HomeNewsMarek Karliner On Unique Doubly-Heavy Hadrons

Marek Karliner On Unique Doubly-Heavy Hadrons

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Within the last day of the ICNFP 2022 convention in Kolympari (Greece), we might take heed to an enlightening presentation by Prof. Marek Karliner (Tel Aviv College), who’s an absolute authority on the matter of the idea of hadron spectroscopy. 
Under is a unrefined transcript of his presentation, whereby I hope I didn’t embrace too many typing errors (usually omissions, as my pace on the keyboard is not so good as it was once). As a warning, the textual content is kind of technical and never appropriate for non-physicists. The gist of it, in case you are curious however cannot delve into it, is that we’re discovering lots of fascinating new construction in particle product of quarks – an entire underlying stage beneath the Mendeleev desk of parts, extra elementary however not much less wealthy of fascinating twists. E.g., these new unique hadrons could retailer very giant binding vitality – means bigger than that we now have exploited because the 1940ies for atomic warfare in addition to for nuclear vegetation. Most likely this may stay eternally an educational commentary solely, however one by no means is aware of!
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On this presentation we are going to see what we perceive by way of idea, concerning multi-quark states. 
Quarks are elementary constructing blocks of hadrons, or to paraphrase Orwell, “All quarks are equal, however heavy quarks are extra equal than others”, within the sense that they’re simpler to investigate in experiment and idea. 

In recent times we now have seen a number of discoveries. LHCb discovered a doubly charmed pentaquark; there’s a sturdy theoretical prediction for a steady (B-B-ubar-dbar) tetraquark; and there may be a lot of so-called hadronic molecules, essentially the most conspicuous is the pentaquark found by LHCb and different states found by Belle and BESIII. We’re, in different phrases, discovering a brand new layer of the periodic desk.

We are able to summarize the scenario by saying that there’s by now fairly sturdy experimental proof for multiquark states, unique hadrons, non-qqbar’ mesons [e.g. (Q-Qbar-q-qbar), (Q-Q-qbar-qbar) states], and non-qq’q” baryons [e.g. of the kind (Qbar-Q-q-q’-q”)].

Two questiosn are key: which extra exotics ought to we count on? And the way are quarks organized inside them? For a few of the objects detected there’s a clear reply, not for all.

In September final 12 months LHCb found the unique slim doubly charmed tetraquark. It’s the first one which has two heavy quarks inside it as an alternative of a heavy quark and a heavy antiquark. They noticed a slim strcture decaying into two D0 mesons and a optimistic pion. This particle lays beneath the edge mass. There’s a query of whether or not these discoveries are backed by theoretical predictions. On this case, sure!

The brand new tetraquark is extraordinarily slim, with a width of lower than half a MeV. This may very well be of about 50 keV. The query is, is that this a four-quark bag or a molecule of D0 mesons? The partial reply to the query is offered by predictions. There have been many predictions for it, and our personal from 2017 was based mostly on the idea of a tightly sure tetraquark. However looking back it’s attainable that it’s a combination, as it’s near threshold and its quantum numbers are the identical of these of a combination.

Tightly sure tetraquarks are easier than different hadrons, as they’ve weak spin interactions and heavy quarks inside them are virtually static. That is key to correct predictions of heavy b-quark exotics.

In 2014 we utilized the theoretical approach to doubly heavy baryons like (ccu), and later to tetraquarks. In 2014 the prediction for (ccq), a state, was 3627+-12 MeV, later discovered as 3621.6+-0.4 MeV by LHCb. This gave us confidence to increase the approach to exotics. We predicted the lifetime of that particle in concordance to noticed worth. For the mass, the prediction depends on the quantity of interplay between the 2 allure quarks. For that we needed to make an assumption, quite daring on the time, that the interplay is precisely equal to half of that of a allure and anticharm, which we all know from experiment. We didn’t know the way good that assumption may very well be, regardless of it being motivated by previous expertise. A posteriori this appears very nicely glad. The binding of two allure quarks is quite giant, offering a lower of the mass of the sure state by 130 MeV. 

The identical toolbox now predicts a steady, deeply sure (B-B-ubar-dbar) tetraquark, which is 215 MeV beneath the BB* threshold. This is able to be the primary manifestly unique steady baryon.

Everyone now agrees that this explicit tetraquark is sure and the robust interplay has no open decay channels, so it’s a steady particle identical to the lambda baryon from the perspective of QCD. It will be extraordinarily fascinating when it’s ultimately found, to see what the mass is. Our prediction is 10389+-12 MeV.

In a way, the doubly heavy tetraquarks are similar to doubly heavy baruons. A baryon (C-C-q) is sort of a (C-C-ubar-dbar) tetraquark, due to fermi statistics: a color antitriplet CC binds to a color triplet q. Within the tetraquark, a (ubar-dbar) mixture is a color triplet. Then you’ve a spin-1 diquark, a spin-zero diquark, they usually bind right into a 1^+ particle. The spin of the particle is more than likely 1 and the parity is optimistic. So it will be fascinating to see what occurs with the double B tetraquark.

As quarks get heavier, the bounds in heavy quarks turns into stronger. The gap to threshold is actually zero for double allure, and it will get important beneath threshold for (b-c), and it’s deep for double backside.

CMS not too long ago noticed a  good high quality sign for the X(3872), which may be very possible a tetraquark, in lead-lead collisions. This provides optimism that we could use heavy ion collisions to see extra unique tetraquarks such because the . The cross sections in heavy ion collisions is far bigger, however backgrounds are bigger. If it may be completed for the X(3872), perhaps it may be completed for others.

To summarize, the primary manifestly unique steady hadron is T(B-Bubar-dbar). We are able to research exotich hadrons which can be hadronic molecules. There are 5 states which can be notably fascinating, they usually share the attribute of being near the 2 meson threshold, they decay into quarkonia and pions, there’s a very giant section area accessible for this decay, but regardless of this they’ve a ridiculously small width. E.g. the Z_b(10650) has a big 1 GeV of section area nevertheless it has a width of two MeV. It is a very robust trace that the particle is a hadronic molecule. Such states decay into two mesons extra typically than to quarkonium, by an element 100.

The lightest hadronic molecule product of a baryon and a meson was predicted after which found just some weeks afterwards. Later LHCb discovered three such states, near threshold. Stability was understood as a result of in an effort to decay, the allure and anticharm within the two hadrons should overlap their wavefunctions; however they’re distant, so the likelihood for making a sure quarkonium is small.

In abstract, there’s a slim (C-C-ubar-dbar) state found by LHCb; it may very well be noticed in heavy ions. It was discovered precisely the place we predicted it to be. There ought to be extra such objects. This results in predictions that there exists a doubly backside tetraquark that ought to be accessible at LHCb. Slender exotics appear to be hadronic molecules, and fairly a couple of have been seen. There are some extra states; e.g., one (C-Cbar-C-Cbar) state decaying into two J/Psi. So, there may be new thrilling spectroscopy and it’s a good instance of idea and experiment collaborating tightly, which in our area is a luxurious lately.

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