Meson

 

 

            Ten to the tenth of them.  They hit a piece of platinum, at ninety-nine hundredths the speed of light, every seven seconds.

 

            But they were so small!  Over half sneaked between the platinum atoms to the other side.  Those that hit weren’t even enough to move the thing!

 

            The student sat in a prefab shed on the other side of a ten-foot concrete wall.  Every time the bell rang, to announce that the machine had completed another cycle, he glanced at a row of registers to see their count augment.  He was waiting impatiently for the one marked T0 to reach 200.  Then the electronics would automatically stop while they went out to change the film in the automatic camera looking at the spark chamber.  After they did that he could go off to the canteen for a coke and candy bar.

 

            He thought: if Pavlov turned off the bell, would I still look at the registers at the right time?   T0 did not advance with every bell.  It recorded the number of times the electronics concluded there was an event worth photographing in the spark chamber, so that a picture was taken and the film wound to another frame.  Sure, after the machine’s protons hit the platinum on the other side of the wall, there were a lot of ð+ coming through the narrow channel cut in the concrete.  There were a lot with just the right velocity for their paths to be bent through 20 degrees by the big magnet and hit the hydrogen target outside the shed, used as a source of protons for the ð+ to hit.  But most of the mesons just went through the target, and of those that didn’t only a small fraction made the kind of reaction chain they were interested in:  ð+ + p  à Ó+ +  K+, and then  Ó+ à  p + ð0.  If this happened and if the proton from the second reaction went to the left rather than the right it would head into the spark chamber.  There was a special device he didn’t understand too well to detect the K+, and it would cause the camera shutter to open and 15,000 volts to activate the spark chamber, so as to photograph what the proton did and test some theories, and also T0 would advance, every minute or so.

 

            The student yawned, and the physicist looked up from working on a circuit with a soldering iron.  “Tired?”  It was 5 AM.  They’d be there another three hours before the day shift came in.

 

            “No, I slept all day yesterday, like a log.  I’m just sick of waiting for T0.”

 

            “Take a break.  I can come get you when it’s time to change the film.”   The physicists in this group, unlike most at the Lab, treated grad students like people.

 

            “That’s OK.  Only 20 more to go.  Besides, we’ll probably have to go get some more hydrogen at the next shutdown.  The level was getting low the last I looked.”  This would involve them putting metal sheathes on their shoes to avoid collecting static electricity near the flammable hydrogen; turning various valves on or off; picking up a heavy container between the two of them and carrying it to an area outside the building; exchanging it for a full one; and retracing all the steps.  Twenty minutes, maybe more.

 

            “I guess you’re right, and I want to finish this.”  The physicist turned back to his circuit.  After an hour checking wire connections he had figured out which component was defective and was replacing it.  He didn’t bother to turn the power off for that, but just held rubber-handled forceps with one hand and a soldering iron with the other.  (He’d get a hefty shock if his hand slipped.)  One of the “shoe-string and sealing wax” men who’d been around even before the machine was built.  He’d told the student a night or two before that they had built all their own circuits when there was only an ordinary cyclotron, and he couldn’t get used to the Lab’s new production shop where you just went in and showed the foreman a schematic and he got you the circuit two days later if there were no snags.

 

            Not much on theory, though.  He asked the student, “did you go to that seminar last week where they covered the sigma decay parameters?”

 

            “Yes, very interesting.”

 

            A cough from the corner of the shed.  A technician was scanning yesterday’s film with a microfilm reader.  (He’d been told to weed out the events where the proton just went through the chamber in a straight line and didn’t interact, so that later they could look carefully at the events where it did something, without wasting time.)  They glanced at him but said nothing.

 

            “What’d they say?  Leave out the math.”

 

            “How can I leave it out?   It’s a mathematical theory, expressed in terms of Lie groups.”

 

            “Lie groups, schmee groups!  I guess you haven’t been around long enough to learn to distill what’s useful in the theoretician’s talk out of all the folderol.  OK, I suppose they’re saying it’s a question of which Lie group governs elementary particles.  So what does the asymmetry parameter in sigma decay turn out to be if the group is what they want?”

 

            “They didn’t get down to the level of calculating empirical quantities.”

 

            “Empirical, schmerical!  Those guys almost never talk to experimenters, and when they do it’s always with the bubble chamber.”  The group that operated the bubble chamber, the student had been learning, seemed to have the ear of everyone important, and its physicists always seemed to be the ones who got mentioned in popular accounts of what went on at the Lab.  But he supposed this was because their device had been invented five years earlier, whereas spark chambers were new.  But the physicists in his group never tired of telling him how worthless the bubble chamber physicists were because they had a special technical crew to operate all their equipment and never got into the nitty-gritty themselves.  “What is empirical is how many times the decay proton scatters to the right when it hits a carbon atom in one of the plates of the spark chamber compared with how many to the left.  The asymmetry parameter is the difference of these divided by their sum, and a theoretical quantity that the theoreticians are supposed to have models of.”

 

            “I think they see it as our job to calculate things like asymmetry parameters from the basic group representations themselves.  I know that means we have to learn some group theory, but don’t you agree they have a point?  After all, we’re testing their theory, and it’s the theory that is interesting, not the asymmetry parameter that derives from it.”

 

            The physicist grew angry.  “I’ll learn group theory when those bastards come down here from cloud nine and learn how to replace a bad capacitor.  Let them take a chance on getting electrocuted before they tell me I have to spend my spare time, which I don’t even have, in learning another crazy new mathematical scheme.  Anyway, we’re not doing this just to test their theory.  It was before your time, but the history is that we put in the proposal for machine time because the overthrown of parity conservation made it possible that there is a non-zero asymmetry parameter, and because we’d perfected the K+ detector, and also of course because we’d developed the spark chamber to make the observations possible.  Let the theoreticians tell us what they want us to look for or not, I don’t care.”

 

            “Sorry, I didn’t understand.”  The student decided against pointing out that the physicist could have turned the power to the circuit off while doing the soldering.  “I hope it doesn’t upset you, but the students from the bubble chamber group told me all the physicists there are learning group theory.”

 

            The physicist threw up his hands.  “That’s because they never get their hands dirty.  I suppose they have time for it.”

 

            The student was looking in his seminar notes.  “Wait a minute.  There is a formula here on how to calculate the ratio of the asymmetry parameter for Ó+ decay to that for Ë0 decay if SU(3) is the right group.  That’ll give us something to compare with experiment once we put numbers into the formula.  Didn’t you say were going to switch over to ð++ n à Ë0 + K+ next week?”

 

            The physicist’s voice lowered.  “If the lithium deuteride for the neutron target gets here on time.”

 

            “Lithium deuteride?  Oh, I get it, that’s lithium hydride but with heavy hydrogen.  But why don’t we just use liquid deuterium instead of hydrogen?”

 

            “It’s too expensive.”

 

            “I see.  Well, where’s the stuff coming from that there might be a problem?”

 

            The physicist looked around to make sure the technician was absorbed in his film scanning, and lowered his voice further.   Livermore.”  Livermore was their sister laboratory but there wasn’t supposed to be any connection because classified research was done there.  The student looked quizzically as the physicist continued, “you see, cost is no problem there, but liquid deuterium is to cumbersome to handle for their purposes, so they use lithium deuteride for a neutron source, you know, for the H-bomb.”

 

            A buzzer sounded.  T0 had reached its quota and all the registers stopped counting.  They got up to go change the film and check the liquid level in the target.

 

            The student said, “I don’t know if I like that.  I was told that we only do unclassified research here, and I believe in academic freedom.”

 

            “We do do only unclassified research, and you have academic freedom.  For instance, another student is writing his thesis on this run if it goes OK, and you’re next in line to write on the next experiment if you like the subject.  Do you want to get your degree so you can stop going through the registration line hassle every semester?”

 

            “You have a point.”

 

            The technician coughed.  They glanced at him as they went out, but said nothing.

 

 

 

(from the early 1980s)                          

 

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