Method of making high performance optical edge and notch filters and resulting products

[0001] This application claims the benefit of U.S. Provisional Application No. 60/637,697, titled High Performance Thin Film Notch Filters, filed on Dec. 21, 2004 by Turan Erdogan, Joseph T. Foss, and Ligang Wang, and is a continuation-in-part of prior U.S. patent application Ser. No. 10/840,134, filed May 6, 2004, which claims the benefit of U.S. Provisional Application Ser. No. 60/468,245, filed May 6, 2003. The entire disclosures of U.S. Provisional Application No. 60/637,697, U.S. patent application Ser. No. 10/840,134, and U.S. Provisional Application No. 60/468,245 are hereby incorporated herein by reference.

[0002] This invention relates to methods of making optical edge filters and optical notch filters and also relates to the resulting improved filters.

[0003] A. Optical Edge Filters, Optical Notch Filters, and Their use

[0004] Optical edge filters and thin-film notch filters are important components in systems for optical measurement and analysis including Raman spectroscopy and fluorescence spectroscopy. Optical edge filters and/or notch filters are used in such systems to block unwanted light that would otherwise constitute or generate spurious optical signals and swamp the signals to be detected and analyzed.

[0005] Optical edge filters block unwanted light having wavelengths above or, alternatively, below a chosen “transition” wavelength λ_T while transmitting light on the unblocked side of λ_T. Edge filters which transmit optical wavelengths longer than λ_T are called long-wave-pass filters (LWP filters), and edge filters which transmit wavelengths shorter than λ_T are short-wave-pass or SWP filters.

[0006] Referring to the drawings, FIGS. 1A and 1B schematically illustrate the spectral transmission of idealized long-wave-pass and short-wave-pass filters respectively. As can be seen from FIG. 1A, a LWP filter blocks light with wavelengths below λ_T and transmits light with wavelengths above λ_T. As shown in FIG. 1B, a SWP filter transmits light with wavelengths below λ_T and blocks light with wavelengths above λ_T. λ_T is the wavelength at which the filter “transitions” from blocking to transmission, or vice versa.

[0007] While an ideal edge filter has a precise transition wavelength λ_T represented by a vertical line at λ_T, real edge filters change from blocking to transmission over a small range of wavelengths and are more accurately represented by a non-vertical but steeply sloped line near λ_T. Similarly, while an ideal edge filter transmits all light in the transmission region (transmission T=1), real filters invariably block a small portion of the light to be transmitted (T<1). The steepness of the line and the proportion of the light transmitted are important parameters in many applications.

[0008] Turning now to FIGS. 1C and 1D, the spectral transmission of an ideal and a realistic notch filter are illustrated respectively. Notch filters block a specific and narrow range of wavelengths (ideally a single laser “line” λ_L) and pass light with high transmission on both sides of the narrow blocking range. Because lasers emit a very small, but non-zero, bandwidth of light, an ideal notch filter blocks light at wavelengths within this bandwidth ((λ_L−(BW/2)) to (λ_L+(BW/2))) with no ripple and perfectly steep (vertical) transition edges, as shown in FIG. 1C. The ideal notch filter passes light at wavelengths longer than the blocking band (λ>(λ_L+(BW/2))) and passes light at wavelengths shorter than the blocking band (λ<(λ_L−(BW/2))). A realistic notch filter does not have complete transmission outside of the blocking band ((λ_L−(BW/2)) to (λ_L+(BW/2))), does not completely block radiation within the blocking band, and has non-vertical transition edges, thereby changing from blocking to transmission over a small range of wavelengths, as shown in FIG. 1D. Accordingly, the steepness of the edges, the transmission amount outside of the blocking band, and the blocking effectiveness within the blocking band are important parameters of notch filters in many applications.

[0009] Edge filters and notch filters are particularly useful in optical measurement and analysis systems that use laser light to excite a sample at one wavelength (or a small band of wavelengths) λ_L and measure or view an optical response of the excited sample at other wavelengths. The excitation light λ_L is delivered to the sample by an excitation light path, and the optical response of the sample is delivered to the eye or measuring instrument by a collection path. Edge filters can be used to block spurious light from the excitation path. Edge filters and/or notch filters can be used to block excitation light from entry into the collection path. The steeper the filter edge(s), the more effectively spurious signals are blocked. In the case of both edge filters and notch filters, the lower the transmission loss, the more light from the sample reaches the measuring instrument.

[0010] Raman spectroscopy is one such optical analysis system. It is based on the fact that when molecular material is irradiated with high intensity light of a given wavelength (or series of wavelengths) λ_L, a small portion of the incident light scattered by the material will be shifted in wavelength above and below λ_L. This Raman shifting is attributed to the interaction of the light with resonant molecular structures within the material, and the spectral distribution of the Raman-shifted light provides a spectral “fingerprint” characteristic of the composition of the material. As a practical example, a Raman probe can identify the contents of a bottle without opening the bottle.

[0011] FIG. 2 is a simplified schematic diagram of a Raman probe 20. In essence, the probe 20 comprises an optical excitation path 22, and a collection path 23. These paths advantageously comprise optical fiber. In operation, excitation light λ_L from a laser 24 passes through the fiber path 22 and one or more edge filters or a narrowband laser-line filter 22A to illuminate a portion of the sample 21 with high intensity light. The edge filter(s)/laser-line filter 22A act(s) to block light outside of λ_L from the sample 21. Light scattered from the sample 21 passes through a notch filter (or one or more edge filters) 23A and then through fiber collection path 23 to a spectral analyzer 25 where the “fingerprint” of the sample is determined.

[0012] The light scattered from the sample 21 is a mixture of unshifted scattered excitation light λ_L Rayleigh scattering) and Raman-shifted light at wavelengths longer and shorter than λ_L. The scattered excitation light λ_L would not only swamp the analyzer, it would also excite spurious Raman scattering in a collection fiber. Thus the unshifted excitation light λ_L should be removed from the collection path. This can be accomplished by disposing a notch filter (or one or more edge filters) 23A between the sample 21 and the collection fiber 23, the notch filter (or edge filter(s)) 23A blocking the unshifted scattered excitation light λ_L.

[0013] Edge filters and notch filters also are useful in fluorescence spectroscopy. Here, laser excitation light λ_L is used to excite longer wavelength emissions from fluorescent markers. The markers can be fluorescent atoms chemically bonded to a biological molecule to track the molecule in a body or cell. Edge filters may be used to reject spurious light from an excitation path and to reject excitation light from a collection path. Notch filters may be used to reject excitation light from the collection path.

[0014] In the case of edge filters, it should now be clear that the steeper the filter slope at the transition wavelength λ_T, the greater the amount of spurious light that can be filtered out. In addition, the steeper the slope, the greater the amount of shifted light from the sample that will reach the analyzer. Similarly, higher levels of transmission of the shifted light through the filters provide more light for analysis. Higher edge filter blocking provides better rejection of the laser excitation light from the spectrum analyzer, thus decreasing the noise and improving both specificity and sensitivity of the measurement. Higher edge-filter transmission enables the maximum signal to reach the analyzer, further improving the signal-to-noise ratio and hence the measurement or image fidelity. A steeper filter edge also permits shifts to be resolved much closer to the excitation wavelength, thus increasing the amount of information from the measurement.

[0015] In the case of notch filters, the steeper the edges of the notch filter at the laser wavelength λ_L, the greater the amount of unshifted excitation light λ_L that can be filtered out before reaching an analyzer. Similarly, the higher the levels of transmission outside of the blocking band, the more information there is for measurement.

[0016] B. Edge Filter and Notch Filter Structure and Conventional Fabrication

[0017] FIG. 3 is a simplified schematic illustration of an optical filter 30, which may be either an edge filter or a notch filter. The optical filter 30 comprises a transparent substrate 31 having a flat major surface 32 supporting many thin coatings 33A, 33B. The thickness of the coatings is exaggerated and the number is reduced for purposes of illustration. Coatings 33A and 33B are typically alternating and of different respective materials chosen to present markedly different indices of refraction (index contrast). The coating indices and thicknesses are chosen and dimensioned to filter impinging light by interference effects in a desired manner. Specifically, if a light beam 34 impinges on the filter, a first wavelength portion 34T of a beam is transmitted and a second wavelength portion 34R is reflected and thus rejected by the filter. What is transmitted and what is reflected depends on the precise thicknesses and indices of the thin coatings.

[0018] Two basic types of thin-film edge filters and thin-film notch filters exist: those based on “soft coatings” and those based on “hard coatings,” both of which are typically manufactured by an evaporation technique (either thermal evaporation or electron-beam evaporation). Hard coating filters, however, may also be manufactured by non-evaporative techniques such as ion-beam sputtering.

[0019] Soft coatings imply literally what the name suggests-they are physically soft and can be readily scratched or damaged. They are fairly porous, which also means they tend to be hygroscopic (absorb water vapor) leading to dynamic changes in the film index and hence the resulting filter spectrum in correlation to local humidity. There are two main reasons soft coatings are used. First, an advantageous larger index contrast can be realized with soft coatings. (The index contrast is the relative difference between the index of refraction of the low-index material and that of the high-index material.) For example, many high-performance soft-coated filters are made using sodium aluminum fluoride (“cryolite”), with a chemical composition of Na₃AlF₆ and an index of about 1.35 for visible wavelengths, and zinc sulfide, with a chemical composition of ZnS and an index of about 2.35. The second reason for using these materials is that the evaporation process can be controlled well for these materials, largely because they have relatively low melting temperatures. Hence it is possible to maintain fairly accurate control over the layer thicknesses even for filter structures with many tens of layers and perhaps even up to 100 layers. As described above, edge filter performance is measured by edge steepness, depth of blocking, and high transmission with low ripple. A larger index contrast and a larger number of layers both yield more steepness and more blocking. High transmission with low ripple is improved with more layers and higher layer thickness accuracy. For these reasons the highest performance conventional thin-film edge filters have been made with soft-coating technology.

[0020] Hard coatings are made with tougher materials (generally oxides), and result from “energetic” deposition processes, in which energy is explicitly supplied to the film itself during the deposition process. This is accomplished with a beam of ions impinging directly on the coating surface. The ion bombardment acts to “hammer” the atoms into place in a more dense, less porous film structure. Such processes are usually called ion-assisted deposition (IAD) processes. High-performance edge filters have been made with ion-assisted electron-beam evaporation. Typically the index contrast available with hard-coating (oxide) thin-film materials is not as high as that of the soft-coating materials, and consequently more layers must be deposited to achieve a comparable level of performance. This problem, coupled with the more difficult to control deposition rates and overall processes of high-melting-temperature oxides, leads to much more stringent requirements on the layer-thickness control techniques to achieve a reasonable level of layer thickness accuracy for good edge steepness and high, low-ripple transmission.

[0021] For the best filters, some kind of “optical monitoring” (direct measurement of filter transmission or reflection during deposition) is necessary to determine when to terminate the deposition of each layer. Optical monitoring can be performed on the actual filters of interest or on “witness pieces” often positioned in the center of the deposition chamber. There are three basic types of optical monitoring algorithms. The first is often called “drop-chip” monitoring, and is based on measuring the transmission (or reflection) vs. time through a new witness piece for each new layer. Since the theoretical transmission vs. time can be calculated accurately for each layer deposited on a blank piece of glass, then a good comparison between the measured and theory curves can be made independent of the history of the deposition (thickness errors in previous layers). This technique is accurate and useful for layers of arbitrary thickness, but it is cumbersome, especially for filters comprised of at least many 10's of layers.

[0022] The second type of monitoring is called “turning-point” monitoring, and is used for depositing layers that are precisely a quarter of a wavelength in thickness (or multiples thereof). The technique is based on the fact that the transmission vs. time reaches a turning point (or extremum) at each multiple of a quarter wave of thickness, so an algorithm is developed to cut layers precisely at the turning points. The elegant feature of this method is that there is inherent compensation for layer thickness errors from previous layers, so long as one adheres to the rule of cutting exactly at turning points. It thus works extremely well even for very thick coatings with even hundreds layers (it is the basis for manufacturing very high-performance filters for DWDM telecom applications, which can have as many as 200–400 quarter-wave layers).

[0023] The third type of monitoring is called “level monitoring,” and is applicable for non-quarter-wave thick layers. Monitoring can be done through the actual filters or through witness piece(s). The concept is to cut layers at predetermined transmission levels, based on a calculated prediction of transmission vs. time for the entire structure. However, because small layer errors lead to large variations in the absolute transmission values, one must instead rely on cutting at the correct transmission level relative to the local maximum and minimum values. Hence the method works well only for non-quarter-wave thick layers that are more than a half-wave thick, so that there is both a maximum and a minimum transmission value in the transmission vs. time curve for that layer. Even in this case, this method does not contain inherent compensation for errors in the thickness of previously deposited layers, and thus is not as forgiving as the turning-point method. However, to obtain an edge filter with high transmission and low ripple requires primarily non-quarter-wave thick layers, and hence turning-point monitoring is not applicable for edge filters.

[0024] Besides thin-film filters, the other predominant type of optical filter used for the applications described herein is the volume holographic filter. These filters accomplish blocking of unwanted excitation light with a “notch” of very low transmission over a relatively narrow bandwidth, and hence are often called “holographic notch filters.” The non-transmitted light is diffracted at an acute angle relative to the direction of the transmitted light. The holograms are exposed and developed in a thick gelatinous film that is typically sandwiched between two glass substrates. Because the film can be relatively thick, allowing a very large number of fringes in the holographic grating, such filters can achieve a narrow notch bandwidth with accordingly steep edges.

[0025] A need in the art exists for an improved method of making optical edge filters and notch filters and for improved edge filters and notch filters having increased edge steepness and increased transmission.

[0026] These problems are addressed and a technical solution achieved in the art by high performance optical edge filters, high performance notch filters, and methods of making the same according to an embodiment of the present invention. In particular, the optical edge filters have an edge steepness less than about 0.8% as measured by dividing (a) the edge width from the 50% transmission wavelength to the optical density 6 (“OD6”) wavelength by (b) the 50% transmission wavelength. The optical edge filters also have an average transmission above about 95%.

[0027] The notch filters exhibit a blocking of OD>6, very high transmission (>90%) outside the notch(es), and a narrow notch bandwidth comparable to that of holographic notch filters. In addition, this performance can be achieved with a single notch or multiple notches. Finally, the inventive notch filters achieve almost the same performance for filters at a 45 degree angle of incidence, with the exception that the blocking is OD>5.

[0028] The methods for making these edge and notch filters accurately determine when deposition of each layer of a filter should terminate. The methods include calculating theoretical transmission data for a layer of the filter and calculating an expected deposition duration for the layer. The methods also include measuring transmission through the layer during deposition for a period less than the expected deposition duration. When the measuring period elapses, a new deposition duration is calculated based upon the theoretical transmission data and the measured transmission data, thereby providing an accurate deposition duration for the layer.

[0048] It is to be understood that these drawings are for illustrating the concepts of the invention and, except for data graphs, are not to scale.

[0049] The invention has four aspects: A) apparatus programmed to make improved optical edge and notch filters; B) the method of making the improved filters; C) the improved filters made by the method and D) applications of the improved filters. These aspects will be described in the order presented.

[0050] A. Apparatus for Making Optical Edge and Notch Filters in Accordance with an Embodiment of the Invention

[0051] Optical edge filters and notch filters in accordance with an embodiment of the invention are made using a computer-controlled deposition system. Advantageously the deposition is an ion beam sputtering deposition system using a beam assist source for depositing hard coatings and having an integral optical monitoring system to monitor deposition. A data processor, responsive to signals from the monitoring system, processes these signals and directs the growth of improved optical edge filters in accordance with algorithms described below.

[0052] FIG. 4 is a schematic view of an advantageous computer-controlled deposition apparatus 400 for practicing ion-assisted, ion-beam sputtering disposition and optical monitoring under data processor control. The apparatus 400 comprises a vacuum chamber 401 having an interior accessible by a sealable port 402 such as an o-ring sealed door. The chamber 401 includes a pump port 402 for coupling to one or more evacuation pumps (not shown) such as mechanical and low pressure cryogenic pumps.

[0053] Within the chamber 401 is a substrate mount 403 which is advantageously a rotatable spindle mount. Also within the chamber are a plurality of material targets, a deposition ion beam source 404, and a mounted substrate 405. One of the targets 406 is positioned in relation to the ion beam source and the substrate so that an ion beam from the source will sputter material from the target onto the substrate in a substantially uniform layer. Typically there are separate targets for each material to be deposited on the substrate, and the targets are movable to and from the sputtering position. There are usually two material targets: one a high optical index material and the other a low index material. The targets are movable so that deposition can be switched automatically from one material to the other.

[0054] An assist ion beam source 407 is disposed in the chamber 401 in position to bombard the substrate 405 with an ion beam. During the deposition of any one material, the substrate is simultaneously bombarded by sputtered material and by ions from the assist ion beam source 407. The assist ion bombardment serves to energize the adhesion of particles onto the surface of the substrate and thereby produce a substantially more dense (“hard”) film than would otherwise be formed by sputter deposition. See J. M. E. Harper et al., “Modification of Thin Film Properties by Ion Bombardment During Deposition,” in Ion Bombardment Modification of Surfaces, Ed. By O. Auciello and R. Kelly, from Beam Modifications of Materials, Vol. 1 (Elsevier, Amsterdam, 1984).

[0055] Both the sputter deposition and the assist bombardment can be activated by a deposition control system 408. The control system 408 can start or stop deposition precisely by turning on and off the deposition ion beam source 404 or by removing or engaging a mechanical shutter (not shown) that covers the substrate. Further details concerning ion beam sputtering deposition systems can be found in U.S. Pat. No. 4,142,958 issued to David Wei et al. on Mar. 6, 1979 and U.S. Pat. No. 4,793,908 issued to Gene Scott et al. on Dec. 27, 1988, both of which are incorporated herein by reference. See also Juergen Becker, “Ion Beam Sputtering,” Handbook of Optical Properties, Vol. 1, Thin Films for Optical Coatings, pgs 189–211, Ed. by R. E. Hummel and K. H. Guenther (CRC Press, Boca Raton, 1995).

[0056] The optical monitoring system advantageously comprises a light source 409, filters 411A and 411B, detectors 412 and 413 and a data processor 414. The light source 409 can be any sufficiently bright, broadband light source, such as a quartz halogen bulb or a Xenon discharge lamp. The detectors can include a reference detector 412 and a signal detector 413. The detectors can be semiconductor (Si) photodiodes, photomultiplier tubes or any other sensitive, low-noise detectors capable of detecting light at the monitoring wavelength.

[0057] In the advantageous arrangement shown here, a beamsplitter 415 picks off a portion 416 of the monitoring light beam 417 from source 409 and detects it with reference detector 412. The signal detector 413 detects the portion 418 of the beam 417 that passes through the coated substrate (or a “witness” substrate) being monitored. Advantageously, the filters 411A and 411B are positioned to ensure that a sufficiently narrow band of wavelengths is monitored.

[0058] The filters 411A, 411B can be narrow band interference filters, adjustable diffraction-grating monochromators or combinations thereof. Advantageously an interference filter is used for reference filter 411A and a monochromator is used for detector filter 411B. Further details concerning optical monitoring of thin films as they are being deposited can be found in U.S. Pat. No. 6,649,208 issued to Wayne Rodgers on Nov. 18, 2003, which is incorporated herein by reference. See also H. Angus Macleod, Thin Film Optical Filters (3^rd Ed., Institute of Physics, Bristol, 2001) and H. A. Macleod, “Turning Value Monitoring of Narrow-Band All-Dielectric Thin-Film Optical Filters,” Optica Acta, vol. 19, pp. 1–28(1972).

[0059] The data processor 414 collects data from the signal and reference detectors 413, 412, implements the mathematics associated with optical monitoring algorithms and instructs the deposition control system 408 when to stop depositing any given thin film layer based on the result of the mathematical calculations prescribed in the algorithm.

[0060] B. Methods of Making the Improved Edge Filters and Notch Filters

[0061] The manner in which the data processor 414 controls the apparatus 400 via the deposition control system 408 to generate the optical edge filters and/or notch filters according to an embodiment of the present invention will now be described. In particular, the data processor 414 is programmed to instruct the apparatus 400 when to stop depositing each layer of the filter being manufactured. In regard to edge filters, the data processor 414 follows two separate processes in determining when deposition of a layer should terminate depending upon whether a long-wave-pass or a short-wave-pass filter is being manufactured. These two processes will be described in turn. A description of the processes performed for manufacturing a notch filter will follow.

[0062] FIG. 4 illustrates the process flow executed by the data processor 414 when manufacturing a long-wave-pass (“LWP”) filter according to an embodiment of the present invention. However, prior to initiating the process of FIG. 4, a design for the LWP filter is prepared. In the exemplary embodiment, the LWP filter has N layers and comprises two materials: a low-refractive-index material and a high-refractive-index material. The exemplary initial design for a steep LWP edge filter includes a quarter-wave (“QW”) stack of (0.5H L 0.5H)^N, where L and H represent layers of high and low index materials with a quarter-wave of optical thickness at the reference wavelength. The reference wavelength is chosen so that the longer-wavelength edge of the QW stopband is close to the desired transition wavelength of the LWP filter design.

[0063] Once the initial design is setup, a desired target spectrum is constructed, which typically includes the wavelength ranges of both the blocking and passband regions, as well as the required blocking level and minimum transmission and allowable ripple within the passband. The edge steepness is thus indirectly defined as the wavelength separation between the blocking region and the passband.

[0064] The layer thicknesses of the initial design are then optimized against the target spectrum by an optimization routine known in the art. Exemplary optimization routines include the variable-metric or simplex methods implemented in standard commercial thin-film design software packages, such as TFCalc by Software Spectra, Inc., and The Essential Macleod by Thin Film Center Inc. Usually, with the proper choice of the initial design, the optimization quickly converges and the optimized structure is not very different from the initial structure. Special treatments may be necessary for the first layer (toward substrate) and the last layer. For instance, the optical thickness of the first layer may need to be manually increased—a typical minimum thickness in this case is two QWs. As for the last layer, it sometimes becomes too thin and thus may be eliminated. The structure should be re-optimized whenever there is any modification to the layer thickness.

[0065] With the LWP filter design at hand, the data processor 414 receives design data and deposition rate data as input at 501. The design data describes the designed thin-film structure of the LWP filter with a physical thickness d_i and an index n_i for each i^th layer. n_i is either n_L or n_H, where n_L is the refractive index of the low-index material and n_H is the refractive index of the high-index material. n_L and n_H are each known as a function of wavelength λ. The deposition rate data describes the known starting deposition rate of the deposition apparatus 400 shown in FIG. 4 for each of the two materials. In the exemplary embodiment, the deposition rate data is within about +/−5% of the actual deposition rate and is in units of Å/sec. The starting rate estimates for each of the two materials are referred to as r_L and r_H, and hence each layer will have a starting rate estimate r_i depending on whether it is made of low-index or high-index material.

[0066] At 502, the transmission T_i as a function of physical thickness d for each i^th layer is calculated at a series of wavelengths in the transmissive band of the finished filter. Consequently, the calculations at 502 result in a series of curves T_i vs. d at each of the series of wavelengths in the transmissive band of the finished filter. Such calculations are performed using standard mathematical methods for calculating the optical properties of thin-film filters. See, for example, H. A. Macleod, Thin-film Optical Filters, 3^rd edition (Institute of Physics, Bristol, 2001).

[0067] Advantageously, instead of calculating each T_i vs. d curve at one corresponding wavelength in the series of wavelengths, each T_i vs. d curve is calculated by averaging a plurality of T_i vs. d curves calculated at a range of wavelengths surrounding the corresponding wavelength. For instance, assume that the series of wavelengths includes 501 nm and 502 nm. Instead of calculating a T_i vs. d curve at just 501 nm, this T_i vs. d curve is advantageously calculated by averaging T_i vs. d curves calculated at, for instance, 500 nm, 501 nm, and 502 nm. Further, the T_i vs. d curve at 502 nm is advantageously calculated by averaging T_i vs. d curves calculated at, for instance, 501 nm, 502 nm, and 503 nm. One skilled in the art will appreciate that invention is not limited to this averaging procedure and the range of wavelengths used.

[0068] At 503, an optical monitoring wavelength λ_m is selected from the series of wavelengths in the transmissive band of the finished filter, thereby identifying a single curve T_i vs. d at λ_m from the series of curves computed at 502. The monitoring wavelength λ_m is determined based on the contrast of the monitoring signal within each layer. The contrast is defined as the relative range of the monitoring signal within the layer of interest. The higher the contrast, the more robust the process flow of FIG. 4 will be with respect to random signal noise.

[0069] Advantageously, the relative separation between the monitoring and cutoff wavelengths should be at least about 2%. Once above 2%, the monitoring wavelength λ_m should be chosen to maximize the contrast of each layer. In addition, the optical thickness of the first layer toward the substrate has a significant impact on the signal contrast for the rest of the structure. Therefore, the optical thickness of the first layer should be close to an odd-integer number of quarter-wavelengths at the monitoring wavelength λ_m.

[0070] Having determined the monitoring wavelength λ_m at 503, processing advances to 504 where it is determined how the deposition duration for each layer will be calculated. For layers that are predicted to have little error between the designed thickness d and a simulated actual thickness, deposition duration is controlled by optically monitoring transmission levels T_m through the layer during deposition. For the other layers, their deposition durations are controlled using an expected deposition time t_i based upon designed (“theoretical”) thickness d_i and deposition rate r_i. Accordingly, at 504, the data processor 414 determines which layers are to be optically monitored and which layers are to be timed using an expected deposition time.

[0071] To determine which layers will be optically monitored, the data processor 414 enters a simulation mode to simulate deposition of each of the layers of the optical filter. Only the layers that are determined by the simulation to have the least amount of error are selected for optical monitoring. The simulation mode is nearly identical to the process described below with reference to 505 to 522, except that layers are not actually deposited at 505 and 506, the processing described at 508 is skipped, and instead of actually measuring transmission data T_m vs. t at 511, it is generated. T_m vs. t is generated by adding random noise to the theoretical data T_i vs. d at λ_m from 502 and 503. In the exemplary embodiment, 0.2% peak-to-peak random noise is used, and the maximum amount of error (“threshold”) to select a layer for optical monitoring is to have no more than about 0.2% error from the theoretical thickness d_i. The error calculation, in this regard, is discussed in more detail below with reference to 518 and 519. The layers that are simulated to exceed the threshold amount of error are flagged to have their deposition duration controlled by the best estimate of the deposition rate r_i for that layer or from an average of the rates of the previous layers of like material (typically 10 to 20 of such layers).

[0072] After determining which layers are to be optically monitored at 504, actual deposition of the layers of the LWP filter begins at 505. In particular, the substrate is loaded into the deposition apparatus 400 of FIG. 4, the apparatus is pumped down to a vacuum, and deposition of the first layer (current layer i) is initiated at 506. The expected deposition time t_i for layer i is calculated as the desired thickness d_i divided by the estimated deposition rate r_i for the layer or from an average of the rates of the previous layers of like material at 507. It should be noted, however, that calculation of the expected deposition time t_i at 507 may be calculated prior to beginning actual deposition of the current layer i at 506.

[0073] After calculating the expected deposition time t_i, it is determined whether the current layer i has been identified as a layer to be optically monitored for controlled deposition duration. If the current layer has not been so identified, deposition of the current layer terminates when the expected deposition time t_i from 507 expires, as shown at 509. After the expected deposition time t_i has expired, processing advances to 521 where the next layer is queued up for deposition, as shown at 510.

[0074] If it is determined at 508 that the current layer i is to be optically monitored, the actual transmission T_m is measured at 511 as a function of actual time transpired t until about 95% of the expected deposition time t_i has elapsed. Once about 95% of t_i has elapsed, a new deposition duration is calculated at 512–520. In particular, at 512, 513, and 514, using the T_i vs. d at λ_m curve from 502 and 503, a two-dimensional (2D) array of additional curves is generated by plotting the values of T_i against a 2D array of time vectors t_jk. In particular, at 513, transmission T_ij is generated by plotting T_i against the values t_j=d/r_j, where r_j represents, for each j, a deposition rate having a value close to the predicted value r_i. That is, the set of all r_j values is a range of values surrounding the predicted value r_i. Accordingly, j is an index that counts the number of r values that come from the range surrounding the predicted value r_i. At 514, for each value of j, transmission T_ijk is generated by plotting T_ij against the values t_jk=t_j+Δt_k, where Δt_k represents various values used for a uniform time shift.

[0075] At 515, it is determined whether there is more than one extremum in the curve T_i vs. d at λ_m. If there is more than one extremum at 515, then each of the 2D array of curves generated at 512–514, is scaled in two ways at 516. First, the mid-point between the two extrema for each T_ijk curve is scaled by a factor so that it equals the mid-point between the two extrema of the measured data T_m vs. t. Second, the maximum and minimum values on each T_ijk curve are scaled by scaling uniformly about their mean so that the difference between the maximum and minimum for each curve T_ijk is the same as that on the measured curve T_m vs. t. If there is one or no extremum at 515, then the mean of each T_ijk curve is scaled at 517 by a uniform factor so that it is equal to the mean of the measured curve T_m vs. t.

[0076] After scaling at 516 or 517, processing advances to 518 where error is calculated. For each of the 2D array of generated T_ijk curves, the root-mean-square (RMS) error between each T_ijk curve and the measured curve T_m vs. t is computed. Typically this computation is performed only for data between about 10% and 95% of the expected deposition time t_i. Afterwards, the values of j and k that yield a minimum RMS error at 518 are identified at 519. Therefore, the curve T_ijk vs. t_ijk is taken to be the best approximation of the actual curve T_m vs. t for layer i. At 520, the curve T_ijk vs. t_ijk is compared against the design curve T_i vs. d at λ_m from 502 and 503, and the time t_ijk at which the layer should be terminated is computed. When the measured time t reaches t_jk, the deposition for the optically monitored layer i is terminated.

[0077] After deposition of the current layer i has completed, the apparatus 400 of FIG. 4 is reconfigured at 521 to start depositing the material associated with layer i+1, and the process loops back to 506. However, if all layers of the filter have been deposited, the LWP filter is complete, and processing stops at 522.

[0078] Turning now to FIG. 5, the process flow executed by the data processor 414 when manufacturing a short-wave-pass (“SWP”) filter according to the exemplary embodiment of the present invention is described. The process illustrated with FIG. 5 is based on the inventor's observation that the inverse of the monitoring trace (i.e., the transmission of the monitoring light as a function of time) within each layer follows a sinusoidal pattern. As will be shown, only four parameters, β₁, β₂, β₃, and θ_m+1, are needed to fully describe the behavior of the monitoring trace for each layer.

[0079] Assume that at the monitoring wavelength the incident medium, deposited materials, and substrate are all lossless (practically true). At normal incidence, each layer may be described by its characteristic matrix:

[0080] $\begin{array}{cc}\left[\begin{array}{cc}\cos \theta & -i\sin \theta /n\\ -\mathrm{in}\sin \theta & \cos \theta \end{array}\right]& \left(1\right)\end{array}$

• • [0081] where n is the refractive index of the layer, θ is the accumulated phase within the layer, and i in equations 1 through 8 (and only in these equations) is the square root of −1, or i=√{square root over (−1)}. (It should be noted that although this specification is described in the context of light striking a filter at normal incidence, one skilled in the art will appreciate that this invention also applies to polarized light striking a filter at non-normal incidence.) θ is expressed as:

[0082] $\begin{array}{cc}\theta =\frac{2\pi }{{\lambda }_m}\mathrm{nd}& \left(2\right)\end{array}$

• • [0083] where d is the metric thickness of the layer and λ_m is the monitoring wavelength. Assuming an assembly of m layers have already been deposited, the transmission of the monitoring light within the (m+1)^st layer, the present layer, may be expressed as:

[0084] $\begin{array}{cc}T=\frac{4n_a{n}_s}{H}& \left(3\right)\end{array}$

• • [0085] where T is the level of monitoring signal within the present layer (transmission), and n_a and n_s are the refractive indices of the incident medium and substrate, respectively. H is defined as:
    H=β₁+β₂ cos 2θ_m+1+β₃ sin 2θ_m+1  (4)

[0086] β₁, β₂, and β₃ are defined as:

[0087] $\begin{array}{cc}{\beta }_1=\frac{n_a^2+n_{m+1}^2}{2}\left({p}^2+\frac{{q}^2}{n_{m+1}^2}\right)+2n_a\mathrm{Re}\left({\mathrm{pq}}^{*}\right)& \left(5\right)\end{array}$

• • [0088] where Re(pq*) is the Real Part of the product of the complex number p and the complex conjugate of the complex number q. p and q are defined in equation (8) below.

[0089] $\begin{array}{cc}{\beta }_2=\frac{n_a^2-n_{m+1}^2}{2}\left({p}^2-\frac{{q}^2}{n_{m+1}^2}\right)& \left(6\right)\\ {\beta }_3=\left(\frac{n_a^2}{n_{m+1}}-n_{m+1}\right)\mathrm{Im}\left(p^{*}q\right)& \left(7\right)\end{array}$

[0090] where θ_l is accumulated phased in the l_th layer. Im(pq*) is the Imaginary Part of the product of the complex conjugate of the number p and the complex number q. p and q are defined as:

[0091] $\begin{array}{cc}\left[\begin{array}{c}p\\ q\end{array}\right]=\prod _{l=1}^m\left[\begin{array}{cc}\cos {\theta }_l& -i\sin {\theta }_l/n_l\\ -{\mathrm{in}}_l\sin {\theta }_l& \cos {\theta }_l\end{array}\right]\left[\begin{array}{c}1\\ n_s\end{array}\right]& \left(8\right)\end{array}$

[0092] Based on the above equations, the relationship between the monitoring trace T and the accumulated phase θm+1 within the present layer is established. The inverse of the monitoring trace is sinusoidal, as demonstrated by the expression for H. Further, only four parameters, β₁, β₂, β₃, and θ_m+1, are needed to fully describe the behavior of the monitoring trace in the present layer. Because the thickness d=r×t, where r is the deposition rate and t is the deposition time, a relationship between T and r or t is also established. If the deposition rate is constant, the accumulated phase θ_m+1 is proportional to the deposition rate. Therefore, during the deposition process, the deposition rate may be retrieved with high accuracy by fitting the in-situ measurement of the monitoring trace to the four parameters.

[0093] With this groundwork, the process of FIG. 5 will now be described in greater detail. However, prior to initiating the process of FIG. 5, a design for the SWP filter is prepared. The process of designing a SWP edge filter is very similar to that of LWP filter, with several exceptions. First, the initial structure is (0.5L H 0.5L)^N. Second, the shorter wavelength edge of the QW stopband should be aligned with the desired cutoff wavelength. Third, if the first layer next to the substrate is a low index layer, it should be removed. Finally, it is advantageous, but not necessary, to artificially increase the optical thickness of the first layer.

[0094] With the design of the SWP filter at hand, the design data, as well as deposition rate data are received as input at 601. The input data has the content and format described with reference to 501 in FIG. 4. At 602, the transmission curves T_i vs. d at a series of wavelengths for each i^th layer are calculated as described with reference to 502 in FIG. 4. Choosing the best monitoring wavelength λ_m at 603 is similar to that described with reference to 503 in FIG. 4, except that it may be more advantageous to select λ_m by taking an average of a series of wavelengths than it is for an LWP filter.

[0095] At 604, the β parameters are calculated for each layer at wavelength λ_m using equations (1) through (8) described above. At 605, a determination is made as to which layers should have their deposition duration controlled by optical monitoring and which layers should have their deposition duration timed using an expected deposition time t_i. Such determination is made by simulating the deposition of each layer and selecting the layers having the least amount of simulated error to be optically monitored. Deposition of the other layers will be timed using the expected deposition time t_i.

[0096] The simulation process occurs by executing the processes of 606 to 617 as described below. However, actual deposition does not occur at 606 and 607, the processing described at 609 is skipped, and instead of measuring T_m vs. t at 612, it is generated. λ_m vs. t is generated by adding random noise to the theoretical data T_i vs. d at λ_m from 602 and 603. In the exemplary embodiment, 0.2% peak-to-peak random noise is used, and the maximum amount of error (“threshold”) to select a layer for optical monitoring is to have no more than about 0.5% error from the theoretical resulting thickness d_i. The error calculation, in this regard, is described in more detail below with reference to 613. The layers that are simulated to exceed the threshold amount of error are flagged to have their deposition duration controlled by the best estimate of the deposition rate r_i for that layer or from an average of the rates of the previous layers of like material (typically 10 to 20 such layers).

[0097] Having determined which layers are to be optically monitored at 605, deposition begins at 606. In particular, a substrate is loaded into the deposition apparatus 400, the apparatus 400 is pumped down to vacuum, and deposition of the first layer (current layer i) is initiated at 607. At 608, the expected deposition time t_i for layer i is calculated as the desired thickness d_i divided by the estimated deposition rate for the layer r_i or from an average of the rates of the previous layers of like material. It should be noted, however, that calculation of the expected deposition time t_i at 608 may be calculated prior to beginning actual deposition of the current layer i at 607.

[0098] At 609 it is determined whether the current layer i was identified as an optically monitored layer at 605. If not, deposition occurs until the expected deposition time t_i expires, and the deposition apparatus is configured for deposition of the next layer, as shown at 610, 611, and 616. If it is determined that the current layer i is an optically monitored layer at 609, the transmission T_m of the current layer is measured at 612 as a function of actual time t transpired, thereby producing a measured curve T_m vs. t_i until about 95% of time t_i has elapsed. Once about 95% of the time t_i has elapsed, a new layer time is calculated at 613 to 615.

[0099] To elaborate, at 613, T_i vs. t (where t=d/r and T_i vs. d at λ_m was calculated and selected at 602 and 603, respectively) is fit to the measured curve T_m vs. t from 612. The T_i vs. t curve is fit to the measured curve T_m vs. t by using a function that minimizes the error between the two curves by varying β₁, β₂, β₃, and the deposition rate r. An example of such a function is the Levenberg-Marquardt method implemented under the name “mrqmin( )” in the book Numerical Recipes in C: The Art of Scientific Computing, by Press, W. H.; Teukolsky, S. A.; Vetterling, W. T.; and Flannery, B. P., 2nd ed., Cambridge University Press, Cambridge, 1995. These calculations result in a calculated deposition rate for the current layer i, or r_ci.

[0100] Because of noise in the overall system and the sensitivity of the high-performance SWP filters to small layer-thickness errors, the calculated rates r_ci tend to be insufficiently accurate if used directly. Therefore, a “best rate” for each layer, r_bi, is calculated at 614 as the average of the calculated rate r_ci and calculated rates r_cj, r_cj+2, . . . , r_c,i−4, r_c,i−2 for a certain number (i−j)/2 of previous layers of the same material. In other words, the best rate is a rolling average of the current and previous rates from layers of like material within a certain window. Typically, this window includes about 20 layers.

[0101] At 615, the best rate r_bi is used to calculate the layer termination time t_t=d/r_bi, and the layer is terminated when the clock reaches this time. Once deposition of the current layer is complete, the deposition apparatus 400 of FIG. 4 is reconfigured at 616 to start depositing the material associated with the next layer i+1, and the process loops back to 607. However, if all layers have been deposited, manufacturing of the SWP filter is compete, and the process ends at 617.

[0102] Having described the processes of making LWP and SWP edge filters, the processes of making a notch filter according to embodiments of the invention will now be described. FIG. 7 illustrates a notch filter coating 701 applicable to both single and multi-notch filters, according to an embodiment of the present invention. The notch filter coating 701 is located on one side 702 of a substrate 703. The notch filter coating 701 includes alternating layers of high-index material 704 and low-index material 705. The materials may be hard oxide coating materials such as SiO₂, Ta₂O₅, Nb₂O₅, HfO₂, TiO₂, and Al₂O₅. Although not shown in FIG. 7, an anti-reflection coating may be present on the side 706 of the substrate 703 opposite to the notch filter coating 701. It should be noted that FIG. 7 is used merely as an illustration, is not to scale, and the number of layers is not necessarily accurate. The notch filter coating 701 may be made according to the method for making SWP coatings described above with reference to FIG. 6.

[0103] FIG. 8 illustrates a multi-notch filter coating that utilizes a notch coating 801 on one side 802 of the substrate 803 and a long-wave-pass (LWP) coating 804 on the other side 805 of the substrate 803. Both the notch filter coating 801 and the LWP coating 804 include layers of alternating high-index material 806 and low-index material 807. The materials may be hard oxide coating materials such as SiO₂, Ta₂O₅, Nb₂O₅, HfO₂, TiO₂, and Al₂O₅. It should be noted that FIG. 8 is used merely as an illustration, is not to scale, and the number of layers is not necessarily accurate. As with FIG. 7, the notch filter coating 801 may be made according to the method for making SWP coatings described above with reference to FIG. 6. The LWP coating 804 may be made according to the method of making LWP coatings described above with reference to FIG. 5.

[0104] According to an embodiment of the present invention, the LWP coating 804 in FIG. 8 may be replaced with a multi-notch filter coating, like the multi-notch filter coating 801. The same and/or different multi-notch filter coatings may be deposited on both sides of the substrate 803. For example, three notches may be deposited on one side of the substrate 803, and three different notches may be deposited on the other side of the substrate 803, to produce a six-notch filter. Alternatively, several notches may be deposited on one side of the substrate 803 and the same several notches may be deposited on the other side of the substrate 803 to increase the OD of the notches. In particular, notches that are “weak,” i.e., have a low OD, are strengthened with corresponding notches of higher OD on the other side of the substrate 803. (It should be noted that, due to interference effects associated with multiple reflections between the two multi-notch coatings on, the total OD associated with the two coatings is not necessarily the sum of the individual OD values.) Further, one side of the substrate 803 may have the same notches as the other side, as well as additional different notches. For instance, one side of the substrate 803 may have two notches, and the other side of the substrate 803 may have the same two notches as well as two additional different notches, thereby resulting in a four-notch filter.

[0105] Although the exemplary methods have been described in the context of manufacturing optical edge filters and notch filters, those skilled in the art will appreciate that such methods apply to manufacturing other types of optical filters, or may easily be modified to manufacture other types of optical filters. For instance, the methods are useful for any filter having even a single layer of critical thickness, such as a Fabry-Perot interferometer, where the layer of critical thickness is the resonance cavity. Further, although the exemplary methods are disclosed as having a particular sequence of events, one skilled in the art will appreciate that many of these events may occur in a different order without departing from the scope of the invention. Accordingly, the methods of the present invention are not limited to producing optical edge and notch filters and are not limited to the particular ordering of events described.

[0106] C. The Improved Filters

[0107] The improved edge filters have the general structure schematically illustrated in FIG. 3 but are made by the processes described herein in connection with FIGS. 5 and 6. In essence, the filters comprise a transparent substrate advantageously having a pair of optically flat planar major surfaces and a plurality of alternating layers of relatively high index and relatively low index materials. The materials may be hard oxide coating materials such as SiO₂, Ta₂O₅, Nb₂O₅, HfO₂, TiO₂, and Al₂O₅.

[0108] The edge filters differ from conventional edge filters primarily in the number of layers (typically more than 100) and in that the thicknesses of layers deposited are controlled by the processes of FIGS. 5 and 6 to produce an edge steepness less than about 0.8%. The edge steepness, in this regard, is measured by dividing (a) the edge width from the 50% transmission wavelength to the optical density 6 (“OD6”) wavelength by (b) the 50% transmission wavelength. Accordingly, lower steepness values indicate greater slope. Optical density (“OD”) is a measure of the blockage encountered by impinging light and is defined as follows:
OD=−log₁₀(T)  (9)

[0109] where T is the transmittance having a value between zero and one. OD6 therefore corresponds to a transmittance of 10⁻⁶.

[0110] Advantageously the edge steepness, as defined above, is less than about 0.463%. However, the edge steepness may be increased if necessary. In addition, the filters so made exhibit an average transmission above about 93% and preferably above at least 95% with ripple below about 2% in the operating range. In the case of a filter for a 532 nanometer laser-line, the operating range is approximately 200 nm from the wavelength at which the filter reaches full transmission. One skilled in the art will appreciate that the operating range is larger with filters for laser-lines at higher wavelengths. Transmission of the filters does not drop below 93% and preferably 95% in the operating range. The filters thus provide performance exceeding that of the highest performing conventional soft-coating filters with a more robust and durable hard-coated structure.

[0111] The edge filters can be constructed with an edge wavelength as short as 325 nm and as long as 1064 nm. It is contemplated that this range may be extended from as low as 250 nm to as high as 2,000 nm using the materials listed above.

[0112] As compared with conventional edge filters, the edge filters of the invention provide substantially higher edge steepness and passband transmission. Table I below presents a comparison between the inventive filters and the best known examples of conventional soft-coated and hard-coated thin-film edge filters. The data in Table I are from filters designed to block a 532 nm laser, where the 50% transmission wavelength is 537 nm. Accordingly, steepness (in percentage) is calculated as Edge Width divided by 537 nm.

[0113]

	TABLE I
	Hard-Coated	Soft-Coated	Inventive
Edge Width (50% to	≈3 nm*	≈4 nm*	<1.4 nm
OD4)
Edge Steepness	≈0.556%	≈0.741%	<0.259%
(50% to OD4)
Edge Width (50% to	≈5 nm*	≈6 nm**	<2.5 nm
OD6)
Edge Steepness	≈0.926%	≈1.111%	<0.463%
(50% to OD6)
Laser-Line	>6.0	>5.0	>6.0
Attenuation (OD)
Average Trans-	Approx. 90%	Approx. 85%	>95% and
mission			<= approx. 100%
*Estimated specification
**Edge width for 50% to OD5 (necessarily less than Edge Width for 50% to OD6)

As can be seen from Table I, the edge filters of the present invention provide an improvement in edge steepness and a reduction of optical loss in the transmission band (optical loss defined as 100%—Average Transmission).

[0114] In addition, the inventive edge filters provide a substantial improvement in reliability and durability over soft-coated thin-film filters (the highest performing conventional filters) because the inventive filters are made exclusively with hard oxide glass, whereas soft-coated filters contain soft salts and organic materials susceptible to damage by humidity and temperature extremes.

[0115] The improved notch filters made by the processes disclosed herein have made it possible to achieve optical notch filtering in a thin-film format (at normal or near-normal incidence) with a blocking of OD>6, very high transmission (>90%) outside the notch(es), and a narrow notch bandwidth comparable to that of holographic notch filters. In addition, this performance can be achieved with a single notch or multiple notches. Finally, the inventive notch filters achieve almost the same performance for filters at a 45 degree angle of incidence, with the exception that the blocking is OD>5.

[0116] Table II summarizes the OD, transmission, and bandwidth specifications of the inventive notch filters (for normal incidence).

[0117]

TABLE II
Property	Value	Comments
Laser Line Blocking	>6 OD	OD = −log10
		(transmission)
Notch Bandwidth	17 nm or 600 cm−1 for	Full width at 50%
(typical)	532 nm	transmission points
Average Passband	>90% & <= 100%
Transmission
Passband Bandwidth*	0.75 × λL to 1.33 × λL	λL is the laser wavelength
Angle Tunability	>1% of laser wave-	Wavelength “blue shift”
	length
Temperature	<5 ppm/° C.	<0.003 nm/° C. at 532
Dependence		nm
*The passband includes the wavelength region indicated, but excludes the notch region.

[0118] Note that the bandwidth shown in Table II is given only for a 532 nm filter. For other laser wavelengths (we have demonstrated these filters for wavelengths between 405 nm and 830 nm), the typical bandwidth is found from the formula:
Notch Bandwidth=55×10⁻⁶×λ_L²+14×10⁻³×λ_L−5.9  (10)

[0119] λ_L is the laser wavelength (in nm) and the Notch Bandwidth (NBW) also is in units of nm. The inventive optical notch filters manufactured in accordance with the invention have been demonstrated to have a transmission greater than 90% and less than or equal to about 100% at wavelengths that are greater than or equal to λ_L+1.3(NBW) and less than or equal to λ_L−1.3(NBW). Further, the inventive notch filters have been demonstrated to have a transmission greater than 90% and less than or equal to about 100% at wavelengths that are greater than or equal to λ_L+0.65(NBW), and less than or equal to λ_L−0.65(NBW). Further still, the inventive notch filters have been demonstrated to have a transmission greater than 90% and less than or equal to about 100% at wavelengths between (λ_L+1.3(NBW)) and λ_L/0.75, and between 0.75(λ_L) and (λ_L−1.3(NBW)). In addition, the inventive notch filters have been demonstrated to have a transmission greater than 90% and less than or equal to about 100% at wavelengths between (λ_L+0.65(NBW)) and λ_L/0.75, and between 0.75(λ_L) and (λ_L−0.65(NBW)).

[0120] Another advantage of the inventive notch filters is that their spectral features largely are unaffected by temperature variations. In particular, spectral features of the inventive notch filters, such as the wavelength at which 50% transmission occurs, or the wavelength at which maximum optical density occurs, shift less than approximately 0.0005% per degree Celsius and greater than approximately 0.00005% per degree Celsius.

[0121] Table III compares filters manufactured in accordance with embodiments of the present invention to prior-art holographic notch filters:

[0122]

TABLE III
	Kaiser	Semrock	Kaiser
	Notch-Plus ™	StopLine ™	SuperNotch-Plus ™
Property	Holographic Filter	Notch Filter	Holographic Filter
Notch Band-	<700 cm−1	<670 cm−1	<350 cm−1
width-fre-
quency (for
532 nm
filter)
Notch Band-	<20 nm	<19 nm	<10 nm
width-wave-
length (for
532 nm
filter)
Laser Line	>6 OD	>6 OD	>6 OD
Blocking
Transmission	>85% % <90%	>90% & <=	>85% & <90%
		approx. 100%

[0123] In addition to the spectral advantages over the prior art of holographic filters, the new thin-film notch filters also offer the following advantages. Blocked light is back-reflected, rather than diverted at an acute angle, thereby simplifying system layout and improving stray-light management. Because the inventive notch filters are thin-film filters, they are very compact and simple to integrate into a variety of optical systems. Further, thin-film filters are inherently lower in cost because many filters are manufactured simultaneously in a parallel approach. Compared to both holographic filters and thin-film filters made with older technologies (e.g., soft coatings), the inventive filters offer far superior reliability and durability because the all-dielectric coatings are based on hard refractory oxide materials. The dense, all-glass coatings used for notch filters, according to an embodiment of the invention, enable almost-zero temperature dependence to maximize the operating temperature range of instruments without the need for expensive compensation hardware. Additionally, the temperature shift for the inventive notch filters is less than 5 ppm per degree Celsius (or less than 0.003 nm per degree Celsius for a 532 nm filter). The coatings used for the inventive notch filters offer a very high laser damage threshold. A 532 nm notch filter has been tested and proven to have a damage threshold above 1 Joule/cm² for a 532 nm laser pulse of 10 ns duration.

[0124] For multi-notch filters, dual-, triple-, and quadruple-notch filters according to an embodiment of the present invention, have been demonstrated to have OD>6 blocking at the laser lines. The examples below show two ways of making a multi-notch filter. In one embodiment of a triple-notch filter, which may have a structure as described with reference to FIG. 7, all of the filtering is done in a single coating 701, and the other side of a single-substrate 703 might be AR-coated to achieve the highest possible transmission. In another embodiment of a triple-notch filter, which may have a structure as described with reference to FIG. 8, a dual-notch filter 801 on one side 802 of the single substrate 803 is combined with a long-wave-pass (LWP) filter 804 on the other side 805 of the substrate to provide the full OD>6 blocking at the shortest of the three blocking wavelengths.

[0125] FIG. 9A illustrates a notch filter 901, which may have a structure as described with reference to FIG. 7 or FIG. 8, at a 45 degree angle of incidence. In this example, red light 902 and blue light 904 passes through the filter 901, and green light 903 is blocked by the filter 901. The transmission v. wavelength graph of the filter 901 is shown in FIG. 9B. FIG. 9C illustrates an expanded view of FIG. 9B. As shown in FIGS. 9A to 9C, and contrary to conventional notch filters, the notch filters made according to the present invention work well at a 45 degree angle of incidence. In particular, the notch filters made in accordance with the invention, when operated at an angle of incidence of approximately 45 degrees, exhibit transmission greater than 90% and less than or equal to approximately 100% at wavelengths that are greater than or equal to λ_L+1.3(NBW) and less than or equal to λ_L1.3(NBW). Further, the notch filters made in accordance with the invention, when operated at an angle of incidence of approximately 45 degrees, exhibit transmission greater than 90% and less than or equal to approximately 100% at wavelengths between (λ_L+1.3(NBW)) and λ_L/0.75, and between 0.75(μ_L) and (μ_L−1.3(NBW)). In addition, the inventive notch filters enable very efficient beamsplitting and complete laser-line blocking all in one filter. (“Very efficient” beamsplitting may be described as almost complete reflection (substantially greater than 99% reflection) of light within a notch region, along with very high transmission (>90% transmission) of light outside of a notch region.) It is believed that the combination of very efficient beamsplitting and complete laser-line blocking in a single notch filter is novel.

[0126] To elaborate, a laser may be introduced into a system by reflecting (with near 100% reflection) off of the filter at 45 degrees, then impinges on a sample, and the desired signal light (e.g. Raman scattering or fluorescence) that leaves the sample passes through the filter with high transmission, while the laser light is blocked with very high optical density (OD>5 for average polarization). A fundamental problem for all thin-film filters at a 45 degree angle of incidence is that there is a large degree of “polarization splitting”—that is, the spectral features associated with s- and p-polarized light shift to very different wavelengths. However, the amount of splitting at either edge of the inventive notch filters are extremely small (<0.5% of the laser wavelength), thus enabling this filter to provide very sharp edges for both polarizations simultaneously (and hence for light of average polarization). (“Very sharp” edges may be described as the wavelength range between the point at which high blocking (e.g., >99% blocking) for all polarizations is achieved and the point at which high transmission (e.g. >90% transmission) for all polarizations is achieved is very small, such as substantially less than 2% of the laser wavelength.) No edge filter operated at a 45 degree angle of incidence is known to provide very sharp edges for both polarizations simultaneously this well.

[0127] The invention can now be more clearly understood by consideration of the following specific examples.

[0128] A steep-edge LWP filter for a 532 nanometer notch was designed and fabricated in accordance with the LWP design strategy described above. The filter blocks the 532 nanometer laser light and light of lesser wavelength but to transmit light of longer wavelength. Appendix A gives the layer structure of the design. The optical thickness is given in units of quarter wavelengths (QWs) at the monitoring wavelength of 568 nanometers. The layers are counted from the substrate outward toward air. The substrate is BK7 glass, marketed by vendors such as Schott Glass. The design has 180 layers with a total metric thickness of 12.7 micrometers.

[0129] FIG. 10 shows the theoretical and measured transmission spectra of the resulting 532 nm LWP edge filter in accordance with an embodiment of the invention. Curve 1001 is the theoretical spectrum, curve 1002 is the measured spectrum, and curve 1003 is the laser wavelength line at 532 nm.

[0130] FIG. 11 illustrates the optical density spectrum of the 532 nm LWP filter. As previously discussed, optical density (OD) is a measure of the blockage encountered by impinging light. Curve 1101 is the theoretical OD spectrum, curve 1102 is the measured OD spectrum, and curve 1103 is the 532 nm laser line. It is noteworthy that the filter edge is so steep that it is difficult to measure with standard spectrophotometry equipment. The apparent “kink” between OD3 and 4 is not real, but rather is produced by the measuring instrument.

[0131] A steep-edge SWP filter was designed and fabricated in accordance with the SWP design strategy described above. The filter is to block the 532 nanometer laser light and light of greater wavelength but to transmit light of shorter wavelength. Appendix B provides the layer structure of the design. The optical thickness is given in QWs at the monitoring wavelength of 510 nm. The substrate is BK7 glass. The design has 180 layers with a total metric thickness of 15.1 micrometers.

[0132] FIG. 12 illustrates the theoretical and measured transmission spectra 1201 and 1202, respectively, of the realized SWP filter. The laser-line at 532 nm is shown at 1203.

[0133] FIG. 13 shows the theoretical and measured optical density spectra 1301 and 1302, respectively, and the laser-line 1303. The apparent “kink” that occurs between about OD 4 and 5 is due to the limitations of the measuring instrument, not the filter.

[0134] A 633 nm single-notch filter having a structure corresponding to that shown in FIG. 7 was manufactured according to the processes described herein. The actual coating structure of this filter is set forth in Appendix C. A graph showing both the designed 1401 and measured 1402 transmission spectrum for this filter is shown at FIG. 14. FIG. 15 shows the designed 1501 and measured 1502 optical density for the manufactured 633 nm single-notch filter.

[0135] A single-coating-triple notch filter having a structure corresponding to that shown in FIG. 7 was manufactured according to the processes described herein. The actual coating structure of this filter is set forth in Appendix D. A graph showing both the designed 1601 and measured 1602 transmission spectrum for this filter is shown at FIG. 16. FIG. 17 shows the designed 1701 and measured 1702 optical density for the manufactured single-coating-triple notch filter.

[0136] A triple-notch (dual-notch plus LWP) filter having a structure corresponding to that shown in FIG. 8 was manufactured according to the processes described herein. The actual coating structure of this filter is set forth in Appendix E. A graph showing both the designed 1801 and measured 1802 transmission spectrum for this filter is shown at FIG. 18. FIG. 19 shows the designed 1901 and measured 1902 optical density for this filter. FIG. 20 separately shows the transmission spectra for the dual-notch coating 2001 and the LWP coating 2002 of this triple-notch filter.

[0137] Characteristics were simulated of a single-notch filter manufacturable by the processes described herein and having a structure corresponding to that shown in FIG. 7. The coating structure of this filter is set forth in Appendix F. The predicted average polarization transmission spectrum 2101, the predicted s polarization transmission spectrum 2102, and the predicted p polarization spectrum for this filter with light impinging at a 45 degree angle of incidence are shown at FIG. 21. FIG. 22 shows the predicted average polarization optical density 2201, the predicted s polarization optical density 2202, and the predicted p polarization optical density 2203 for this filter with light impinging at a 45 degree angle of incidence.

[0138] A quadruple-notch (triple-notch plus LWP) filter having a structure corresponding to that shown in FIG. 8 was manufactured according to the processes described herein. The actual coating structure of this filter is set forth in Appendix G. A graph showing both the designed 2301 and measured 2302 transmission spectrum for this filter is shown at FIG. 23. FIG. 24 shows the designed 2401 and measured 2402 optical density for this filter.

[0139] D. Applications of the Filters

[0140] The inventive filters can improve the performance of a variety of optical analysis systems that excite a sample of material with light of a first wavelength to produce a measurable or viewable response of light at a second wavelength different from the first. Such systems, which include Raman spectroscopy and fluorescence spectroscopy, are typically of the construction schematically shown in FIG. 2. They comprise a source of excitation light, an optical path coupling the excitation light to the sample, and one or more first filters in the path between the source and the sample for blocking light at some wavelengths different from the excitation light. They also include an optical path coupling the optical response light from the sample to an analyzer or viewer, and one or more second filters in the path between the sample and the analyzer or viewer for blocking some light other than the optical response. As previously discussed, the first filter(s) may be one or more edge filters, and the second filter(s) may be one or more notch filters and/or edge filters.

[0141] One or more optical edge filters and/or notch filters in accordance with an embodiment of the invention can substantially improve the performance of such optical analytical systems. The greater steepness of edge slope in the edge filter(s) permit(s) return of response wavelengths closer to the excitation wavelength providing an increase in the information content of the returned response. The greater steepness of edge slope in the notch filter provides better blocking of unshifted scattered excitation light in the returned response. The reduction in transmission loss means that the enhanced information return response will be at higher brightness, and the greater hardness and durability of the inventive filters permits a more robust and versatile instrument.

[0142] It is to be understood that the exemplary embodiments are merely illustrative of the present invention and that many variations of the above-described embodiment can be devised by one skilled in the art without departing from the scope of the invention. It is therefore intended that all such variations be included within the scope of the following claims and their equivalents.

[0143]

APPENDIX A
Layer #	Material	Optical Thickness	Metric Thickness (nm)
1	Ta2O5	2.5790	171.93
2	SiO2	0.7851	74.97
3	Ta2O5	0.7323	48.82
4	SiO2	0.7163	68.40
5	Ta2O5	0.8253	55.02
6	SiO2	0.8398	80.19
7	Ta2O5	0.8490	56.60
8	SiO2	0.7960	76.01
9	Ta2O5	0.8058	53.72
10	SiO2	0.8080	77.15
11	Ta2O5	0.8513	56.75
12	SiO2	0.8356	79.79
13	Ta2O5	0.8351	55.67
14	SiO2	0.8029	76.67
15	Ta2O5	0.8280	55.20
16	SiO2	0.8286	79.12
17	Ta2O5	0.8510	56.73
18	SiO2	0.8276	79.03
19	Ta2O5	0.8295	55.30
20	SiO2	0.8124	77.57
21	Ta2O5	0.8402	56.01
22	SiO2	0.8333	79.57
23	Ta2O5	0.8466	58.44
24	SiO2	0.8209	78.39
25	Ta2O5	0.8324	55.49
26	SiO2	0.8202	78.32
27	Ta2O5	0.8441	56.27
28	SiO2	0.8337	79.61
29	Ta2O5	0.8420	56.13
30	SiO2	0.8193	78.23
31	Ta2O5	0.8345	55.63
32	SiO2	0.8262	78.89
33	Ta2O5	0.8475	56.50
34	SiO2	0.8296	79.22
35	Ta2O5	0.8385	55.90
36	SiO2	0.8197	78.27
37	Ta2O5	0.8379	55.86
38	SiO2	0.8305	79.30
39	Ta2O5	0.8472	56.48
40	SiO2	0.8259	78.86
41	Ta2O5	0.8363	55.75
42	SiO2	0.8223	78.52
43	Ta2O5	0.8424	56.16
44	SiO2	0.8311	79.36
45	Ta2O5	0.8432	56.21
46	SiO2	0.8242	78.70
47	Ta2O5	0.8375	55.83
48	SiO2	0.8250	78.78
49	Ta2O5	0.8439	56.26
50	SiO2	0.8305	79.30
51	Ta2O5	0.8417	56.11
52	SiO2	0.8223	78.52
53	Ta2O5	0.8391	55.94
54	SiO2	0.8276	79.03
55	Ta2O5	0.8445	56.30
56	SiO2	0.8282	79.08
57	Ta2O5	0.8402	56.01
58	SiO2	0.8237	78.65
59	Ta2O5	0.8405	56.03
60	SiO2	0.8285	79.11
61	Ta2O5	0.8447	56.31
62	SiO2	0.8264	78.91
63	Ta2O5	0.8391	55.94
64	SiO2	0.8242	78.70
65	Ta2O5	0.8433	56.22
66	SiO2	0.8284	79.10
67	Ta2O5	0.8436	56.24
68	SiO2	0.8256	78.83
69	Ta2O5	0.8382	55.88
70	SiO2	0.8260	78.87
71	Ta2O5	0.8445	56.30
72	SiO2	0.8279	79.05
73	Ta2O5	0.8424	56.16
74	SiO2	0.8242	78.70
75	Ta2O5	0.8400	56.00
76	SiO2	0.8276	79.03
77	Ta2O5	0.8445	56.30
78	SiO2	0.8266	78.93
79	Ta2O5	0.8402	56.01
80	SiO2	0.8246	78.74
81	Ta2O5	0.8432	56.21
82	SiO2	0.8275	79.02
83	Ta2O5	0.8429	56.19
84	SiO2	0.8262	78.89
85	Ta2O5	0.8402	56.01
86	SiO2	0.8265	78.92
87	Ta2O5	0.8417	56.11
88	SiO2	0.8282	79.08
89	Ta2O5	0.8435	56.23
90	SiO2	0.8244	78.72
91	Ta2O5	0.8399	55.99
92	SiO2	0.8275	79.02
93	Ta2O5	0.8436	56.24
94	SiO2	0.8275	79.02
95	Ta2O5	0.8403	56.02
96	SiO2	0.8252	78.80
97	Ta2O5	0.8423	56.15
98	SiO2	0.8278	79.04
99	Ta2O5	0.8426	56.17
100	SiO2	0.8260	78.87
101	Ta2O5	0.8405	56.03
102	SiO2	0.8257	78.84
103	Ta2O5	0.8444	56.29
104	SiO2	0.8268	78.95
105	Ta2O5	0.8414	56.09
106	SiO2	0.8256	78.83
107	Ta2O5	0.8412	56.08
108	SiO2	0.8268	78.95
109	Ta2O5	0.8433	56.22
110	SiO2	0.8266	78.93
111	Ta2O5	0.8409	56.06
112	SiO2	0.8259	78.86
113	Ta2O5	0.8424	56.16
114	SiO2	0.8266	78.93
115	Ta2O5	0.8424	56.16
116	SiO2	0.8265	78.92
117	Ta2O5	0.8406	56.04
118	SiO2	0.8260	78.87
119	Ta2O5	0.8426	56.17
120	SiO2	0.8275	79.02
121	Ta2O5	0.8421	56.14
122	SiO2	0.8249	78.77
123	Ta2O5	0.8405	56.03
124	SiO2	0.8270	78.97
125	Ta2O5	0.8424	56.16
126	SiO2	0.8282	79.08
127	Ta2O5	0.8400	56.00
128	SiO2	0.8245	78.73
129	Ta2O5	0.8421	56.14
130	SiO2	0.8273	79.00
131	Ta2O5	0.8432	56.21
132	SiO2	0.8257	78.84
133	Ta2O5	0.8397	55.98
134	SiO2	0.8246	78.74
135	Ta2O5	0.8429	56.19
136	SiO2	0.8288	79.14
137	Ta2O5	0.8412	56.08
138	SiO2	0.8239	78.67
139	Ta2O5	0.8403	56.02
140	SiO2	0.8261	78.88
141	Ta2O5	0.8423	56.15
142	SiO2	0.8283	79.09
143	Ta2O5	0.8409	56.06
144	SiO2	0.8220	78.49
145	Ta2O5	0.8396	55.97
146	SiO2	0.8283	79.09
147	Ta2O5	0.8441	56.27
148	SiO2	0.8262	78.89
149	Ta2O5	0.8379	55.86
150	SiO2	0.8197	78.27
151	Ta2O5	0.8429	56.19
152	SiO2	0.8307	79.32
153	Ta2O5	0.8420	56.13
154	SiO2	0.8217	78.46
155	Ta2O5	0.8357	55.71
156	SiO2	0.8223	78.52
157	Ta2O5	0.8450	56.33
158	SiO2	0.8308	79.33
159	Ta2O5	0.8372	55.81
160	SiO2	0.8161	77.93
161	Ta2O5	0.8354	55.69
162	SiO2	0.8263	78.90
163	Ta2O5	0.8474	56.40
164	SiO2	0.8253	78.81
165	Ta2O5	0.8288	55.25
166	SiO2	0.8103	77.37
167	Ta2O5	0.8391	55.94
168	SiO2	0.8318	79.43
169	Ta2O5	0.8423	56.15
170	SiO2	0.8083	77.18
171	Ta2O5	0.8178	54.52
172	SiO2	0.8087	77.22
173	Ta2O5	0.8436	56.24
174	SiO2	0.8224	78.53
175	Ta2O5	0.8187	54.58
176	SiO2	0.7696	73.49
177	Ta2O5	0.8021	53.47
178	SiO2	0.7686	73.39
179	Ta2O5	0.7329	48.86
180	SiO2	1.5674	149.67

[0144]

APPENDIX B
Layer #	Material	Optical Thickness	Metric Thickness (nm)
1	Ta2O5	1.5070	89.32
2	SiO2	1.1544	98.77
3	Ta2O5	1.3342	79.08
4	SiO2	1.1510	98.48
5	Ta2O5	1.1930	70.71
6	SiO2	1.1508	98.46
7	Ta2O5	1.2262	72.68
8	SiO2	1.1508	98.46
9	Ta2O5	1.1812	70.01
10	SiO2	1.1501	98.40
11	Ta2O5	1.1692	69.30
12	SiO2	1.1503	98.42
13	Ta2O5	1.1852	70.25
14	SiO2	1.1503	98.42
15	Ta2O5	1.1635	68.96
16	SiO2	1.1500	98.39
17	Ta2O5	1.1530	68.34
18	SiO2	1.1501	98.40
19	Ta2O5	1.1765	69.73
20	SiO2	1.1503	98.42
21	Ta2O5	1.1721	69.47
22	SiO2	1.1500	98.39
23	Ta2O5	1.1534	68.36
24	SiO2	1.1500	98.39
25	Ta2O5	1.1621	68.88
26	SiO2	1.1501	98.40
27	Ta2O5	1.1635	68.96
28	SiO2	1.1500	98.39
29	Ta2O5	1.1483	68.06
30	SiO2	1.1500	98.39
31	Ta2O5	1.1608	68.80
32	SiO2	1.1501	98.40
33	Ta2O5	1.1699	69.34
34	SiO2	1.1501	98.40
35	Ta2O5	1.1566	68.49
36	SiO2	1.1500	98.39
37	Ta2O5	1.1574	68.60
38	SiO2	1.1501	98.40
39	Ta2O5	1.1665	69.14
40	SiO2	1.1501	98.40
41	Ta2O5	1.1544	68.42
42	SiO2	1.1499	98.38
43	Ta2O5	1.1505	68.19
44	SiO2	1.1500	98.39
45	Ta2O5	1.1640	68.99
46	SiO2	1.1501	98.40
47	Ta2O5	1.1591	68.70
48	SiO2	1.1500	98.39
49	Ta2O5	1.1517	68.26
50	SiO2	1.1500	98.39
51	Ta2O5	1.1625	68.90
52	SiO2	1.1501	98.40
53	Ta2O5	1.1608	68.80
54	SiO2	1.1500	98.39
55	Ta2O5	1.1508	68.21
56	SiO2	1.1500	98.39
57	Ta2O5	1.1589	68.69
58	SiO2	1.1501	98.40
59	Ta2O5	1.1628	68.92
60	SiO2	1.1500	98.39
61	Ta2O5	1.1534	68.36
62	SiO2	1.1500	98.39
63	Ta2O5	1.1567	68.56
64	SiO2	1.1500	98.39
65	Ta2O5	1.1623	68.89
66	SiO2	1.1500	98.39
67	Ta2O5	1.1544	68.42
68	SiO2	1.1500	98.39
69	Ta2O5	1.1549	68.45
70	SiO2	1.1500	98.39
71	Ta2O5	1.1620	68.87
72	SiO2	1.1500	98.39
73	Ta2O5	1.1576	68.61
74	SiO2	1.1500	98.39
75	Ta2O5	1.1544	68.42
76	SiO2	1.1500	98.39
77	Ta2O5	1.1596	68.73
78	SiO2	1.1500	98.39
79	Ta2O5	1.1582	68.65
80	SiO2	1.1500	98.39
81	Ta2O5	1.1537	68.38
82	SiO2	1.1500	98.39
83	Ta2O5	1.1576	68.61
84	SiO2	1.1500	98.39
85	Ta2O5	1.1608	68.80
86	SiO2	1.1500	98.39
87	Ta2O5	1.1562	68.53
88	SiO2	1.1500	98.39
89	Ta2O5	1.1561	68.52
90	SiO2	1.1500	98.39
91	Ta2O5	1.1604	68.78
92	SiO2	1.1500	98.39
93	Ta2O5	1.1578	68.61
94	SiO2	1.1500	98.39
95	Ta2O5	1.1537	68.38
96	SiO2	1.1500	98.39
97	Ta2O5	1.1591	68.70
98	SiO2	1.1501	98.40
99	Ta2O5	1.1603	68.77
100	SiO2	1.1500	98.39
101	Ta2O5	1.1532	68.35
102	SiO2	1.1500	98.39
103	Ta2O5	1.1567	68.56
104	SiO2	1.1501	98.40
105	Ta2O5	1.1621	68.88
106	SiO2	1.1500	98.39
107	Ta2O5	1.1552	68.47
108	SiO2	1.1500	98.39
109	Ta2O5	1.1557	68.50
110	SiO2	1.1500	98.39
111	Ta2O5	1.1635	68.96
112	SiO2	1.1501	98.40
113	Ta2O5	1.1569	68.57
114	SiO2	1.1500	98.39
115	Ta2O5	1.1516	68.27
116	SiO2	1.1500	98.39
117	Ta2O5	1.1603	68.77
118	SiO2	1.1501	98.40
119	Ta2O5	1.1593	68.71
120	SiO2	1.1500	98.39
121	Ta2O5	1.1530	68.34
122	SiO2	1.1500	98.39
123	Ta2O5	1.1608	68.80
124	SiO2	1.1501	98.40
125	Ta2O5	1.1640	68.99
126	SiO2	1.1500	98.39
127	Ta2O5	1.1539	68.39
128	SiO2	1.1500	98.39
129	Ta2O5	1.1569	68.57
130	SiO2	1.1501	98.40
131	Ta2O5	1.1642	69.00
132	SiO2	1.1501	98.40
133	Ta2O5	1.1562	68.53
134	SiO2	1.1500	98.39
135	Ta2O5	1.1554	68.48
136	SiO2	1.1500	98.39
137	Ta2O5	1.1643	69.01
138	SiO2	1.1501	98.40
139	Ta2O5	1.1579	68.63
140	SiO2	1.1500	98.39
141	Ta2O5	1.1513	68.24
142	SiO2	1.1500	98.39
143	Ta2O5	1.1626	68.91
144	SiO2	1.1501	98.40
145	Ta2O5	1.1665	69.14
146	SiO2	1.1501	98.40
147	Ta2O5	1.1576	68.61
148	SiO2	1.1500	98.39
149	Ta2O5	1.1643	69.01
150	SiO2	1.1501	98.40
151	Ta2O5	1.1687	69.27
152	SiO2	1.1501	98.40
153	Ta2O5	1.1520	68.28
154	SiO2	1.1499	98.38
155	Ta2O5	1.1569	68.57
156	SiO2	1.1501	98.40
157	Ta2O5	1.1758	69.69
158	SiO2	1.1502	98.41
159	Ta2O5	1.1685	69.26
160	SiO2	1.1501	98.40
161	Ta2O5	1.1655	69.08
162	SiO2	1.1502	98.41
163	Ta2O5	1.1812	70.01
164	SiO2	1.1503	98.42
165	Ta2O5	1.1739	69.58
166	SiO2	1.1501	98.40
167	Ta2O5	1.1716	69.44
168	SiO2	1.1505	98.43
169	Ta2O5	1.2062	71.49
170	SiO2	1.1507	98.45
171	Ta2O5	1.2025	71.27
172	SiO2	1.1506	98.44
173	Ta2O5	1.2021	71.25
174	SiO2	1.1512	98.49
175	Ta2O5	1.2828	76.03
176	SiO2	1.1521	98.57
177	Ta2O5	1.3081	77.53
178	SiO2	1.1524	98.60
179	Ta2O5	1.3750	81.50
180	SiO2	0.5780	49.45

[0145]

APPENDIX C
633 nm single-notch filter example
Total number of layers: 152
Reference wavelength: 632.8 nm
Layer #	Material	Metric Thickness (nm)
1	Ta2O5	139.28811
2	SiO2	213.911479
3	Ta2O5	138.698607
4	SiO2	222.923555
5	Ta2O5	142.834465
6	SiO2	224.190623
7	Ta2O5	139.953649
8	SiO2	222.700222
9	Ta2O5	140.723242
10	SiO2	225.591053
11	Ta2O5	140.069792
12	SiO2	226.494695
13	Ta2O5	139.733658
14	SiO2	230.057231
15	Ta2O5	138.455212
16	SiO2	230.012006
17	Ta2O5	137.652405
18	SiO2	231.491287
19	Ta2O5	137.112544
20	SiO2	230.898071
21	Ta2O5	136.56315
22	SiO2	232.401128
23	Ta2O5	136.193571
24	SiO2	233.290131
25	Ta2O5	135.525826
26	SiO2	234.138504
27	Ta2O5	135.235488
28	SiO2	234.436992
29	Ta2O5	134.751592
30	SiO2	234.215835
31	Ta2O5	134.700197
32	SiO2	235.215953
33	Ta2O5	134.319285
34	SiO2	235.23197
35	Ta2O5	134.141431
36	SiO2	236.26591
37	Ta2O5	133.852823
38	SiO2	235.692752
39	Ta2O5	133.791075
40	SiO2	236.227239
41	Ta2O5	133.634831
42	SiO2	236.023971
43	Ta2O5	133.498929
44	SiO2	236.819458
45	Ta2O5	133.389332
46	SiO2	236.800651
47	Ta2O5	133.236556
48	SiO2	236.754549
49	Ta2O5	133.258851
50	SiO2	236.738611
51	Ta2O5	133.165059
52	SiO2	236.713197
53	Ta2O5	133.1584
54	SiO2	237.328616
55	Ta2O5	133.033007
56	SiO2	237.0356
57	Ta2O5	133.04785
58	SiO2	237.337405
59	Ta2O5	132.968077
60	SiO2	236.786098
61	Ta2O5	132.962244
62	SiO2	237.399614
63	Ta2O5	132.890701
64	SiO2	237.228576
65	Ta2O5	132.901903
66	SiO2	237.587371
67	Ta2O5	132.884176
68	SiO2	237.211067
69	Ta2O5	132.866745
70	SiO2	237.156016
71	Ta2O5	132.8752
72	SiO2	237.333498
73	Ta2O5	132.832563
74	SiO2	237.392681
75	Ta2O5	132.885776
76	SiO2	237.666196
77	Ta2O5	132.834586
78	SiO2	237.116806
79	Ta2O5	132.858486
80	SiO2	237.326207
81	Ta2O5	132.83121
82	SiO2	237.021654
83	Ta2O5	132.902491
84	SiO2	237.650372
85	Ta2O5	132.904564
86	SiO2	237.21769
87	Ta2O5	132.926435
88	SiO2	237.306033
89	Ta2O5	132.918344
90	SiO2	236.899546
91	Ta2O5	132.965657
92	SiO2	237.091782
93	Ta2O5	133.046134
94	SiO2	237.269179
95	Ta2O5	133.067987
96	SiO2	237.056435
97	Ta2O5	133.103914
98	SiO2	237.000356
99	Ta2O5	133.073437
100	SiO2	236.439923
101	Ta2O5	133.217288
102	SiO2	236.905146
103	Ta2O5	133.335387
104	SiO2	236.553741
105	Ta2O5	133.463364
106	SiO2	236.834114
107	Ta2O5	133.484189
108	SiO2	235.9224
109	Ta2O5	133.581673
110	SiO2	235.998739
111	Ta2O5	133.725284
112	SiO2	235.754216
113	Ta2O5	133.941867
114	SiO2	235.94738
115	Ta2O5	134.182591
116	SiO2	235.531469
117	Ta2O5	134.219385
118	SiO2	234.742682
119	Ta2O5	134.41059
120	SiO2	234.584301
121	Ta2O5	134.738459
122	SiO2	234.055298
123	Ta2O5	135.211026
124	SiO2	234.545358
125	Ta2O5	135.481658
126	SiO2	233.143237
127	Ta2O5	135.728033
128	SiO2	232.701538
129	Ta2O5	136.048534
130	SiO2	231.152273
131	Ta2O5	136.595729
132	SiO2	231.748662
133	Ta2O5	137.530855
134	SiO2	230.960454
135	Ta2O5	137.947255
136	SiO2	230.072331
137	Ta2O5	138.451153
138	SiO2	227.742065
139	Ta2O5	138.497134
140	SiO2	225.988236
141	Ta2O5	140.177979
142	SiO2	226.801241
143	Ta2O5	141.49776
144	SiO2	226.145332
145	Ta2O5	143.665141
146	SiO2	228.484731
147	Ta2O5	144.557317
148	SiO2	223.516892
149	Ta2O5	145.28608
150	SiO2	228.838173
151	Ta2O5	146.633943
152	SiO2	112.925644

[0146]

APPENDIX D
Triple Notch Filter - Example 1
Total number of layers: 120
Layer #	Material	Metric Thickness (nm)
1	Ta2O5	151.12
2	SiO2	217
3	Ta2O5	171.64
4	SiO2	229.88
5	Ta2O5	173.23
6	SiO2	201.44
7	Ta2O5	183.5
8	SiO2	270.79
9	Ta2O5	145.34
10	SiO2	233.66
11	Ta2O5	151.48
12	SiO2	288.84
13	Ta2O5	182.25
14	SiO2	170.12
15	Ta2O5	203.39
16	SiO2	226.94
17	Ta2O5	180.4
18	SiO2	263.07
19	Ta2O5	120.98
20	SiO2	92.79
21	Ta2O5	194.26
22	SiO2	248.44
23	Ta2O5	147.55
24	SiO2	364.18
25	Ta2O5	80.89
26	SiO2	283.31
27	Ta2O5	179.72
28	SiO2	160.01
29	Ta2O5	102.43
30	SiO2	171.99
31	Ta2O5	203.75
32	SiO2	292.8
33	Ta2O5	193.03
34	SiO2	142.13
35	Ta2O5	119.82
36	SiO2	367.16
37	Ta2O5	179.8
38	SiO2	96.24
39	Ta2O5	205.85
40	SiO2	172.98
41	Ta2O5	170.21
42	SiO2	236.3
43	Ta2O5	54.01
44	SiO2	259.02
45	Ta2O5	97.77
46	SiO2	141.69
47	Ta2O5	175.48
48	SiO2	143.74
49	Ta2O5	152.44
50	SiO2	256.19
51	Ta2O5	186.63
52	SiO2	169.46
53	Ta2O5	66.38
54	SiO2	95.6
55	Ta2O5	171.86
56	SiO2	130.02
57	Ta2O5	123.68
58	SiO2	354.01
59	Ta2O5	219.38
60	SiO2	86.66
61	Ta2O5	200.09
62	SiO2	95.49
63	Ta2O5	128.88
64	SiO2	252.19
65	Ta2O5	155.48
66	SiO2	78.93
67	Ta2O5	193.21
68	SiO2	109.59
69	Ta2O5	227.4
70	SiO2	108.66
71	Ta2O5	181.63
72	SiO2	235.01
73	Ta2O5	178.47
74	SiO2	157
75	Ta2O5	209.59
76	SiO2	97.4
77	Ta2O5	65.33
78	SiO2	239.19
79	Ta2O5	119.79
80	SiO2	143.37
81	Ta2O5	122.2
82	SiO2	294.51
83	Ta2O5	205.8
84	SiO2	99.03
85	Ta2O5	211.92
86	SiO2	340.42
87	Ta2O5	141.04
88	SiO2	275.84
89	Ta2O5	200.67
90	SiO2	99.19
91	Ta2O5	103.35
92	SiO2	290.15
93	Ta2O5	179.76
94	SiO2	227.27
95	Ta2O5	196.98
96	SiO2	151.68
97	Ta2O5	205.66
98	SiO2	93.75
99	Ta2O5	193.92
100	SiO2	210.8
101	Ta2O5	147.71
102	SiO2	178.36
103	Ta2O5	107.16
104	SiO2	92.93
105	Ta2O5	202.39
106	SiO2	265.16
107	Ta2O5	116.18
108	SiO2	130.33
109	Ta2O5	143.89
110	SiO2	250.52
111	Ta2O5	196.66
112	SiO2	356.2
113	Ta2O5	180.33
114	SiO2	415.76
115	Ta2O5	155.37
116	SiO2	189.38
117	Ta2O5	100.78
118	SiO2	205.98
119	Ta2O5	94.38
120	SiO2	78.28

[0147]

APPENDIX E
Triple Notch Filter - Example 2
Layer #	Material	Metric Thickness (nm)
Side 1 Coating (dual-notch filter coating):
Total number of layers: 182
1	Ta2O5	114.153439
2	SiO2	157.717654
3	Ta2O5	93.775614
4	SiO2	151.16149
5	Ta2O5	94.674041
6	SiO2	153.177853
7	Ta2O5	103.330594
8	SiO2	136.813886
9	Ta2O5	123.221684
10	SiO2	170.165231
11	Ta2O5	131.802866
12	SiO2	183.052286
13	Ta2O5	113.731231
14	SiO2	190.263665
15	Ta2O5	109.033293
16	SiO2	197.218221
17	Ta2O5	117.499573
18	SiO2	177.377991
19	Ta2O5	128.187949
20	SiO2	153.245943
21	Ta2O5	138.270341
22	SiO2	156.06567
23	Ta2O5	138.799491
24	SiO2	175.892865
25	Ta2O5	111.031003
26	SiO2	176.275269
27	Ta2O5	108.18978
28	SiO2	69.395768
29	Ta2O5	125.750681
30	SiO2	161.92254
31	Ta2O5	80.222207
32	SiO2	156.885469
33	Ta2O5	82.843287
34	SiO2	177.228343
35	Ta2O5	105.576423
36	SiO2	108.649611
37	Ta2O5	133.440193
38	SiO2	150.061469
39	Ta2O5	99.706309
40	SiO2	159.044032
41	Ta2O5	142.29338
42	SiO2	260.832475
43	Ta2O5	100.621191
44	SiO2	204.029954
45	Ta2O5	138.556941
46	SiO2	197.31996
47	Ta2O5	119.275496
48	SiO2	79.241534
49	Ta2O5	38.649707
50	SiO2	194.279972
51	Ta2O5	117.970841
52	SiO2	101.317606
53	Ta2O5	116.649342
54	SiO2	86.423162
55	Ta2O5	106.866918
56	SiO2	171.463451
57	Ta2O5	88.669544
58	SiO2	94.453435
59	Ta2O5	123.339871
60	SiO2	178.026171
61	Ta2O5	126.463133
62	SiO2	216.184838
63	Ta2O5	96.986333
64	SiO2	221.49827
65	Ta2O5	98.358886
66	SiO2	165.895218
67	Ta2O5	105.83176
68	SiO2	166.715711
69	Ta2O5	62.200485
70	SiO2	141.712221
71	Ta2O5	142.288195
72	SiO2	276.477646
73	Ta2O5	105.035264
74	SiO2	128.703943
75	Ta2O5	90.234135
76	SiO2	177.307184
77	Ta2O5	89.075119
78	SiO2	90.540569
79	Ta2O5	101.505992
80	SiO2	159.415818
81	Ta2O5	97.202491
82	SiO2	175.720535
83	Ta2O5	37.388654
84	SiO2	151.427469
85	Ta2O5	142.952872
86	SiO2	138.37107
87	Ta2O5	139.214391
88	SiO2	161.411918
89	Ta2O5	97.112001
90	SiO2	129.914329
91	Ta2O5	134.878447
92	SiO2	133.556056
93	Ta2O5	172.842172
94	SiO2	165.902157
95	Ta2O5	109.01547
96	SiO2	179.235282
97	Ta2O5	93.081471
98	SiO2	235.132262
99	Ta2O5	94.507558
100	SiO2	180.248743
101	Ta2O5	103.966842
102	SiO2	151.429185
103	Ta2O5	89.321644
104	SiO2	218.852726
105	Ta2O5	99.344103
106	SiO2	197.235949
107	Ta2O5	88.921128
108	SiO2	148.713969
109	Ta2O5	83.639602
110	SiO2	142.596972
111	Ta2O5	122.495755
112	SiO2	108.518164
113	Ta2O5	74.482388
114	SiO2	143.88971
115	Ta2O5	109.781714
116	SiO2	133.173706
117	Ta2O5	115.265969
118	SiO2	78.616539
119	Ta2O5	105.110668
120	SiO2	215.958027
121	Ta2O5	37.701767
122	SiO2	164.218016
123	Ta2O5	128.468658
124	SiO2	171.639224
125	Ta2O5	94.15999
126	SiO2	120.467284
127	Ta2O5	126.390211
128	SiO2	139.13556
129	Ta2O5	61.089981
130	SiO2	146.147387
131	Ta2O5	96.952437
132	SiO2	138.688893
133	Ta2O5	109.292782
134	SiO2	122.811223
135	Ta2O5	68.085994
136	SiO2	136.051226
137	Ta2O5	116.260881
138	SiO2	124.50687
139	Ta2O5	89.970705
140	SiO2	142.168433
141	Ta2O5	69.084155
142	SiO2	148.777999
143	Ta2O5	131.197681
144	SiO2	60.311187
145	Ta2O5	96.187059
146	SiO2	123.528594
147	Ta2O5	102.422788
148	SiO2	128.350868
149	Ta2O5	108.014485
150	SiO2	128.522579
151	Ta2O5	76.936842
152	SiO2	117.161904
153	Ta2O5	112.360414
154	SiO2	137.892631
155	Ta2O5	85.703113
156	SiO2	139.033299
157	Ta2O5	82.154875
158	SiO2	125.658942
159	Ta2O5	111.108391
160	SiO2	141.083905
161	Ta2O5	70.362136
162	SiO2	136.557935
163	Ta2O5	95.533347
164	SiO2	134.59897
165	Ta2O5	100.468621
166	SiO2	138.552046
167	Ta2O5	75.619664
168	SiO2	130.234071
169	Ta2O5	104.758228
170	SiO2	140.001703
171	Ta2O5	87.542283
172	SiO2	140.070545
173	Ta2O5	84.584695
174	SiO2	142.914639
175	Ta2O5	105.431785
176	SiO2	130.68232
177	Ta2O5	91.421305
178	SiO2	154.264364
179	Ta2O5	111.859298
180	SiO2	171.979159
181	Ta2O5	128.597735
182	SiO2	88.984374
Side 2 Coating (LWP coating):
Total number of layers: 92
1	Ta2O5	116.088031
2	SiO2	156.080041
3	Ta2O5	106.596232
4	SiO2	200.382664
5	Ta2O5	28.199931
6	SiO2	62.137413
7	Ta2O5	41.708366
8	SiO2	42.343909
9	Ta2O5	51.054043
10	SiO2	59.506799
11	Ta2O5	35.932895
12	SiO2	54.587367
13	Ta2O5	50.349591
14	SiO2	61.44422
15	Ta2O5	36.083168
16	SiO2	50.886042
17	Ta2O5	54.096038
18	SiO2	56.61749
19	Ta2O5	35.224914
20	SiO2	60.09087
21	Ta2O5	48.702367
22	SiO2	58.717084
23	Ta2O5	37.691627
24	SiO2	56.469018
25	Ta2O5	49.794435
26	SiO2	55.675671
27	Ta2O5	36.44051
28	SiO2	58.416781
29	Ta2O5	52.889348
30	SiO2	55.277351
31	Ta2O5	37.091512
32	SiO2	59.219815
33	Ta2O5	48.714621
34	SiO2	55.366964
35	Ta2O5	36.672424
36	SiO2	62.401163
37	Ta2O5	48.715399
38	SiO2	53.696184
39	Ta2O5	39.799015
40	SiO2	59.798715
41	Ta2O5	49.008374
42	SiO2	52.094972
43	Ta2O5	38.641915
44	SiO2	61.044881
45	Ta2O5	46.880749
46	SiO2	58.897418
47	Ta2O5	37.976951
48	SiO2	59.908084
49	Ta2O5	47.700491
50	SiO2	55.525992
51	Ta2O5	36.49871
52	SiO2	62.877184
53	Ta2O5	49.532916
54	SiO2	50.960957
55	Ta2O5	40.054229
56	SiO2	63.001077
57	Ta2O5	46.502656
58	SiO2	55.825009
59	Ta2O5	35.497826
60	SiO2	66.045386
61	Ta2O5	45.688436
62	SiO2	53.864834
63	Ta2O5	40.834133
64	SiO2	62.032116
65	Ta2O5	45.704171
66	SiO2	54.643351
67	Ta2O5	37.651991
68	SiO2	63.758016
69	Ta2O5	46.395918
70	SiO2	54.935054
71	Ta2O5	37.056207
72	SiO2	64.475794
73	Ta2O5	48.996168
74	SiO2	50.792097
75	Ta2O5	37.019818
76	SiO2	65.188044
77	Ta2O5	47.744456
78	SiO2	48.824458
79	Ta2O5	37.772169
80	SiO2	69.082305
81	Ta2O5	50.798138
82	SiO2	36.906081
83	Ta2O5	41.827675
84	SiO2	72.011966
85	Ta2O5	45.644578
86	SiO2	27.997071
87	Ta2O5	52.947732
88	SiO2	86.408622
89	Ta2O5	21.662357
90	SiO2	41.675003
91	Ta2O5	63.907358
92	SiO2	88.987848

[0148]

APPENDIX F
45 Degree Single Notch Filter Example
Total number of layers: 186
Total metric thickness: 31.5 μm
Reference wavelength: 532.0 nm
Layer #	Material	Metric Thickness (nm)
1	Ti2O5	123.60
2	SiO2	203.72
3	Ti2O5	123.36
4	SiO2	209.59
5	Ti2O5	126.07
6	SiO2	209.34
7	Ti2O5	123.84
8	SiO2	207.84
9	Ti2O5	125.09
10	SiO2	212.20
11	Ti2O5	125.77
12	SiO2	213.54
13	Ti2O5	125.30
14	SiO2	215.37
15	Ti2O5	124.23
16	SiO2	214.55
17	Ti2O5	123.32
18	SiO2	214.94
19	Ti2O5	123.38
20	SiO2	215.84
21	Ti2O5	123.16
22	SiO2	216.67
23	Ti2O5	122.92
24	SiO2	217.79
25	Ti2O5	122.17
26	SiO2	217.20
27	Ti2O5	121.85
28	SiO2	217.86
29	Ti2O5	121.85
30	SiO2	218.04
31	Ti2O5	121.73
32	SiO2	219.12
33	Ti2O5	121.41
34	SiO2	219.14
35	Ti2O5	120.98
36	SiO2	218.93
37	Ti2O5	120.93
38	SiO2	219.38
39	Ti2O5	120.91
40	SiO2	219.61
41	Ti2O5	120.87
42	SiO2	220.41
43	Ti2O5	120.54
44	SiO2	219.95
45	Ti2O5	120.34
46	SiO2	220.12
47	Ti2O5	120.40
48	SiO2	220.20
49	Ti2O5	120.43
50	SiO2	220.68
51	Ti2O5	120.30
52	SiO2	220.81
53	Ti2O5	120.06
54	SiO2	220.50
55	Ti2O5	120.09
56	SiO2	220.71
57	Ti2O5	120.14
58	SiO2	220.72
59	Ti2O5	120.11
60	SiO2	221.29
61	Ti2O5	119.97
62	SiO2	220.83
63	Ti2O5	119.88
64	SiO2	220.84
65	Ti2O5	119.91
66	SiO2	221.00
67	Ti2O5	120.02
68	SiO2	221.17
69	Ti2O5	119.90
70	SiO2	221.37
71	Ti2O5	119.70
72	SiO2	220.89
73	Ti2O5	119.74
74	SiO2	221.25
75	Ti2O5	119.88
76	SiO2	221.18
77	Ti2O5	119.91
78	SiO2	221.56
79	Ti2O5	119.76
80	SiO2	221.26
81	Ti2O5	119.68
82	SiO2	221.06
83	Ti2O5	119.78
84	SiO2	221.28
85	Ti2O5	119.84
86	SiO2	221.33
87	Ti2O5	119.77
88	SiO2	221.55
89	Ti2O5	119.65
90	SiO2	221.08
91	Ti2O5	119.67
92	SiO2	221.32
93	Ti2O5	119.76
94	SiO2	221.23
95	Ti2O5	119.82
96	SiO2	221.50
97	Ti2O5	119.78
98	SiO2	221.47
99	Ti2O5	119.68
100	SiO2	221.13
101	Ti2O5	119.72
102	SiO2	221.24
103	Ti2O5	119.82
104	SiO2	221.23
105	Ti2O5	119.89
106	SiO2	221.60
107	Ti2O5	119.73
108	SiO2	221.02
109	Ti2O5	119.67
110	SiO2	221.05
111	Ti2O5	119.82
112	SiO2	221.11
113	Ti2O5	120.00
114	SiO2	221.27
115	Ti2O5	119.87
116	SiO2	221.27
117	Ti2O5	119.78
118	SiO2	220.85
119	Ti2O5	119.83
120	SiO2	221.11
121	Ti2O5	119.99
122	SiO2	220.89
123	Ti2O5	120.04
124	SiO2	221.30
125	Ti2O5	119.99
126	SiO2	220.81
127	Ti2O5	119.91
128	SiO2	220.55
129	Ti2O5	120.07
130	SiO2	220.76
131	Ti2O5	120.23
132	SiO2	220.86
133	Ti2O5	120.29
134	SiO2	220.79
135	Ti2O5	120.09
136	SiO2	220.09
137	Ti2O5	120.22
138	SiO2	220.34
139	Ti2O5	120.50
140	SiO2	220.26
141	Ti2O5	120.60
142	SiO2	220.43
143	Ti2O5	120.55
144	SiO2	219.83
145	Ti2O5	120.53
146	SiO2	219.37
147	Ti2O5	120.79
148	SiO2	219.55
149	Ti2O5	121.13
150	SiO2	219.40
151	Ti2O5	121.27
152	SiO2	219.46
153	Ti2O5	121.17
154	SiO2	218.22
155	Ti2O5	121.30
156	SiO2	218.14
157	Ti2O5	121.87
158	SiO2	218.01
159	Ti2O5	122.23
160	SiO2	218.04
161	Ti2O5	122.39
162	SiO2	217.18
163	Ti2O5	122.25
164	SiO2	215.81
165	Ti2O5	122.74
166	SiO2	215.99
167	Ti2O5	123.61
168	SiO2	215.56
169	Ti2O5	124.16
170	SiO2	215.84
171	Ti2O5	124.05
172	SiO2	213.33
173	Ti2O5	123.76
174	SiO2	212.14
175	Ti2O5	125.08
176	SiO2	212.08
177	Ti2O5	126.39
178	SiO2	213.29
179	Ti2O5	128.31
180	SiO2	215.71
181	Ti2O5	128.69
182	SiO2	212.95
183	Ti2O5	129.07
184	SiO2	216.23
185	Ti2O5	129.24
186	SiO2	106.98

[0149]

APPENDIX G
Quadruple-notch Filter Example
Layer #	Material	Metric Thickness (nm)
Side 1 Coating (triple-notch filter coating):
Total number of layers = 152
Total thickness = 19.40648 micrometers
1	Nb2O5	101.92
2	SiO2	162.5
3	Nb2O5	92.46
4	SiO2	156.76
5	Nb2O5	91.04
6	SiO2	153.88
7	Nb2O5	199.39
8	SiO2	170.78
9	Nb2O5	87.39
10	SiO2	150.74
11	Nb2O5	100.5
12	SiO2	124.45
13	Nb2O5	85.14
14	SiO2	142.78
15	Nb2O5	88.34
16	SiO2	148.85
17	Nb2O5	101.38
18	SiO2	185.73
19	Nb2O5	194.95
20	SiO2	189.19
21	Nb2O5	97.25
22	SiO2	184.79
23	Nb2O5	98.53
24	SiO2	336.62
25	Nb2O5	101.18
26	SiO2	143.35
27	Nb2O5	89.86
28	SiO2	194.69
29	Nb2O5	191.09
30	SiO2	178.48
31	Nb2O5	83.11
32	SiO2	126.39
33	Nb2O5	100.86
34	SiO2	175.48
35	Nb2O5	119.67
36	SiO2	40
37	Nb2O5	121.17
38	SiO2	140.9
39	Nb2O5	80.77
40	SiO2	195.29
41	Nb2O5	80.27
42	SiO2	146.36
43	Nb2O5	95.81
44	SiO2	116.65
45	Nb2O5	84.42
46	SiO2	156.08
47	Nb2O5	109.8
48	SiO2	147.36
49	Nb2O5	71.34
50	SiO2	158.05
51	Nb2O5	97.78
52	SiO2	54.35
53	Nb2O5	96.24
54	SiO2	189.42
55	Nb2O5	83.79
56	SiO2	147.78
57	Nb2O5	89.43
58	SiO2	116.73
59	Nb2O5	87.44
60	SiO2	118.84
61	Nb2O5	91.55
62	SiO2	183.51
63	Nh205	72.48
64	SiO2	155.62
65	Nb2O5	101.34
66	SiO2	102.32
67	Nb2O5	175.64
68	SiO2	161.6
69	Nb2O5	101.38
70	SiO2	190.1
71	Nh205	109.54
72	SiO2	138.02
73	Nb2O5	83.95
74	SiO2	201.74
75	Nb2O5	76.68
76	SiO2	151.87
77	Nb2O5	96.69
78	SiO2	104.51
79	Nb2O5	71.13
80	SiO2	143.51
81	Nb2O5	93.38
82	SiO2	159.31
83	Nb2O5	92.66
84	SiO2	134.29
85	Nb2O5	109.58
86	SiO2	64.3
87	Nb2O5	95.83
88	SiO2	80.61
89	Nb2O5	121.17
90	SiO2	158.16
91	Nb2O5	126.18
92	SiO2	304.12
93	Nb2O5	91.08
94	SiO2	142.31
95	Nb2O5	116.44
96	SiO2	142.9
97	Nb2O5	102.19
98	SiO2	155.26
99	Nb2O5	42.77
100	SiO2	117.74
101	Nb2O5	96.83
102	SiO2	157.4
103	Nb2O5	80.23
104	SiO2	170.92
105	Nb2O5	80.26
106	SiO2	152.18
107	Nb2O5	59.5
108	SiO2	150.8
109	Nb2O5	55.05
110	SiO2	179.98
111	Nb2O5	72.95
112	SiO2	147.86
113	Nb2O5	113.24
114	SiO2	113.94
115	Nb2O5	75.53
116	SiO2	148.34
117	Nb2O5	86.68
118	SiO2	151.37
119	Nb2O5	112.12
120	SiO2	187.87
121	Nb2O5	173.08
122	SiO2	142.73
123	Nh2O5	111.37
124	SiO2	130.1
125	Nb2O5	111.36
126	SiO2	169.22
127	Nb2O5	40.48
128	SiO2	165.45
129	Nb2O5	80.24
130	SiO2	152.88
131	Nb2O5	93.66
132	SiO2	142.15
133	Nb2O5	101.36
134	SiO2	139.3
135	Nb2O5	68.39
136	SiO2	169.49
137	Nb2O5	103.48
138	SiO2	375.72
139	Nb2O5	104.58
140	SiO2	334.56
141	Nb2O5	109.17
142	SiO2	145.03
143	Nb2O5	90.92
144	SiO2	154.29
145	Nb2O5	78.49
146	SiO2	140.27
147	Nb2O5	92.97
148	SiO2	144.86
149	Nb2O5	93.92
150	SiO2	153.94
151	Nb2O5	88.36
152	SiO2	72.56
Side 2 Coating (long-wave-pass filter coating):
Total number of layers = 62
Total thickness = 2.94689 micrometers
1	Nb2O5	20.02
2	SiO2	50.32
3	Nb2O5	35.28
4	SiO2	54.08
5	Nb2O5	31.38
6	SiO2	62.56
7	Nb2O5	34.52
8	SiO2	56.07
9	Nb2O5	34.68
10	SiO2	62.44
11	Nb2O5	33.45
12	SiO2	58.99
13	Nb2O5	35.4
14	SiO2	60.77
15	Nb2O5	33.56
16	SiO2	60.87
17	Nb2O5	34.43
18	SiO2	60.55
19	Nb2O5	34.81
20	SiO2	60.22
21	Nb2O5	34.69
22	SiO2	61.21
23	Nb2O5	34.13
24	SiO2	61.26
25	Nb2O5	34.84
26	SiO2	59.87
27	Nb2O5	34.51
28	SiO2	61.73
29	Nb2O5	34.78
30	SiO2	59.61
31	Nb2O5	34.7
32	SiO2	62.29
33	Nb2O5	34.39
34	SiO2	59.12
35	Nb2O5	35.16
36	SiO2	62.52
37	Nb2O5	33.71
38	SiO2	59.14
39	Nb2O5	35.78
40	SiO2	62.24
41	Nb2O5	32.88
42	SiO2	59.83
43	Nb2O5	36.47
44	SiO2	61.3
45	Nb2O5	32.22
46	SiO2	62.34
47	Nb2O5	36.1
48	SiO2	58.96
49	Nb2O5	33.41
50	SiO2	62.89
51	Nb2O5	35.17
52	SiO2	57.13
53	Nb2O5	34.31
54	SiO2	62.12
55	Nb2O5	35.25
56	SiO2	54.53
57	Nb2O5	33.72
58	SiO2	65.6
59	Nb2O5	32.81
60	SiO2	44.44
61	Nb2O5	37.87
62	SiO2	107.46