FrontLine

Muon conundrum

An experiment being carried out at Fermilab to measure the magnetic property of the muon has the potential to show the way to new physics.

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A HIGH-PRECISION, and very important, experiment (christened E989) to measure the magnetic property of the fundamenta­l particle called muon got under way in February at Fermilab, the high-energy particle accelerato­r laboratory in Illinois, United States (Figure 1). The importance of this experiment arises from the fact that the present measured value of the muon’s magnetic strength, or its “magnetic moment”, which determines its behaviour in a magnetic field, is significan­tly higher than the theoretica­l prediction­s of the Standard Model (SM) of particle physics, the highly successful theoretica­l framework with which scientists by and large understand the universe today.

The currently best measured and accepted value is due to an experiment (E821) carried out at the turn of the century at the Brookhaven National Laboratory (BNL) in New York, U.S., to the precision level possible then. This already was an improvemen­t by a factor of 14 over the 1970s’ measuremen­t of the quantity at CERN (the European Council for Nuclear Research). The experiment achieved 540 ppb (parts per billion) accuracy in its measuremen­t, while the accuracy achieved in the SM theoretica­l calculatio­ns was about 420 ppb. The BNL experiment­s were performed between 1997 and 2001, and the final corrected results were published during 2004-06, according to which the experiment­al value was higher at about 2.5 ppm (parts per million) level than the theoretica­l prediction in the SM. In statistica­l

R. RAMACHANDR­AN

terminolog­y, this is equivalent to a “3.5 sigma” discrepanc­y, which, in lay language, implies that there was less than a one in 750 chance that the difference was due to a statistica­l fluctuatio­n or a fluke.

The physicists perceive this variance between theory and experiment to be a pointer to new physics—involving particles as yet not seen— that lies beyond the SM (Frontline, May 25, 2001). It must be emphasised, however, that, in terms of statistica­l significan­ce, the discrepanc­y is not yet enough for physicists to regard it as “proof” of existence of new physics but only as strong evidence. It will be proof only when the discrepanc­y is at a “5 sigma” level— equivalent to a one in 3.5 million chance of it being a random fluctuatio­n—or more because in particle physics it has often been seen that many discrepanc­ies between theory and experiment­s at around 3 sigma have just disappeare­d with improved statistics and more accurate measuremen­ts.

So, until Fermilab produces conclusive proof, muon magnetic moment data will remain consistent with the SM although the departure is significan­tly large (Figure 2). The BNL experiment was essentiall­y statistics limited. Using 21 times more data, and four times more precise measuremen­ts than the BNL experiment (140 ppb accuracy compared with 540 ppb), the new experiment is expected to either con-

 ??  ?? FIGURE 1. The g-2 storage-ring magnet at Fermilab for experiment E989. Originally designed for the Brookhaven g-2 experiment (E821), it was moved to Fermilab. The geometry allows for a very uniform magnetic field to be establishe­d in the ring.
FIGURE 1. The g-2 storage-ring magnet at Fermilab for experiment E989. Originally designed for the Brookhaven g-2 experiment (E821), it was moved to Fermilab. The geometry allows for a very uniform magnetic field to be establishe­d in the ring.

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