|WikiProject Physics||(Rated C-class, Mid-importance)|
|A news item involving Majorana fermion was featured on Wikipedia's main page in the In the news section on 4 October 2014.|
& Neutrinos, et al
I added a bit about Majorana/Dirac neutrinos and the neutralino. HEL 17:53, 30 September 2006 (UTC)
Please check this artical: http://www.nature.com/news/quest-for-quirky-quantum-particles-may-have-struck-gold-1.10124 Rick Smit (talk) 14:33, 1 March 2012 (UTC)
- The news is wrong. They discovered evidence for a Majorana quasiparticle. That's not the same thing, and is discussed in the quasiparticle section of the article. Modest Genius talk 13:41, 16 April 2012 (UTC)
- The news is wrong. "the Majorana particle" and the Majorana fermion has already been discovered as quasiparticle in any superconductors long time ago. The Delft group was looking for protect zero-energy modes (or "Majorana zero modes"), which are not Majorana fermions. — Preceding unsigned comment added by 22.214.171.124 (talk) 16:32, 26 May 2012 (UTC)
- The thing is that quasiparticle fermionic excitations in superconductors are actually Majorana fermions. This is not contested, and while there may be no experiment dedicated to observe pairwise annihilation of those, this is rooted in the modern theory of superconductivity. I think the difference between Majorana fermions and Majorana bound states/zero modes is explained fairly well in the corresponding section. Anton.akhmerov (talk) 14:27, 27 December 2012 (UTC)--
- Guys, please try to make this article readable for non-experts. We all know that for getting fame, news articles are unclear on purpose. The wording that should be used everywhere here is truly "quasiparticle fermionic excitations" or so. The wording particle is missleading as it implicitely refers to as fundamental particles. — Preceding unsigned comment added by 126.96.36.199 (talk) 20:48, 4 October 2014 (UTC)
- This is not correct, please see the discussion in Majorana fermion#Majorana bound states as well as discussion below; both clarify the terminology matters quite accurately. In particular, it isn't appropriate to use "fermionic" when referring to Majorana zero modes/bound states. As far as particle/quasiparticle goes, I believe the article it quite accurate. If you see any place where the terms are not used correctly, fix it (but do keep in mind the fermion/bound state distinction) Anton.akhmerov (talk) 21:00, 4 October 2014 (UTC)
With regards the recent "Detection" section, I suggest the following changes:
1. "In 2014, Majorana bound states were observed for the first time by the Princeton University scientists using a low-temperature scanning tunneling microscope" --> "In 2014, evidence of Majorana Bound States was observed for the first time using a low-temperature scanning tunneling microscope, by scientists at Princeton University".
2. "Physicist Jason Alicea of California Institute of Technology, not involved in the research, said the study offered "compelling evidence" for Majorana fermions" --> "Physicist Jason Alicea of California Institute of Technology, not involved in the research, said the study offered "compelling evidence" for Majorana fermions but that "we should keep in mind possible alternative explanations—even if there are no immediately obvious candidates"".
I feel these alterations would lend the article a more objective tone, which is particularly important given its recent inclusion in Wikipedia's front page news segment. By all means, if anyone has any objections I would be happy to hear them.188.8.131.52 (talk) 13:41, 5 October 2014 (UTC)
- This is very reasonable. I would suggest an even further modification, which would make the descriptions of the Princeton and the earlier Delft experiments more comparable. Both experiments received comparable amount of attention, both provide rather detailed and very high quality measurements, but neither allows to conclude with full certainty that the observed conductance peak is due to Majoranas. Also the detection subsection shouldn't really be separate from the preceding discussion. Anton.akhmerov (talk) 17:41, 5 October 2014 (UTC)
I have made the above changes as well as "The Majorana bound states appeared..." -> "It was suggested that Majorana bound states appeared...". I also agree with Anton that it is unnatural to have the separate "Detection" section for Yazdani et al.'s work, perhaps we could get some comments on this before merging it with the section which mentions the Delft work.184.108.40.206 (talk) 18:09, 5 October 2014 (UTC)
- Since no Majorana fermions have been discovered, nowhere. Modest Genius talk 13:48, 18 April 2012 (UTC)
unsourced content moved from main article:
In fact, if we define Majorana fermions as fermions that are identical to their antiparticle, then the quasi-particles in any superconductors will be Majorana fermions (even without vortex). This is because the quasi-particles in any superconductors are fermions that can annihilate with itself. Such kind of "Majorana fermion" (ie the one that is actually introduced by Majorana) has already been found in superconductors. What people are looking for recently is actually Majorana zero mode inside of a vortex or other defects of a superconductor. The Majorana zero mode, as a zero-dimensional object, does not have Bose/Fermi statistics as defined by exchange and braiding. A vortex that carries a Majorana zero mode has a non-Abelian statistics, which is also not a fermion. So the "Majorana zero modes" are very different from the Majorana fermions introduced by Majorana. Refering "Majorana zero modes" as "Majorana fermions" can be very confusing. 220.127.116.11 (talk) 13:48, 18 April 2012 (UTC)
particle-antiparticle in superconductor
In a conventional superconductor, electrons are paired from opposite spin bands. The quasiparticles are then electrons and holes from opposite spin bands, so they are not each others antiparticle. Mathematically, the creation and annihilation operators in a conventional superconductor are related by γ_up(E) = γ^†_down(-E), so even at E=0 one has γ_up=γ^†_down, which is not the required Majorana relation γ=γ^†. (The subscripts "up" and "down" refer to the spin bands.) This is why the discovery of Majorana fermions in a superconductor is a highly unusual event, and nothing something common, as was suggested in a recent edit of the article. — Preceding unsigned comment added by Brienanni (talk • contribs) 16:24, 26 May 2012 (UTC)
- The fermions that Majorana actually introduced carry spin-1/2. So Majorana fermions carry spin-1/2. It is well known that the anti-particle of a spin-up Majorana fermions is a spin-down Majorana fermions. This is exactly the property the quasiparticles in spin-singlet superconductors. So the quasiparticles in spin-singlet superconductors are the real Majorana fermions introduced by Majorana. Since the complex conjugate of spin-1/2 representation of SO(3) is the same spin-1/2 representation, we may regard the spin-1/2 Majorana fermions as their own anti-particles. The "Majorana relation γ=γ^†" defines the Majorana zero mode, which is not the Majorana fermions introduced by Majorana. The real Majorana fermions can propagate in space, while Majorana zero mode cannot propagate. So please do not confuse a zero mode with Majorana fermions. Majorana fermions is defined very nicely in the first a few lines of this article. The second half of the article really confuses the matter, and is inconsistent with the nice definition in beginning of the article. The second half of the article should belong to a new Wiki article under a name such as "topologically protected zero-energy mode". Although such a notion was not introduced by Majorana, we can still call it Majorana zero-mode. — Preceding unsigned comment added by 18.104.22.168 (talk) 16:58, 26 May 2012 (UTC)
Let me try to clarify things a bit without math. There is a simple way to see if a particle is a Majorana fermion or not: take two of them, and ask if they can annihilate each other. In a spin-singlet superconductor, the quasiparticle excitations are a superposition of an electron from one spin band and a hole from the other spin band. Two of these excitations cannot annihilate each other, simply because you cannot fill a hole in one spin band with an electron from the other spin band. So the quasiparticle excitations of a spin-singlet superconductor are not Majorana fermions.
In the experiment mentioned in the article a spin-triplet pairing is induced, so that the quasiparticle excitations combine an electron and hole from the same spin band. Two such excitations can annihilate. In that sense one can call them Majorana fermions, even though this is a very different object than the fundamental particle introduced by Majorana. Brienanni (talk) 19:33, 26 May 2012 (UTC)
- Thank you for the explanation. My point is that the fermion introduced by Majorana does carry spin-1/2. For such kind of particle, a spin-up fermion cannot annihilate a spin-up fermion. So according to your reasoning, the fermions introduced by Majorana (just like the quasiparticle excitations of a spin-singlet superconductor) are not Majorana fermions. I do agree with you that, in the presence of spin-orbital coupling, spin is not conserved and quasiparticles in superconductor can always annihilate with themselves. We may also call those fermions Majorana fermions, despite that they do not carry spin-1/2 while the fermions introduced by Majorana do carry spin-1/2. In any case, the thing described by the Majorana relation γ=γ^† at E=0 is a zero-mode. It is not the propagating Majorana fermion. — Preceding unsigned comment added by 22.214.171.124 (talk) 20:54, 26 May 2012 (UTC)
Majorana particle same thing?
I've just read about the Dartmouth research on what they call "majoranas" or "majorana particles". Are these the same thing as described in this article? If not, I think there needs to be a new article to treat these separately. Tmangray (talk) 16:11, 1 August 2012 (UTC)
Some times, "majoranas" refers to the majorana zero-modes, which are not "majorana particles" and are not "majorana fermions". So we should remove "majoranas". Also, we should have two articles: this article about "majorana fermions" and another article about "majorana zero mode". — Preceding unsigned comment added by 126.96.36.199 (talk) 09:13, 18 September 2012 (UTC)
- You are doing it wrong. This is a right way. And make edit summaries please, 188.8.131.52, I already asked you. Incnis Mrsi (talk) 15:11, 18 September 2012 (UTC)
- While I definitely agree that Majorana zero mode is not a fermion, and should technically not be called a Majorana fermion, I would like to note that the Majorana zero modes are most frequently called Majorana fermions both in specialized as well as in popular literature. At least as it stands recently, Majorana zero mode is the most relevant meaning of 'Majorana fermion' (check e.g. google news). Due to this, I think the most reasonable decision would be to keep the articles not split, with the difference between the two closely related concepts clearly explained. --Anton.akhmerov (talk) 08:38, 30 September 2012 (UTC)
I concur: splitting the articles into two separate ones would create more confusion than clarification. It's better to just explain the different meanings of the word in one article. We already have separate articles for Majorana fermion, equation, and spinor, and merging would seem to make more sense than splitting. Brienanni (talk) 09:56, 30 September 2012 (UTC)
We should split this article into two. "Majorana fermion" and "Majorana zero mode" are not closely related concepts. If we compare "Majorana fermion" to an "apple", "Majorana zero mode" will be a "lake". We should not try to explain to people that an "apple" is a "lake" in this wiki page, as well as in other publications. — Preceding unsigned comment added by 184.108.40.206 (talk) 06:50, 5 October 2012 (UTC)
220.127.116.11, please take a look into WP:What_Wikipedia_is_not. Wikipedia articles are not intended to be read like a textbook or a scientific journal, and article titles should reflect common usage of the words. Majorana zero modes were popularized under the name 'Majorana fermions' by the media. Additionally this term is used by Kitaev, and by many after him. Regarding your remark, I agree that we shouldn't explain that an apple is a lake. We should however also not rename the "jellyfish" Wikipedia article into "Cnidaria" just because jellyfish are not fish. We might want to explain how a koala bear differs from a bear. --Anton.akhmerov (talk) 02:46, 16 October 2012 (UTC)