LIDT of 1 J/cm2 at nm scales to 0.7 J/cm2 at 532 nm):

You now have a wavelength-adjusted energy density, which you will use in the following step.

Beam diameter is also important to know when comparing damage thresholds. While the LIDT, when expressed in units of J/cm², scales independently of spot size; large beam sizes are more likely to illuminate a larger number of defects which can lead to greater variances in the LIDT [4]. For data presented here, a <1 mm beam size was used to measure the LIDT. For beams sizes greater than 5 mm, the LIDT (J/cm2) will not scale independently of beam diameter due to the larger size beam exposing more defects.

The pulse length must now be compensated for. The longer the pulse duration, the more energy the optic can handle. For pulse widths between 1 - 100 ns, an approximation is as follows:

Use this formula to calculate the Adjusted LIDT for an optic based on your pulse length. If your maximum energy density is less than this adjusted LIDT maximum energy density, then the optic should be suitable for your application. Keep in mind that this calculation is only used for pulses between 10-9 s and 10-7 s. For pulses between 10-7 s and 10-4 s, the CW LIDT must also be checked before deeming the optic appropriate for your application.

Please note that we have a buffer built in between the specified damage thresholds online and the tests which we have done, which accommodates variation between batches. Upon request, we can provide individual test information and a testing certificate. Contact Tech Support for more information.

[1] R. M. Wood, Optics and Laser Tech. 29, 517 ().
[2] Roger M. Wood, Laser-Induced Damage of Optical Materials (Institute of Physics Publishing, Philadelphia, PA, ).
[3] C. W. Carr et al., Phys. Rev. Lett. 91, ().
[4] N. Bloembergen, Appl. Opt. 12, 661 ().

In order to illustrate the process of determining whether a given laser system will damage an optic, a number of example calculations of laser induced damage threshold are given below. For assistance with performing similar calculations, we provide a spreadsheet calculator that can be downloaded by clicking the LIDT Calculator button. To use the calculator, enter the specified LIDT value of the optic under consideration and the relevant parameters of your laser system in the green boxes. The spreadsheet will then calculate a linear power density for CW and pulsed systems, as well as an energy density value for pulsed systems. These values are used to calculate adjusted, scaled LIDT values for the optics based on accepted scaling laws. This calculator assumes a Gaussian beam profile, so a correction factor must be introduced for other beam shapes (uniform, etc.). The LIDT scaling laws are determined from empirical relationships; their accuracy is not guaranteed. Remember that absorption by optics or coatings can significantly reduce LIDT in some spectral regions. These LIDT values are not valid for ultrashort pulses less than one nanosecond in duration.

Figure 71A  A Gaussian beam profile has about twice the maximum intensity of a uniform beam profile.

CW Laser Example
Suppose that a CW laser system at nm produces a 0.5 W Gaussian beam that has a 1/e2 diameter of 10 mm. A naive calculation of the average linear power density of this beam would yield a value of 0.5 W/cm, given by the total power divided by the beam diameter:

However, the maximum power density of a Gaussian beam is about twice the maximum power density of a uniform beam, as shown in Figure 71A. Therefore, a more accurate determination of the maximum linear power density of the system is 1 W/cm.

An AC127-030-C achromatic doublet lens has a specified CW LIDT of 350 W/cm, as tested at nm. CW damage threshold values typically scale directly with the wavelength of the laser source, so this yields an adjusted LIDT value:

The adjusted LIDT value of 350 W/cm x ( nm / nm) = 298 W/cm is significantly higher than the calculated maximum linear power density of the laser system, so it would be safe to use this doublet lens for this application.

Pulsed Nanosecond Laser Example: Scaling for Different Pulse Durations
Suppose that a pulsed Nd:YAG laser system is frequency tripled to produce a 10 Hz output, consisting of 2 ns output pulses at 355 nm, each with 1 J of energy, in a Gaussian beam with a 1.9 cm beam diameter (1/e2). The average energy density of each pulse is found by dividing the pulse energy by the beam area:

As described above, the maximum energy density of a Gaussian beam is about twice the average energy density. So, the maximum energy density of this beam is ~0.7 J/cm2.

The energy density of the beam can be compared to the LIDT values of 1 J/cm2 and 3.5 J/cm2 for a BB1-E01 broadband dielectric mirror and an NB1-K08 Nd:YAG laser line mirror, respectively. Both of these LIDT values, while measured at 355 nm, were determined with a 10 ns pulsed laser at 10 Hz. Therefore, an adjustment must be applied for the shorter pulse duration of the system under consideration. As described on the previous tab, LIDT values in the nanosecond pulse regime scale with the square root of the laser pulse duration:

This adjustment factor results in LIDT values of 0.45 J/cm2 for the BB1-E01 broadband mirror and 1.6 J/cm2 for the Nd:YAG laser line mirror, which are to be compared with the 0.7 J/cm2 maximum energy density of the beam. While the broadband mirror would likely be damaged by the laser, the more specialized laser line mirror is appropriate for use with this system.

Pulsed Nanosecond Laser Example: Scaling for Different Wavelengths
Suppose that a pulsed laser system emits 10 ns pulses at 2.5 Hz, each with 100 mJ of energy at nm in a 16 mm diameter beam (1/e2) that must be attenuated with a neutral density filter. For a Gaussian output, these specifications result in a maximum energy density of 0.1 J/cm2. The damage threshold of an NDUV10A Ø25 mm, OD 1.0, reflective neutral density filter is 0.05 J/cm2 for 10 ns pulses at 355 nm, while the damage threshold of the similar NE10A absorptive filter is 10 J/cm2 for 10 ns pulses at 532 nm. As described on the previous tab, the LIDT value of an optic scales with the square root of the wavelength in the nanosecond pulse regime:

This scaling gives adjusted LIDT values of 0.08 J/cm2 for the reflective filter and 14 J/cm2 for the absorptive filter. In this case, the absorptive filter is the best choice in order to avoid optical damage.

Pulsed Microsecond Laser Example
Consider a laser system that produces 1 µs pulses, each containing 150 µJ of energy at a repetition rate of 50 kHz, resulting in a relatively high duty cycle of 5%. This system falls somewhere between the regimes of CW and pulsed laser induced damage, and could potentially damage an optic by mechanisms associated with either regime. As a result, both CW and pulsed LIDT values must be compared to the properties of the laser system to ensure safe operation.

If this relatively long-pulse laser emits a Gaussian 12.7 mm diameter beam (1/e2) at 980 nm, then the resulting output has a linear power density of 5.9 W/cm and an energy density of 1.2 x 10-4 J/cm2 per pulse. This can be compared to the LIDT values for a WPQ10E-980 polymer zero-order quarter-wave plate, which are 5 W/cm for CW radiation at 810 nm and 5 J/cm2 for a 10 ns pulse at 810 nm. As before, the CW LIDT of the optic scales linearly with the laser wavelength, resulting in an adjusted CW value of 6 W/cm at 980 nm. On the other hand, the pulsed LIDT scales with the square root of the laser wavelength and the square root of the pulse duration, resulting in an adjusted value of 55 J/cm2 for a 1 µs pulse at 980 nm. The pulsed LIDT of the optic is significantly greater than the energy density of the laser pulse, so individual pulses will not damage the wave plate. However, the large average linear power density of the laser system may cause thermal damage to the optic, much like a high-power CW beam.

For more information, please visit Optical Glass Lenses.