Bandwidth and Community Expectations

Derek Lowe has posted an article about X-ray lasers in chemistry, which amused me because of the following bit:

Enter the femtosecond X-ray laser. A laser will put out the cleanest X-ray beam that anyone’s ever seen, a completely coherent one at an exact (and short) wavelength which should give wonderful reflection data.

This is funny to somebody in my end of the science business, because we usually think of femtosecond lasers as have an extremely broad spectrum, not an “exact wavelength.” It’s a striking example of something I see all the time with chemists– what chemists think of as “narrow,” atomic physicists think of as “broad-band.”

Who’s right? Everybody…

The key question here is how to build up a short-duration pulse. If you want a beam of light that has a short duration in time, the only way to get that is through adding together a large number of different frequencies. You can think of this as a consequence of the energy-time uncertainty principle:

Δ E Δ t ≥ h/4 π

(though it almost makes more sense to saw that energy-time uncertainty is a consequence of the need to add frequencies to get short pulses). The uncertainty in time multiplied by the uncertainty in energy has to be greater than or equal to some minimum value, meaning that if you want a small time uncertainty, you need to accept a large energy uncertainty. Energy is proportional to frequency, so a large energy uncertainty means a large frequency uncertainty.

To make a 20fs laser pulse, as in one of Derek’s examples, you need a bandwidth of roughly 5 x 1013 Hertz– that is, the frequency uncertainty has to be at least that big, so the laser frequency is known only to +/- 5 x 1013 Hz. That’s a huge number, roughly equal to the absolute frequency of far-infrared light.

Of course, if you’re talking about a femtosecond X-ray laser, you’re dealing with a much larger base frequency– 2.9×1018 Hz for the 12 keV laser in Derek’s example. The uncertainty is a small fraction of the total– about 1.7×10-5, or not quite 20ppm. That’s pretty darn good, by everyday standards.

In my part of the scientific world, though, that’s an absolutely terrible laser. The frequency of visible light (taking 500 nm as the center of the range) is around 6×1014 Hz, so the same fractional uncertainty would correspond to a laser with a bandwidth of 1010 Hz, or 10 GHz. That’s roughly ten thousand times larger than the minimum frequency resolution I need for my experiments. I’d prefer my laser to have a frequency spread something like a million times smaller than that.

That’s why most precision spectroscopy experiments use continuous-wave lasers– the frequency spread you get from leaving your laser on all the time can be extremely small, and is usually limited by technical issues, not quantum uncertainty. Fairly ordinary diode-laser systems, the sort you can make in an undergrad laboratory, have a bandwidth of less than a megahertz (1MHz = 106 Hz), and the features we measure in our advanced spectroscopy labs are separated by only a few hundred MHz, and the natural width of those features is on the order of 1MHz. If I can get a laser to scan over 2 GHz, I call that a good day in the lab.

Chemists, on the other hand, generally show spectroscopic data with a wavelength scale measured in tens or hundreds of nanometers. If they see a feature narrower than 1014Hz, they gush about how narrow it is. I always have to make sure that my students explain the scale they’re talking about when presenting things to the summer colloquium series, because otherwise, the chemists assume we’re talking about lasers that span half of the visible spectrum.

So, whether a femtosecond laser is a single-frequency source or a broad-band source really depends on what the expectations of your particular research community are. By the standards of chemistry, it’s incredibly narrow, but for laser spectroscopy types, it’s comically broad.

(Which is not to say that femtosecond lasers are not interesting– on the contrary, this is a really exciting field. The exciting thing is not the spectral purity of the lasers, though, but the fact that the pulses are so short– you can use them to stroboscopically follow chemical reactions or electron dynamics in real time, and that’s way cool.)

Comments

  1. #1 Zack
    September 23, 2008

    If you don’t mind a basic question, what happens when you have a continuous-wave laser with a nice narrow frequency spread, and then using downstream optics you prevent it from shining on a target except in really short pulses? I imagine the frequency spread seen at the target has to go up but I don’t know what the mechanism would be.

  2. #2 Grad
    September 23, 2008

    Shouldn’t it just be the convolution of the CW spectrum with the spectrum of the pulse envelope? The pulse envelope will be very wide (consider the spectrum of a square wave for instance) so this should give you the wider bandwidth that you’re expecting.

    This answer has nothing to do with lasers, but I don’t see why the solution should be the same.

  3. #3 MRW
    September 23, 2008

    Well, some of us chemists do do *atomic* spectrometry.

  4. #4 BW
    September 24, 2008

    I’m hurt. I’m a chemist, and I used a CW, ring-dye laser to do molecular spectroscopy. When I say ‘narrow’, even physicists must agree… ;)

  5. #5 perry
    September 24, 2008

    I used to sell laser programs to radar jocks by talking about the large amount of laser bandwidth, which was comparable to or greater than their carrier frequency! They thought it was some wild assed kind of radar, and didn’t know it was light! Of course bandwidth is good, so our arguments were not wrong. The marketing was needed though as the radar jocks ruled the roost, and lasers were considered flash gordon junk!