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N-BK7 Mounted Spherical Singlet Lens Kits


  • Plano-Convex, Plano-Concave, Bi-Convex, and Bi-Concave Kits
  • Offered Uncoated or with an AR Coating
  • Ø1/2", Ø1", or Ø2" Options

Lenses and Cases
are Clearly Labeled

LSC01

Related Items


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Spherical Singlet Lens Kit Selection Guide
Mounted N-BK7
Unmounted N-BK7
Mounted UV Fused Silica
Mounted Calcium Fluoride (CaF2)
Damage Thresholds
-A Coating 7.5 J/cm2 (532 nm, 10 ns, 10 Hz, Ø0.504 mm)
-B Coating 7.5 J/cm2 (810 nm, 10 ns, 10 Hz, Ø0.144 mm)
-C Coating 7.5 J/cm2 (1542 nm, 10 ns, 10 Hz, Ø0.123 mm)
Mounted Spherical Singlet Photo

Features

  • N-BK7 Mounted Spherical Singlets Packaged into Kits
  • Kits Contain Ø1/2", Ø1", or Ø2" Lenses
  • Available Uncoated or with One of Three AR Coatings
    • -A (350 - 700 nm)
    • -B (650 - 1050 nm)
    • -C (1050 - 1620 nm)
  • Surface Quality: 40-20 Scratch-Dig
  • Each Lens Housing is Laser Engraved and SM Compatible
  • Offered at a Savings Over Purchasing the Lenses Individually

Thorlabs has taken its most popular Ø1/2", Ø1", and Ø2" N-BK7 spherical singlet lenses, housed them in laser-engraved SM-compatible lens tubes, and packaged them into kits. Each kit combines various lenses from our plano-convex, plano-concave, bi-convex, and/or bi-concave lines.

The lenses, which are laser quality with a 40-20 scratch-dig surface finish to ensure minimal scattering, are available uncoated or with one of three broadband antireflection coatings: -A for the 350 - 700 nm range, -B for the 650 - 1050 nm range, or -C for the 1050 - 1620 nm range. See the Graphs tab for detailed coating information.

Each black anodized lens housing features external SM05 (0.535"-40), SM1 (1.035"-40), or SM2 (2.035"-40) threading, making it directly compatible with the multitude of Thorlabs mounts and housings that feature this thread standard. In addition, the housings are laser engraved with the item number, lens type, focal length, and antireflection coating range (if applicable).

In addition to the mounted N-BK7 lenses featured here, Thorlabs also offers a line of unmounted, N-BK7 spherical singlets with either a -A (350 - 700 nm) or -B (650 - 1050 nm) antireflection coating as well as a line of mounted, UVFS spherical singlets that are either uncoated or have a UV AR coating for the 290 - 370 nm range deposited on both sides.

Lens Type Function
Plano Convex Plano-Convex lenses have a positive focal length and near-best-form shape for infinite and finite conjugate applications. They can be employed to converge collimated beams or collimate light from a point source. To minimize the introduction of spherical aberration, a collimated light source should be incident on the curved surface of the lens when being focused and a point light source should be incident on the planar surface when being collimated. They are best used where one conjugate point (object distance S or image distance S') is more than five times the other.
Bi Convex Bi-Convex lenses have a positive focal length and are most suitable for use when the object and image are on opposite sides of the lens and the ratio of the object-to-image distance (conjugate ratio) is between 0.2 and 5.0.
Plano Concave Plano-Concave lenses have a negative focal length and are typically used to cause a collimated beam to diverge as in a Galilean-type beam expander or telescope. Since the spherical aberration of the plano-concave lens is negative, it can be used to balance the aberration of the other lenses.
Bi Concave Like plano-concave lenses, bi-concave lenses have negative focal lengths and can be used to increase the divergence of a beam of light. They are best suited for situations where the incident beam of light is converging.
Positive Meniscus Positive meniscus lenses are designed to minimize spherical aberration. One surface of the lens is convex, while the other surface is concave. When used in combination with another lens, a positive meniscus lens will shorten the focal length, and increase the NA of the system. These lenses are commonly used to achieve tighter beam focusing when paired with another positive lens.
Negative Meniscus Negative meniscus (convex-concave) lenses, which are thinner in the middle than at the edges and cause light rays to diverge, are designed to minimize third-order spherical aberration. They are often used in conjunction with other lenses to increase the focal length, and therefore decrease the numerical aperture (NA), of an optical assembly.

The following tables display all of the lenses included with the lens kits sold on this page. Click "More" to see the full list of lenses included with each kit. Once expanded, each lens item number in the table can be clicked to view our standard support documents, more product information, and individual purchasing options.

Ø1/2" N-BK7 Spherical Singlet Lens Kits

LSA01 Uncoated Ø1/2" Mounted Singlet Lens Kit
LSA01-A Ø1/2" Mounted Singlet Lens Kit (ARC: 350 - 700 nm)
LSA01-B Ø1/2" Mounted Singlet Lens Kit (ARC: 650 - 1050 nm)
LSA01-C Ø1/2" Mounted Singlet Lens Kit (ARC: 1050 - 1620 nm)
  • Reciprocal of Focal Length in Meters
  • Due to substrate limitations, these lenses are instead made from N-SF11 glass, which has greater dispersion than N-BK7. For more information, please visit our Optical Substrates page.
  • This lens is only available as part of a kit. Please contact tech support to purchase this lens individually.

Ø1" N-BK7 Plano-Convex Spherical Singlet Lens Kits

LSB01 Uncoated Ø1" Plano-Convex Mounted Singlet Lens Kit
LSB01-A Ø1" Plano-Convex Mounted Singlet Lens Kit (ARC: 350 - 700 nm)
LSB01-B Ø1" Plano-Convex Mounted Singlet Lens Kit (ARC: 650 - 1050 nm)
LSB01-C Ø1" Plano-Convex Mounted Singlet Lens Kit (ARC: 1050 - 1620 nm)
  • Reciprocal of Focal Length in Meters

Ø1" N-BK7 Bi-Convex Spherical Singlet Lens Kits

LSB02 Uncoated Ø1" Bi-Convex Mounted Singlet Lens Kit
LSB02-A Ø1" Bi-Convex Mounted Singlet Lens Kit (ARC: 350 - 700 nm)
LSB02-B Ø1" Bi-Convex Mounted Singlet Lens Kit (ARC: 650 - 1050 nm)
LSB02-C Ø1" Bi-Convex Mounted Singlet Lens Kit (ARC: 1050 - 1620 nm)
  • Reciprocal of Focal Length in Meters

Ø1" N-BK7 Plano- and Bi-Convex Spherical Singlet Lens Kits

LSB03 Uncoated Ø1" Bi-Convex Mounted Singlet Lens Kit
LSB03-A Ø1" Bi-Convex Mounted Singlet Lens Kit (ARC: 350 - 700 nm)
LSB03-B Ø1" Bi-Convex Mounted Singlet Lens Kit (ARC: 650 - 1050 nm)
LSB03-C Ø1" Bi-Convex Mounted Singlet Lens Kit (ARC: 1050 - 1620 nm)
  • Reciprocal of Focal Length in Meters

Ø1" N-BK7 Spherical Singlet Lens Kits

LSB04 Uncoated Ø1" Mounted Singlet Lens Kit
LSB04-A Ø1" Mounted Singlet N-BK7 Lens Kit (ARC: 350 - 700 nm)
LSB04-B Ø1" Mounted Singlet N-BK7 Lens Kit (ARC: 650 - 1050 nm)
LSB04-C Ø1" Mounted Singlet N-BK7 Lens Kit (ARC: 1050 - 1620 nm)
  • Reciprocal of Focal Length in Meters
  • Due to substrate limitations, these lenses are made from N-SF11 glass, which has greater dispersion than N-BK7. For more information, please visit our Optical Substrates page.

Ø2" N-BK7 Plano-Conxex Spherical Singlet Lens Kits

LSC01 Uncoated Ø2" Mounted Plano-Convex Singlet Lens Kit
LSC01-A Ø2" Mounted Plano-Convex Singlet Lens Kit (ARC: 350 - 700 nm)
LSC01-B Ø2" Mounted Plano-Convex Singlet Lens Kit (ARC: 650 - 1050 nm)
LSC01-C Ø2" Mounted Plano-Convex Singlet Lens Kit (ARC: 1050 - 1620 nm)
  • Reciprocal of Focal Length in Meters

The N-BK7 lens kits on this page can be ordered uncoated or with AR coatings optimized for one of the following ranges: 350 - 700 nm (designated with -A), 650 - 1050 nm (designated with -B), or 1050 - 1620 nm (designated with -C). The first figure below contains transmission curves for a 25 mm thick, uncoated N-BK7 substrate, while the second figure indicates the performance of our AR coatings as a function of wavelength. Our high-performance, multi-layer AR coatings have an average reflectance of less than 0.5% (per surface) across the specified wavelength ranges. Broadband coatings have a typical absorption of 0.25%, which is not shown in the reflectivity plots.

B AR Coating
Click to Enlarge

Click Here for Raw Data
The blue shaded region indicates the specified 650 - 1050 nm wavelength range for optimum performance.
A AR Coating
Click to Enlarge

Click Here for Raw Data
The blue shaded region indicates the specified 350 - 700 nm wavelength range for optimum performance.
C AR Coating
Click to Enlarge

Click Here for Raw Data
The blue shaded region indicates the specified 1050 - 1620 nm wavelength range for optimum performance.
N-BK7 Window Transmission
Click to Enlarge

Click Here for Raw Data

Thorlabs' Standard Broadband Antireflection Coatings

Damage Threshold Specifications
Coating Designation
(Item # Suffix)
Damage Threshold
-A 7.5 J/cm2 (532 nm, 10 ns, 10 Hz, Ø0.504 mm)
-B 7.5 J/cm2 (810 nm, 10 ns, 10 Hz, Ø0.144 mm)
-C 7.5 J/cm2 (1542 nm, 10 ns, 10 Hz, Ø0.123 mm)

Damage Threshold Data for Thorlabs' N-BK7 Singlet Lenses

The specifications to the right are measured data for Thorlabs' AR-coated N-BK7 spherical single lenses. Damage threshold specifications are constant for a given coating type, regardless of the size of the lens.

 

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 11254 and ISO 21254 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.

LIDT metallic mirror
The photograph above is a protected aluminum-coated mirror after LIDT testing. In this particular test, it handled 0.43 J/cm2 (1064 nm, 10 ns pulse, 10 Hz, Ø1.000 mm) before damage.
LIDT BB1-E02
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.

Linear Power Density Scaling

LIDT in linear power density vs. pulse length and spot size. For long pulses to CW, linear power density becomes a constant with spot size. This graph was obtained from [1].

Intensity Distribution

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 1310 nm scales to 5 W/cm at 655 nm):

CW Wavelength Scaling

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:

Energy Density Scaling

LIDT in energy density vs. pulse length and spot size. For short pulses, energy density becomes a constant with spot size. This graph was obtained from [1].

  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 1064 nm scales to 0.7 J/cm2 at 532 nm):

Pulse Wavelength Scaling

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:

Pulse Length Scaling

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 (1998).
[2] Roger M. Wood, Laser-Induced Damage of Optical Materials (Institute of Physics Publishing, Philadelphia, PA, 2003).
[3] C. W. Carr et al., Phys. Rev. Lett. 91, 127402 (2003).
[4] N. Bloembergen, Appl. Opt. 12, 661 (1973).


Posted Comments:
ludoangot  (posted 2015-09-11 12:18:50.06)
Could you offer a kit with SM1 mounted concave lenses? They are only available as part of the LSB03-X kit. Also it would be very nice to be able to purchase individual mounted lenses, or to propose the option to have any lens you offer mounted in the appropriate mount and engraved with its specifications.
besembeson  (posted 2015-10-01 10:38:01.0)
Response from Bweh at Thorlabs USA: Thanks for the feedback. We don't have such an individual kit at this time, and I agree it is a good idea to have a "build your own lens kit". We will review this.
bdada  (posted 2011-10-19 14:07:00.0)
Response from Buki at Thorlabs: Thank you for your feedback. We are working now on updating our website shortly with more information on the orientation of the lens within the cell. Please contact TechSupport@thorlabs.com if you have further questions about this matter.
user  (posted 2011-10-18 15:34:41.0)
Would be nice if your website documentation showed orientation of lens in cell. (If it's there, I can't find it) Which side is CX? Would be nice if also drqwn on lens cell itself. I figured out the orientation but geez.

Ø1/2" N-BK7 Spherical Singlet Lens Kits

Lens Type Lens Orientation Focal Lengths (mm) Dioptersa Included Lens Item Numbersb
Plano Convex info icon 15, 20, 25, 30, 40, 50, 100 +66.7, +50.0, +40.0, +33.3,
+25.0, +20.0, +10.0
LA1540, LA1074, LA1560, LA1289,
LA1304, LA1213, LA1207
Bi Convex info icon 15, 20, 25, 30, 40, 50, 100 +66.7, +50.0, +40.0, +33.3,
+25.0, +20.0, +10.0
LB1092, LB1450, LB1014, LB1258,
LB1378, LB1844, LB1187
Plano Concave info icon -15, -25, -30, -50 -66.7, -40.0, -33.3, -20.0 LC2265, LC1054, LC1060, LC1439
Bi Concave info icon -15, -25, -30, -50 -66.7, -40.0, -33.3, -20.0 LD2060, LD1569, LD1903, LD1357
  • Reciprocal of Focal Length in Meters
  • For AR-coated lens kits, add the coating code to the item numbers listed above (e.g., LSA01-A contains LA1540-A)
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LSA01 Support Documentation
LSA01Ø1/2" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, Uncoated, 22 pc
$811.59
Today
LSA01-A Support Documentation
LSA01-AØ1/2" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, AR Coating: 350-700 nm, 22 pc
$1,020.44
Today
LSA01-B Support Documentation
LSA01-BØ1/2" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, AR Coating: 650-1050 nm, 22 pc
$1,020.44
Today
LSA01-C Support Documentation
LSA01-CØ1/2" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, AR Coating: 1050-1620 nm, 22 pc
$1,072.37
Today

Ø1" N-BK7 Plano-/Bi- Convex/Concave Lens Kits

Lens Type Lens Orientation Focal Lengths (mm) Dioptersa Included Lens Item Numbersb
Plano Convex info icon 25.4, 35, 50, 75, 100, 125, 150, 200, 250, 300, 400, 500, 750, 1000 +39.4, +28.6, +20.0, +13.3, +10.0, +8.0, +6.7, +5.0, +4.0, +3.3, +2.5, +2.0, +1.3, +1.0 LA1951, LA1027, LA1131, LA1608, LA1509, LA1986, LA1433, LA1708, LA1461, LA1172, LA1908, LA1978, LA1464, LA1484
Bi Convex info icon 25.4, 35, 50, 75, 100, 125, 150, 200, 250, 300, 400, 500, 750, 1000 +39.4, +28.6, +20.0, +13.3, +10.0, +8.0, +6.7, +5.0, +4.0, +3.3, +2.5, +2.0, +1.3, +1.0 LB1761, LB1811, LB1471, LB1901, LB1676, LB1904, LB1437, LB1945, LB1056, LB1779, LB1391, LB1869, LB1475, LB1409
Plano Concave info icon -30, -50, -75, -100 -33.3, -20.0, -13.3, -10.0 LC2679, LC1715, LC1582, LC1120
Bi Concave info icon -30, -50, -75 -33.3, -20.0, -13.3 LD2297, LD1464, LD1170
  • Reciprocal of the Focal Lengths in Meters
  • For AR-coated lens kits, add the coating code to the item numbers listed above (e.g., LSB04-A contains LA1951-A)
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LSB04 Support Documentation
LSB04Ø1" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, Uncoated, 35 pc
$1,327.76
Today
LSB04-A Support Documentation
LSB04-AØ1" N-BK7 Plano-/Bi- Convex/Concave Lens Kit AR Coating: 350-700 nm, 35 pc
$1,659.97
Today
LSB04-B Support Documentation
LSB04-BØ1" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, AR Coating: 650-1050 nm, 35 pc
$1,659.97
Today
LSB04-C Support Documentation
LSB04-CØ1" N-BK7 Plano-/Bi- Convex/Concave Lens Kit, AR Coating: 1050-1620 nm, 35 pc
$1,759.53
Today

Ø1" N-BK7 Plano-Convex Lens Kits

Lens Orientation Focal Lengths (mm) Dioptersa Included Lens Item Numbersb
info icon 25.4, 35, 50, 75, 100, 125, 150,
200, 250, 300, 400, 500, 750, 1000
+39.4, +28.6, +20.0, +13.3, +10.0, +8.0, +6.7,
+5.0, +4.0, +3.3, +2.5, +2.0, +1.3, +1.0
LA1951, LA1027, LA1131, LA1608, LA1509,
LA1986, LA1433, LA1708, LA1461, LA1172,
LA1908, LA1978, LA1464, LA1484
  • Reciprocal of Focal Lengths in Meters
  • For AR-coated lens kits, add the coating code to the item numbers listed above (e.g., LSB01-A contains LA1951-A)
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LSB01 Support Documentation
LSB01Ø1" N-BK7 Plano-Convex Lens Kit, Uncoated, 14 pc
$584.34
Today
LSB01-A Support Documentation
LSB01-AØ1" N-BK7 Plano-Convex Lens Kit, AR Coating: 350-700 nm, 14 pc
$715.28
Today
LSB01-B Support Documentation
LSB01-BØ1" N-BK7 Plano-Convex Lens Kit, AR Coating: 650-1050 nm, 14 pc
$715.28
Today
LSB01-C Support Documentation
LSB01-CØ1" N-BK7 Plano-Convex Lens Kit, AR Coating: 1050-1620 nm, 14 pc
$758.56
Today

Ø1" N-BK7 Plano-Convex and Bi-Convex Lens Kits

Lens Type Lens Orientation Focal Lengths (mm) Dioptersa Inlcuded Lens Item Numbersb
Plano Convex info icon 25.4, 35, 50, 75, 100, 125, 150,
200, 250, 300, 400, 500, 750, 1000
+39.4, +28.6, +20.0, +13.3,
+10.0, +8.0, +6.7, +5.0, +4.0,
+3.3, +2.5, +2.0, +1.3, +1.0
LA1951, LA1027, LA1131, LA1608, LA1509,
LA1986, LA1433, LA1708, LA1461, LA1172,
LA1908, LA1978, LA1464, LA1484
Bi Convex info icon 25.4, 35, 50, 75, 100, 125, 150,
200, 250, 300, 400, 500, 750, 1000
+39.4, +28.6, +20.0, +13.3,
+10.0, +8.0, +6.7, +5.0, +4.0,
+3.3, +2.5, +2.0, +1.3, +1.0
LB1761, LB1811, LB1471, LB1901, LB1676,
LB1904, LB1437, LB1945, LB1056, LB1779,
LB1391, LB1869, LB1475, LB1409
  • For AR-coated lens kits, add the coating code to the item numbers listed above (e.g., LSB03-A contains LA1951-A)
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LSB03 Support Documentation
LSB03Ø1" N-BK7 Plano-Convex and Bi-Convex Lens Kit, Uncoated, 28 pc
$1,069.13
Today
LSB03-A Support Documentation
LSB03-AØ1" N-BK7 Plano-Convex and Bi-Convex Lens Kit, AR Coating: 350-700 nm, 28 pc
$1,339.66
Today
LSB03-B Support Documentation
LSB03-BØ1" N-BK7 Plano-Convex and Bi-Convex Lens Kit, AR Coating: 650-1050 nm, 28 pc
$1,339.66
Today
LSB03-C Support Documentation
LSB03-CØ1" N-BK7 Plano-Convex and Bi-Convex Lens Kit, AR Coating: 1050-1620 nm, 28 pc
$1,428.39
Today

Ø1" N-BK7 Bi-Convex Lens Kits

Lens Orientation Focal Lengths (mm) Dioptersa Included Lens Item Numbersb
info icon 25.4, 35, 50, 75, 100, 125, 150,
200, 250, 300, 400, 500, 750, 1000
+39.4, +28.6, +20.0, +13.3,
+10.0, +8.0, +6.7, +5.0, +4.0,
+3.3, +2.5, +2.0, +1.3, +1.0
LB1761, LB1811, LB1471, LB1901, LB1676, LB1904, LB1437,
LB1945, LB1056, LB1779, LB1391, LB1869, LB1475, LB1409
  • Reciprocal of the Focal Lengths in Meters
  • For AR-coated lens kits, add the coating code to the item numbers listed above (e.g., LSB02-A contains LB1761-A)
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LSB02 Support Documentation
LSB02Ø1" N-BK7 Bi-Convex Lens Kit, Uncoated, 14 pc
$615.72
Today
LSB02-A Support Documentation
LSB02-AØ1" N-BK7 Bi-Convex Lens Kit, AR Coating: 350-700 nm, 14 pc
$747.74
Today
LSB02-B Support Documentation
LSB02-BØ1" N-BK7 Bi-Convex Lens Kit, AR Coating: 650-1050 nm, 14 pc
$747.74
Today
LSB02-C Support Documentation
LSB02-CØ1" N-BK7 Bi-Convex Lens Kit, AR Coating: 1050-1620 nm, 14 pc
$791.03
Today

Ø2" N-BK7 Plano-Convex Lens Kits

Lens Orientation Focal Lengths (mm) Dioptersa Included Lens Item Numbersb
info icon 75, 100, 125, 150, 200,
300, 400, 500, 750, 1000
+13.3, +10.0, +8.0, +6.7, +5.0,
+3.3, +2.5, +2.0,+1.3, +1.0
LA1145, LA1050, LA1384, LA1417, LA1979,
LA1256, LA1725, LA1380, LA1727, LA1779
  • Reciprocal of the Focal Length in Meters
  • For AR-coated lens kits, add the coating code to the item numbers listed above (e.g., LSC01A contains LA1145-A)
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
LSC01 Support Documentation
LSC01Ø2" N-BK7 Plano-Convex Lens Kit, Uncoated, 10 pc
$644.94
Today
LSC01-A Support Documentation
LSC01-AØ2" N-BK7 Plano-Convex Lens Kit, AR Coating: 350-700 nm, 10 pc
$740.17
Today
LSC01-B Support Documentation
LSC01-BØ2" N-BK7 Plano-Convex Lens Kit, AR Coating: 650-1050 nm, 10 pc
$740.17
Today
LSC01-C Support Documentation
LSC01-CØ2" N-BK7 Plano-Convex Lens Kit, AR Coating: 1050-1620 nm, 10 pc
$769.39
Today
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