At the HCP conference in Kyoto, we’re expecting to see some updated (and perhaps new) measurements concerning the recently discovered Higgs-like particle. Presentations from the ATLAS and CMS experiments at the Large Hadron Collider [LHC] are coming shortly.
First things first — based on the questions I’m getting from reporters and other non-experts, I need to emphasize right away that it is very unlikely that anything dramatic is going to happen here. ATLAS and CMS only just co-discovered this particle in July; the amount of data that is available now is only about twice as much as was available in July, and that is nowhere near enough for the big questions about the Higgs-like particle to be resolved. We will not know after today whether it is a Higgs at all, whether it is a Standard Model Higgs or not, or whether any particular speculative idea beyond the Standard Model is now excluded. What we are likely to see is some incremental changes in what we know.
Knowledge about nature does not come easy. We discovered the top quark in 1995, and we are still learning about its properties today — there were over a dozen talks about the top quark earlier in this conference. And we will still be learning important things about the Higgs during the coming few decades. We’ve no choice but to be patient.
But here are the new results (below, SM is short-hand for “Standard Model”); see here for a discussion of the main July results:
ATLAS Higgs decays to lepton, anti-lepton, neutrino and anti-neutrino (using 13 inverse femtobarns of 8 TeV data from 2012, more than twice what they had in July; 2011 data is not used, since, as in July, the method used is different from the method used in 2011.) Excess observed roughly consistent with an SM-like Higgs; if one assumes Higgs mass of 125 GeV/c² and SM-like production modes, the rate for this process is 1.5 ± 0.6 times the SM expectation. This is a
good bit smaller than was obtained in July [1.9 ± 0.7 assuming 126 GeV/c²] for the 5 inverse femtobarns of 2012 data (not combined with 2011 data). It isn’t clear yet whether this is purely due to statistics, or whether there were also changes in the background estimates (the speaker seemed to indicate there were.)
CMS Higgs decays to lepton, anti-lepton, neutrino and anti-neutrino (using 12 inverse femtobarns of 8 TeV data along with 7 TeV data from 2011.) No unexpected excess across mass range seen except roughly in low Higgs mass region, where excess consistent with 0.74±0.25 of SM expectation if one assumes a 125 GeV/c² Higgs (3.1 standard deviations significance away from no Higgs.) The central value has climbed slightly since July; the error has gone down somewhat. [Reading off a plot from the CMS paper, it looks as though the July result was something like 0.6±0.4 of SM expectation.] A couple of other relatively minor results shown.
ATLAS Higgs decay to two lepton/anti-lepton pairs: apparently no update at this conference.
CMS Higgs decays to two lepton/anti-lepton pairs (using 12.2 inverse femtobarns of 8 TeV data along with 7 TeV data from 2011.) Old result from July was about 0.7±0.4-ish of SM expectation. Now have 2:1 signal over background; expect 6.5 background, 12.5 signal, for a total of 19 expected; 17 are observed. Using kinematics, find 4.5 sigma detection (compare 3.2 sigma in July). Find 0.8 + 0.35 – 0.28 of SM expectation.
Mass 126.2 ± 0.6 ± 0.2 GeV/c² .
No sign of any heavy Higgs-like particles.
Measurement of spin and parity attempted — claim to exclude pseudoscalar [odd-parity] alternative to scalar expectation; pseudoscalar hypothesis has only 2.4% probability (about 2.5 standard deviations) of being consistent with the data. This makes the new particle, in this respect, even more consistent with a typical Standard Model-like Higgs particle.
ATLAS Higgs decay to two photons: no update at this conference
CMS Higgs decay to two photons: no update at this conference
[Obviously the big question: why no photon updates from either experiment, and no four-lepton update from ATLAS?]
ATLAS Higgs decay to a tau lepton/anti-lepton pair: based on 2011 data and 13 inverse femtobarns of 2012 data (previously ATLAS only had presented a result for 2011 data, so this is a big jump forward — almost four times the data, plus many improvements, I am sure.) Result: neither evidence for, nor exclusion of, the new particle decaying to tau/anti-tau. Rate is at 0.7 ± 0.7 times SM expectation, consistent both with 0 (no Higgs decaying this way) and with 1 (SM Higgs decay). The central value for the Gluon Fusion process is close to 2.4 times expectation and that of Vector Boson Fusion is close to zero, but the errors are huge. Large uncertainties make it impossible to conclude anything yet except that this process cannot be in significant excess beyond SM expectation.
CMS Higgs decay to a tau lepton/anti-lepton pair: based on 2011 data plus 12 inverse femtobarns of 2012 data (previously CMS had presented a result for 2011 and July 2012 data, so this is naively a small step forward — not even twice the data. But what about possible improvements?) Improved missing energy reconstruction; improves resolution and pile-up dependence, which has a big positive impact on the measurement. New event requirements, particularly on events that might come from Vector Boson Fusion. Big changes in the events that actually come into the analysis. Result: 0.72±0.52 times the Standard Model expectation, amusingly almost the same as ATLAS! And similarly, consistent both with 0 (no Higgs decaying this way) and with 1 (SM Higgs expectation).
In short, all that hullabaloo about a deficit in the rate for Higgs decays to tau/anti-tau was much ado about nothing. With a better (and very significantly changed) measurement with more data, it’s gone, at least for now. Well, you were warned: this is a very hard measurement, and clearly we will not have a precise measurement of the rate for Higgs decaying to tau/anti-tau for some years to come. Think 2016 for something convincing.
ATLAS Higgs produced with a W or Z and decaying to a bottom quark/antiquark pair: 2011 data plus 13 inverse femtobarns of 2012 data. Many big improvements, but… Result: -0.4 ± 0.7 (statistical) ± 0.8 (systematic) times SM expectation; not at all significant yet.
CMS Higgs produced with a W or Z and decaying to a bottom quark/antiquark pair 2011 data plus 12 inverse femtobarns of 2012 data. Result: 1.3 +0.7-0.6, two standard deviations away from zero. (Not sure why CMS has much smaller errors than ATLAS, but CMS is doing more with boosted-Higgs techniques…)
Also, reanalysis of search for Higgs produced along with a bottom quark or antiquark (arising in speculative models with more than one Higgs particle) shows no signal in the region where a hint was seen at the Tevatron.
Combination of CDF and DZero (from the Tevatron collider) Higgs produced with a W or Z and decaying to a bottom quark/antiquark pair: moderate update from summer, claim to find rate equal to 1.56 ±0.72 times SM expectation, a bit more than 2 standard deviations away from zero (smaller than it was before, so both less significant than it was in July and also less in conflict with LHC results.)
Strength of interaction of the new particle with W and Z particles compared to expectation for a generic Higgs
- ATLAS: W strength/Z strength = 1.07 +0.35 – 0.27 of Higgs expectation
- CMS: W strength/Z strength = about 0.98 +- about 0.2 of Higgs expectation [my reading of a plot; precise numbers not given in CMS talk]
Summing up — ATLAS, CMS and the Tevatron have updated some of their measurements (though a few updates are noticeably missing). The main new result that there is now considerable evidence that the new particle is not a pseudoscalar (i.e. negative parity) particle, which means it remains consistent with a Standard Model-like Higgs particle. Meanwhile there are no significant deviations from the expectations for a Standard Model-like Higgs particle — the ones that were hinted at before have either evaporated (for now) or remain unchanged. Also, there is now increasing evidence that the strengths with which this particle interacts with W and with Z particles are in just the ratio one would expect for a Higgs particle of some type; this is a crucial test of whether it is a Higgs or not. However, many of the measurements are still very imprecise, and many other measurements haven’t even been attempted yet. It will be many years before we will have the precision, and the broad range of additional studies, that are necessary for us to draw deep conclusions about nature.
[And no, for those who just can’t stop thinking about supersymmetry — there’s nothing in the updated results that has a significant new implication for or against supersymmetry.]