The Photonics Spotlight
The Photonics Spotlight – associated with the Encyclopedia of Laser Physics and Technology – is a “blog” (web log) with the purpose of highlighting interesting news and useful information in the area of photonics, particularly laser technology and applications. The content can be related to particularly interesting scientific papers or to other forms of publications, reporting for example cute new techniques, special achievements, or useful hints.
Note that the Spotlight articles (as well as those of the Encyclopedia) are citable. Permanent links are given for each article.
This blog is operated by Dr. Rüdiger Paschotta of RP Photonics Consulting. Comments and suggestions are welcome. The news items are definitely not available for advertising, but advertisers can order banners on the right column of this page.
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Simulation Software: Use Commercial Products of Home-Made Software?
Posted on 2012-02-03 as a part of the Photonics Spotlight.
Permanent link: http://www.rp-photonics.com/spotlight_2012_02_03.html
Author: Dr. Rüdiger Paschotta, RP Photonics Consulting GmbH
The article helps to find a rational decision on this issue, considering a number of important aspects, such as the time to get started, the issue of software validation, flexibility and user friendliness.
When you need to do some simulation and modeling, a basic question often arises: should you develop your own software to do this, or better take a commercial product?
I am admittedly not neutral on this issue, as I am obviously happy if people decide to buy my own modeling software, such as
- RP Fiber Power for fiber laser and amplifier design
- RP Resonator for resonator design (mainly for bulk lasers)
- RP ProPulse for pulse propagation simulations, e.g. in mode-locked lasers, regenerative amplifiers and fibers
Anyway, I can contribute some thoughts on that question which may help you to arrive a rational conclusion. It turns out that a number of aspects should be considered in this context.
Time to Get Started
In most cases, the time to get familiar with some commercial software is quite small compared with the time to develop some software oneself. So in this respect, commercial software often has a big plus. However, it can also turn into a big waste of time if you start with some software which works for the simple cases but later out turns out not to be sufficiently flexible (see below) so that you still have to turn to something else later on.
Is the Code Correct?
That can be a big issue. Anyone can easily make errors when developing simulation and design software, and obviously such errors can severely hurt you. For example, you may be mislead by them and subsequently try out things in the lab which cannot work.
Definitely, any such software should be carefully validated before it is used. This is a process which takes substantial time and experience. (I have actually devoted another article to the problem of software validation). If you develop such software yourself, you may be under pressure to get results quickly and do only some superficial testing. On the other hand, you may find it hard to trust some anonymous developer at some software company. So preferably you will use software developed by somebody who is known to be most competent, experienced and careful.
User Friendliness and Flexibility
Obviously, it will help you if a software is user friendly, as this makes your work easier, more efficient and also safer. (The risk of introducing errors in the software handling is much greater if you don't have a well engineered user interface!) On the other hand, you want something really flexible, working also in more sophisticated cases, as it is no point to do only some simple things with a software and have no solutions for the most interesting cases.
Unfortunately, it is not easy to achieve user friendliness and flexibility, let alone to combine them in one product. Some products come with a really beautiful graphical interface, where you simply put together some model with a few mouse clicks. However, this approach tends to severely limit your flexibility, as some general structures are hard-coded and cannot be changed. For example, there are optimizations where you can only adjust parameters but not the general type of the used figure of merit. In other cases, you may easily set up some chain of optical components, but cannot deviate from a linear chain.
As a more concrete example, imagine that you want to simulate the operation of a regenerative amplifier, where you inject a pulse, let it circulate say 50 times, then eject it and replenish the energy by pumping the crystal for some time. Now you may want to vary some parameter (e.g., the initial pulse energy) and check out what you get after multiple amplification/pumping cycles. If you have to arrange all that manually for each parameter value, it may drive you crazy before your results are complete.
Scripting vs. Forms and Graphical User Interfaces
Initially, my software always had to be controlled by writing scripts, containing certain commands and mathematical expressions. That gave the user the full flexibility, but required some initial investment to get acquainted to the script language. Well, starting out with some demo scripts one gets into it quite quickly, but some potential users were concerned to spend too much time. Other companies offered software with a purely graphical interface, which was easier to get started with, but totally lacked flexibility. I then considered to offer forms in addition, but I still didn't want to confront the user with a hard choice between two totally different approaches, each one still having its characteristic limitations. I finally managed to find the right combination, best implemented in my RP Fiber Power software:
- You can work with simple forms, but you can put mathematical expressions instead of plain numbers into most form fields. For example, this allows you to specify any time-dependent powers, and not only choose from some given selection of simple temporal shapes.
- When a simulation is executed, the software writes a script based on your form inputs and then executes that. If you do really complicated stuff, just go as far as possible with the forms and then refine further the automatically generated script - which is much easier than starting from scratch with script programming.
- The forms also offer various opportunities to inject additional script code for special purposes such as adding a special graph or certain calculated labels to some diagram, or to import some input data from files.
This approach nicely combines the simplicity of filling out forms with the great flexibility of scripting. It even avoids the hard break when moving from forms to scripting.
Obviously, such features are really difficult to implement. You surely cannot invest that much time when developing some own code for a project, and many software companies cannot offer it either.
Can the Next Colleague Take Over?
A typical situation at universities (but also in some companies) is that some clever guy puts together some ingenious programs which allow him to efficiently to do his job. Only, when he later leaves the place, nobody can take this over, as nobody will understand his source code within a reasonable time. So the next guy will start from scratch. Obviously, this is very inefficient in the long run, and leads to periods of time where the productivity of the team is severely reduced. When working with some well engineered software, this won't happen: the work is not done by tweaking the source code, but on a level which is much easier to access. Also, technical support is available to sort out any remaining problems. So the continuity is much more easily maintained.
Some Conclusions
There can be very good reasons to stick to home-made code, particularly when available commercial software is too limited in its flexibility. If it is not really usable to do the job also in more complicated cases, don't bother to start with it.
On the other hand, if you know a trustworthy commercial software combining a convenient user interface with high flexibility, it is hard to defend the do-it-yourself approach. That will take much more time, will presumably lead to something which is more prone to errors (both in the code and during the handling), and makes it difficult to transfer the job to somebody else. Well, if you want to force your boss to keep you employed forever, this may be the way to go! Your boss however, should want to avoid that, even if it costs some money upfront, as it would be silly to ignore the difference in productivity. One cannot spend that much time on developing software before making this effectively more expensive than buying a commercial software. After all, it is obviously more efficient if one guy (or team) makes an excellent software to be used by many, compared with everyone implementing a quick-and-dirty solution himself.
Sometimes, people say that it would great to have some good commercial software, but they cannot afford it. The question is then whether they can afford to work in less efficient ways, such as paying salaries over long times for the same amount of work and not fully utilizing some expensive infrastructure. Obviously, if you are under pressure to be economically efficient, you should choose the most efficient solution rather than the one which requires the smallest possible initial investment. If you can't, you may get out of business some time later.
Kerr-lens Mode-locked Thin-disk Laser
Posted on 2011-12-23 (revised on 2011-12-28) as a part of the Photonics Spotlight.
Permanent link: http://www.rp-photonics.com/spotlight_2011_12_23.html
Author: Dr. Rüdiger Paschotta, RP Photonics Consulting GmbH
Ref.: O. Pronin et al., “High-power 200 fs Kerr-lens mode-locked thin-disk oscillator”, Opt. Lett. 36 (24), 4746 (2011)
The history of mode-locked thin-disk lasers has a curious twist. Originally, there was a patent saying that semiconductor saturable absorber mirrors (SESAMs) would be unsuitable for mode locking of such lasers; only Kerr lens mode locking (KLM) would work. However, a research team at ETH Zürich (which I supervised at that time) then demonstrated the first mode-locked thin-disk laser exactly with a SESAM (J. Aus der Au et al., Opt. Lett. 25 (11), 859 (2000)), while the attempts of another group with Kerr lens mode locking apparently failed. 11 years later, there is now the paper by Oleg Pronin et al. at the Max-Planck Institute for Quantum Optics in Garching, Germany (see the reference above), reporting a Kerr-lens mode-locked thin-disk laser. It is based on an Yb:YAG thin-disk laser head, as are most other mode-locked thin-disk lasers so far. There is a version with KLM alone, and one which uses a (weak) SESAM in addition for self-starting mode locking and better stability.
What makes that result particularly interesting is the very short pulse duration – down to 200 fs, or 270 fs with a higher output power of up to 45 W. Previously, mode-locked thin-disk Yb:YAG lasers could only be operated with pulse durations around 700 to 800 fs, because only there we obtain a helpful effect from spatial hole burning in the disk (see R. Paschotta et al., Appl. Phys. B 72 (3), 267 (2001)). Forcing such a laser to a pulse duration like 200 fs requires a saturable absorber with larger modulation depth (because spectral filtering by the limited gain bandwidth). With a SESAM, this can lead into trouble with Q-switching instabilities and with excessive heating. KLM does not involve additional heating and may have saturation characteristics which make it easier to avoid Q-switching instabilities.
Another interesting point will be whether a Kerr lens mode-locked thin-disk laser can be sufficiently stable for making a commercial product. One may say that titanium–sapphire lasers with KLM have been sold for many years, but that alone would not be fully convincing, since (a) this is mostly for applications in research, where the demands on stability are lower than for industrial applications, and (b) the issues may be more serious for the large effective mode areas required in a high-power laser.
Are Compact Resonators More Stable?
Posted on 2011-06-10 as a part of the Photonics Spotlight.
Permanent link: http://www.rp-photonics.com/spotlight_2011_06_10.html
Author: Dr. Rüdiger Paschotta, RP Photonics Consulting GmbH
Ref.: encyclopedia articles on optical resonators, alignment sensitivity, resonator design
One of the widespread myths in photonics is that the more compact an optical resonator (e.g., a laser resonator) is, the more robust and stable it will be. As with nearly every myth, there is some truth in it. Surely, it is easier to make a compact mechanical setup stable and thus to prevent vibrations, for example, from having strong effects on the alignment. However, the sensitivity of the resonator to small misalignments (called alignment sensitivity) is in fact often increased when the resonator length is reduced. As a result, the overall robustness may be decreased, despite the tentatively more robust mechanical properties.
A Simple Example
A simple example demonstrates that point convincingly, without using complicated calculations or software. Imagine that we need a simple linear resonator, consisting of a plane mirror and a concave (focusing) mirror. The latter must have a suitable radius of curvature such that the fundamental mode has a certain beam radius in the resonator. (For a laser resonator, the right mode size is often very important for obtaining good beam quality, a high slope efficiency, etc.) The shorter the resonator, the weaker will be the required curvature of the focusing mirror.
Now imagine a small angular misalignment of the curved mirror, while the plane mirror remains fixed. This misalignment simply makes the resonator mode shift transversely to a new position, where it is again perpendicular to the surface of the curved mirror. (Obviously, the mode always has to be perpendicular to both mirror surfaces.) It becomes clear now that a weak curvature – as needed for a short resonator – implies a larger transverse shift of the mode for a given misalignment angle. And this is bad. Consider, for example, such a shift in the resonator of an end-pumped laser: it will decrease the overlap between the laser beam and the pumped region.
The Problem is Common
One may believe that the discussed example is only an unusual pathological case, but it isn't: any type of resonator will exhibit this problem if you try to make it shorter and shorter while maintaining the mode size. Fundamentally, you are then pushing the resonator into a regime where the effect of diffraction becomes weak (simply because there is little propagation distance), mirror curvatures have to become correspondingly weaker, and the alignment becomes very sensitive. It is not good to have a resonator length far below the Rayleigh length of the intracavity beam.
A common case is that of a Q-switched laser, which we like to be compact partly because this gives us the shortest pulse duration. The mode size, however, cannot be reduced arbitrarily, because we often need to extract energy from the whole pumped volume in the laser crystal without employing higher-order modes (which would spoil the beam quality), and possibly because a too small mode leads to optical damage of resonator components. We then run exactly into that problem: the resonator will be compact and mechanically stable, but its alignment sensitivity may nevertheless be high.
Well, you might think, this simply means that we need a very good mechanical setup, and initially align that very carefully. However, misalignment is not only caused by mechanical tilts, but also by thermal effects such as thermal lensing in the laser crystal. Even exceptional mechanical stability can therefore not fully solve this problem.
A Deep Understanding Helps
Even though the problem is fundamental and cannot be eliminated with a simple design trick, it is essential to precisely understand such issues when designing laser resonators. First of all, one needs to be aware of the problem, and know that compactness is not necessarily the key to stability. Furthermore, one can at least select the best possible laser resonator design. What “best possible” means, depends on the concrete requirements. Therefore, finding the best solution is only possible after carefully analyzing these requirements, including the relative importance of various design goals. Having done this, one can decide for a type of design and finally employ advanced laser resonator design software to optimize the design.
Older Postings
- 2011-05-28: Explanation for the Mode Instability in High-power Fiber Amplifiers with Few-mode Fibers
- 2011-03-13: What if Solid-State Laser Transitions Would Be Much Stronger?
- 2011-02-10: Fiber Lasers: More Difficult to Design than Bulk Lasers
- 2011-01-05: Femtosecond Fiber Amplifiers: Unlimited Peak Power?
- 2010-09-02: Why LEDs are Energy-efficient, and Why They Could Well Increase Energy Consumption
- 2010-07-27: Special SESAMs for Mode-locked High-power Lasers?
- 2010-07-12: Laser Development: Get an Expert Early on!
- 2010-06-09: Poor Man's Isolator
- 2010-05-14: Plagiarism, Exploiting the Encyclopedia of Laser Physics and Technology
- 2010-04-26: Resolution and Accuracy of Measurements
- 2010-04-16: Why Large Mode Area Waveguides Do Not Work for Laser Diodes
- 2010-04-08: Creating a Top-hat Laser Beam Focus
- 2010-03-22: All-in-one Concepts versus Modular Concepts
- 2010-03-15: Spatial Walk-off and Beam Quality in Nonlinear Frequency Conversion
- 2010-03-09: Nonlinearities in Fiber Amplifier Modeling
- 2010-03-03: Thresholds for Nonlinear Effects in Fiber Amplifiers
- 2010-02-26: New Scientific Paper: Timing Jitter and Phase Noise of Mode-locked Fiber Lasers
- 2010-02-06: Scientific Conferences and Publications: Emphasize Device Performance or Insight?
- 2010-01-29: Far From Maturity: The Photonics Industry
- 2010-01-22: Pumping Fiber Lasers with Fiber Lasers
- 2010-01-11: Beams of Laser Pointers: Visible in Air?
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- 2009-12-13: Johnson–Nyquist Noise in Photodiode Circuits
- 2009-12-08: Increased Output Power of a Laser with Forced Tuning
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- 2009-09-01: Fresnel Reflections from Double Interfaces
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- 2009-08-14: Progress on Green Laser Diodes
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- 2009-07-23: Submit Photographs for the Encyclopedia of Laser Physics and Technology
- 2009-07-21: Signal-to-Noise Ratio and Measurement Bandwidth
- 2009-07-09: Gain-guiding Index-antiguiding Fibers
- 2009-06-29: Doing Things Properly: It's the Economy, Stupid!
- 2009-06-23: Coherence – a Black-or-White Issue?
- 2009-06-08: Prizes of the European Physical Society
- 2009-06-02: 5 Years of RP Photonics Consulting
- 2009-05-22: Interference Effects with Imbalanced Intensity Levels
- 2009-05-13: The Minimum Time–Bandwidth Product
- 2009-04-28: SPIE Field Guides
- 2009-04-19: Last Chance to Get the Encyclopedia of Laser Physics and Technology Cheaper
- 2009-04-17: Miniature Laser Projectors – The Next Big Laser Thing?
- 2009-04-06: Laser Pointers in Soccer Games: Not Necessarily Harmless
- 2009-04-05: Stability of Resonators – an Ambiguous Term
- 2009-03-19: Scientific Progress: not as Straight a Process as it Seems
- 2009-03-07: Complicated Pulse Shapes from Q-switched Fiber Lasers
- 2009-03-02: User Interfaces for Simulation Software
- 2009-02-13: Laser Beam Deflections: The Angle–Diameter Product
- 2009-01-12: Chaotic Lasing Generates Random Numbers
- 2009-01-05: Extremely Long Mode-locked Fiber Laser
- 2008-12-16: Why Fiber Amplifiers, not Fiber Lasers?
- 2008-11-25: The Gouy Phase Shift Speeds up Light
- 2008-11-08: Validating Numerical Simulation Software
- 2008-10-20: Rate Equations – An Example for Stiff Sets of Differential Equations
- 2008-10-03: Wavelength-Tunable Lasers: Does the Tuner Degrade the Power Efficiency?
- 2008-09-24: Decoupling Pulse Duration and Pulse Energy
- 2008-09-10: Unpolarized Single-Frequency Output
- 2008-08-28: Photographs for the Encyclopedia of Laser Physics and Technology
- 2008-08-15: Print Version of the Encyclopedia of Laser Physics and Technology
- 2008-07-26: Beat Signals with Zero Linewidth
- 2008-07-13: The Simplified History of the Michelson–Morley Experiment
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- 2008-06-20: All-in-One Ultrafast Laser Systems
- 2008-06-13: Heisenberg's Uncertainty Principle and the Transform Limit
- 2008-06-06: Fiber Lasers Which Are No Fiber Lasers
- 2008-05-25: Einstein and the Laser
- 2008-05-13: Easier Self-Starting Passive Mode Locking for Short Lasers
- 2008-05-05: Length of a Photon
- 2008-04-28: Different Kinds of Polarization
- 2008-04-22: Abused Photonics Terms: Coherence
- 2008-04-15: Abused Photonics Terms: Modes
- 2008-04-02: Solitons: Lower Dispersion, Stronger Dispersive Effects!
- 2008-03-26: Mode-Locked Lasers: Lower Average Powers in Shorter Pulses
- 2008-03-17: Ultrafast Fiber Lasers: Re-Inventing Mode Locking
- 2008-03-10: Automatic Phase Matching
- 2008-03-04: What is a “High” Laser Beam Quality?
- 2008-02-22: Launching Light from a Bulb into a Single-Mode Fiber
- 2008-02-14: How Laser Development Can Go Wrong
- 2008-02-12: Factor 2 in the Equation for Cross-Phase Modulation
- 2008-02-03: Quantifying the Chirp of Ultrashort Pulses
- 2008-01-27: Beam Quality in Second-Harmonic Generation
- 2008-01-14: Frequency Doubling: Long Pulses Cause Trouble
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- 2007-12-18: The Role of Laser Safety Goggles
- 2007-12-11: The Idler Wave - Essential for Parametric Amplification and Oscillation
- 2007-12-03: New Paper on Power Scaling of Lasers
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- 2007-10-31: Thermal Equilibrium in Laser Crystals
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- 2007-07-06: Promoting Dangerous Practices in Laser Labs
- 2007-07-01: Nonsensical Regulations Undermine Laser Safety
- 2007-06-24: The Plague of a Narrow Emission Linewidth
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- 2007-05-19: Why Strong Birefringence in Fibers Helps
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- 2007-04-28: Easier Launching into Fibers with Large Mode Area?
- 2007-04-16: Questions and Answers on Shot Noise
- 2007-04-01: The Ideal Pump Intensity Distribution in an End-Pumped Solid-State Laser
- 2007-03-23: Explaining the Nature of Photons to Lay Persons
- 2007-03-16: Time To Market and the Economics of Laser Development - or How to Cause Great Financial Damage without Spending Money
- 2007-03-11: Divided-Pulse Amplification
- 2007-03-09: The Trouble with Crystal and Coating Damage
- 2007-03-05: More Efficient Frequency Doubling with Shorter Pulses?
- 2007-02-26: No Laser, no Result?
- 2007-02-22: Lossy Laser Cavities
- 2007-02-16: The Science of Biophotons
- 2007-02-09: Papers Reporting Yet Another Laser Crystal
- 2007-02-04: Continuing Struggle for Larger Fiber Mode Areas
- 2007-01-27: Noise Figure of Amplifiers
- 2007-01-21: Operation Far Above Threshold
- 2007-01-15: Origins of Heating in Laser Crystals
- 2007-01-09: The Myth of Fiber-Optic Polar Bears
- 2007-01-05: Why the Encyclopedia of Laser Physics and Technology is Successful
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- 2006-12-16: Dangerous Green Laser Pointers
- 2006-12-09: The Laser Industry - High Tech or Low Tech?
- 2006-12-03: Diffraction in Optical Fibers
- 2006-11-28: The Role of Diffraction in Optical Resonators
- 2006-11-21: The Resonator Mystery
- 2006-11-16: Laser Models - not Always Useful
- 2006-11-04: Nd:YVO4 Laser with Polarization-Independent Pump Absorption
- 2006-11-02: Reflection Spectrum of Tilted Dielectric Mirrors
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- 2006-10-16: Using a Current Amplifier for Optical Power Measurements and Recording with a Photodiode
- 2006-10-15: Fivehundred Articles in the Encyclopedia of Laser Physics and Technology
- 2006-10-09: Correct Specifications for Laser Noise - Valuable but Hard to Obtain
- 2006-10-04: Higher-Order Modes of Fibers: a Solution for Single-Mode Guidance with Large Mode Area?
- 2006-10-01: Stability Zones of Laser Resonators
- 2006-09-29: Frequency Dependence of the Conversion Efficiency for Frequency Doubling
- 2006-09-22: Coherence Length of Ultrashort Pulses
- 2006-09-21: Power Scaling Limits of Optical Parametric Amplifiers
- 2006-09-16: Q-switched Lasers: YAG versus Vanadate
- 2006-09-06: Quenching Degrades the Efficiency of Some Ytterbium-Doped Gain Media
- 2006-09-03: Single-Frequency Operation Stabilized by Spatial Hole Burning
- 2006-09-03: Resolution of Conundrum: Threshold Power for Parametric Nonlinear Interactions
- 2006-09-01: Test Yourself with the Photonics Quiz
- 2006-08-23: Lasers with Nonlinear Input-Output Characteristics
- 2006-08-20: Lower Noise from Longer Lasers
- 2006-08-18: Resolution of Conundrum: No Magnetic Field on the Axis of a Coil
- 2006-08-15: The Effect of a Double Pass in a Frequency Doubler
- 2006-08-12: Understanding Quasi-Three-Level Lasers
- 2006-08-10: Single-Mode Fibers with Large Mode Areas
- 2006-08-01: Lasers Disturbed by Vacuum?
- 2006-07-30: Threshold Power for Parametric Nonlinear Interactions
- 2006-07-24: Beam Distortions in Laser Cavities
- 2006-07-23: Single-Atom Lasers
- 2006-07-22: No Magnetic Field on the Axis of a Coil?
- 2006-07-21: Photonics and Laser Technology Blogs – Where Are They?
- 2006-07-16: Spontaneous Emission and Amplifier Noise
- 2006-07-14: Lasers Like it Cool
- 2006-07-10: Strength of Thermal Lensing Effects
- 2006-07-05: Laser Design: Side Product or the Basis of Laser Development?
- 2006-07-01: Lifting the Confusion Concerning Doping Concentrations
- 2006-07-01: Characterizing a Cavity with a Frequency Comb
- 2006-07-01: With Wavelength Combs to Picometer Resolution
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